This study measures the spatial clustering of submillimeter galaxies (SMGs) at redshifts of 1-3 using data from a submillimeter survey of galaxies in the Extended Chandra Deep Field South. The authors detect clustering between SMGs and galaxies at over 4 sigma significance. They estimate an autocorrelation length of 7.7-2.3 h-1 Mpc for SMGs, corresponding to dark matter halo masses of log(Mhalo[h-1 M⊙]) = 12.8-0.5. Based on simulations, the descendants of z=2 SMGs are expected to be massive elliptical galaxies in moderate- to high-mass groups today.
The document summarizes a study that uses strong and weak gravitational lensing to analyze the mass distribution of 28 galaxy clusters. Key findings include:
- The concentration parameter cvir is found to steeply decrease with increasing mass, approximately following cvir ∝ Mvir-0.59±0.12, consistent with theoretical predictions for high-mass clusters but observationally inferred concentrations are higher for lower-mass clusters possibly due to baryon cooling effects.
- Stacking weak lensing shear profiles also supports a steep mass-concentration relation.
- Stacking weak lensing shear maps with position angle information from strong lensing indicates significant ellipticity of the mean mass distribution, with a best-fit ellipticity
This document reports on evidence for spatial variation in the fine structure constant α from observations of quasar absorption spectra. A sample of 153 measurements from the ESO Very Large Telescope (VLT) probing a different region of the universe suggests α was larger in the past, opposite to previous findings from the Keck telescope. Combining the two datasets reveals a significant spatial dipole in α, with the maximum variation in the direction of right ascension 17.3 hours, declination -61 degrees. Detailed analysis found no systematic effects that could mimic this result.
Science with small telescopes - exoplanetsguest8aa6ebb
The search for extrasolar planets has become one of the most attractive problems in modern astrophysics. The biggest observatories in the world are involved in this task as well as little amateur instruments. There is also a huge variety of astronomical methods used for their investigation. Here I present the projects for searching for exoplanets by transit method and our observations of the planet WASP-2b. We observed a transit on 3/4 August 2008 with a 354 mm Schmidt-Cassegrain Celestron telescope and CCD SBIG STL 11000M camera. By precise photometry made using MaximDL software we obtained the light curve of the star system. Decrease of brightness by 0.02m is detected. Analyzing our data we estimate the radius of the planet and inclination of its orbit. Our results are in good correlation with the published information in literature.
A massive protocluster of galaxies at a redshift of z<5.3Sérgio Sacani
This document describes the discovery of a massive protocluster of galaxies located approximately 1 billion years after the Big Bang (redshift of z=5.3). The protocluster contains overdense regions of massive galaxies extending over 13 megaparsecs. It contains an extremely luminous starburst galaxy with large molecular gas reserves and a luminous quasar. Together, these objects place a minimum total mass of over 4×1011 solar masses in this early cluster, consistent with cosmological simulations of the earliest galaxy clusters. This discovery provides evidence for the hierarchical formation of massive structures in the early universe.
1. This document describes a multiwavelength campaign on the Seyfert 1 galaxy Mrk 509 using five satellites and two ground-based facilities.
2. The campaign aims to study several open questions about active galactic nuclei (AGN), including the location and physics of outflows from AGN, the nature of continuum emission, the geometry and physical state of the X-ray broad emission line region, and the Fe-K line complex.
3. The observations cover more than five decades in frequency, from 2 μm to 200 keV, and include a simultaneous set of deep XMM-Newton and INTEGRAL observations over seven weeks. This allows the authors to disentangle different components and study time variability
1. VFTS 682 is a very massive star located 29 pc in projection from the young massive cluster R136 in the Tarantula Nebula of the LMC.
2. Spectral modeling finds it has an unusually high luminosity of log(L/L) = 6.5, corresponding to a present-day mass of ~150 solar masses.
3. Its isolation and mass pose the question of whether it formed in situ, which would profoundly impact theories of massive star formation, or if it was ejected from R136, making it the most massive runaway star known.
This document summarizes an X-ray study of the supernova remnant G352.7-0.1 using data from XMM-Newton and Chandra observations. Prior observations revealed G352.7-0.1 has a shell-like radio morphology but center-filled thermal X-ray morphology, classifying it as a mixed-morphology supernova remnant. The new observations confirm the X-ray emission comes from the interior and is dominated by ejecta. Spectra from XMM-Newton are fit by a single thermal component with enhanced silicon and sulfur. Some Chandra spectra require a second thermal component to fit, with solar abundances providing a better physical model. No evidence of overionization was found. A neutron
The behaviour of_dark_matter_associated_with_4_bright_cluster_galaxies_in_the...Sérgio Sacani
The document presents new Hubble Space Telescope imaging and Very Large Telescope integral-field spectroscopy of galaxy cluster Abell 3827. It finds that each of the four central galaxies in the cluster's 10 kpc core retains an associated massive dark matter halo. At least one galaxy is offset from its dark matter halo, with an offset of 1.62+0.50−0.47 kpc, within the uncertainties of mass modeling and statistical errors. If interpreted as evidence for self-interacting dark matter, this offset implies a dark matter self-interaction cross-section of (1.7 ± 0.7)×10−4 cm2/g.
The document summarizes a study that uses strong and weak gravitational lensing to analyze the mass distribution of 28 galaxy clusters. Key findings include:
- The concentration parameter cvir is found to steeply decrease with increasing mass, approximately following cvir ∝ Mvir-0.59±0.12, consistent with theoretical predictions for high-mass clusters but observationally inferred concentrations are higher for lower-mass clusters possibly due to baryon cooling effects.
- Stacking weak lensing shear profiles also supports a steep mass-concentration relation.
- Stacking weak lensing shear maps with position angle information from strong lensing indicates significant ellipticity of the mean mass distribution, with a best-fit ellipticity
This document reports on evidence for spatial variation in the fine structure constant α from observations of quasar absorption spectra. A sample of 153 measurements from the ESO Very Large Telescope (VLT) probing a different region of the universe suggests α was larger in the past, opposite to previous findings from the Keck telescope. Combining the two datasets reveals a significant spatial dipole in α, with the maximum variation in the direction of right ascension 17.3 hours, declination -61 degrees. Detailed analysis found no systematic effects that could mimic this result.
Science with small telescopes - exoplanetsguest8aa6ebb
The search for extrasolar planets has become one of the most attractive problems in modern astrophysics. The biggest observatories in the world are involved in this task as well as little amateur instruments. There is also a huge variety of astronomical methods used for their investigation. Here I present the projects for searching for exoplanets by transit method and our observations of the planet WASP-2b. We observed a transit on 3/4 August 2008 with a 354 mm Schmidt-Cassegrain Celestron telescope and CCD SBIG STL 11000M camera. By precise photometry made using MaximDL software we obtained the light curve of the star system. Decrease of brightness by 0.02m is detected. Analyzing our data we estimate the radius of the planet and inclination of its orbit. Our results are in good correlation with the published information in literature.
A massive protocluster of galaxies at a redshift of z<5.3Sérgio Sacani
This document describes the discovery of a massive protocluster of galaxies located approximately 1 billion years after the Big Bang (redshift of z=5.3). The protocluster contains overdense regions of massive galaxies extending over 13 megaparsecs. It contains an extremely luminous starburst galaxy with large molecular gas reserves and a luminous quasar. Together, these objects place a minimum total mass of over 4×1011 solar masses in this early cluster, consistent with cosmological simulations of the earliest galaxy clusters. This discovery provides evidence for the hierarchical formation of massive structures in the early universe.
1. This document describes a multiwavelength campaign on the Seyfert 1 galaxy Mrk 509 using five satellites and two ground-based facilities.
2. The campaign aims to study several open questions about active galactic nuclei (AGN), including the location and physics of outflows from AGN, the nature of continuum emission, the geometry and physical state of the X-ray broad emission line region, and the Fe-K line complex.
3. The observations cover more than five decades in frequency, from 2 μm to 200 keV, and include a simultaneous set of deep XMM-Newton and INTEGRAL observations over seven weeks. This allows the authors to disentangle different components and study time variability
1. VFTS 682 is a very massive star located 29 pc in projection from the young massive cluster R136 in the Tarantula Nebula of the LMC.
2. Spectral modeling finds it has an unusually high luminosity of log(L/L) = 6.5, corresponding to a present-day mass of ~150 solar masses.
3. Its isolation and mass pose the question of whether it formed in situ, which would profoundly impact theories of massive star formation, or if it was ejected from R136, making it the most massive runaway star known.
This document summarizes an X-ray study of the supernova remnant G352.7-0.1 using data from XMM-Newton and Chandra observations. Prior observations revealed G352.7-0.1 has a shell-like radio morphology but center-filled thermal X-ray morphology, classifying it as a mixed-morphology supernova remnant. The new observations confirm the X-ray emission comes from the interior and is dominated by ejecta. Spectra from XMM-Newton are fit by a single thermal component with enhanced silicon and sulfur. Some Chandra spectra require a second thermal component to fit, with solar abundances providing a better physical model. No evidence of overionization was found. A neutron
The behaviour of_dark_matter_associated_with_4_bright_cluster_galaxies_in_the...Sérgio Sacani
The document presents new Hubble Space Telescope imaging and Very Large Telescope integral-field spectroscopy of galaxy cluster Abell 3827. It finds that each of the four central galaxies in the cluster's 10 kpc core retains an associated massive dark matter halo. At least one galaxy is offset from its dark matter halo, with an offset of 1.62+0.50−0.47 kpc, within the uncertainties of mass modeling and statistical errors. If interpreted as evidence for self-interacting dark matter, this offset implies a dark matter self-interaction cross-section of (1.7 ± 0.7)×10−4 cm2/g.
This paper analyzes Spitzer observations of the Eagle Nebula to study the energetics and evolution of dust. The observations show a shell of emission within the nebula at mid-IR wavelengths that is distinct from the morphology at longer wavelengths. Spectral energy distributions are measured across the nebula and modeled to constrain dust properties and heating sources. Two possible interpretations are proposed for the nature of the mid-IR shell: 1) dust processing in shocks driven by stellar winds, or 2) emission from a hot plasma where dust is collisionally heated. The goal is to better understand dust evolution in massive star forming regions.
This document summarizes Herschel observations of the Fornax galaxy cluster at 100, 160, 250, 350, and 500 μm. It identifies 11 bright galaxies detected at 500 μm that can be compared to previous observations of galaxies in the Virgo cluster. Stellar and far-infrared luminosities are calculated for each galaxy, and modified blackbody curves are fit to derive dust masses and temperatures. The dust properties of Fornax galaxies are found to be broadly similar to those of Virgo galaxies. Fornax shows higher far-infrared luminosity density but lower gas density than Virgo, indicating gas loss in the cluster environment.
A possible carbonrich_interior_in_superearth_55_cancrieSérgio Sacani
1) The document analyzes the possibility that the interior of the super-Earth exoplanet 55 Cancri e could be carbon-rich rather than oxygen-rich.
2) Models that assume an oxygen-rich interior with iron, silicates, and a water envelope cannot fully explain 55 Cancri e's mass and radius measurements. However, a carbon-rich interior containing iron, silicon carbide, and/or carbon could explain the observations without needing a volatile envelope.
3) A carbon-rich interior for 55 Cancri e is plausible given the reported carbon-rich composition of its host star, though more data is needed on the star's elemental abundances and the planet's atmosphere.
This document describes observations of Cepheid variables in the host galaxies of two Type Ia supernovae, SN 1995al in NGC 3021 and SN 2002fk in NGC 1309, using the Hubble Space Telescope. The observations aim to increase the sample of reliably calibrated supernovae to improve the measurement of the Hubble constant. New Cepheids were discovered, including many with periods over 60 days. Metallicity measurements of the galaxies' H II regions were also consistent with solar metallicity. The new data on the supernovae and Cepheids will help strengthen the distance ladder and reduce systematic uncertainties in the determination of the Hubble constant.
This study uses asteroseismology to reveal fast core rotation in red giant stars, finding that the cores rotate at least 10 times faster than the surface by analyzing rotational splitting of mixed modes. Mixed modes that probe the core show larger rotational splitting than modes dominated by the outer layers, indicating non-rigid rotation that increases towards the stellar interior. Models are able to reproduce the observations, confirming theoretical predictions of a steep rotational gradient within red giant cores.
This document describes a study searching for supermassive black holes (SMBHs) with masses below 107 solar masses by looking for signs of low-level nuclear activity in nearby galaxies that are not known to be active galactic nuclei (AGNs). The study uses Chandra X-ray Observatory data to select for X-ray emission, a signature of AGNs, focusing on late-type spiral and dwarf galaxies most likely to host low-mass SMBHs. Preliminary results applying this technique to six nearby spiral galaxies find nuclear X-ray sources in all six, with NGC 3169 and NGC 4102 likely confirmed as AGNs and NGC 3184 and NGC 5457 possibly hosting AGNs.
1) The document analyzes the correlation function of the 6dF Galaxy Survey (6dFGS) and detects a Baryon Acoustic Oscillation (BAO) signal.
2) This BAO detection allows constraining the distance-redshift relation at an effective redshift of zeff = 0.106, achieving a distance measure of DV(zeff) = 456 ± 27 Mpc.
3) The low effective redshift of 6dFGS makes it competitive with Cepheids and low-z supernovae in constraining the Hubble constant, yielding a value of H0 = 67 ± 3.2 km s−1 Mpc−1.
The Large APEX Bolometer Camera (LABOCA) is a new 295-bolometer submillimeter camera operating at 870 μm that has been commissioned for use on the 12 m Atacama Pathfinder Experiment (APEX) telescope. LABOCA offers unprecedented mapping capabilities for submillimeter continuum emission due to APEX's efficiency and the excellent atmospheric transmission at the site. LABOCA is designed to map large areas of the sky rapidly without the need for a chopping secondary mirror by using fast scanning techniques and correlating signals across the array to remove atmospheric contributions.
Search for microscopic black hole signatures at the large hadron colliderSérgio Sacani
The CMS Collaboration at the LHC searched for microscopic black hole signatures using 35 pb-1 of 7 TeV proton-proton collision data. No significant excess beyond standard model expectations was observed in events with high total transverse energy. Limits are set on the minimum black hole mass in the range of 3.5-4.5 TeV for various parameters in the large extra dimensions model. These are the first direct limits on black hole production at a particle collider.
The relation between_gas_and_dust_in_the_taurus_molecular_cloudSérgio Sacani
This document summarizes a study of the relationship between gas and dust in the Taurus molecular cloud. The authors compare hydrogen column densities derived from dust extinction measurements with carbon monoxide column densities derived from 12CO and 13CO observations. They find a linear relationship between visual extinction (AV) and carbon monoxide column density (N(CO)) between AV of 3-10 magnitudes. However, in other regions the relationship is flattened for AV greater than 4 magnitudes. Accounting for temperature gradients and CO depletion, they estimate the total hydrogen mass of Taurus to be about 1.5x104 solar masses and derive a CO-to-H2 conversion factor.
A filament of dark matter between two clusters of galaxiesCarlos Bella
1) The document reports the detection of a dark matter filament connecting two galaxy clusters, Abell 222 and Abell 223, using weak gravitational lensing.
2) Parametric modeling finds that a filament component provides a significantly better fit than models with just three galaxy clusters, and the filament contributes a mass comparable to an additional galaxy cluster.
3) Combining the lensing detection with X-ray observations places an upper limit of 0.09 on the hot gas fraction in the filament.
The document presents observations of the starburst galaxy NGC 253 using near-infrared imaging and spectroscopy as well as mid-infrared spectroscopy. The observations are used to derive physical properties of the starburst such as the star formation rate, stellar population, and evolutionary stage. Evolutionary synthesis modeling is applied to interpret the observations and show that the starburst in NGC 253 is in a late phase, has been ongoing for 20-30 million years, and is consistent with a modified Salpeter initial mass function.
Catch me if_you_can_is_there_a_runaway_mass_black_hole_in_the_orion_nebula_cl...Sérgio Sacani
This document describes a study investigating the dynamical evolution of the Orion Nebula Cluster through N-body simulations. The simulations assume the cluster was initially much more compact than currently observed, based on evidence that a large fraction of gas was expelled during formation. This likely led to strong few-body relaxation effects early in the cluster's evolution. The simulations find that three-body interactions among massive stars could have ejected them from the cluster while also forming a very massive object through runaway stellar mergers. This object may have collapsed directly into a massive (~100 solar mass) black hole, which could explain the velocity dispersion of stars in the Trapezium system at the cluster core. The simulations further suggest this putative black hole has a ~70
Evidence for an intermediate-mass black hole in the globular cluster NGC 6624Sérgio Sacani
This document summarizes evidence for an intermediate-mass black hole located at the center of the globular cluster NGC 6624. The authors present over 25 years of timing observations of the millisecond pulsar PSR B1820-30A, which is located very close to the cluster center. Modeling of the higher order rotational frequency derivatives reveals that the pulsar is likely in a high-eccentricity orbit around a massive companion with a mass greater than 7500 solar masses located at the cluster center, which would be an intermediate-mass black hole. Additional evidence from modeling the cluster gravitational potential and dynamics supports the presence of a central black hole with a minimum mass of around 60,000 solar masses. The observations of this
This document summarizes a study analyzing far-infrared spectra of Saturn's rings obtained by the Cassini spacecraft. The authors modeled the spectra to estimate the size distribution of regolith grains on ring particles. They found that the spectra were best fit by a broad size distribution ranging from 1 micron to 1-10 cm, with a power law index of around 3. This suggests that the largest regolith grains are comparable in size to the smallest visible ring particles. The abundance of smaller grains was found to increase with decreasing solar phase angle, likely due to cooling effects in Saturn's shadow.
A rapidly spinning_supermassive_black_hole_at_the_centre_of_ngc1365Sérgio Sacani
1) XMM-Newton and NuSTAR observed the galaxy NGC 1365 simultaneously over 130 ks, detecting broadband X-ray emission from 3-79 keV.
2) The observations revealed variable absorption below 10 keV and prominent broad emission features between 5-7 keV and 10-30 keV, indicative of relativistic reflection from an accretion disk near a spinning supermassive black hole.
3) Time-resolved spectral analysis was able to disentangle the variable absorption component from the relativistic reflection component. Absorption-dominated models without reflection could be ruled out statistically and on physical grounds.
The local nanohertz gravitational-wave landscape from supermassive black hole...Sérgio Sacani
This document describes a study that uses data from the 2MASS galaxy catalog and galaxy merger rates from the Illustris simulation to construct probabilistic models of the local nanohertz gravitational wave landscape detectable by pulsar timing arrays. It finds an average of 91±7 ongoing supermassive black hole binary mergers within 225 Mpc emitting continuous gravitational waves. Using all-sky gravitational wave sensitivity maps, it estimates that at least one of these sources could be detected within 10 years with current pulsar timing arrays. Accounting for the positions of the best pulsars, the sensitivity is increased by a factor of 4, detecting more sources.
Grb 130606a as_a_probe_of_the_intergalactic_medium_and_the_interstelar_medium...Sérgio Sacani
This document summarizes observations of the gamma-ray burst GRB 130606A at a redshift of z=5.913 using spectroscopy from the MMT and Gemini telescopes. The high quality spectra exhibit a smooth near-infrared continuum that is sharply cut off by Lyman-alpha absorption at z=5.91, with some flux transmitted through the Lyman-alpha forest at lower redshifts. Metal absorption lines in the host galaxy are used to constrain its metallicity between -1.7 and -0.5 solar. Transmission in the Lyman-alpha forest is found to evolve consistently with previous quasar observations. An extended region at z=5.77 shows no Lyman-alpha transmission,
Multi wavelenth observations and surveys of galaxy clustersJoana Santos
This document provides an overview of galaxy clusters, focusing on their baryonic components (intracluster medium and galaxies) and how they relate to the cluster's physical properties like mass. It discusses that galaxy clusters form hierarchically through gravitational collapse. The intracluster medium, which makes up most of the baryonic mass, emits X-rays and has been heated to temperatures of millions of degrees. The document reviews properties of the intracluster medium like density, temperature, metallicity, and how they can be measured from X-ray spectra. It also discusses upcoming surveys that will advance the study of galaxy clusters.
This document provides a catalog of mobile apps related to astronomy education. It lists over 50 apps, each with the title, developer, download link, and brief description. The apps cover a wide range of topics including planetarium programs, astronomical clocks, images from space telescopes, exoplanet data, and tools for observing the sky. Suggestions for additional apps to include in the catalog are welcome.
A empresa de tecnologia anunciou um novo produto, um smartphone com câmera de alta resolução e bateria de longa duração. O aparelho também possui armazenamento expansível e processador rápido. O lançamento está programado para o próximo mês com preço inicial de US$ 499.
This paper analyzes Spitzer observations of the Eagle Nebula to study the energetics and evolution of dust. The observations show a shell of emission within the nebula at mid-IR wavelengths that is distinct from the morphology at longer wavelengths. Spectral energy distributions are measured across the nebula and modeled to constrain dust properties and heating sources. Two possible interpretations are proposed for the nature of the mid-IR shell: 1) dust processing in shocks driven by stellar winds, or 2) emission from a hot plasma where dust is collisionally heated. The goal is to better understand dust evolution in massive star forming regions.
This document summarizes Herschel observations of the Fornax galaxy cluster at 100, 160, 250, 350, and 500 μm. It identifies 11 bright galaxies detected at 500 μm that can be compared to previous observations of galaxies in the Virgo cluster. Stellar and far-infrared luminosities are calculated for each galaxy, and modified blackbody curves are fit to derive dust masses and temperatures. The dust properties of Fornax galaxies are found to be broadly similar to those of Virgo galaxies. Fornax shows higher far-infrared luminosity density but lower gas density than Virgo, indicating gas loss in the cluster environment.
A possible carbonrich_interior_in_superearth_55_cancrieSérgio Sacani
1) The document analyzes the possibility that the interior of the super-Earth exoplanet 55 Cancri e could be carbon-rich rather than oxygen-rich.
2) Models that assume an oxygen-rich interior with iron, silicates, and a water envelope cannot fully explain 55 Cancri e's mass and radius measurements. However, a carbon-rich interior containing iron, silicon carbide, and/or carbon could explain the observations without needing a volatile envelope.
3) A carbon-rich interior for 55 Cancri e is plausible given the reported carbon-rich composition of its host star, though more data is needed on the star's elemental abundances and the planet's atmosphere.
This document describes observations of Cepheid variables in the host galaxies of two Type Ia supernovae, SN 1995al in NGC 3021 and SN 2002fk in NGC 1309, using the Hubble Space Telescope. The observations aim to increase the sample of reliably calibrated supernovae to improve the measurement of the Hubble constant. New Cepheids were discovered, including many with periods over 60 days. Metallicity measurements of the galaxies' H II regions were also consistent with solar metallicity. The new data on the supernovae and Cepheids will help strengthen the distance ladder and reduce systematic uncertainties in the determination of the Hubble constant.
This study uses asteroseismology to reveal fast core rotation in red giant stars, finding that the cores rotate at least 10 times faster than the surface by analyzing rotational splitting of mixed modes. Mixed modes that probe the core show larger rotational splitting than modes dominated by the outer layers, indicating non-rigid rotation that increases towards the stellar interior. Models are able to reproduce the observations, confirming theoretical predictions of a steep rotational gradient within red giant cores.
This document describes a study searching for supermassive black holes (SMBHs) with masses below 107 solar masses by looking for signs of low-level nuclear activity in nearby galaxies that are not known to be active galactic nuclei (AGNs). The study uses Chandra X-ray Observatory data to select for X-ray emission, a signature of AGNs, focusing on late-type spiral and dwarf galaxies most likely to host low-mass SMBHs. Preliminary results applying this technique to six nearby spiral galaxies find nuclear X-ray sources in all six, with NGC 3169 and NGC 4102 likely confirmed as AGNs and NGC 3184 and NGC 5457 possibly hosting AGNs.
1) The document analyzes the correlation function of the 6dF Galaxy Survey (6dFGS) and detects a Baryon Acoustic Oscillation (BAO) signal.
2) This BAO detection allows constraining the distance-redshift relation at an effective redshift of zeff = 0.106, achieving a distance measure of DV(zeff) = 456 ± 27 Mpc.
3) The low effective redshift of 6dFGS makes it competitive with Cepheids and low-z supernovae in constraining the Hubble constant, yielding a value of H0 = 67 ± 3.2 km s−1 Mpc−1.
The Large APEX Bolometer Camera (LABOCA) is a new 295-bolometer submillimeter camera operating at 870 μm that has been commissioned for use on the 12 m Atacama Pathfinder Experiment (APEX) telescope. LABOCA offers unprecedented mapping capabilities for submillimeter continuum emission due to APEX's efficiency and the excellent atmospheric transmission at the site. LABOCA is designed to map large areas of the sky rapidly without the need for a chopping secondary mirror by using fast scanning techniques and correlating signals across the array to remove atmospheric contributions.
Search for microscopic black hole signatures at the large hadron colliderSérgio Sacani
The CMS Collaboration at the LHC searched for microscopic black hole signatures using 35 pb-1 of 7 TeV proton-proton collision data. No significant excess beyond standard model expectations was observed in events with high total transverse energy. Limits are set on the minimum black hole mass in the range of 3.5-4.5 TeV for various parameters in the large extra dimensions model. These are the first direct limits on black hole production at a particle collider.
The relation between_gas_and_dust_in_the_taurus_molecular_cloudSérgio Sacani
This document summarizes a study of the relationship between gas and dust in the Taurus molecular cloud. The authors compare hydrogen column densities derived from dust extinction measurements with carbon monoxide column densities derived from 12CO and 13CO observations. They find a linear relationship between visual extinction (AV) and carbon monoxide column density (N(CO)) between AV of 3-10 magnitudes. However, in other regions the relationship is flattened for AV greater than 4 magnitudes. Accounting for temperature gradients and CO depletion, they estimate the total hydrogen mass of Taurus to be about 1.5x104 solar masses and derive a CO-to-H2 conversion factor.
A filament of dark matter between two clusters of galaxiesCarlos Bella
1) The document reports the detection of a dark matter filament connecting two galaxy clusters, Abell 222 and Abell 223, using weak gravitational lensing.
2) Parametric modeling finds that a filament component provides a significantly better fit than models with just three galaxy clusters, and the filament contributes a mass comparable to an additional galaxy cluster.
3) Combining the lensing detection with X-ray observations places an upper limit of 0.09 on the hot gas fraction in the filament.
The document presents observations of the starburst galaxy NGC 253 using near-infrared imaging and spectroscopy as well as mid-infrared spectroscopy. The observations are used to derive physical properties of the starburst such as the star formation rate, stellar population, and evolutionary stage. Evolutionary synthesis modeling is applied to interpret the observations and show that the starburst in NGC 253 is in a late phase, has been ongoing for 20-30 million years, and is consistent with a modified Salpeter initial mass function.
Catch me if_you_can_is_there_a_runaway_mass_black_hole_in_the_orion_nebula_cl...Sérgio Sacani
This document describes a study investigating the dynamical evolution of the Orion Nebula Cluster through N-body simulations. The simulations assume the cluster was initially much more compact than currently observed, based on evidence that a large fraction of gas was expelled during formation. This likely led to strong few-body relaxation effects early in the cluster's evolution. The simulations find that three-body interactions among massive stars could have ejected them from the cluster while also forming a very massive object through runaway stellar mergers. This object may have collapsed directly into a massive (~100 solar mass) black hole, which could explain the velocity dispersion of stars in the Trapezium system at the cluster core. The simulations further suggest this putative black hole has a ~70
Evidence for an intermediate-mass black hole in the globular cluster NGC 6624Sérgio Sacani
This document summarizes evidence for an intermediate-mass black hole located at the center of the globular cluster NGC 6624. The authors present over 25 years of timing observations of the millisecond pulsar PSR B1820-30A, which is located very close to the cluster center. Modeling of the higher order rotational frequency derivatives reveals that the pulsar is likely in a high-eccentricity orbit around a massive companion with a mass greater than 7500 solar masses located at the cluster center, which would be an intermediate-mass black hole. Additional evidence from modeling the cluster gravitational potential and dynamics supports the presence of a central black hole with a minimum mass of around 60,000 solar masses. The observations of this
This document summarizes a study analyzing far-infrared spectra of Saturn's rings obtained by the Cassini spacecraft. The authors modeled the spectra to estimate the size distribution of regolith grains on ring particles. They found that the spectra were best fit by a broad size distribution ranging from 1 micron to 1-10 cm, with a power law index of around 3. This suggests that the largest regolith grains are comparable in size to the smallest visible ring particles. The abundance of smaller grains was found to increase with decreasing solar phase angle, likely due to cooling effects in Saturn's shadow.
A rapidly spinning_supermassive_black_hole_at_the_centre_of_ngc1365Sérgio Sacani
1) XMM-Newton and NuSTAR observed the galaxy NGC 1365 simultaneously over 130 ks, detecting broadband X-ray emission from 3-79 keV.
2) The observations revealed variable absorption below 10 keV and prominent broad emission features between 5-7 keV and 10-30 keV, indicative of relativistic reflection from an accretion disk near a spinning supermassive black hole.
3) Time-resolved spectral analysis was able to disentangle the variable absorption component from the relativistic reflection component. Absorption-dominated models without reflection could be ruled out statistically and on physical grounds.
The local nanohertz gravitational-wave landscape from supermassive black hole...Sérgio Sacani
This document describes a study that uses data from the 2MASS galaxy catalog and galaxy merger rates from the Illustris simulation to construct probabilistic models of the local nanohertz gravitational wave landscape detectable by pulsar timing arrays. It finds an average of 91±7 ongoing supermassive black hole binary mergers within 225 Mpc emitting continuous gravitational waves. Using all-sky gravitational wave sensitivity maps, it estimates that at least one of these sources could be detected within 10 years with current pulsar timing arrays. Accounting for the positions of the best pulsars, the sensitivity is increased by a factor of 4, detecting more sources.
Grb 130606a as_a_probe_of_the_intergalactic_medium_and_the_interstelar_medium...Sérgio Sacani
This document summarizes observations of the gamma-ray burst GRB 130606A at a redshift of z=5.913 using spectroscopy from the MMT and Gemini telescopes. The high quality spectra exhibit a smooth near-infrared continuum that is sharply cut off by Lyman-alpha absorption at z=5.91, with some flux transmitted through the Lyman-alpha forest at lower redshifts. Metal absorption lines in the host galaxy are used to constrain its metallicity between -1.7 and -0.5 solar. Transmission in the Lyman-alpha forest is found to evolve consistently with previous quasar observations. An extended region at z=5.77 shows no Lyman-alpha transmission,
Multi wavelenth observations and surveys of galaxy clustersJoana Santos
This document provides an overview of galaxy clusters, focusing on their baryonic components (intracluster medium and galaxies) and how they relate to the cluster's physical properties like mass. It discusses that galaxy clusters form hierarchically through gravitational collapse. The intracluster medium, which makes up most of the baryonic mass, emits X-rays and has been heated to temperatures of millions of degrees. The document reviews properties of the intracluster medium like density, temperature, metallicity, and how they can be measured from X-ray spectra. It also discusses upcoming surveys that will advance the study of galaxy clusters.
This document provides a catalog of mobile apps related to astronomy education. It lists over 50 apps, each with the title, developer, download link, and brief description. The apps cover a wide range of topics including planetarium programs, astronomical clocks, images from space telescopes, exoplanet data, and tools for observing the sky. Suggestions for additional apps to include in the catalog are welcome.
A empresa de tecnologia anunciou um novo produto, um smartphone com câmera de alta resolução e bateria de longa duração. O aparelho também possui armazenamento expansível e processador rápido. O lançamento está programado para o próximo mês com preço inicial de US$ 499.
First detection of_molecular_gas_in_shells_in_cena_galaxySérgio Sacani
This document reports the first detection of molecular gas (CO) in the shells of the galaxy Centaurus A (Cen A), located 15 kpc from the galaxy's center. The ratio of CO to HI emission in the shells matches what is found in the galaxy's central regions, which is unexpected given typical metallicity gradients in galaxies. The detection of molecular gas in the shells provides evidence that molecular gas in galaxy mergers may be spread further from nuclear regions than previously thought. The dynamics of the gas can be understood if the interstellar medium is considered clumpy and less dissipative than assumed, allowing dense gas to orbit with stars and form shells.
The document summarizes the period of the universe known as the Dark Age, which occurred between the emission of the cosmic microwave background radiation and the formation of the first stars. During this time, the universe was nearly homogeneous and dark as the first structures like galaxies and stars had yet to form. The Cold Dark Matter model and observations of the cosmic microwave background and distant galaxies provide evidence that the first stars likely formed around redshift 20, ending the Dark Age and beginning the process of reionization. The formation of these first stars required the presence of dark matter for structure to grow and cooling mechanisms like molecular hydrogen to allow gas to collapse into the progenitors of stars.
This document provides an overview and context for a study of the symbiotic star SS Leporis using interferometric imaging with the PIONIER instrument on the VLTI. Key points:
- SS Leporis is a long-period interacting binary system composed of an A star accreting material from an evolved M giant companion, presenting an "Algol paradox" where the more evolved star is less massive.
- Previous studies have not fully constrained the system morphology and characteristics. New interferometric observations with PIONIER were obtained to directly probe the inner parts of the system.
- The observations were used to perform aperture synthesis imaging and model the system as a binary surrounded by a circumbinary disc. This provides the
This document presents observations of ACT-CL J0102−4915, a massive galaxy cluster discovered by the Atacama Cosmology Telescope (ACT) via its strong Sunyaev-Zeldovich signal. Optical and X-ray observations reveal that it is undergoing a major merger between components with a mass ratio of 2:1 at a redshift of 0.87. Chandra X-ray data show significant temperature variations across the cluster from 6.6 keV to 22 keV, indicating a hot, luminous system undergoing a merger. The cluster appears to be an excellent example of a "bullet cluster" system at high redshift.
This document summarizes the results of a study using Herschel Space Observatory data to analyze the physical properties of dust in the RCW 120 H ii region. The study finds:
1) Dust temperatures in RCW 120 range from around 30 K in the interior decreasing to 20 K in the photo-dissociation region and 10 K in nearby infrared dark clouds.
2) There is tentative evidence of an anti-correlation between dust temperature and the dust emissivity index β, with cooler dust having higher β values, consistent with some previous studies.
3) RCW 120 appears to be in the process of destroying its photo-dissociation region boundary and leaked radiation from the interior may be influencing the
The document describes simulations of a collision between the Moon and a companion moon approximately 1/3 the diameter of the Moon. The simulations found that at the modeled subsonic impact velocity, the companion moon did not form an impact crater but was instead accreted onto the Moon's surface. This added material contributed a hemispheric layer comparable to the extent and thickness of the lunar farside highlands. The collision also displaced the Moon's magma ocean to the opposite hemisphere, potentially explaining the observed concentration of KREEP materials. The findings suggest this late accretion event could explain the geological dichotomy between the lunar near and farside regions.
This document reports the discovery of 96 new infrared open clusters and stellar groups in the Milky Way disk as part of the VISTA Variables in the Vía Láctea (VVV) survey. The authors conducted a visual search of VVV survey images towards known star-forming regions, finding compact, young (less than 5 Myr old) clusters that are faint and highly reddened. Photometry was performed on candidate clusters and color-magnitude diagrams were analyzed to determine properties like reddening, distance, and age for relatively populated clusters by fitting isochrones. Most of the newly discovered clusters likely trace early epochs of star formation in the Galaxy.
This document summarizes a study examining the center of the supernova remnant SNR 0509-67.5 in the Large Magellanic Cloud to search for an ex-companion star that could distinguish between single-degenerate and double-degenerate progenitor models of Type Ia supernovae. High-resolution Hubble Space Telescope images show no point sources within the conservative 3-sigma error ellipse of the remnant's center down to a magnitude limit of V=26.9, corresponding to an absolute magnitude 4.2 magnitudes fainter than possible for any published single-degenerate model. This rules out all single-degenerate progenitor scenarios and supports a double-degenerate origin for this particular Type Ia supern
The significance of_the_integrated_sachs_wolfe_effect_revisitedSérgio Sacani
The document discusses revisiting measurements of the integrated Sachs-Wolfe (ISW) effect in light of new data. It updates the data set used in a previous study to include the latest cosmic microwave background and large-scale structure data. Testing finds the updated results are consistent with previous measurements, with the combined ISW detection significance being 4.4 sigma. The paper also addresses criticisms raised about potential systematic errors, focusing on a rotation test of maps, but finds no evidence of additional contamination.
The document summarizes research on concentric ring structures surrounding lunar basins. Key findings include:
1) Several lunar maria resemble giant impact craters, surrounded by concentric mountain rings.
2) Mare Nectaris, the prototype structure, has greater complexity than previously observed, including the prominent Altai Scarp mountain range.
3) Lunar basins tend to be surrounded by more than one concentric mountain ring and exhibit radial fault systems, with flooding more common inside inner rings. Concentric ring structures provide evidence the basins predate later crater impacts and flooding.
Creation of cosmic structure in the complex galaxy cluster merger abell 2744Sérgio Sacani
Abell 2744 is one of the most actively merging galaxy clusters known, appearing to have "dark", "ghost", "bullet", and "stripped" substructures of around 1014 solar masses each. The cluster shows a complex phenomenology that will challenge simulations to reproduce. The authors present a detailed strong lensing, weak lensing, and X-ray analysis of Abell 2744, identifying 34 strongly lensed images around the massive Southern core and producing the most detailed mass map to date. They find evidence that the Southern core and Northwestern substructure are post-merger systems similar to the Bullet Cluster viewed from an angle, and derive a new constraint on the self-interaction cross section of dark matter particles. They
The Lunar Reconnaissance Orbiter Camera (LROC) has collected over 400 gigabits of image data per day and has mapped the entire moon at high resolutions between 0.5 and 2 meters per pixel. The Narrow Angle Camera (NAC) has collected over 580,000 images at incidence angles less than 91 degrees, while the Wide Angle Camera (WAC) has collected 34 complete global datasets with unique lighting geometries. LROC has been in a low 50 km orbit for over 2 years, providing fantastic datasets and the opportunity to image Apollo landing sites and other targets of interest up close.
Kepler 16- a transiting circumbinary planetSérgio Sacani
This document summarizes the discovery of Kepler-16b, the first confirmed circumbinary planet. Kepler-16b orbits two stars and was detected via the transit method as it passed in front of the larger of the two stars. This provided direct evidence of the planet and precise measurements of its mass, radius, and orbital parameters. The discovery enhances confidence in other circumbinary planet detections which had previously only been inferred from timing variations in stellar eclipses.
The Mini-RF radar on the Lunar Reconnaissance Orbiter has revealed new details about impact melt deposits and ejecta flows on the lunar surface. Long melt flows from the craters Tycho and Glushko show variations in radar backscatter and polarization that resemble features of terrestrial lava flows. Small craters also exhibit a variety of melt deposits including ponds and flows. Some features appear to be ejecta flows from debris rather than melted rock. Impact melt flows have very high polarization ratios, suggesting rough surfaces at the centimeter to decimeter scale. In some cases, melt ponds and flows are seen without an identifiable source crater. These observations provide insights into similar features on Venus and the emplacement of melted rock
This document discusses restoring habitable conditions on Mars through planetary ecosynthesis or terraforming. It reviews the scientific feasibility and environmental ethics. Key points include:
- Mars was once warmer and had liquid water, but lost its atmosphere over time due to its small size. Warming Mars tens of degrees could make it habitable again within 100 years.
- Two alternative habitable states are possible: an oxygen-rich atmosphere like Earth, or a CO2 atmosphere with nitrogen and oxygen at lower levels. An oxygen-rich atmosphere would take over 100,000 years to produce.
- Processes that depleted Mars' early atmosphere included carbonate formation, loss to space from solar wind, and impacts removing atmosphere. Earth recy
Ultraviolet signposts of resonant dynamics in the starburst ringed sab galaxy...Sérgio Sacani
1) The document analyzes ultraviolet images of the starburst-ringed galaxy M94, finding emission from the nucleus, inner disk, bright inner ring of H II regions, and two outer knots of hot stars.
2) Optical and ultraviolet spectroscopy of the nucleus and inner disk indicate a 107-108 year old stellar population with some low-level star formation and LINER activity.
3) Analysis of multi-wavelength data suggests that star formation in M94 is being driven by ring-bar dynamics involving structures like the nuclear mini-bar, inner ring, oval disk, and outer ring.
This study examines the clustering properties and redshift evolution of bias for 593 X-ray selected AGN from the XMM-Newton survey in the COSMOS field with spectroscopic redshifts below z=4. The authors find evidence that the bias factor increases with redshift for the total AGN population, from b=2.30 at z=0.92 to b=4.37 at z=1.94. Splitting the sample, they observe a similar increase in bias with redshift for broad-line and unobscured AGN, corresponding to a constant halo mass of logM~13.28 and logM~13, respectively. The observed bias factors cannot be reproduced by models assuming AGN are triggered
A weak lensing_mass_reconstruction_of _the_large_scale_filament_massive_galax...Sérgio Sacani
This study reports the first weak-lensing detection of a large-scale filament funneling matter onto the core of the massive galaxy cluster MACSJ0717.5+3745. The analysis is based on Hubble Space Telescope images covering an area of 10x20 arcmin^2 around the cluster. A weak-lensing mass reconstruction detects the filament within 3 sigma and measures its projected length as ~4.5 h^-1 Mpc and mean density as (2.92±0.66)×10^8 h74 M⊙ kpc^-2. Assuming constraints on the filament's geometry based on galaxy velocities, the three-dimensional length is estimated to be 18 h^-1 M
Three newly discovered_globular_clusters_in_ngc6822Sérgio Sacani
This document describes the discovery of three new globular clusters in the Local Group dwarf irregular galaxy NGC 6822. The authors present optical photometry of the clusters from archival CFHT/Megacam data. Two clusters are luminous and compact, while the third is a lower luminosity diffuse cluster. The positions of the new clusters are consistent with the linear alignment of previously known clusters in NGC 6822. Studying globular cluster systems in dwarf galaxies provides insights into the formation of larger galaxies through accretion and mergers.
Forming intracluster gas in a galaxy protocluster at a redshift of 2.16Sérgio Sacani
Galaxy clusters are the most massive gravitationally bound structures in the Universe, comprising thousands of galaxies and
pervaded by a diffuse, hot “intracluster medium” (ICM) that dominates the baryonic content of these systems. The formation
and evolution of the ICM across cosmic time1
is thought to be driven by the continuous accretion of matter from the large-scale
filamentary surroundings and dramatic merger events with other clusters or groups. Until now, however, direct observations of
the intracluster gas have been limited only to mature clusters in the latter three-quarters of the history of the Universe, and we
have been lacking a direct view of the hot, thermalized cluster atmosphere at the epoch when the first massive clusters formed.
Here we report the detection (about 6σ) of the thermal Sunyaev-Zeldovich (SZ) effect2
in the direction of a protocluster. In fact,
the SZ signal reveals the ICM thermal energy in a way that is insensitive to cosmological dimming, making it ideal for tracing
the thermal history of cosmic structures3
. This result indicates the presence of a nascent ICM within the Spiderweb protocluster
at redshift z = 2.156, around 10 billion years ago. The amplitude and morphology of the detected signal show that the SZ
effect from the protocluster is lower than expected from dynamical considerations and comparable with that of lower-redshift
group-scale systems, consistent with expectations for a dynamically active progenitor of a local galaxy cluster.
The characterization of_the_gamma_ray_signal_from_the_central_milk_way_a_comp...Sérgio Sacani
This document analyzes the gamma-ray signal from the central Milky Way that is consistent with emission from annihilating dark matter particles. The authors re-examine Fermi data using cuts on an event parameter to improve gamma-ray maps and more easily separate components. They find the GeV excess is robust and well-fit by a 36-51 GeV dark matter particle annihilating to bottom quarks with a cross section of 1-3×10−26 cm3/s. The signal extends over 10 degrees from the Galactic Center and is spherically symmetric, disfavoring explanations from millisecond pulsars or gas interactions.
A giant ring_like_structure_at_078_z_086_displayed_by_gr_bsSérgio Sacani
This document describes the discovery of a giant ring-like structure in the observable universe displayed by 9 gamma ray bursts (GRBs) between redshifts of 0.78 and 0.86. The ring has a diameter of 1720 Mpc, over five times larger than the expected transition scale to homogeneity. The ring lies at a distance of 2770 Mpc with major and minor diameters of 43° and 30°, respectively. The probability of this structure occurring by random chance is calculated to be 2 × 10-6. This ring-shaped feature contradicts the cosmological principle of large-scale homogeneity and isotropy, and the physical mechanism responsible is unknown.
This document summarizes a study that uses cosmological simulations to model the formation of stellar halos around galaxies via the tidal disruption of accreted dwarf galaxies. The simulations follow the dynamical evolution and disruption of satellites from high redshift in a fully cosmological setting. The simulations produce stellar halos with masses and density profiles consistent with observations of the Milky Way and M31. The stellar halos show complex structures composed of well-mixed components, tidal streams, shells, and other substructures rather than smooth distributions.
Detection of an_unindentified_emission_line_in_the_stacked_x_ray_spectrum_of_...Sérgio Sacani
1. Researchers detected a previously unknown emission line in the stacked X-ray spectrum of 73 galaxy clusters observed by XMM-Newton. 2. The line was detected at an energy of 3.55-3.57 keV and was seen independently in subsamples of clusters. 3. The line was also detected in Chandra observations of the Perseus cluster but not in observations of the Virgo cluster. 4. The nature of this line is unclear - it could be a thermal line from an undetected element, or potentially the decay line of a hypothesized dark matter particle called a sterile neutrino. Further observations are needed to determine the origin of the line.
Small scatter and_nearly_isothermal_mass_profiles_to_four_half_light_radii_fr...Sérgio Sacani
This document summarizes the results of a study analyzing the total mass density profiles of 14 early-type galaxies using two-dimensional stellar kinematic data out to large radii of 2-6 half-light radii. The study finds that the total density profiles are well described by a nearly-isothermal power law with density proportional to radius from 0.1 to at least 4 half-light radii. The average logarithmic slope is -2.19 with a small scatter of only 0.11. This places tight constraints on galaxy formation models and illustrates the power of extended two-dimensional stellar kinematic observations.
Direct detection of ultralight dark matter bound to the Sun with space quantu...Sérgio Sacani
Recent advances in quantum sensors, including atomic clocks, enable searches for a broad range of dark matter candidates. The question of the dark matter distribution in the Solar system critically affects the reach of dark matter direct detection experiments. Partly motivated by the NASA Deep Space Atomic Clock and the Parker Solar Probe, we show that space quantum sensors present new opportunities for ultralight dark matter searches, especially for dark matter states bound to the Sun. We show that space quantum sensors can probe unexplored parameter space of ultralight dark matter, covering theoretical relaxion targets motivated by naturalness and Higgs mixing. If a two-clock system were able to make measurements on the interior of the solar system, it could probe this highly sensitive region directly and set very strong constraints on the existence of such a bound-state halo in our solar system. We present sensitivity projections for space-based probes of ultralight dark matter, which couples to electron, photon and gluon fields, based on current and future atomic, molecular and nuclear clocks
We report the discovery of spiral galaxies that are as optically luminous as elliptical brightest cluster
galaxies, with r-band monochromatic luminosity Lr = 8 14L (4:3 7:5 1044 erg s 1). These
super spiral galaxies are also giant and massive, with diameter D = 57 134 kpc and stellar mass
Mstars = 0:3 3:4 1011M. We nd 53 super spirals out of a complete sample of 1616 SDSS
galaxies with redshift z < 0:3 and Lr > 8L. The closest example is found at z = 0:089. We use
existing photometry to estimate their stellar masses and star formation rates (SFRs). The SDSS
and WISE colors are consistent with normal star-forming spirals on the blue sequence. However, the
extreme masses and rapid SFRs of 5 65M yr 1 place super spirals in a sparsely populated region
of parameter space, above the star-forming main sequence of disk galaxies. Super spirals occupy a
diverse range of environments, from isolation to cluster centers. We nd four super spiral galaxy
systems that are late-stage major mergers{a possible clue to their formation. We suggest that super
spirals are a remnant population of unquenched, massive disk galaxies. They may eventually become
massive lenticular galaxies after they are cut o from their gas supply and their disks fade.
The discovery of a giant arc associated with the galaxy cluster IDCS J1426.5+3508 at z=1.75 is reported. HST imaging reveals an arc-like object with a length-to-width ratio greater than 10, located near the brightest cluster galaxy. Attempts to measure the redshift of the arc through spectroscopy were unsuccessful. The existence of such a massive, strongly lensing cluster at this early epoch poses challenges for the standard ΛCDM model of structure formation.
The atacama cosmology_telescope_measuring_radio_galaxy_bias_through_cross_cor...Sérgio Sacani
A radiação cósmica de micro-ondas aponta para a matéria escura invisível, marcando o ponto onde jatos de material viajam a velocidades próximas da velocidade da luz, de acordo com uma equipe internacional de astrônomos. O principal autor do estudo, Rupert Allison da Universidade de Oxford apresentou os resultados no dia 6 de Julho de 2015 no National Astronomy Meeting em Venue Cymru, em Llandudno em Wales.
Atualmente, ninguém sabe ao certo do que a matéria escura é feita, mas ela é responsável por cerca de 26% do conteúdo de energia do universo, com galáxias massivas se formando em densas regiões de matéria escura. Embora invisível, a matéria escura se mostra através do efeito gravitacional – uma grande bolha de matéria escura puxa a matéria normal (como elétrons, prótons e nêutrons) através de sua própria gravidade, eventualmente se empacotando conjuntamente para criar as estrelas e galáxias inteiras.
Muitas das maiores dessas são galáxias ativas com buracos negros supermassivos em seus centros. Alguma parte do gás caindo diretamente na direção do buraco negro é ejetada como jatos de partículas e radiação. As observações feitas com rádio telescópios mostram que esses jatos as vezes se espalham por milhões de anos-luz desde a galáxia – mais distante até mesmo do que a extensão da própria galáxia.
Os cientistas esperam que os jatos possam viver em regiões onde existe um excesso de concentração da matéria escura, maior do que o da média. Mas como a matéria escura é invisível, testar essa ideia não é algo tão direto.
A spectroscopic sample_of_massive_galaxiesSérgio Sacani
This document describes a study of 16 massive galaxies at z ~ 2 selected from the 3D-HST spectroscopic survey based on the detection of a strong 4000 Angstrom break in their spectra. Spectroscopy and imaging from HST/WFC3 are used to determine accurate redshifts, stellar population properties, and structural parameters. The sample significantly increases the number of spectroscopically confirmed evolved galaxies at z ~ 2 with robust size measurements. The analysis populates the mass-size relation and finds it is consistent with local relations but with smaller sizes by a factor of 2-3. A model is presented where the observed size evolution is explained by quenching of increasingly larger star-forming galaxies at a rate set by
This document summarizes research determining the velocity vector of the Andromeda Galaxy (M31) relative to the Milky Way using Hubble Space Telescope measurements of M31's proper motion. N-body models of M31 are used to correct for internal stellar motions within M31. The results imply M31 is on a radial orbit towards the Milky Way. The velocity vector is then used to estimate the mass of the Local Group, obtaining a value of (3.17 ± 0.57) × 1012 M☉. It is also implied M33 is likely bound to M31.
An unindetified line_in_xray_spectra_of_the_adromeda_galaxy_and_perseus_galax...Sérgio Sacani
This document summarizes an analysis of X-ray spectra from the Andromeda galaxy and Perseus galaxy cluster observed with the XMM-Newton X-ray observatory. The analysis identified a weak unidentified line at an energy of approximately 3.5 keV in the spectra of both objects. The line strength increases towards the centers of the objects and is stronger in Perseus than in Andromeda. The line properties are consistent with originating from the decay of dark matter particles, though an instrumental or astrophysical source cannot be ruled out based on individual objects. Future detections or non-detections in additional targets could help reveal the nature of this line.
SPECTROSCOPIC CONFIRMATION OF THE EXISTENCE OF LARGE, DIFFUSE GALAXIES IN THE...Sérgio Sacani
We recently identified a population of low surface brightness objects in the field of the z = 0.023 Coma cluster,
using the Dragonfly Telephoto Array. Here we present Keck spectroscopy of one of the largest of these “ultradiffuse
galaxies” (UDGs), confirming that it is a member of the cluster. The galaxy has prominent absorption
features, including the Ca II H+K lines and the G-band, and no detected emission lines. Its radial velocity of
cz=6280±120 km s−1 is within the 1σ velocity dispersion of the Coma cluster. The galaxy has an effective
radius of 4.3 ± 0.3 kpc and a Sérsic index of 0.89 ± 0.06, as measured from Keck imaging. We find no indications
of tidal tails or other distortions, at least out to a radius of ∼2re. We show that UDGs are located in a previously
sparsely populated region of the size—magnitude plane of quiescent stellar systems, as they are ∼6 mag fainter
than normal early-type galaxies of the same size. It appears that the luminosity distribution of large quiescent
galaxies is not continuous, although this could largely be due to selection effects. Dynamical measurements are
needed to determine whether the dark matter halos of UDGs are similar to those of galaxies with the same
luminosity or to those of galaxies with the same size.
The document describes measurements of the proper motion of the Andromeda Galaxy (M31) using Hubble Space Telescope imaging data from multiple fields observed at two epochs separated by 5-7 years. Background galaxies in the images are used as stationary reference objects to measure the displacement of thousands of M31 stars between epochs. This allows determining M31's absolute proper motion with an accuracy of 12 microarcseconds per year, providing crucial information about M31 and the Local Group's dynamics and future evolution.
Observational evidence against long lived spiral arms in galaxies1Sérgio Sacani
This document presents evidence against the theory of long-lived spiral arms in galaxies. The authors analyze simulations and observations to test whether spiral patterns are quasi-stationary features with a constant pattern speed, as implied by density wave theory. They find that in simulations with imposed spiral potentials, gas and young stars are spatially ordered as expected. However, in more realistic simulations where spirals form naturally, the gas and stars are coincident with the spiral potential minors and not separated. Analyzing observations of 12 galaxies, the authors calculate angular cross-correlations between different star formation tracers but find no systematic offsets, contrary to the predictions of stationary spiral density waves. This suggests spiral density waves are not important for explaining spiral structure in
This document summarizes the results of a 180 ks Chandra-LETGS observation of Mrk 509 as part of a larger multi-wavelength campaign. The observation detected several absorption features in the X-ray spectrum originating from an ionized absorber, including ions with three distinct ionization degrees. The lowest ionized component is slightly redshifted and not in pressure equilibrium with the others, likely belonging to the host galaxy's interstellar medium. The other two components are outflowing at velocities of around -200 and -455 km/s. Simultaneous HST-COS observations detected 13 UV kinematic components, and at least three can be associated with the X-ray components, providing evidence that the UV and X-
Similar to Laboca survey of_extended_chandra_deep_field_south (20)
Compositions of iron-meteorite parent bodies constrainthe structure of the pr...Sérgio Sacani
Magmatic iron-meteorite parent bodies are the earliest planetesimals in the Solar System,and they preserve information about conditions and planet-forming processes in thesolar nebula. In this study, we include comprehensive elemental compositions andfractional-crystallization modeling for iron meteorites from the cores of five differenti-ated asteroids from the inner Solar System. Together with previous results of metalliccores from the outer Solar System, we conclude that asteroidal cores from the outerSolar System have smaller sizes, elevated siderophile-element abundances, and simplercrystallization processes than those from the inner Solar System. These differences arerelated to the formation locations of the parent asteroids because the solar protoplane-tary disk varied in redox conditions, elemental distributions, and dynamics at differentheliocentric distances. Using highly siderophile-element data from iron meteorites, wereconstruct the distribution of calcium-aluminum-rich inclusions (CAIs) across theprotoplanetary disk within the first million years of Solar-System history. CAIs, the firstsolids to condense in the Solar System, formed close to the Sun. They were, however,concentrated within the outer disk and depleted within the inner disk. Future modelsof the structure and evolution of the protoplanetary disk should account for this dis-tribution pattern of CAIs.
Signatures of wave erosion in Titan’s coastsSérgio Sacani
The shorelines of Titan’s hydrocarbon seas trace flooded erosional landforms such as river valleys; however, it isunclear whether coastal erosion has subsequently altered these shorelines. Spacecraft observations and theo-retical models suggest that wind may cause waves to form on Titan’s seas, potentially driving coastal erosion,but the observational evidence of waves is indirect, and the processes affecting shoreline evolution on Titanremain unknown. No widely accepted framework exists for using shoreline morphology to quantitatively dis-cern coastal erosion mechanisms, even on Earth, where the dominant mechanisms are known. We combinelandscape evolution models with measurements of shoreline shape on Earth to characterize how differentcoastal erosion mechanisms affect shoreline morphology. Applying this framework to Titan, we find that theshorelines of Titan’s seas are most consistent with flooded landscapes that subsequently have been eroded bywaves, rather than a uniform erosional process or no coastal erosion, particularly if wave growth saturates atfetch lengths of tens of kilometers.
SDSS1335+0728: The awakening of a ∼ 106M⊙ black hole⋆Sérgio Sacani
Context. The early-type galaxy SDSS J133519.91+072807.4 (hereafter SDSS1335+0728), which had exhibited no prior optical variations during the preceding two decades, began showing significant nuclear variability in the Zwicky Transient Facility (ZTF) alert stream from December 2019 (as ZTF19acnskyy). This variability behaviour, coupled with the host-galaxy properties, suggests that SDSS1335+0728 hosts a ∼ 106M⊙ black hole (BH) that is currently in the process of ‘turning on’. Aims. We present a multi-wavelength photometric analysis and spectroscopic follow-up performed with the aim of better understanding the origin of the nuclear variations detected in SDSS1335+0728. Methods. We used archival photometry (from WISE, 2MASS, SDSS, GALEX, eROSITA) and spectroscopic data (from SDSS and LAMOST) to study the state of SDSS1335+0728 prior to December 2019, and new observations from Swift, SOAR/Goodman, VLT/X-shooter, and Keck/LRIS taken after its turn-on to characterise its current state. We analysed the variability of SDSS1335+0728 in the X-ray/UV/optical/mid-infrared range, modelled its spectral energy distribution prior to and after December 2019, and studied the evolution of its UV/optical spectra. Results. From our multi-wavelength photometric analysis, we find that: (a) since 2021, the UV flux (from Swift/UVOT observations) is four times brighter than the flux reported by GALEX in 2004; (b) since June 2022, the mid-infrared flux has risen more than two times, and the W1−W2 WISE colour has become redder; and (c) since February 2024, the source has begun showing X-ray emission. From our spectroscopic follow-up, we see that (i) the narrow emission line ratios are now consistent with a more energetic ionising continuum; (ii) broad emission lines are not detected; and (iii) the [OIII] line increased its flux ∼ 3.6 years after the first ZTF alert, which implies a relatively compact narrow-line-emitting region. Conclusions. We conclude that the variations observed in SDSS1335+0728 could be either explained by a ∼ 106M⊙ AGN that is just turning on or by an exotic tidal disruption event (TDE). If the former is true, SDSS1335+0728 is one of the strongest cases of an AGNobserved in the process of activating. If the latter were found to be the case, it would correspond to the longest and faintest TDE ever observed (or another class of still unknown nuclear transient). Future observations of SDSS1335+0728 are crucial to further understand its behaviour. Key words. galaxies: active– accretion, accretion discs– galaxies: individual: SDSS J133519.91+072807.4
Discovery of An Apparent Red, High-Velocity Type Ia Supernova at 𝐳 = 2.9 wi...Sérgio Sacani
We present the JWST discovery of SN 2023adsy, a transient object located in a host galaxy JADES-GS
+
53.13485
−
27.82088
with a host spectroscopic redshift of
2.903
±
0.007
. The transient was identified in deep James Webb Space Telescope (JWST)/NIRCam imaging from the JWST Advanced Deep Extragalactic Survey (JADES) program. Photometric and spectroscopic followup with NIRCam and NIRSpec, respectively, confirm the redshift and yield UV-NIR light-curve, NIR color, and spectroscopic information all consistent with a Type Ia classification. Despite its classification as a likely SN Ia, SN 2023adsy is both fairly red (
�
(
�
−
�
)
∼
0.9
) despite a host galaxy with low-extinction and has a high Ca II velocity (
19
,
000
±
2
,
000
km/s) compared to the general population of SNe Ia. While these characteristics are consistent with some Ca-rich SNe Ia, particularly SN 2016hnk, SN 2023adsy is intrinsically brighter than the low-
�
Ca-rich population. Although such an object is too red for any low-
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cosmological sample, we apply a fiducial standardization approach to SN 2023adsy and find that the SN 2023adsy luminosity distance measurement is in excellent agreement (
≲
1
�
) with
Λ
CDM. Therefore unlike low-
�
Ca-rich SNe Ia, SN 2023adsy is standardizable and gives no indication that SN Ia standardized luminosities change significantly with redshift. A larger sample of distant SNe Ia is required to determine if SN Ia population characteristics at high-
�
truly diverge from their low-
�
counterparts, and to confirm that standardized luminosities nevertheless remain constant with redshift.
Evidence of Jet Activity from the Secondary Black Hole in the OJ 287 Binary S...Sérgio Sacani
Wereport the study of a huge optical intraday flare on 2021 November 12 at 2 a.m. UT in the blazar OJ287. In the binary black hole model, it is associated with an impact of the secondary black hole on the accretion disk of the primary. Our multifrequency observing campaign was set up to search for such a signature of the impact based on a prediction made 8 yr earlier. The first I-band results of the flare have already been reported by Kishore et al. (2024). Here we combine these data with our monitoring in the R-band. There is a big change in the R–I spectral index by 1.0 ±0.1 between the normal background and the flare, suggesting a new component of radiation. The polarization variation during the rise of the flare suggests the same. The limits on the source size place it most reasonably in the jet of the secondary BH. We then ask why we have not seen this phenomenon before. We show that OJ287 was never before observed with sufficient sensitivity on the night when the flare should have happened according to the binary model. We also study the probability that this flare is just an oversized example of intraday variability using the Krakow data set of intense monitoring between 2015 and 2023. We find that the occurrence of a flare of this size and rapidity is unlikely. In machine-readable Tables 1 and 2, we give the full orbit-linked historical light curve of OJ287 as well as the dense monitoring sample of Krakow.
Candidate young stellar objects in the S-cluster: Kinematic analysis of a sub...Sérgio Sacani
Context. The observation of several L-band emission sources in the S cluster has led to a rich discussion of their nature. However, a definitive answer to the classification of the dusty objects requires an explanation for the detection of compact Doppler-shifted Brγ emission. The ionized hydrogen in combination with the observation of mid-infrared L-band continuum emission suggests that most of these sources are embedded in a dusty envelope. These embedded sources are part of the S-cluster, and their relationship to the S-stars is still under debate. To date, the question of the origin of these two populations has been vague, although all explanations favor migration processes for the individual cluster members. Aims. This work revisits the S-cluster and its dusty members orbiting the supermassive black hole SgrA* on bound Keplerian orbits from a kinematic perspective. The aim is to explore the Keplerian parameters for patterns that might imply a nonrandom distribution of the sample. Additionally, various analytical aspects are considered to address the nature of the dusty sources. Methods. Based on the photometric analysis, we estimated the individual H−K and K−L colors for the source sample and compared the results to known cluster members. The classification revealed a noticeable contrast between the S-stars and the dusty sources. To fit the flux-density distribution, we utilized the radiative transfer code HYPERION and implemented a young stellar object Class I model. We obtained the position angle from the Keplerian fit results; additionally, we analyzed the distribution of the inclinations and the longitudes of the ascending node. Results. The colors of the dusty sources suggest a stellar nature consistent with the spectral energy distribution in the near and midinfrared domains. Furthermore, the evaporation timescales of dusty and gaseous clumps in the vicinity of SgrA* are much shorter ( 2yr) than the epochs covered by the observations (≈15yr). In addition to the strong evidence for the stellar classification of the D-sources, we also find a clear disk-like pattern following the arrangements of S-stars proposed in the literature. Furthermore, we find a global intrinsic inclination for all dusty sources of 60 ± 20◦, implying a common formation process. Conclusions. The pattern of the dusty sources manifested in the distribution of the position angles, inclinations, and longitudes of the ascending node strongly suggests two different scenarios: the main-sequence stars and the dusty stellar S-cluster sources share a common formation history or migrated with a similar formation channel in the vicinity of SgrA*. Alternatively, the gravitational influence of SgrA* in combination with a massive perturber, such as a putative intermediate mass black hole in the IRS 13 cluster, forces the dusty objects and S-stars to follow a particular orbital arrangement. Key words. stars: black holes– stars: formation– Galaxy: center– galaxies: star formation
JAMES WEBB STUDY THE MASSIVE BLACK HOLE SEEDSSérgio Sacani
The pathway(s) to seeding the massive black holes (MBHs) that exist at the heart of galaxies in the present and distant Universe remains an unsolved problem. Here we categorise, describe and quantitatively discuss the formation pathways of both light and heavy seeds. We emphasise that the most recent computational models suggest that rather than a bimodal-like mass spectrum between light and heavy seeds with light at one end and heavy at the other that instead a continuum exists. Light seeds being more ubiquitous and the heavier seeds becoming less and less abundant due the rarer environmental conditions required for their formation. We therefore examine the different mechanisms that give rise to different seed mass spectrums. We show how and why the mechanisms that produce the heaviest seeds are also among the rarest events in the Universe and are hence extremely unlikely to be the seeds for the vast majority of the MBH population. We quantify, within the limits of the current large uncertainties in the seeding processes, the expected number densities of the seed mass spectrum. We argue that light seeds must be at least 103 to 105 times more numerous than heavy seeds to explain the MBH population as a whole. Based on our current understanding of the seed population this makes heavy seeds (Mseed > 103 M⊙) a significantly more likely pathway given that heavy seeds have an abundance pattern than is close to and likely in excess of 10−4 compared to light seeds. Finally, we examine the current state-of-the-art in numerical calculations and recent observations and plot a path forward for near-future advances in both domains.
Anti-Universe And Emergent Gravity and the Dark UniverseSérgio Sacani
Recent theoretical progress indicates that spacetime and gravity emerge together from the entanglement structure of an underlying microscopic theory. These ideas are best understood in Anti-de Sitter space, where they rely on the area law for entanglement entropy. The extension to de Sitter space requires taking into account the entropy and temperature associated with the cosmological horizon. Using insights from string theory, black hole physics and quantum information theory we argue that the positive dark energy leads to a thermal volume law contribution to the entropy that overtakes the area law precisely at the cosmological horizon. Due to the competition between area and volume law entanglement the microscopic de Sitter states do not thermalise at sub-Hubble scales: they exhibit memory effects in the form of an entropy displacement caused by matter. The emergent laws of gravity contain an additional ‘dark’ gravitational force describing the ‘elastic’ response due to the entropy displacement. We derive an estimate of the strength of this extra force in terms of the baryonic mass, Newton’s constant and the Hubble acceleration scale a0 = cH0, and provide evidence for the fact that this additional ‘dark gravity force’ explains the observed phenomena in galaxies and clusters currently attributed to dark matter.
The binding of cosmological structures by massless topological defectsSérgio Sacani
Assuming spherical symmetry and weak field, it is shown that if one solves the Poisson equation or the Einstein field
equations sourced by a topological defect, i.e. a singularity of a very specific form, the result is a localized gravitational
field capable of driving flat rotation (i.e. Keplerian circular orbits at a constant speed for all radii) of test masses on a thin
spherical shell without any underlying mass. Moreover, a large-scale structure which exploits this solution by assembling
concentrically a number of such topological defects can establish a flat stellar or galactic rotation curve, and can also deflect
light in the same manner as an equipotential (isothermal) sphere. Thus, the need for dark matter or modified gravity theory is
mitigated, at least in part.
EWOCS-I: The catalog of X-ray sources in Westerlund 1 from the Extended Weste...Sérgio Sacani
Context. With a mass exceeding several 104 M⊙ and a rich and dense population of massive stars, supermassive young star clusters
represent the most massive star-forming environment that is dominated by the feedback from massive stars and gravitational interactions
among stars.
Aims. In this paper we present the Extended Westerlund 1 and 2 Open Clusters Survey (EWOCS) project, which aims to investigate
the influence of the starburst environment on the formation of stars and planets, and on the evolution of both low and high mass stars.
The primary targets of this project are Westerlund 1 and 2, the closest supermassive star clusters to the Sun.
Methods. The project is based primarily on recent observations conducted with the Chandra and JWST observatories. Specifically,
the Chandra survey of Westerlund 1 consists of 36 new ACIS-I observations, nearly co-pointed, for a total exposure time of 1 Msec.
Additionally, we included 8 archival Chandra/ACIS-S observations. This paper presents the resulting catalog of X-ray sources within
and around Westerlund 1. Sources were detected by combining various existing methods, and photon extraction and source validation
were carried out using the ACIS-Extract software.
Results. The EWOCS X-ray catalog comprises 5963 validated sources out of the 9420 initially provided to ACIS-Extract, reaching a
photon flux threshold of approximately 2 × 10−8 photons cm−2
s
−1
. The X-ray sources exhibit a highly concentrated spatial distribution,
with 1075 sources located within the central 1 arcmin. We have successfully detected X-ray emissions from 126 out of the 166 known
massive stars of the cluster, and we have collected over 71 000 photons from the magnetar CXO J164710.20-455217.
The debris of the ‘last major merger’ is dynamically youngSérgio Sacani
The Milky Way’s (MW) inner stellar halo contains an [Fe/H]-rich component with highly eccentric orbits, often referred to as the
‘last major merger.’ Hypotheses for the origin of this component include Gaia-Sausage/Enceladus (GSE), where the progenitor
collided with the MW proto-disc 8–11 Gyr ago, and the Virgo Radial Merger (VRM), where the progenitor collided with the
MW disc within the last 3 Gyr. These two scenarios make different predictions about observable structure in local phase space,
because the morphology of debris depends on how long it has had to phase mix. The recently identified phase-space folds in Gaia
DR3 have positive caustic velocities, making them fundamentally different than the phase-mixed chevrons found in simulations
at late times. Roughly 20 per cent of the stars in the prograde local stellar halo are associated with the observed caustics. Based
on a simple phase-mixing model, the observed number of caustics are consistent with a merger that occurred 1–2 Gyr ago.
We also compare the observed phase-space distribution to FIRE-2 Latte simulations of GSE-like mergers, using a quantitative
measurement of phase mixing (2D causticality). The observed local phase-space distribution best matches the simulated data
1–2 Gyr after collision, and certainly not later than 3 Gyr. This is further evidence that the progenitor of the ‘last major merger’
did not collide with the MW proto-disc at early times, as is thought for the GSE, but instead collided with the MW disc within
the last few Gyr, consistent with the body of work surrounding the VRM.
Observation of Io’s Resurfacing via Plume Deposition Using Ground-based Adapt...Sérgio Sacani
Since volcanic activity was first discovered on Io from Voyager images in 1979, changes
on Io’s surface have been monitored from both spacecraft and ground-based telescopes.
Here, we present the highest spatial resolution images of Io ever obtained from a groundbased telescope. These images, acquired by the SHARK-VIS instrument on the Large
Binocular Telescope, show evidence of a major resurfacing event on Io’s trailing hemisphere. When compared to the most recent spacecraft images, the SHARK-VIS images
show that a plume deposit from a powerful eruption at Pillan Patera has covered part
of the long-lived Pele plume deposit. Although this type of resurfacing event may be common on Io, few have been detected due to the rarity of spacecraft visits and the previously low spatial resolution available from Earth-based telescopes. The SHARK-VIS instrument ushers in a new era of high resolution imaging of Io’s surface using adaptive
optics at visible wavelengths.
Earliest Galaxies in the JADES Origins Field: Luminosity Function and Cosmic ...Sérgio Sacani
We characterize the earliest galaxy population in the JADES Origins Field (JOF), the deepest
imaging field observed with JWST. We make use of the ancillary Hubble optical images (5 filters
spanning 0.4−0.9µm) and novel JWST images with 14 filters spanning 0.8−5µm, including 7 mediumband filters, and reaching total exposure times of up to 46 hours per filter. We combine all our data
at > 2.3µm to construct an ultradeep image, reaching as deep as ≈ 31.4 AB mag in the stack and
30.3-31.0 AB mag (5σ, r = 0.1” circular aperture) in individual filters. We measure photometric
redshifts and use robust selection criteria to identify a sample of eight galaxy candidates at redshifts
z = 11.5 − 15. These objects show compact half-light radii of R1/2 ∼ 50 − 200pc, stellar masses of
M⋆ ∼ 107−108M⊙, and star-formation rates of SFR ∼ 0.1−1 M⊙ yr−1
. Our search finds no candidates
at 15 < z < 20, placing upper limits at these redshifts. We develop a forward modeling approach to
infer the properties of the evolving luminosity function without binning in redshift or luminosity that
marginalizes over the photometric redshift uncertainty of our candidate galaxies and incorporates the
impact of non-detections. We find a z = 12 luminosity function in good agreement with prior results,
and that the luminosity function normalization and UV luminosity density decline by a factor of ∼ 2.5
from z = 12 to z = 14. We discuss the possible implications of our results in the context of theoretical
models for evolution of the dark matter halo mass function.
THE IMPORTANCE OF MARTIAN ATMOSPHERE SAMPLE RETURN.Sérgio Sacani
The return of a sample of near-surface atmosphere from Mars would facilitate answers to several first-order science questions surrounding the formation and evolution of the planet. One of the important aspects of terrestrial planet formation in general is the role that primary atmospheres played in influencing the chemistry and structure of the planets and their antecedents. Studies of the martian atmosphere can be used to investigate the role of a primary atmosphere in its history. Atmosphere samples would also inform our understanding of the near-surface chemistry of the planet, and ultimately the prospects for life. High-precision isotopic analyses of constituent gases are needed to address these questions, requiring that the analyses are made on returned samples rather than in situ.
Multi-source connectivity as the driver of solar wind variability in the heli...Sérgio Sacani
The ambient solar wind that flls the heliosphere originates from multiple
sources in the solar corona and is highly structured. It is often described
as high-speed, relatively homogeneous, plasma streams from coronal
holes and slow-speed, highly variable, streams whose source regions are
under debate. A key goal of ESA/NASA’s Solar Orbiter mission is to identify
solar wind sources and understand what drives the complexity seen in the
heliosphere. By combining magnetic feld modelling and spectroscopic
techniques with high-resolution observations and measurements, we show
that the solar wind variability detected in situ by Solar Orbiter in March
2022 is driven by spatio-temporal changes in the magnetic connectivity to
multiple sources in the solar atmosphere. The magnetic feld footpoints
connected to the spacecraft moved from the boundaries of a coronal hole
to one active region (12961) and then across to another region (12957). This
is refected in the in situ measurements, which show the transition from fast
to highly Alfvénic then to slow solar wind that is disrupted by the arrival of
a coronal mass ejection. Our results describe solar wind variability at 0.5 au
but are applicable to near-Earth observatories.
Gliese 12 b: A Temperate Earth-sized Planet at 12 pc Ideal for Atmospheric Tr...Sérgio Sacani
Recent discoveries of Earth-sized planets transiting nearby M dwarfs have made it possible to characterize the
atmospheres of terrestrial planets via follow-up spectroscopic observations. However, the number of such planets
receiving low insolation is still small, limiting our ability to understand the diversity of the atmospheric
composition and climates of temperate terrestrial planets. We report the discovery of an Earth-sized planet
transiting the nearby (12 pc) inactive M3.0 dwarf Gliese 12 (TOI-6251) with an orbital period (Porb) of 12.76 days.
The planet, Gliese 12 b, was initially identified as a candidate with an ambiguous Porb from TESS data. We
confirmed the transit signal and Porb using ground-based photometry with MuSCAT2 and MuSCAT3, and
validated the planetary nature of the signal using high-resolution images from Gemini/NIRI and Keck/NIRC2 as
well as radial velocity (RV) measurements from the InfraRed Doppler instrument on the Subaru 8.2 m telescope
and from CARMENES on the CAHA 3.5 m telescope. X-ray observations with XMM-Newton showed the host
star is inactive, with an X-ray-to-bolometric luminosity ratio of log 5.7 L L X bol » - . Joint analysis of the light
curves and RV measurements revealed that Gliese 12 b has a radius of 0.96 ± 0.05 R⊕,a3σ mass upper limit of
3.9 M⊕, and an equilibrium temperature of 315 ± 6 K assuming zero albedo. The transmission spectroscopy metric
(TSM) value of Gliese 12 b is close to the TSM values of the TRAPPIST-1 planets, adding Gliese 12 b to the small
list of potentially terrestrial, temperate planets amenable to atmospheric characterization with JWST.
Gliese 12 b, a temperate Earth-sized planet at 12 parsecs discovered with TES...Sérgio Sacani
We report on the discovery of Gliese 12 b, the nearest transiting temperate, Earth-sized planet found to date. Gliese 12 is a
bright (V = 12.6 mag, K = 7.8 mag) metal-poor M4V star only 12.162 ± 0.005 pc away from the Solar system with one of the
lowest stellar activity levels known for M-dwarfs. A planet candidate was detected by TESS based on only 3 transits in sectors
42, 43, and 57, with an ambiguity in the orbital period due to observational gaps. We performed follow-up transit observations
with CHEOPS and ground-based photometry with MINERVA-Australis, SPECULOOS, and Purple Mountain Observatory,
as well as further TESS observations in sector 70. We statistically validate Gliese 12 b as a planet with an orbital period of
12.76144 ± 0.00006 d and a radius of 1.0 ± 0.1 R⊕, resulting in an equilibrium temperature of ∼315 K. Gliese 12 b has excellent
future prospects for precise mass measurement, which may inform how planetary internal structure is affected by the stellar
compositional environment. Gliese 12 b also represents one of the best targets to study whether Earth-like planets orbiting cool
stars can retain their atmospheres, a crucial step to advance our understanding of habitability on Earth and across the galaxy.
The importance of continents, oceans and plate tectonics for the evolution of...Sérgio Sacani
Within the uncertainties of involved astronomical and biological parameters, the Drake Equation
typically predicts that there should be many exoplanets in our galaxy hosting active, communicative
civilizations (ACCs). These optimistic calculations are however not supported by evidence, which is
often referred to as the Fermi Paradox. Here, we elaborate on this long-standing enigma by showing
the importance of planetary tectonic style for biological evolution. We summarize growing evidence
that a prolonged transition from Mesoproterozoic active single lid tectonics (1.6 to 1.0 Ga) to modern
plate tectonics occurred in the Neoproterozoic Era (1.0 to 0.541 Ga), which dramatically accelerated
emergence and evolution of complex species. We further suggest that both continents and oceans
are required for ACCs because early evolution of simple life must happen in water but late evolution
of advanced life capable of creating technology must happen on land. We resolve the Fermi Paradox
(1) by adding two additional terms to the Drake Equation: foc
(the fraction of habitable exoplanets
with significant continents and oceans) and fpt
(the fraction of habitable exoplanets with significant
continents and oceans that have had plate tectonics operating for at least 0.5 Ga); and (2) by
demonstrating that the product of foc
and fpt
is very small (< 0.00003–0.002). We propose that the lack
of evidence for ACCs reflects the scarcity of long-lived plate tectonics and/or continents and oceans on
exoplanets with primitive life.
A Giant Impact Origin for the First Subduction on EarthSérgio Sacani
Hadean zircons provide a potential record of Earth's earliest subduction 4.3 billion years ago. Itremains enigmatic how subduction could be initiated so soon after the presumably Moon‐forming giant impact(MGI). Earlier studies found an increase in Earth's core‐mantle boundary (CMB) temperature due to theaccumulation of the impactor's core, and our recent work shows Earth's lower mantle remains largely solid, withsome of the impactor's mantle potentially surviving as the large low‐shear velocity provinces (LLSVPs). Here,we show that a hot post‐impact CMB drives the initiation of strong mantle plumes that can induce subductioninitiation ∼200 Myr after the MGI. 2D and 3D thermomechanical computations show that a high CMBtemperature is the primary factor triggering early subduction, with enrichment of heat‐producing elements inLLSVPs as another potential factor. The models link the earliest subduction to the MGI with implications forunderstanding the diverse tectonic regimes of rocky planets.
Climate extremes likely to drive land mammal extinction during next supercont...Sérgio Sacani
Mammals have dominated Earth for approximately 55 Myr thanks to their
adaptations and resilience to warming and cooling during the Cenozoic. All
life will eventually perish in a runaway greenhouse once absorbed solar
radiation exceeds the emission of thermal radiation in several billions of
years. However, conditions rendering the Earth naturally inhospitable to
mammals may develop sooner because of long-term processes linked to
plate tectonics (short-term perturbations are not considered here). In
~250 Myr, all continents will converge to form Earth’s next supercontinent,
Pangea Ultima. A natural consequence of the creation and decay of Pangea
Ultima will be extremes in pCO2 due to changes in volcanic rifting and
outgassing. Here we show that increased pCO2, solar energy (F⨀;
approximately +2.5% W m−2 greater than today) and continentality (larger
range in temperatures away from the ocean) lead to increasing warming
hostile to mammalian life. We assess their impact on mammalian
physiological limits (dry bulb, wet bulb and Humidex heat stress indicators)
as well as a planetary habitability index. Given mammals’ continued survival,
predicted background pCO2 levels of 410–816 ppm combined with increased
F⨀ will probably lead to a climate tipping point and their mass extinction.
The results also highlight how global landmass configuration, pCO2 and F⨀
play a critical role in planetary habitability.
Taking AI to the Next Level in Manufacturing.pdfssuserfac0301
Read Taking AI to the Next Level in Manufacturing to gain insights on AI adoption in the manufacturing industry, such as:
1. How quickly AI is being implemented in manufacturing.
2. Which barriers stand in the way of AI adoption.
3. How data quality and governance form the backbone of AI.
4. Organizational processes and structures that may inhibit effective AI adoption.
6. Ideas and approaches to help build your organization's AI strategy.
How to Interpret Trends in the Kalyan Rajdhani Mix Chart.pdfChart Kalyan
A Mix Chart displays historical data of numbers in a graphical or tabular form. The Kalyan Rajdhani Mix Chart specifically shows the results of a sequence of numbers over different periods.
AppSec PNW: Android and iOS Application Security with MobSFAjin Abraham
Mobile Security Framework - MobSF is a free and open source automated mobile application security testing environment designed to help security engineers, researchers, developers, and penetration testers to identify security vulnerabilities, malicious behaviours and privacy concerns in mobile applications using static and dynamic analysis. It supports all the popular mobile application binaries and source code formats built for Android and iOS devices. In addition to automated security assessment, it also offers an interactive testing environment to build and execute scenario based test/fuzz cases against the application.
This talk covers:
Using MobSF for static analysis of mobile applications.
Interactive dynamic security assessment of Android and iOS applications.
Solving Mobile app CTF challenges.
Reverse engineering and runtime analysis of Mobile malware.
How to shift left and integrate MobSF/mobsfscan SAST and DAST in your build pipeline.
Fueling AI with Great Data with Airbyte WebinarZilliz
This talk will focus on how to collect data from a variety of sources, leveraging this data for RAG and other GenAI use cases, and finally charting your course to productionalization.
In the realm of cybersecurity, offensive security practices act as a critical shield. By simulating real-world attacks in a controlled environment, these techniques expose vulnerabilities before malicious actors can exploit them. This proactive approach allows manufacturers to identify and fix weaknesses, significantly enhancing system security.
This presentation delves into the development of a system designed to mimic Galileo's Open Service signal using software-defined radio (SDR) technology. We'll begin with a foundational overview of both Global Navigation Satellite Systems (GNSS) and the intricacies of digital signal processing.
The presentation culminates in a live demonstration. We'll showcase the manipulation of Galileo's Open Service pilot signal, simulating an attack on various software and hardware systems. This practical demonstration serves to highlight the potential consequences of unaddressed vulnerabilities, emphasizing the importance of offensive security practices in safeguarding critical infrastructure.
LF Energy Webinar: Carbon Data Specifications: Mechanisms to Improve Data Acc...DanBrown980551
This LF Energy webinar took place June 20, 2024. It featured:
-Alex Thornton, LF Energy
-Hallie Cramer, Google
-Daniel Roesler, UtilityAPI
-Henry Richardson, WattTime
In response to the urgency and scale required to effectively address climate change, open source solutions offer significant potential for driving innovation and progress. Currently, there is a growing demand for standardization and interoperability in energy data and modeling. Open source standards and specifications within the energy sector can also alleviate challenges associated with data fragmentation, transparency, and accessibility. At the same time, it is crucial to consider privacy and security concerns throughout the development of open source platforms.
This webinar will delve into the motivations behind establishing LF Energy’s Carbon Data Specification Consortium. It will provide an overview of the draft specifications and the ongoing progress made by the respective working groups.
Three primary specifications will be discussed:
-Discovery and client registration, emphasizing transparent processes and secure and private access
-Customer data, centering around customer tariffs, bills, energy usage, and full consumption disclosure
-Power systems data, focusing on grid data, inclusive of transmission and distribution networks, generation, intergrid power flows, and market settlement data
Main news related to the CCS TSI 2023 (2023/1695)Jakub Marek
An English 🇬🇧 translation of a presentation to the speech I gave about the main changes brought by CCS TSI 2023 at the biggest Czech conference on Communications and signalling systems on Railways, which was held in Clarion Hotel Olomouc from 7th to 9th November 2023 (konferenceszt.cz). Attended by around 500 participants and 200 on-line followers.
The original Czech 🇨🇿 version of the presentation can be found here: https://www.slideshare.net/slideshow/hlavni-novinky-souvisejici-s-ccs-tsi-2023-2023-1695/269688092 .
The videorecording (in Czech) from the presentation is available here: https://youtu.be/WzjJWm4IyPk?si=SImb06tuXGb30BEH .
Have you ever been confused by the myriad of choices offered by AWS for hosting a website or an API?
Lambda, Elastic Beanstalk, Lightsail, Amplify, S3 (and more!) can each host websites + APIs. But which one should we choose?
Which one is cheapest? Which one is fastest? Which one will scale to meet our needs?
Join me in this session as we dive into each AWS hosting service to determine which one is best for your scenario and explain why!
Freshworks Rethinks NoSQL for Rapid Scaling & Cost-EfficiencyScyllaDB
Freshworks creates AI-boosted business software that helps employees work more efficiently and effectively. Managing data across multiple RDBMS and NoSQL databases was already a challenge at their current scale. To prepare for 10X growth, they knew it was time to rethink their database strategy. Learn how they architected a solution that would simplify scaling while keeping costs under control.
Monitoring and Managing Anomaly Detection on OpenShift.pdfTosin Akinosho
Monitoring and Managing Anomaly Detection on OpenShift
Overview
Dive into the world of anomaly detection on edge devices with our comprehensive hands-on tutorial. This SlideShare presentation will guide you through the entire process, from data collection and model training to edge deployment and real-time monitoring. Perfect for those looking to implement robust anomaly detection systems on resource-constrained IoT/edge devices.
Key Topics Covered
1. Introduction to Anomaly Detection
- Understand the fundamentals of anomaly detection and its importance in identifying unusual behavior or failures in systems.
2. Understanding Edge (IoT)
- Learn about edge computing and IoT, and how they enable real-time data processing and decision-making at the source.
3. What is ArgoCD?
- Discover ArgoCD, a declarative, GitOps continuous delivery tool for Kubernetes, and its role in deploying applications on edge devices.
4. Deployment Using ArgoCD for Edge Devices
- Step-by-step guide on deploying anomaly detection models on edge devices using ArgoCD.
5. Introduction to Apache Kafka and S3
- Explore Apache Kafka for real-time data streaming and Amazon S3 for scalable storage solutions.
6. Viewing Kafka Messages in the Data Lake
- Learn how to view and analyze Kafka messages stored in a data lake for better insights.
7. What is Prometheus?
- Get to know Prometheus, an open-source monitoring and alerting toolkit, and its application in monitoring edge devices.
8. Monitoring Application Metrics with Prometheus
- Detailed instructions on setting up Prometheus to monitor the performance and health of your anomaly detection system.
9. What is Camel K?
- Introduction to Camel K, a lightweight integration framework built on Apache Camel, designed for Kubernetes.
10. Configuring Camel K Integrations for Data Pipelines
- Learn how to configure Camel K for seamless data pipeline integrations in your anomaly detection workflow.
11. What is a Jupyter Notebook?
- Overview of Jupyter Notebooks, an open-source web application for creating and sharing documents with live code, equations, visualizations, and narrative text.
12. Jupyter Notebooks with Code Examples
- Hands-on examples and code snippets in Jupyter Notebooks to help you implement and test anomaly detection models.
Connector Corner: Seamlessly power UiPath Apps, GenAI with prebuilt connectorsDianaGray10
Join us to learn how UiPath Apps can directly and easily interact with prebuilt connectors via Integration Service--including Salesforce, ServiceNow, Open GenAI, and more.
The best part is you can achieve this without building a custom workflow! Say goodbye to the hassle of using separate automations to call APIs. By seamlessly integrating within App Studio, you can now easily streamline your workflow, while gaining direct access to our Connector Catalog of popular applications.
We’ll discuss and demo the benefits of UiPath Apps and connectors including:
Creating a compelling user experience for any software, without the limitations of APIs.
Accelerating the app creation process, saving time and effort
Enjoying high-performance CRUD (create, read, update, delete) operations, for
seamless data management.
Speakers:
Russell Alfeche, Technology Leader, RPA at qBotic and UiPath MVP
Charlie Greenberg, host
What is an RPA CoE? Session 1 – CoE VisionDianaGray10
In the first session, we will review the organization's vision and how this has an impact on the COE Structure.
Topics covered:
• The role of a steering committee
• How do the organization’s priorities determine CoE Structure?
Speaker:
Chris Bolin, Senior Intelligent Automation Architect Anika Systems
Introduction of Cybersecurity with OSS at Code Europe 2024Hiroshi SHIBATA
I develop the Ruby programming language, RubyGems, and Bundler, which are package managers for Ruby. Today, I will introduce how to enhance the security of your application using open-source software (OSS) examples from Ruby and RubyGems.
The first topic is CVE (Common Vulnerabilities and Exposures). I have published CVEs many times. But what exactly is a CVE? I'll provide a basic understanding of CVEs and explain how to detect and handle vulnerabilities in OSS.
Next, let's discuss package managers. Package managers play a critical role in the OSS ecosystem. I'll explain how to manage library dependencies in your application.
I'll share insights into how the Ruby and RubyGems core team works to keep our ecosystem safe. By the end of this talk, you'll have a better understanding of how to safeguard your code.
zkStudyClub - LatticeFold: A Lattice-based Folding Scheme and its Application...Alex Pruden
Folding is a recent technique for building efficient recursive SNARKs. Several elegant folding protocols have been proposed, such as Nova, Supernova, Hypernova, Protostar, and others. However, all of them rely on an additively homomorphic commitment scheme based on discrete log, and are therefore not post-quantum secure. In this work we present LatticeFold, the first lattice-based folding protocol based on the Module SIS problem. This folding protocol naturally leads to an efficient recursive lattice-based SNARK and an efficient PCD scheme. LatticeFold supports folding low-degree relations, such as R1CS, as well as high-degree relations, such as CCS. The key challenge is to construct a secure folding protocol that works with the Ajtai commitment scheme. The difficulty, is ensuring that extracted witnesses are low norm through many rounds of folding. We present a novel technique using the sumcheck protocol to ensure that extracted witnesses are always low norm no matter how many rounds of folding are used. Our evaluation of the final proof system suggests that it is as performant as Hypernova, while providing post-quantum security.
Paper Link: https://eprint.iacr.org/2024/257
"Scaling RAG Applications to serve millions of users", Kevin GoedeckeFwdays
How we managed to grow and scale a RAG application from zero to thousands of users in 7 months. Lessons from technical challenges around managing high load for LLMs, RAGs and Vector databases.
1. Mon. Not. R. Astron. Soc. 000, 1–13 (2011) Printed 5 December 2011 (MN L TEX style file v2.2)
A
The LABOCA Survey of the Extended Chandra Deep Field South:
Clustering of submillimetre galaxies
Ryan C. Hickox1,2,3⋆ , J. L. Wardlow1,4 , Ian Smail5 , A. D. Myers6, D. M. Alexander1 ,
A. M. Swinbank5 , A. L. R. Danielson5 , J. P. Stott1 , S. C. Chapman7 , K. E. K. Coppin8,
J. S. Dunlop9 , E. Gawiser10, D. Lutz11 , P. van der Werf12, A. Weiß13
arXiv:1112.0321v1 [astro-ph.GA] 1 Dec 2011
1 Department of Physics, Durham University, South Road, Durham DH1 3LE
2 STFC Postdoctoral Fellow
3 Department of Physics and Astronomy, Dartmouth College, 6127 Wilder Laboratory, Hanover, NH 03755, USA
4 Department of Physics & Astronomy, University of California, Irvine, CA 92697, USA
5 Institute for Computational Cosmology, Durham University, South Road, Durham DH1 3LE
6 Department of Physics and Astronomy, University of Wyoming, Laramie, WY 82071, USA
7 Institute of Astronomy, Madingley Road, Cambridge CB3 0HA
8 Department of Physics, McGill University, Ernest Rutherford Building, 3600 Rue University, Montreal, Quebec H3A 2T8, Canada
9 Institute for Astronomy, University of Edinburgh, Royal Observatory, Edinburgh EH9 3HJ
10 Department of Physics and Astronomy, Rutgers, The State University of New Jersey, Piscataway, NJ 08854, USA
11 Max-Planck-Institut f¨ r extraterrestrische Physik, Postfach 1312, 85741 Garching, Germany
u
12 Leiden Observatory, Leiden University, NL 2300 RA Leiden, The Netherlands
13 Max-Planck-Institut f¨ r Radioastronomie, Auf dem H¨ gel 69, 53121, Bonn, Germany
u u
5 December 2011
ABSTRACT
We present a measurement of the spatial clustering of submillimetre galaxies (SMGs) at
z = 1–3. Using data from the 870 µm LABOCA submillimetre survey of the Extended Chan-
dra Deep Field South, we employ a novel technique to measure the cross-correlation between
SMGs and galaxies, accounting for the full probability distributions for photometric redshifts
of the galaxies. From the observed projected two-point cross-correlation function we derive
the linear bias and characteristic dark matter halo masses for the SMGs. We detect cluster-
ing in the cross-correlation between SMGs and galaxies at the > 4σ level. Accounting for
the clustering of galaxies from their autocorrelation function, we estimate an autocorrelation
+1.8
length for SMGs of r0 = 7.7−2.3 h−1 Mpc assuming a power-law slope γ = 1.8, and derive
+0.3
a corresponding dark matter halo mass of log(Mhalo [h−1 M⊙ ]) = 12.8−0.5 . Based on the
evolution of dark matter haloes derived from simulations, we show that that the z = 0 descen-
dants of SMGs are typically massive (∼ 2–3 L∗ ) elliptical galaxies residing in moderate- to
+0.3
high-mass groups (log(Mhalo [h−1 M⊙ ]) = 13.3−0.5 ). From the observed clustering we esti-
mate an SMG lifetime of ∼100 Myr, consistent with lifetimes derived from gas consumption
times and star-formation timescales, although with considerable uncertainties. The clustering
of SMGs at z ∼ 2 is consistent with measurements for optically-selected quasi-stellar ob-
jects (QSOs), supporting evolutionary scenarios in which powerful starbursts and QSOs oc-
cur in the same systems. Given that SMGs reside in haloes of characteristic mass ∼ 6 × 1012
h−1 M⊙ , we demonstrate that the redshift distribution of SMGs can be described remarkably
well by the combination of two effects: the cosmological growth of structure and the evolution
of the molecular gas fraction in galaxies. We conclude that the powerful starbursts in SMGs
likely represent a short-lived but universal phase in massive galaxy evolution, associated with
the transition between cold gas-rich, star-forming galaxies and passively evolving systems.
Key words: galaxies: evolution – galaxies: high-redshift – galaxies: starburst – large-scale
structure of the Universe – submillimetre.
⋆ E-mail: ryan.c.hickox@dartmouth.edu
c 2011 RAS
2. 2 Ryan C. Hickox et al.
1 INTRODUCTION
-27.5
Submillimetre galaxies (SMGs) are a population of high-redshift
ultraluminous infrared galaxies (ULIRGs) selected through their -27.6
redshifted far-infrared emission in the submillimetre waveband
(e.g., Smail, Ivison & Blain 1997; Barger et al. 1998; Hughes et al.
1998; Blain et al. 2002). The redshift distribution of this popu- -27.7
lation appears to peak at z ∼ 2.5 (e.g., Chapman et al. 2003,
Dec (deg)
2005; Wardlow et al. 2011), so that SMGs are at their common- -27.8
est around the same epoch as the peak in powerful active galactic
nuclei (AGN) and specifically quasi-stellar objects (QSOs) (e.g.,
Richards et al. 2006; Assef et al. 2011). This correspondence may -27.9
indicate an evolutionary link between SMGs and QSOs, similar
to that suggested at low redshift between ULIRGs and QSOs by
-28.0
Sanders et al. (1988). However there is little direct overlap (∼ a
few percent) between the high-redshift SMG and QSO popula-
tions (e.g., Page et al. 2004; Chapman et al. 2005; Stevens et al. -28.1 SMGs galaxies
2005; Alexander et al. 2008; Wardlow et al. 2011). The immense
far-infrared luminosities of SMGs are widely believed to arise from 53.5 53.4 53.3 53.2 53.1 53.0 52.9 52.8
intense, but highly-obscured, gas-rich starbursts (e.g., Greve et al. RA (deg)
2005; Alexander et al. 2005; Pope et al. 2008; Tacconi et al. 2006,
2008; Ivison et al. 2011), suggesting that they may represent the Figure 1. Two-dimensional distribution of the 50 LESS SMGs and
formation phase of the most massive local galaxies: giant ellipti- ∼ 50,000 IRAC galaxies in the ECDFS that are used in our analysis. The
cals (e.g., Eales et al. 1999; Swinbank et al. 2006). SMGs shown represent the subset of the 126 SMGs in the full LESS sam-
ple (Weiß et al. 2009) that are in the redshift range 1 < z < 3 and are
SMGs and QSOs may thus represent phases in an evolu-
in regions of good photometry, and so are used in this analysis. The IRAC
tionary sequence that eventually results in the population of lo-
galaxies are chosen to reside at 0.5 < z < 3.5. The SMGs are shown here
cal massive elliptical galaxies. This is a compelling picture, but individually, while the density of galaxies is given by the grayscale. The
testing the evolutionary links is challenging due to the lack of an blank areas represent regions which are excluded from the analysis, includ-
easily-measured and conserved observable to tie the various pop- ing areas of poor photometry (for example around bright stars) or additional
ulations together. For example, the stellar masses of both QSOs sources identified by eye in the vicinity of SMG, as discussed in §2. The
and SMGs are difficult to measure reliably due to either the high density of IRAC galaxies in the field enables an accurate measurement
brightness of the nuclear emission in the QSOs (e.g., Croom et al. of the SMG-galaxy cross-correlation function.
2004; Kotilainen et al. 2009) or strong dust obscuration and po-
tentially complex star-formation histories for the SMGs (e.g.,
Hainline et al. 2011; Wardlow et al. 2011; but see also Dunlop
2011; Michałowski et al. 2011), while the details of the high-
14 SMGs (1 < z < 3)
redshift star formation that produced local massive elliptical galax- All IRAC galaxies 4000
ies are likewise poorly constrained (e.g., Allanson et al. 2009). De- 12 Galaxies for angular
autocorrelation
riving dynamical masses for QSO hosts from rest-frame optical
Number of galaxies
Number of SMGs
spectroscopy is difficult due to the very broad emission lines from 10 3000
the AGN, while dynamical mass measurements using CO emis-
8
sion in gas-rich QSOs are also challenging, due to the potential
non-isotropic orientation of the QSO hosts on the sky and the 2000
6
lack of high-resolution velocity fields necessary to solve for this
(Coppin et al. 2008), as well as the general difficulties in model- 4
1000
ing CO kinematics (e.g., Tacconi et al. 2006; Bothwell et al. 2010;
Engel et al. 2010). 2
Another possibility is to compare source populations via 0 0
the masses of their central black holes. For QSOs and the pop- 0.5 1.0 1.5 2.0 2.5 3.0 3.5
ulation of SMGs that contain broad-line AGN, the black hole z
mass can be estimated using virial techniques based on the
broad emission lines (e.g., Vestergaard 2002; Peterson et al. 2004; Figure 2. Redshift distributions for the IRAC galaxy sample in the redshift
Vestergaard & Peterson 2006; Kollmeier et al. 2006; Shen et al. range 0.5 < z < 3.5 (dotted line), and the SMG sample in the range
2008). Such studies generally find that SMGs have small black 1 < z < 3 (solid line). The histogram for galaxies has been scaled so
holes relative to the local black hole-galaxy mass relations (e.g., that the distribution can be directly compared to that of the SMGs. Also
shown is the redshift distribution for 11,241 galaxies (dashed line) selected
Alexander et al. 2008; Carrera et al. 2011), while the black holes in
to match the overlap in the redshift distributions of the SMGs and galaxies,
z ∼ 2 QSOs tend to lie above the local relation, with masses sim- as used in the galaxy autocorrelation measurement (§3.2). For the SMGs,
ilar to those in local massive ellipticals (e.g., Decarli et al. 2010; 44% have spectroscopic redshifts, while the remainder of the SMGs and all
Bennert et al. 2010; Merloni et al. 2010). These results suggest that the IRAC galaxies have redshift estimates from photometric redshift calcu-
SMGs represent an earlier evolutionary stage, prior to the QSO lations (Wardlow et al. 2011).
phase in which the black hole reaches its final mass. However, high-
redshift virial black hole mass estimates are highly uncertain (e.g.,
c 2011 RAS, MNRAS 000, 1–13
3. Clustering of SMGs 3
Marconi et al. 2008; Fine et al. 2010; Netzer & Marziani 2010) amplitude, along with their relationship to QSOs and ellipticals, re-
and may suffer from significant selection effects (e.g., Lauer et al. mains uncertain.
2007; Shen & Kelly 2010; Kelly et al. 2010), and so conclusions To make improved measurements of the clustering of SMGs,
about connections between populations are necessarily limited. we need either much larger survey areas (see Cooray et al. 2010 for
The difficulties discussed above lead us to take another route a wide-field clustering measurement for far-IR detected sources) or
to compare SMGs to high-redshift QSOs and low-redshift el- the inclusion of redshift information (to allow us to reduce the ef-
lipticals: through their clustering. Spatial correlation measure- fects of projection on our clustering measurements). To this end, we
ments provide information about the characteristic bias and hence have reanalysed the Weiß et al. (2009) survey of ECDFS using new
mass of the haloes in which galaxies reside (e.g., Kaiser 1984; spectroscopic and photometric redshift constraints on the counter-
Bardeen et al. 1986), and so provide a robust mass estimate that is parts to SMGs (Wardlow et al. 2011) as well as a large catalogue
free of many of the systematics in measuring stellar or black hole of “normal” (less-active) galaxies in the same field. We employ a
masses. The observed clustering of SMGs and QSOs can thus allow new clustering analysis methodology (Myers, White & Ball 2009)
us to test whether these populations are found in similar haloes and to calculate the projected spatial cross-correlation between SMGs
so may evolve into each other over short timescales. With knowl- and galaxies, to obtain the tightest constraint to date on the cluster-
edge of how haloes evolve over cosmic time (e.g., Lacey & Cole ing amplitude of SMGs.
1993; Fakhouri, Ma & Boylan-Kolchin 2010), we can also explore This paper is organised as follows. In § 2 we introduce the
the links to modern elliptical galaxies (e.g., Overzier et al. 2003), as SMG and galaxy samples, and in § 3 we give an overview of the
well as the higher-redshift progenitors of SMGs. Clustering mea- methodology used to measure correlation functions and estimate
surements can also provide constraints on theoretical studies that dark matter (DM) halo masses. In § 4 we present the results, explore
explore the nature of SMGs in a cosmological context. Recent mod- the effects of photometric redshift errors, compare with previous
els for SMGs as relatively long-lived (> 0.5 Gyr) star formation measurements, and discuss our results in the context of the physical
episodes in the most massive galaxies, driven by the early collapse drivers, lifetimes, and evolutionary paths of SMGs. In § 5 we sum-
of the dark matter halo (Xia et al. 2011), or powered by steady ac- marise our conclusions. Throughout this paper we assume a cos-
cretion of intergalactic gas (Dav´ et al. 2010), yield strong cluster-
e mology with Ωm = 0.3 and ΩΛ = 0.7. For direct comparison with
ing for bright sources (850 µm fluxes > a few mJy) with correlation other works, we assume H0 = 70 km s−1 Mpc−1 (except for co-
lengths r0 10 h−1 Mpc. In contrast, models in which SMGs are moving distances and DM halo masses, which are explicitly given
short-lived bursts in less massive galaxies, with large luminosities in terms of h = H0 /(100 km s−1 Mpc−1 )). In order to easily com-
produced by a top-heavy initial mass function, predict significantly pare to estimated halo masses in other recent works on QSO clus-
ˆ
tering (e.g., Croom et al. 2005; Myers et al. 2006; da Angela et al.
weaker clustering with r0 ∼ 6 h−1 Mpc (Almeida, Baugh & Lacey
2011). 2008; Ross et al. 2009), we assume a normalisation for the mat-
ter power spectrum of σ8 = 0.84. All quoted uncertainties are 1σ
Attempts to measure the clustering of SMGs from their (68% confidence).
projected two-dimensional distribution on the sky have for
the most part been ambiguous (Scott et al. 2002; Borys et al.
2003; Webb et al. 2003; Weiß et al. 2009; Williams et al. 2011;
Lindner et al. 2011). Weiß et al. (2009) used the largest, contigu-
ous extragalactic 870-µm survey (of the Extended Chandra Deep 2 SMG AND GALAXY SAMPLES
Field South; ECDFS), to derive the clustering of > 5-mJy SMGs
∼ Our SMG sample comes from the survey of the ECDFS using the
from their projected distribution on the sky. They estimated a cor- Large APEX BOlometer CAmera (Siringo et al. 2009, LABOCA)
relation length of 13 ± 6h−1 Mpc. Most recently, Williams et al. on the Atacama Pathfinder EXperiment (G¨ sten et al. 2006, APEX)
u
(2011) analysed a 1100-µm survey of a region of the COSMOS 12-m telescope (the LABOCA ECDFS Submillimetre Survey, or
field and placed 1-σ upper limits on the clustering of bright SMGs LESS; Weiß et al. 2009). LESS mapped the full 0.35 deg2 ECDFS
(with apparent 870-µm fluxes > 8–10 mJy) of > 6–12 h−1 Mpc.
∼ ∼ to a 870-µm noise level of ∼ 1.2 mJy beam−1 and detected 126
Other work has attempted to improve on angular correla- SMGs at > 3.7σ significance (Weiß et al. 2009, equivalent to a
tion measurements by including redshift information. Using the false-detection rate of ∼ 4%). Radio and mid-infrared counter-
spectroscopic redshift survey of 73 SMGs with 870-µm fluxes of parts to LESS SMGs were identified by Biggs et al. (2011) using
> 5 mJy spread across seven fields from Chapman et al. (2005), a maximum-likelihood technique. Spectroscopic and photometric
∼
Blain et al. (2004) estimated a clustering amplitude from the num- redshifts were obtained for a significant fraction of these counter-
bers of pairs of SMGs within a 1000-km s−1 wide velocity win- parts by Wardlow et al. (2011) and we refer the reader to that work
dow. They derived an effective correlation length of 6.9 ± 2.1 for more details. For this study, we restrict our analysis to the 50
h−1 Mpc, suggesting that SMGs are strongly clustered. How- SMGs that have secure counterparts at z = 1–3 and do not lie close
ever their methodology was subsequently criticised by (Adelberger to bright stars (as discussed below). The upper limit of z = 3 on the
2005), who suggested that accounting for angular clustering of sample is included to maximize overlap in redshift space with the
sources and the redshift selection function significantly increases galaxy sample, in order to obtain a significant cross-correlation sig-
the uncertainties. Using data from the Chandra Deep Field-North, nal, while the lower bound of z = 1 is included to prevent the SMG
Blake et al. (2006) computed the angular cross-correlation between sample from being biased toward low redshifts. Of the SMGs in the
SMGs and galaxies in slices of spectroscopic and photometric red- sample, 22 SMGs (44%) have spectroscopic redshifts (Danielson
shift. They obtained a significant SMG-galaxy cross-correlation et al., in preparation) and the remainder have photometric redshifts
signal, with hints that SMGs are more strongly clustered than the with a typical precision of σz /(1+z) ∼ 0.1 (Wardlow et al. 2011).
optically-selected galaxies, although with only marginal (∼ 2σ) The 870-µm flux distribution for the SMGs having secure counter-
significance. Previous work has therefore pointed toward SMGs parts (Biggs et al. 2011) is consistent with that for all LESS SMGs
being a strongly clustered population, but their precise clustering Weiß et al. (2009), indicating that the requirement that SMGs have
c 2011 RAS, MNRAS 000, 1–13
4. 4 Ryan C. Hickox et al.
secure counterparts does not strongly bias the fluxes of our SMG
sample. 0.005
galaxy 1
galaxy 2
galaxy 3
For the cross-correlation analysis, we also require a compar-
ison population in the same field. For this we adopt the ∼ 50,000 0.004
galaxies detected in the Spitzer IRAC/MUSYC Public Legacy Sur-
vey in the Extended CDF-South (Damen et al. 2011). We use an
f(χ) (h Mpc-1)
IRAC selected sample to ensure that each galaxy has photom- 0.003
SMG redshift
etry in a sufficient number of bands, and over a wide enough
wavelength range, to allow robust estimates of photometric red-
0.002
shift. Photo-zs are calculated using template fits to the optical and
IRAC photometry in an identical method to that used for the SMGs
(see Wardlow et al. 2011). The fits are performed with HYPER - Z 0.001
(Bolzonella, Miralles & Pell´ 2000) and the resulting redshift dis-
o
tribution, compared to that for the SMGs, is shown in Figure 2.
0.000
The photometric analysis uses chi-squared minimisation, which al-
3000 3500 4000 4500 5000
lows the calculation of confidence intervals for the best-fit redshift.
Comoving distance χ (h-1 Mpc)
These can be presented as a probability distribution function (PDF)
for the redshift, or equivalently, the comoving line-of-sight distance
χ (calculated for our assumed cosmology). We define the PDF for Figure 3. Example probability distribution functions for three IRAC galax-
ies and an SMG. We mark the “best” (peak) comoving distance for each
each galaxy as f (χ), where f (χ)dχ = 1. Examples of the PDFs
galaxy. Note that for each galaxy in this example, the line-of-sight distance
for the galaxies are shown in Figure 3. between the “peak” redshift of the galaxy and the SMG redshift is far too
Finally, in order to calculate the correlation functions, we large for them to be physically associated. However, because of the uncer-
first create random catalogues of “galaxies” at random positions tainty in the galaxy redshifts (shown by the PDFs), there is a non-negligible
within the actual spatial coverage of our survey. Like many fields, probability that the galaxies lie close to the line-of-sight distance of the
the ECDFS contains several bright stars with large haloes, around SMG.
which few galaxies are detected. Therefore, we use the background
map produced by SE XTRACTOR (Bertin & Arnouts 1996) from
in the redshift distributions of the galaxies and SMGs. Our cluster-
the combined IRAC image during the source extraction proce-
ing analysis is identical in most respects to the QSO-galaxy cross-
dure to create a mask. This mask is applied to the random cat-
correlation study presented in Hickox et al. (2011, hereafter H11).
alogues, the SMGs and the IRAC galaxies, so that the positions
Because the method is somewhat involved, we present only the key
of the random galaxies are unbiased with respect to the SMG
details here and refer the reader to H11 for a full discussion.
and IRAC galaxy samples, and thus the mask does not affect the
cross-correlation measurement. As discussed in Biggs et al. (2011)
and Wardlow et al. (2011), some of the SMG identifications were 3.1 Cross-correlation method
performed manually by examining the regions around the SMGs.
These additional sources are excluded from the clustering analysis The two-point correlation function ξ(r) is defined as the probability
so as not to bias the results. The sky positions of the SMGs and above Poisson of finding a galaxy in a volume element dV at a
galaxies that are outside the masked regions are shown in Figure 1. physical separation r from another randomly chosen galaxy, such
that
dP = n[1 + ξ(r)]dV, (1)
3 CORRELATION ANALYSIS where n is the mean space density of the galaxies in the sample.
The projected correlation function wp (R) is defined as the integral
To measure the spatial clustering of SMGs, we can in principle
of ξ(r) along the line of sight,
derive the autocorrelation of the SMGs themselves. However, as
πmax
we have discussed, current SMG samples are too limited in size and
wp (R) = 2 ξ(R, π)dπ, (2)
available redshift information to make this feasible. Alternatively, 0
we can measure the cross-correlation of a population with a sample
where R and π are the projected comoving separations between
of other sources (for example, less-active galaxies) which populate
galaxies in the directions perpendicular and parallel, respectively,
the same volume (e.g., Gawiser et al. 2001; Adelberger & Steidel
to the mean line of sight from the observer to the two galaxies.
2005; Blake et al. 2006; Coil et al. 2007; Hickox et al. 2009). The
By integrating along the line of sight, we eliminate redshift-space
much larger number of galaxies in the ECDFS (∼ 1000 × more
distortions owing to the peculiar motions of galaxies, which dis-
than the SMGs in a comparable redshift range) allows far greater
tort the line-of-sight distances measured from redshifts. wp (R) has
statistical accuracy in the measurement of clustering.
been used to measure correlations in a number of surveys (e.g.,
To calculate the real-space projected cross-correlation func-
Zehavi et al. 2005; Li et al. 2006; Gilli et al. 2007; Coil et al. 2007,
tion wp (R) between SMGs and galaxies we employ a method de-
2008; Wake et al. 2008a; Myers, White & Ball 2009; Hickox et al.
rived by Myers, White & Ball (2009). This method enables us to
2009; Coil et al. 2009; Gilli et al. 2009; Krumpe, Miyaji & Coil
take advantage of the full photo-z PDF for each galaxy, by weight-
2010; Donoso et al. 2010; Hickox et al. 2011; Starikova et al. 2011;
ing pairs of SMGs and galaxies based on the probability of their
Allevato et al. 2011).
overlap in redshift space. This method allows us to calculate the
In the range of separations 0.3 r 50 h−1 Mpc, ξ(r) for
SMG-galaxy cross-correlation using the full sample of z ≈ 50, 000
galaxies and QSOs is roughly observed to be a power-law,
IRAC galaxies, while the derive the clustering of the galaxies them-
selves using a smaller sample that is selected to match the overlap ξ(r) = (r/r0 )−γ , (3)
c 2011 RAS, MNRAS 000, 1–13
5. Clustering of SMGs 5
with γ typically ≈1.8 (e.g., Zehavi et al. 2005; Coil et al. 2008, evolution of large scale structure, and because the use of a flux-
2007; Ross et al. 2009). For sufficiently large πmax such that we limited sample means we select more luminous galaxies at higher
average over all line-of-sight peculiar velocities, wp (R) can be di- z. This will affect the measurements of relative bias between SMGs
rectly related to ξ(r) (for a power law parameterisation) by and galaxies, since the redshift distribution of the SMGs peaks at
γ higher z than that for the galaxies and so relatively higher-z galax-
r0 Γ(1/2)Γ[(γ − 1)/2]
wp (R) = R . (4) ies dominate the cross-correlation signal. To account for this in our
R Γ(γ/2) measurement of galaxy autocorrelation, we randomly select galax-
To calculate wp (R) for the cross-correlation between SMGs ies based on the overlap of the PDFs with the SMGs in comoving
and galaxies, we use the method of M09, which accounts for the distance (in the formalism of § 3.1 this is fi,j for each galaxy, av-
photometric redshift probability distribution for each galaxy indi- eraged all SMGs). We select the galaxies so their distribution in
vidually. Following M09, the projected cross-correlation function redshift is equivalent to the weighted distribution for all galaxies
can be calculated using: (weighted by fi,j ). The redshift distribution of this galaxy sam-
ple is shown in Figure 2. We use this smaller galaxy sample to
DS DG (R) calculate the angular autocorrelation of IRAC galaxies.
wp (R) = NR NS ci,j − ci,j (5)
DS RG (R)
i,j i,j
where 3.3 Uncertainties and model fits
ci,j = fi,j / 2
fi,j . (6) We estimate uncertainties on the clustering directly from the data
i,j
using bootstrap resampling. Following H11, we divide the field into
a small number of sub-areas (we choose Nsub = 8), and for each
Here R is the projected comoving distance from each SMG, for bootstrap sample we randomly draw a total of 3Nsub sub-areas
a given angular separation θ and radial comoving distance to the (with replacement), which has been shown to best approximate the
SMG of χ∗ , such that R = χ∗ θ. DS DG and DS RG are the intrinsic uncertainties in the clustering amplitude (Norberg et al.
number of SMG–galaxy and SMG–random pairs in each bin of 2009). To account for shot noise owing to the relatively small size
R, and NS and NR are the total numbers of SMGs and random of the SMG sample, we take the sets of 3Nsub bootstrap sub-
galaxies, respectively. fi,j is defined as the average value of the ra- areas and randomly draw from them (with replacement) a sample
dial PDF f (χ) for each galaxy i, in a window of size ∆χ around of sources (SMGs or galaxies) equal in size to the parent sample;
the comoving distance to each spectroscopic source j. We use only pairs including these sources are used in the resulting cross-
∆χ = 100 h−1 Mpc to effectively eliminate redshift space dis- correlation calculation. We use the bootstrap results to derive the
tortions, although the results are insensitive to the details of this covariance between different bins of R, calculating the covariance
choice. We refer the reader to M09 and H11 for a detailed deriva- matrix using Equation 12 of H11.
tion and discussion of these equations. In this calculation as well We fit the observed wp (R) with two models: a power law and
as in the galaxy autocorrelation, we account for the integral con- a simple bias model (described in § 3.4). We compute model param-
straint as described in H11. This correction increases the observed eters by minimising χ2 (taking into account the covariance matrix
clustering amplitude by ≈15%. as in Equation 13 of H11) and derive 1σ errors in each parame-
ter by the range for which ∆χ2 = 1. We use the same formal-
ism for computing fits to the angular correlation functions, where
3.2 Galaxy autocorrelation ω(θ) = Aθ−δ . We convert A and δ to real-space clustering param-
To estimate DM halo masses for the SMGs, we calculate the rel- eters r0 and γ following the procedure described in § 4.6 of H11.
ative bias between SMGs and galaxies, from which we derive the
absolute bias of the SMGs relative to DM. As discussed below, 3.4 Absolute bias and dark matter halo mass
calculation of absolute bias (and thus halo mass) requires a mea-
surement of the autocorrelation function of the IRAC galaxies. The The masses of the DM haloes in which galaxies and SMGs reside
large size of the galaxy sample enables us to derive the clustering are reflected in their absolute clustering bias babs relative to the DM
2
of the galaxies accurately from the angular autocorrelation function distribution. The linear bias babs is given by the ratio of the autocor-
ω(θ) alone. Although we expect the photometric redshifts for the relation function of the galaxies (or SMGs) to that of the DM. We
IRAC galaxies to be reasonably well-constrained (as discussed in determine babs following the method outlined in § 4.7 of H11, sim-
§ 2), by using the angular correlation function we minimize any un- ilar to the approach used previously by a number of studies (e.g.,
certainties relating to individual galaxy photo-zs for this part of the Myers et al. 2006, 2007; Coil et al. 2007, 2008, 2009; Hickox et al.
analysis. The resulting clustering measured for the galaxies has sig- 2009); in what follows we briefly describe this procedure.
nificantly smaller uncertainties than that for the SMG-galaxy cross- We first calculate the two-point autocorrelation of DM as
correlation. a function of redshift. We use the HALOFIT code of Smith et al.
We calculate the angular autocorrelation function ω(θ) using (2003) assuming our standard cosmology, and the slope of the ini-
the Landy & Szalay (1993) estimator: tial fluctuation power spectrum, Γ = Ωm h = 0.21, to derive
the DM power spectrum, and thus its projected correlation func-
1 DM
tion wp (R), averaged over the redshift distribution for which the
ω(θ) = (DD − 2DR + RR), (7)
RR SMGs and galaxies overlap. We then fit the observed wp (R) of the
where DD, DR, and RR are the number of data-data, data- SMG-galaxy cross-correlation, on scales 0.3–15 h−1 Mpc, with a
DM
random, and random-random galaxy pairs, respectively, at a sep- model comprising a simple linear scaling of wp (R). The best-fit
aration θ, where each term is scaled according to the total numbers linear scaling of the DM correlation function corresponds to bS bG ,
of SMGs, galaxies, and randoms. the product of the linear biases for the SMGs and galaxies, respec-
The galaxy autocorrelation varies with redshift, owing to the tively. This simple model produces a goodness-of-fit comparable
c 2011 RAS, MNRAS 000, 1–13
6. 6 Ryan C. Hickox et al.
105
SMG-galaxy cross-correlation (1<z<3) galaxy autocorrelation
104 10 -1
103
wp(R)/R
10-2
ω (θ)
102
dark
mat
101 -3
ter
dar
km 10
atte
r
100
10-1 10-4
0.1 1.0 10.0 0.1 1.0 10.0
R (h-1 Mpc) θ (arcmin)
Figure 4. The projected SMG-galaxy cross-correlation function (derived Figure 5. The angular autocorrelation function of IRAC galaxies, selected
using Equation 5). Uncertainties are estimated from bootstrap resampling. to match the overlap of the SMGs and galaxies in redshift space. Uncer-
A power-law fit to wp (R) is shown by the solid line, and the projected tainties are estimated from bootstrap resampling. The angular correlation
correlation function for DM is shown by the dotted line. Fits are performed function for DM, evaluated for the redshift distributions of the galaxies, is
over the range in separation of R = 0.3–15 h−1 Mpc. Both the power law shown by the dotted gray line. The power law fit was performed on scales
model with γ = 1.8 and a linear scaling of the DM correlation function 0.3′ –10′ and is shown as the solid line. Both the power law model with
provide satisfactory fits to the observed wp (R). Together with the observed δ = 0.8 and a linear scaling of the DM correlation function provide sat-
galaxy autocorrelation, this measurement yields the clustering amplitude isfactory fits to the observed ω(θ). The observed amplitude of the galaxy
and DM halo mass for the SMGs, as described in § 4. autocorrelation yields the absolute bias of the galaxies, which we use to
obtain the absolute bias and DM halo mass of the SMGs.
to that of the power-law model in which the slope γ is allowed to
float. law model, and show the correlation function of the DM calcu-
To determine bS we therefore need to estimate bG . We obtain lated as in § 3.4, which we fit to the data through a linear scal-
bG for the galaxies from their angular autocorrelation in a similar ing. The power-law and linear bias fit parameters are presented
manner to that applied to the SMG–galaxy cross-correlation. Again in in Table 1. For SMGs the observed real-space projected cross-
we calculate the autocorrelation for the DM ωDM (θ), by integrat- correlation is well-detected on all scales from 0.1–15 h−1 Mpc, and
ing the power spectrum from HALOFIT using Equation (A6) of the power-law fits return γ ∼ 1.8, similar to many previous corre-
Myers et al. (2007). We fit the observed ω(θ) with a linear scaling lation function measurements for galaxies (e.g., Zehavi et al. 2005;
of ωDM (θ) on scales 0.3′ –10′ (corresponding to 0.3–10 h−1 Mpc Coil et al. 2008) and QSOs (e.g., Coil et al. 2007; Ross et al. 2009).
at z = 2). This linear scaling corresponds to b2 and thus (combined
G The best-fit parameters for the SMG-galaxy cross-correlation are
with the cross-correlation measurement) yields the SMG bias bS . r0,SG = 5.3 ± 0.8 h−1 Mpc, γ = 1.7 ± 0.2. If we fix the value
Finally, we convert bG and bS to Mhalo using the prescription of of γ to 1.8, we obtain r0,SG = 5.1 ± 0.6 h−1 Mpc, corresponding
Sheth, Mo & Tormen (2001), as described in H11. This character- to a clustering signal that is significant at the > 4σ level, the most
istic Mhalo corresponds to the top-hat virial mass (see e.g., Peebles significant measurement of SMG clustering to date. From the fit of
1993, and references therein), in the simplified case in which all the DM model, we obtain bS bG = 5.83 ± 1.36.
objects in a given sample reside in haloes of the same mass. This We next compute the autocorrelation of IRAC galaxies for the
assumption is justified by the fact (as discussed below in § 4.4) that sample described in § 3.2. The observed ω(θ) is shown in Fig. 5,
SMGs have a very small number density compared to the popu- along with the corresponding power-law fit and scaled correlation
lation of similarly-clustered DM haloes, such that it is reasonable function for DM, calculated as discussed in §3.4. Fit parameters
that SMGs may occupy haloes in a relatively narrow range in mass. are given in Table 1. The power-law model fits well on the chosen
We note that this method differs from some prescriptions in the lit- scales of 0.3′ –10′ . The best-fit power law parameters are r0,GG =
erature which assume that sources occupy all haloes above some 3.3 ± 0.3 and γ = 1.8 ± 0.2, and the best-fit scaled DM model
minimum mass; this is particularly relevant for populations with yields b2 = 2.99 ± 0.40 or bG = 1.73 ± 0.12.
G
high number densities that could exceed the numbers of available This accurate value for bG yields bS = 3.37 ± 0.82 for the
DM haloes over a limited mass range. Given the halo mass func- SMGs. Converting this to DM halo mass using the prescription
tion at z ∼ 2 (e.g., Tinker et al. 2008) the derived minimum mass of Sheth, Mo & Tormen (2001) as described in §3.4, we arrive at
is typically a factor of ∼2 lower, for the same clustering amplitude, log (Mhalo [h−1 M⊙ ]) = 12.8+0.3 . The corresponding halo mass
−0.5
than the “average” mass quoted here. for the galaxies is log (Mhalo [h−1 M⊙ ]) = 11.5 ± 0.2.
For comparison with other studies that attempted to directly
measure the autocorrelation function of SMG, it is useful to present
the SMG clustering in terms of effective power-law parameters for
4 RESULTS AND DISCUSSION
their autocorrelation. Assuming linear bias, the SMG autocorrela-
2
The projected cross-correlation function of the SMG sample with tion can be inferred from the cross-correlation by ξSS = ξSG /ξGG
the IRAC galaxies is shown in Figure 4. We plot the best-fit power- (e.g., Coil et al. 2009). Adopting a fixed γ = 1.8 for the SMG-
c 2011 RAS, MNRAS 000, 1–13
7. Clustering of SMGs 7
Table 1. Correlation results
Power law fitc Bias model fitd Halo masse
Subset Nsrc a z b r0 (h−1 Mpc) γ χ2
ν bS bG (b2 )
G bS (bG ) χ2
ν (log h−1 M⊙ )
SMGs 50 2.02 7.7+1.8
−2.3 1.8 ± 0.2 0.8 5.83 ± 1.36 3.37 ± 0.82 0.7 12.8+0.3
−0.5
galaxies 11,241 2.13 3.3 ± 0.3 1.8 ± 0.2 1.8 2.99 ± 0.40 1.73 ± 0.12 1.8 11.5 ± 0.2
a Number of objects in the SMG sample and in the galaxy sample used for the galaxy autocorrelation.
b Median redshift for the SMG sample and for the galaxy sample used for the galaxy autocorrelation.
c Power law model parameters are for the autocorrelation of SMGs (derived from SMG-galaxy projected spatial cross-
correlation, along with the galaxy angular autocorrelation) and galaxies (derived from their angular autocorrelation).
d Parameters derived from the observed linear fit of the DM model to the observed correlation function, in order to obtain the
the absolute bias for the SMGs and galaxies (denoted bS and bG , respectively). The linear scaling from the fit corresponds to
bS bG for the SMG-galaxy cross-correlation, and b2 for the galaxy autocorrelation, which in turn yield bG and bS .
G
e DM halo mass derived from the absolute bias, using the method described in § 3.4.
galaxy cross-correlation, we thus obtain r0,SS = 7.7+1.8 h−1 Mpc
−2.3 submm flux limits are shown in Figure 6a. Our measurement is sig-
for the autocorrelation of the SMGs. nificantly more accurate than previous measurements, owing to the
inclusion of redshift information and the improved statistics in the
cross-correlation. The uncertainties are comparable to those quoted
4.1 Effects of SMG photo-z errors by Blain et al. (2004) who estimated r0 using counts of close pairs
in redshift space from spectroscopic surveys. However, these au-
One uncertainty in our estimate of wp (R) for the SMG-galaxy thors did not account for significant additional sources of error, as
cross-correlation is due to the lack of accurate (that is, spectro- discussed by Adelberger (2005). Uncertainties in the redshift se-
scopic) redshifts for roughly half of the SMG population. As de- lection function for spectroscopic objects, along with the presence
scribed in § 3, in calculating wp (R) for the cross-correlation, we of redshift spikes and angular clustering of sources, can strongly
simply assume that the SMGs lie exactly at the best redshifts from impact the number of expected pair counts for an unclustered dis-
the photo-z analysis of Wardlow et al. (2011). Any uncertainties tribution, and therefore significantly affect the results for the clus-
in the SMGs photo-zs could therefore affect the resulting cluster- tering amplitude (Adelberger 2005). In Figure 6a the large error
ing measurement. (Note that photo-z uncertainties in the galaxies bars for the Blain et al. (2004) point represent the increase in the
are accounted for implicitly in the correlation analysis, as we uti- uncertainty by 60% due to angular clustering of sources and red-
lize the full galaxy photo-z PDFs.) To examine the effects of SMG shift spikes (as estimated by Adelberger 2005), but does not in-
photo-z errors, we follow the procedure outlined in § 6.3 of H11. clude the additional uncertainty on the redshift selection function.
We take advantage of the 44% of SMGs that do have spectroscopic Nonetheless, our measurement of r0 is consistent with most previ-
redshifts, and determine how errors in those redshifts affect the ob- ous angular clustering estimates as well as the Blain et al. (2004)
served correlation amplitude. result, and represents a significant improvement in precision.
Specifically, we shift the redshifts of the spectroscopic SMGs
As discussed in § 3.4, we convert the observed clustering
by offsets ∆z/(1+z) selected from a Gaussian random distribution
amplitude to Mhalo by assuming that SMGs obey simple linear
with dispersion σz /(1 + z). To ensure that this step does not arti-
bias relative to the dark matter and reside in haloes of similar
ficially smear out the redshift distribution beyond the range probed
mass. Motivated by the presence of a large overdensity of SMGs
by the galaxies, we require that the random redshifts lie between
and powerful star-forming galaxies in one redshift survey field,
1 < z < 3; any random redshift that lies outside this range is dis-
Chapman et al. (2009) proposed that SMGs obey “complex bias”
carded and a new redshift is selected from the random distribution.
that depends on large-scale environment and merger history, and
Using these new redshifts we recalculate wp (R), using the full for-
that they may reside in somewhat smaller haloes than would be in-
malism described in § 3. We perform the calculation 10 times for
ferred from a linear bias model. Future studies using significantly
each of several values of σz /(1 + z) from 0.05 up to 0.3 (corre-
larger SMG samples may be able to confirm the existence of more
sponding to the range of photo-z uncertainties). For each trial we
complex clustering, but for the present analysis we adopt the sim-
obtain the relative bias by calculating the mean ratio of wp (R), on
plest scenario and derive Mhalo assuming linear bias.
scales 1–10 h−1 Mpc, relative to the wp (R) for the best estimates
of redshift. We then average the ten trials at each σz , and find that at The characteristic halo mass we measure for SMGs is simi-
most the photo-z errors cause the clustering amplitude to decrease lar to that measured for bright far-IR sources (with fluxes > 30
by ∼ 10%. The precise magnitude of this effect is unclear given mJy at 250 µm) detected by the Herschel Space Observatory us-
the range of uncertainties in the SMG photo-z estimates, but it is is ing an angular clustering analysis (Cooray et al. 2010). While it re-
significantly smaller than the statistical uncertainties. We therefore mains uncertain to what extent bright 250 µm sources and 850 µm-
neglect this effect in our final error estimates. selected SMGs represent a common population, both samples com-
prise the luminous end of the star-forming galaxy population de-
tected at those wavelengths and so may represent physically similar
systems. In contrast, our observed SMG clustering is significantly
4.2 Comparison with previous results
stronger than that reported by Amblard et al. (2011) for “submil-
Here we compare our results to other measurements of SMG clus- limetre galaxies” based on a power-spectrum analysis of Herschel
tering in the literature. The observed clustering may depend on the 350 µm maps, which yields a minimum Mhalo of ∼ 3 × 1011 M⊙ .
flux limit of the submm sample, as discussed by Williams et al. The differences in clustering amplitude compared to SMGs result
(2011); measurements of r0 that use SMG samples with similar from the fact that the power spectrum analysis includes unresolved
c 2011 RAS, MNRAS 000, 1–13
8. 8 Ryan C. Hickox et al.
faint sources corresponding to far fainter far-IR luminosities, char-
acteristic of typical z ∼ 2 star-forming galaxies rather than the 20
powerful, luminous starbursts that are conventionally referred to as (a)
SMGs in the literature.
15
Weiss et al. (2009)
r0 (h-1 Mpc)
4.3 Progenitors and descendants of SMGs Webb et al. (2003)
Our improved clustering measurement allows us to place SMGs 10
Williams et al. (2011)
in the context of the cosmological history of star formation and
This work
growth of DM structures. Because the clustering amplitude of dark
matter haloes and their evolution with redshift are directly predicted 5
by simulations and analytic theory, we can use the observed clus-
tering to connect the SMG populations to their descendants and Blain et al. (2004)
progenitors, estimate lifetimes, and constrain starburst triggering 0
mechanisms. 3 4 5 6
We first compare the clustering amplitude of SMGs with other 850 µm flux limit (mJy)
galaxy populations over a range of redshifts1 . Figure 6b shows the
approximate ranges of measurements of r0 for a variety of galaxy
and AGN populations. We also show the evolution of r0 with red- 15 clusters
shift for DM haloes of different masses, determined by fitting a (b)
power law with γ = 1.8 to the DM correlation function output by 1014 h-1 MO
•
HALOFIT . Finally, we show the observed r0 for the current SMG 1013 h-1 MO
•
sample, along with the expected evolution in r0 for haloes that 10
r0 (h-1 Mpc)
~2-3 L*
have the observed Mhalo for SMGs at z = 2, calculated using ellipticals
LRGs
SMGs QSOs
the median growth rate of haloes as a function of Mhalo and z
(Fakhouri, Ma & Boylan-Kolchin 2010)2 . red galaxies 1012 h-1 MO
•
Figure 6b shows that while the DM halo mass for the SMGs 5 QSOs
will increase with time from z ∼ 2 to z = 0, the observed r0
stays essentially constant, meaning that the progenitors and descen- blue galaxies MIPS SFGs LBGs
1011 h-1 MO
•
dants of SMGs will be populations with similar clustering ampli-
tudes. Our measurement of r0 shows that the clustering of SMGs 0
is consistent with optically-selected QSOs (e.g., Croom et al. 0.0 0.5 1.0 1.5 2.0 2.5 3.0
ˆ
2005; Myers et al. 2006; da Angela et al. 2008; Ross et al. 2009). z
SMGs are more strongly clustered than the typical star-forming
galaxy populations at all redshifts (e.g. Adelberger et al. 2005; Figure 6. (a) Our new measurement of the autocorrelation length r0 for
Gilli et al. 2007; Hickox et al. 2009; Zehavi et al. 2011), and are SMGs, compared to previous results using samples with similar ∼850 µm
clustered similarly or weaker than massive, passive systems (e.g., flux limits. The two sets of error bars on the Webb et al. (2003) measure-
Quadri et al. 2007, 2008; Wake et al. 2008b; Blanc et al. 2008; ment indicate statistical (±3 h−1 Mpc) and systematic (±3 h−1 Mpc) un-
Kim et al. 2011; Zehavi et al. 2011). The clustering results indicate certainties separately. On the Blain et al. (2004) measurement, the smaller
that SMGs will likely evolve into the most massive, luminous early errors represent the uncertainties quoted by the authors, while the larger
type galaxies at low redshift. We note that the descendants of typi- errors account for angular clustering and redshift spikes as estimated by
Adelberger (2005). Our results are consistent with previous measurements
cal SMGs are not likely to reside in massive clusters at z = 0, but
and represent a significant improvement in precision. (b) Our measure-
into moderate- to high-mass groups of ∼ a few ×1013 h−1 M⊙ .
ment of the autocorrelation length r0 of SMGs, compared to the approxi-
Although some SMGs could evolve into massive cluster galaxies, mate r0 (with associated measurement uncertainties) for a variety of galaxy
the observed clustering suggests that most will end up in less mas- and AGN populations: optically-selected SDSS QSOs at 0 < z < 3
sive systems. (Myers et al. 2006; Ross et al. 2009), Lyman-break galaxies (LBGs) at
A schematic picture of the evolution of SMGs is 1.5 z 3.5 (Adelberger et al. 2005), MIPS 24 µm-selected star-forming
shown in Figure 7, which shows evolution in the mass of galaxies at 0 < z < 1.4 (Gilli et al. 2007), typical red and blue galax-
haloes with redshift as traced by their median growth rate ies at 0.25 z 1 from the AGES (Hickox et al. 2009) and DEEP2
(Fakhouri, Ma & Boylan-Kolchin 2010). The typical progenitors (Coil et al. 2008) spectroscopic surveys, luminous red galaxies (LRGs) at
of SMGs would have Mhalo ∼ 1012 h−1 M⊙ at z ∼ 5, which cor- 0 < z < 0.7 (Wake et al. 2008b), and optically-selected galaxy clusters at
responds to the host haloes of bright LBGs at those redshifts (e.g., 0.1 < z < 0.3 (Estrada, Sefusatti & Frieman 2009). In addition, we show
the full range of r0 for low-redshift galaxies with r-band luminosities in the
Hamana et al. 2004; Lee et al. 2006). At low redshift, the SMG
range 1.5 to 3.5 L∗ , derived from the luminosity dependence of clustering
descendants will have Mhalo = (0.6–5) × 1013 h−1 M⊙ . Halo presented by Zehavi et al. (2011); these luminous galaxies are primarily el-
occupation distribution fits to galaxy clustering suggest that these lipticals, as discussed in § 4.3. Dotted lines show r0 versus redshift for DM
haloes host galaxies with luminosities L ∼ 2–3L∗ (Zehavi et al. haloes of different masses. The thick solid line shows the expected evolu-
tion in r0 , accounting for the increase in mass of the halo, for a halo with
mass corresponding to the best-fit estimate for SMGs at z = 2. The results
1 Myers et al. (2006) and Ross et al. (2009) determine r from QSOs as- indicate that SMGs are clustered similarly to QSOs at z ∼ 2 and can be
0
suming a power law correlation function with γ = 2. To estimate r0 for expected to evolve into luminous elliptical galaxies in the local Universe.
γ = 1.8, we multiply the quoted values by 0.8, appropriate for fits over the
range 1 R 100 h−1 Mpc.
c 2011 RAS, MNRAS 000, 1–13
9. Clustering of SMGs 9
2011), which has been shown to contain a somewhat smaller den-
sity of SMGs compared to other surveys (Weiß et al. 2009).
14.0 The ratio of these space densities yields a duty cycle (the frac-
tion of haloes that host an SMG at any given time) of ∼ 10%. We
13.5 ~2-3 L* assume the SMGs occupy the redshift range 1.5 < z < 2.5, which
ellipticals
log(Mhalo [h-1 MO])
includes roughly half of the SMGs in the Wardlow et al. (2011)
•
SMGs
sample and corresponds to ∆t = 1.6 Gyr. We thus obtain a life-
13.0 time for SMGs of tSMG = 110+280 Myr. Clearly, even our im-
−80
proved measurement of SMG clustering yields only a weak con-
12.5 straint on the lifetime, but this is consistent with lifetimes esti-
QSOs mated from gas consumption times and star-formation timescales
12.0
(e.g., Greve et al. 2005; Tacconi et al. 2006; Hainline et al. 2011)
bright and theoretical models of SMG fueling through mergers (e.g.,
LBGs
Mihos & Hernquist 1994; Springel, Di Matteo & Hernquist 2005;
11.5
Narayanan et al. 2010).
0 1 2 3 4 5
z Constraints on SMG descendants from clustering can also
yield insights into their their formation histories. Measurements
of the stellar plus molecular gas masses of SMGs from SED fit-
Figure 7. Broad schematic for the evolution of halo mass versus redshift
ting and dynamical studies are in the range ∼ (1–5) × 1011 M⊙
for SMGs, showing the approximate halo masses corresponding to likely
progenitors and descendants of SMGs. Lines indicate the median growth (Swinbank et al. 2006; Wardlow et al. 2011; Hainline et al. 2011;
rates of haloes with redshift (Fakhouri, Ma & Boylan-Kolchin 2010). SMG Ivison et al. 2011; Michałowski et al. 2011). While these estimates
host haloes are similar to those those of QSOs at z ∼ 2, and correspond to can be uncertain by factors of a few, they are in a similar range to
bright LBGs at z ∼ 5 (Hamana et al. 2004; Lee et al. 2006) and ∼ 2–3L∗ the stellar masses of SMG descendants as indicated by their clus-
ellipticals at z = 0 (Zehavi et al. 2011; Stott et al. 2011). tering, as discussed above. This correspondence suggests that if a
significant fraction of the molecular gas is converted to stars dur-
ing the SMG phase, then these galaxies will subsequently experi-
2011), a population dominated by ellipticals with predominantly ence relatively little growth in mass from z ∼ 2 to the present.
slow-rotating kinematics (e.g., Tempel et al. 2011; Cappellari et al. This in turn puts limits on the star formation history. Star-forming
2011). Assuming typical mass-to-light ratios for massive galaxies galaxies at z ∼ 2 typically exhibit specific star formation rates of
(e.g., Baldry, Glazebrook & Driver 2008), these luminosities ˙
M⋆ /M⋆ ∼ 2 Gyr−1 (Elbaz et al. 2011), at which the SMGs would
correspond to stellar masses ∼ (1.5–2.5) × 1011 M⊙ , in close only need to form stars for 500 Myr in order to double in mass.
agreement with direct measurements of the relationship between We may therefore conclude, from the clustering and stellar masses
halo mass and central galaxy stellar mass for X-ray selected groups alone, that the SMGs evolve from star-forming to passive states
and clusters, for which log M⋆ ≈ 0.27 log Mhalo + 7.6 (Stott et al. relatively quickly (within a Gyr or so) after the starburst phase,
2011). and that the descendants spend most of their remaining time as
relatively passive systems. This scenario is consistent with mea-
surements of the stellar populations in ∼ 2–3 L∗ ellipticals, which
4.4 SMG lifetime and star formation history have typical ages of ∼10 Gyr and show little evidence for younger
components (e.g., Nelan et al. 2005; Allanson et al. 2009), imply-
We next estimate the SMG lifetime, making the simple assumption ing that the vast majority of stars were formed above z ∼ 2 with
that every dark matter halo of similar mass passes through an SMG little additional star formation at lower redshifts.
phase3 , so that The halo masses of SMGs may also provide insight into
nSMG the processes that prevent their descendants from forming new
tSMG = ∆t , (8)
nhalo stars. Star formation can be shut off rapidly at the end of the
where ∆t is the time interval over the redshift range covered by the SMG phase, either by exhaustion of the gas supply, or by energy
SMG sample, and nSMG and nhalo are the space densities of SMGs input from a QSO (e.g., Di Matteo, Springel & Hernquist 2005;
and DM haloes, respectively. Springel, Di Matteo & Hernquist 2005). Powerful winds are ob-
Using the halo mass function of Tinker et al. (2008), the served in luminous AGN (e.g., Feruglio et al. 2010; Fischer et al.
space density of haloes with log (Mhalo [h−1 M⊙ ]) = 12.8+0.3 2010; Sturm et al. 2011; Greene et al. 2011) and have also been
−0.5
is dnhalo /d ln M = (2.1+7.3 ) × 10−4 Mpc−3 . We adopt a space seen in some SMGs (e.g., Alexander et al. 2010, Harrison et al. in
−1.5
−5 −3
density of SMGs at z ∼ 2 of ∼ 2 × 10 Mpc , correspond- preparation), although for the SMGs is unclear whether the winds
ing to results from previous surveys (e.g., Chapman et al. 2005; are driven by the starburst or AGN. Even if the formation of stars
Coppin et al. 2006; Schael et al. in preparation). This density is is rapidly quenched, over longer timescales the galaxy would be
∼ 50% higher than that observed in the LESS field (Wardlow et al. expected to accrete further gas from the surrounding halo, result-
ing in significant additional star formation (e.g., Bower et al. 2006;
Croton et al. 2006). Recent work suggests that energy from ac-
2 creting supermassive black holes, primarily in the form of radio-
Note that here we use the median growth rate of haloes, which for haloes
of ∼ 1013 h−1 M⊙ is ≈35% lower than the mean growth rate, owing to
bright relativistic jets, can couple to the hot gas in the surround-
the long high-mass tail in the halo mass distribution. ing halo, producing a feedback cycle that prevents rapid cooling
3 If the average halo experiences more or fewer SMG phases in the given (e.g., Rafferty, McNamara & Nulsen 2008). This mechanical black
time interval, the lifetime of each episode will be correspondingly shorter hole feedback is an key ingredient of successful models for the pas-
or longer, respectively. sive galaxy population (e.g., Croton et al. 2006; Bower et al. 2006;
c 2011 RAS, MNRAS 000, 1–13
10. 10 Ryan C. Hickox et al.
Springel, Di Matteo & Hernquist 2005; Hopkins et al. 2006), sec-
1.2 ular instabilities (e.g., Mo, Mao & White 1998; Bower et al. 2006;
halo mass crossing rate
x molecular gas fraction Genzel et al. 2008) or accretion of recycled cold gas from evolved
normalized number counts; fmol
1.0 stars (Ciotti & Ostriker 2007; Ciotti, Ostriker & Proga 2010), and
is similar to the mass at which galaxy populations transition from
0.8 star-forming to passive (e.g., Coil et al. 2008; Brown et al. 2008;
Conroy & Wechsler 2009; Tinker & Wetzel 2010). The observed
0.6 fmol clustering of SMGs at z ∼ 2 from the present work is con-
sistent with that for QSOs, as well as highly active obscured
objects including powerful obscured AGN (H11; Allevato et al.
0.4
2011) and dust-obscured galaxies (Brodwin et al. 2008). Thus
these may indeed represent different phases in the same evolu-
0.2 tionary sequence, and energy input from the QSO may be re-
sponsible for the rapid quenching of star formation at the end
0.0
of the SMG phase (e.g., Di Matteo, Springel & Hernquist 2005;
0 2 4 6
Springel, Di Matteo & Hernquist 2005) as discussed in § 4.4.
z
A connection with QSOs may imply that triggering of SMGs
is also related (at least indirectly) to the mass of the parent DM
Figure 8. Redshift distribution of LESS SMGs (Wardlow et al. 2011), com- halo. In this case, the evolution of large-scale structure may broadly
pared to the simple models for SMG triggering based on the rate at which
explain why the SMG population peaks at z ∼ 2.5 and falls at
haloes cross a threshold mass Mthresh = 6 × 1012 h−1 M⊙ (see § 4.5).
The uncertainties in the number counts are an approximation of Poisson
higher and lower redshifts. In the simplest possible such scenario,
counting statistics (Gehrels 1986). The black dotted line shows the (arbi- SMG activity is triggered when the halo reaches a certain mass
trarily normalized) number of haloes crossing this threshold in each red- Mhalo = Mthresh (see Figure 16 of Hickox et al. 2009 for a
shift interval (Equation 9) while the dashed red line shows this distribution schematic illustration of this picture). In a given volume, the num-
multiplied by the evolution in the molecular gas fraction (Equation 10), ber of haloes crossing this mass threshold as a function of redshift
where fmol is taken from the model predictions of Lagos et al. (2011) and is:
is shown by the gray dot-dashed line. The remarkable agreement between dNthresh dV
the second model and the observed number counts suggests that the evolu- ˙
∝ nhalo (Mthresh , z)Mhalo (Mthresh , z)tSMG , (9)
tion of the SMG population can be described simply in terms of two quan-
dz dz
tities: the growth of DM structures and the variation with redshift of the ˙
where nhalo and Mhalo are the number density (e.g., Tinker et al.
molecular gas fraction in galaxies. 2008) and typical growth rate (Fakhouri, Ma & Boylan-Kolchin
2010), respectively, of haloes of mass Mthresh at redshift z, tSMG
is the SMG lifetime, and dV /dz is the differential comoving vol-
Bower, McCarthy & Benson 2008; Somerville et al. 2008). Inter- ume over the survey area. If an SMG is triggered every time a halo
estingly, the clustering of radio galaxies at z 0.8 indicates that reaches Mthresh , then the observed number density of SMGs will
they reside in haloes of mass 1013 h−1 M⊙ (e.g., Wake et al. be proportional to dNthresh /dz. However, the huge star forma-
2008a; Hickox et al. 2009; Mandelbaum et al. 2009; Donoso et al. tion rates of SMGs require a large reservoir of molecular gas (e.g.,
2010; Fine et al. 2011), precisely the environments that will host Greve et al. 2005; Tacconi et al. 2006, 2008), and the molecular gas
the descendants of SMGs. Thus the strong observed clustering for fraction increases strongly with redshift (e.g., Tacconi et al. 2010;
SMGs can relate them directly to the radio-bright active galactic Geach et al. 2011; Lagos et al. 2011). This evolution may explain
nucleus population that may regulate their subsequent star forma- why the most powerful starbursts at low redshift (ULIRGs) have
tion. lower typical SFRs than z ∼ 2 SMGs (e.g., Le Floc’h et al. 2005;
Rodighiero et al. 2010). Therefore it may be reasonable to assume
that the number counts of SMGs also depend on fmol , with the
4.5 Evolutionary links with QSOs and the SMG redshift simplest possible prescription being:
distribution dNSMG dNthresh
∝ fmol (z). (10)
Finally, the observed clustering of SMGs provides insights into dz dz
the processes that trigger and (possibly) shut off their rapid star In Figure 8 we show the observed redshift distribution of
formation activity. As discussed in § 1, powerful local starbursts LESS SMGs (Wardlow et al. 2011), compared to the distributions
(i.e. ULIRGs) are predominantly associated with major mergers predicted by Equations (9) and (10), assuming Mthresh = 6 × 1012
and appear to be associated with the fueling of luminous QSOs as h−1 M⊙ . For simplicity, the evolution in fmol is taken from pre-
part of an evolutionary sequence (e.g., Sanders et al. 1988). How- dictions of the GALFORM model of Lagos et al. (2011), which
ever it is unclear if a similar connection exists between SMGs and agrees broadly with observations (see Figure 2 of Geach et al.
high-z QSOs. One robust prediction of any evolutionary picture is 2011) and so provides a simple parameterisation of the current em-
that SMGs and QSOs must display comparable large-scale clus- pirical limits on the molecular gas fraction in galaxies. It is clear
tering, since the evolutionary timescales are significantly smaller from Figure 8 that there is remarkable correspondence between our
than those for the growth of DM haloes. At all redshifts, QSOs extremely simple prescription and the observed redshifts of SMGs.
are found in haloes of similar mass ∼ a few ×1012 h−1 M⊙ Of course this “model” does not account for a wide range of pos-
ˆ
(e.g., Croom et al. 2005; Myers et al. 2006; da Angela et al. 2008; sible complications and the normalisations of the distributions are
Ross et al. 2009; Figure 6). The characteristic Mhalo provides arbitrary. However, this exercise clearly demonstrates that if SMGs,
a strong constraint on models of QSO fueling by the major like QSOs, are found in haloes of a characteristic mass, then their
mergers of gas-rich galaxies (e.g., Kauffmann & Haehnelt 2000; observed redshift distribution may be explained simply by two ef-
c 2011 RAS, MNRAS 000, 1–13