This study compares the structural evolution of galaxies from observations in the Cosmic Assembly Near-infrared Deep Extragalactic Legacy Survey (CANDELS) to cosmological simulations with and without radiative pressure (RP) feedback. Axis ratio distributions are obtained from simulated galaxies of different stellar masses, sizes, and redshifts and compared to observed distributions from CANDELS. Preliminary results show axis ratios decrease towards higher redshifts for simulated galaxies viewed face-on, similarly to CANDELS observations, and simulations with RP feedback generally have lower axis ratios than without at z > 1.5. More analysis is needed to determine how RP feedback affects galaxy structure and morphology over cosmic time.
A statistical analysis_of_the_accuracy_of_the_digitized_magnitudes_of_photome...Sérgio Sacani
We present a statistical analysis of the accuracy of the digitized magnitudes of photometric plates on
the time scale of decades. In our examination of archival Johnson B photometry from the Harvard
DASCH archive, we nd a median RMS scatter of lightcurves of order 0.15mag over the range B
9 17 for all calibrations. Slight underlying systematics (trends or
ux discontinuities) are on a level
of . 0:2mag per century (1889{1990) for the majority of constant stars. These historic data can
be unambiguously used for processes that happen on scales of magnitudes, and need to be carefully
examined in cases approaching the noise
oor. The characterization of these limits in photometric
stability may guide future studies in their use of plate archives. We explain these limitations for the
example case of KIC8462852, which has been claimed to dim by 0:16mag per century, and show that
this trend cannot be considered as signicant.
Mapping spiral structure on the far side of the Milky WaySérgio Sacani
Little is known about the portion of the Milky Way lying beyond the Galactic center at distances
of more than 9 kiloparsec from the Sun. These regions are opaque at optical wavelengths
because of absorption by interstellar dust, and distances are very large and hard to measure.
We report a direct trigonometric parallax distance of 20:4þ2:8
2:2 kiloparsec obtained with the Very
Long Baseline Array to a water maser source in a region of active star formation. These
measurements allow us to shed light on Galactic spiral structure by locating the ScutumCentaurus
spiral arm as it passes through the far side of the Milky Way and to validate a
kinematic method for determining distances in this region on the basis of transverse motions.
Todo mundo sabe que os raios produzidos pela Estrela da Morte em Guerra nas Estrelas não pode existir na vida real, porém no universo existem fenômenos que as vezes conseguem superar até a mais surpreendente ficção.
A galáxia Pictor A, é um desses objetos que possuem fenômenos tão espetaculares quanto aqueles exibidos no cinema. Essa galáxia localiza-se a cerca de 500 milhões de anos-luz da Terra e possui um buraco negro supermassivo no seu centro. Uma grande quantidade de energia gravitacional é lançada, à medida que o material cai em direção ao horizonte de eventos, o ponto sem volta ao redor do buraco negro. Essa energia produz um enorme jato de partículas que viajam a uma velocidade próxima da velocidade da luz no espaço intergaláctico, chamado de jato relativístico.
Para obter imagens desse jato, os cientistas usaram o Observatório de Raios-X Chandra, da NASA várias vezes durante 15 anos. Os dados do Chandra, apresentados em azul nas imagens, foram combinados com os dados obtidos em ondas de rádio a partir do Australia Telescope Compact Array, e são aparesentados em vermelho nas imagens.
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.
A statistical analysis_of_the_accuracy_of_the_digitized_magnitudes_of_photome...Sérgio Sacani
We present a statistical analysis of the accuracy of the digitized magnitudes of photometric plates on
the time scale of decades. In our examination of archival Johnson B photometry from the Harvard
DASCH archive, we nd a median RMS scatter of lightcurves of order 0.15mag over the range B
9 17 for all calibrations. Slight underlying systematics (trends or
ux discontinuities) are on a level
of . 0:2mag per century (1889{1990) for the majority of constant stars. These historic data can
be unambiguously used for processes that happen on scales of magnitudes, and need to be carefully
examined in cases approaching the noise
oor. The characterization of these limits in photometric
stability may guide future studies in their use of plate archives. We explain these limitations for the
example case of KIC8462852, which has been claimed to dim by 0:16mag per century, and show that
this trend cannot be considered as signicant.
Mapping spiral structure on the far side of the Milky WaySérgio Sacani
Little is known about the portion of the Milky Way lying beyond the Galactic center at distances
of more than 9 kiloparsec from the Sun. These regions are opaque at optical wavelengths
because of absorption by interstellar dust, and distances are very large and hard to measure.
We report a direct trigonometric parallax distance of 20:4þ2:8
2:2 kiloparsec obtained with the Very
Long Baseline Array to a water maser source in a region of active star formation. These
measurements allow us to shed light on Galactic spiral structure by locating the ScutumCentaurus
spiral arm as it passes through the far side of the Milky Way and to validate a
kinematic method for determining distances in this region on the basis of transverse motions.
Todo mundo sabe que os raios produzidos pela Estrela da Morte em Guerra nas Estrelas não pode existir na vida real, porém no universo existem fenômenos que as vezes conseguem superar até a mais surpreendente ficção.
A galáxia Pictor A, é um desses objetos que possuem fenômenos tão espetaculares quanto aqueles exibidos no cinema. Essa galáxia localiza-se a cerca de 500 milhões de anos-luz da Terra e possui um buraco negro supermassivo no seu centro. Uma grande quantidade de energia gravitacional é lançada, à medida que o material cai em direção ao horizonte de eventos, o ponto sem volta ao redor do buraco negro. Essa energia produz um enorme jato de partículas que viajam a uma velocidade próxima da velocidade da luz no espaço intergaláctico, chamado de jato relativístico.
Para obter imagens desse jato, os cientistas usaram o Observatório de Raios-X Chandra, da NASA várias vezes durante 15 anos. Os dados do Chandra, apresentados em azul nas imagens, foram combinados com os dados obtidos em ondas de rádio a partir do Australia Telescope Compact Array, e são aparesentados em vermelho nas imagens.
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.
Sheet1Your Name:Section #:Part IIYourColor# ofGalaxyGalaxyObservedIndexemissionNameTypeColorB (B_T)V (V_T)(B - V)Spectra?linesDescription of spectraExample:NGC 3310spiralblue & orange11.1510.80.35Yes44241.6 to 5103.6 A, 4 -5 emission lines and 2 absorption linesNGC 224NGC 598NGC 5194NGC 4579NGC 4303NGC 5055NGC 4826NGC 3623NGC 3627NGC 628NGC 1068NGC 3031NGC 5236NGC 4501NGC 4569NGC 4548NGC 4736NGC 3351NGC 3368NGC 4192NGC 4254NGC 4321NGC 5457NGC 4594NGC 4258NGC 3556NGC 3992NGC 3034NGC 4027NGC 4314NGC 955NGC 221NGC 4472NGC 4621NGC 4649NGC 4486NGC 4552NGC 3379NGC 205NGC 2300NGC 4261NGC 4881NGC 3377UGC 145UGC 206NGC 147UGC 387NGC 185NGC 227UGC 579NGC 315UGC 610NGC 380NGC 385NGC 393NGC 392NGC 410NGC 4261NGC 430NGC 507UGC 973NGC 533Part IIIQuestions from "Appleby Galaxy Zoo Lab Project v.July 2010.doc"#1.Average color index of spirals:Average color index of ellipticals:#2.A color index of less than 0.45 is considered red.A color index greater than 0.45 is considered blue.Which are redder: spirals or ellipticals?:(#3.)Choose one of your galaxies above and copy-paste its spectrum to a word document.Use circles to identify at least 5 absorption lines ("dips").Use circles to identify at least 1 emission line ("peak").Hint: See "NGC 3310 Example spectra.doc"#4.How do elliptical and spiral spectra differ?:#5.How do the quantity of emission lines differ between galaxy types?:#6.Object ID 587731520668631247Galaxy type:Reason for classification type:http://cas.sdss.org/astro/en/tools/explore/obj.asp?id=587731520668631247
Sheet2
Sheet3
Our Expanding Universe
Description:
In the early 20th century, astronomers made an amazing discovery that changed everything they thought they understood about the universe. The discovery made was that almost every galaxy is moving away from us. Before this discovery, astronomers knew that the universe was full of stars and nebulae, but they had no idea that some of the nebulae were actually other galaxies, or that these galaxies were moving away from us.
When Hubble and Humason first made this discovery, they plotted the distance to the galaxies on one axis versus the recessional speed of the galaxies on the other axis and found that they were correlated. The tight correlation implied a fundamental relationship, which led to the calculation of what is now known as the Hubble constant. The relationship is known as Hubble’s Law. As any law in science, it merely describes the way the data behave and does not explain why. The explanation for why galaxies appear to be moving away from us at faster rates the farther they are away from us comes from the Big Bang theory. Theories seek to explain why, while laws simply describe repeated observable behavior.
According to the Big Bang theory, the Hubble constant describes the rate at which the universe is expanding. Hubble first determined the value of this constant to be 500 km/s/Mpc. This value means that for each Megaparsec of distance from us an object is, its distance from us is.
The abundance of_x_shaped_radio_sources_vla_survey_of_52_sources_with_off_axi...Sérgio Sacani
Devem existir menos buracos negros supermassivos binários nos núcleos das galáxias do que se pensava anteriormente, disse uma equipe de cientistas da Universidade de Brandeis em Waltaham, Massachussets, e do Instituto de Pesquisa Raman em Bangalore, na Índia.
A maior parte das galáxias massivas no universo devem abrigar no mínimo um buraco negro supermassivo em seus núcleos.
Quando duas galáxias colidem, seus buracos negros se juntam, formando uma dança colossal que resulta numa combinação de par. Esse processo é a mais intensa fonte de ondas gravitacionais no universo, que ainda precisam ser diretamente detectadas.
“As ondas gravitacionais representam a próxima fronteira da astrofísica, e sua detecção levará a novas ideias sobre o universo. É importante se ter a maior quantidade de informação possível sobre as fontes dessas ondas”, disse o Dr. David Roberts, um membro da equipe da Universidade de Brandeis.
Strehl Ratio with Higher-Order Parabolic FilterIJMER
In all the branches of science, engineering and technology, it is known that the output due to
an input impulse function, spatial or temporal, is never an impulse. There is a spread of the input impulse
function in the output due to the noise introduced by the physical device. It was Strehl who first
introduced the important image-quality assessment parameter “Definitionshelligkeit” or simply known
as the Strehl Ratio (SR) after his name. In this paper, we have studied this parameter for an optical system apodised with the higher-order super-resolving parabolic filters. The results obtained have been discussed graphically
A new universal formula for atoms, planets, and galaxiesIOSR Journals
In this paper a new universal formula about the rotation velocity distribution of atoms, planets, and galaxies is presented. It is based on a new general formula based on the relativistic Schwarzschild/Minkowski metric, where it has been possible to obtain expressions for the rotation velocity - and mass distribution versus the distance to the atomic nucleus, planet system centre, and galactic centre. A mathematical proof of this new formula is also given. This formula is divided into a Keplerian(general relativity)-and a relativistic(special relativity) part. For the atomic-and planet systems the Keplerian distribution is followed, which is also in accordance with observations.
According to the rotation velocity distribution of the galaxies the rotation velocity increases very rapidly from the centre and reaches a plateau which is constant out to a great distance from the centre. This is in accordance with observations and is also in accordance with the main structure of rotation velocity versus distance from different galaxy measurements.
Computer simulations were also performed to establish and verify the rotation velocity distributions in the atomic – planetary- and galaxy system, according to this paper. These computer simulations are in accordance with observations in two and three dimensions. It was also possible to study the matching percentage in these calculations showing a much higher matching percentage between theoretical and observational values by this new formula.
Distinguishing Dark Matter, Modified Gravity, and Modified Inertia with the I...Sérgio Sacani
The missing gravity in galaxies requires dark matter, or alternatively a modification of gravity
or inertia. These theoretical possibilities of fundamental importance may be distinguished by the
statistical relation between the observed centripetal acceleration of particles in orbital motion and
the expected Newtonian acceleration from the observed distribution of baryons in galaxies. Here
predictions of cold dark matter halos, modified gravity, and modified inertia are compared and tested
by a statistical sample of galaxy rotation curves from the Spitzer Photometry and Accurate Rotation
Curves database. Modified gravity under an estimated mean external field correctly predicts the
observed statistical relation of accelerations from both the inner and outer parts of rotation curves.
Taken at face value there is a 6.9σ difference between the inner and outer parts on an acceleration
plane which would be inconsistent with current proposals of modified inertia. Removing galaxies with
possible systematic concerns such as central bulges or special inclinations does not change this trend.
Cold dark matter halos predict a systematically deviating relation from the observed one. All aspects
of rotation curves are most naturally explained by modified gravity.
IOSR Journal of Applied Physics (IOSR-JAP) is an open access international journal that provides rapid publication (within a month) of articles in all areas of physics and its applications. The journal welcomes publications of high quality papers on theoretical developments and practical applications in applied physics. Original research papers, state-of-the-art reviews, and high quality technical notes are invited for publications.
Is Betelgeuse Really Rotating? Synthetic ALMA Observations of Large-scale Con...Sérgio Sacani
The evolved stages of massive stars are poorly understood, but invaluable constraints can be derived from spatially resolved observations of nearby red supergiants, such as Betelgeuse. Atacama Large Millimeter/submillimeter Array (ALMA) observations of Betelgeuse showing a dipolar velocity field have been interpreted as evidence for a projected rotation rate of about 5 km s−1. This is 2 orders of magnitude larger than predicted by single-star evolution, which led to suggestions that Betelgeuse is a binary merger. We propose instead that large-scale convective motions can mimic rotation, especially if they are only partially resolved. We support this claim with 3D CO5BOLDsimulations of nonrotating red supergiants that we postprocessed to predict ALMA images and SiO spectra. We show that our synthetic radial velocity maps have a 90% chance of being falsely interpreted as evidence for a projected rotation rate of 2 km s−1 or larger for our fiducial simulation. We conclude that we need at least another ALMA observation to firmly establish whether Betelgeuse is indeed rapidly rotating. Such observations would also provide insight into the role of angular momentum and binary interaction in the late evolutionary stages. The data will further probe the structure and complex physical processes in the atmospheres of red supergiants, which are immediate progenitors of supernovae and are believed to be essential in the formation of gravitational-wave sources.
Orbital configurations of spaceborne interferometers for studying photon ring...Sérgio Sacani
Recent advances in technology coupled with the progress of observational
radio astronomy methods resulted in achieving a major milestone of astrophysics - a direct image of the shadow of a supermassive black hole, taken
by the Earth-based Event Horizon Telescope (EHT). The EHT was able to
achieve a resolution of ∼20 µas, enabling it to resolve the shadows of the
black holes in the centres of two celestial objects: the supergiant elliptical
galaxy M87 and the Milky Way Galaxy. The EHT results mark the start of a
new round of development of next generation Very Long Baseline Interferometers (VLBI) which will be able to operate at millimetre and sub-millimetre
wavelengths. The inclusion of baselines exceeding the diameter of the Earth
and observation at as short a wavelength as possible is imperative for further development of high resolution astronomical observations. This can be
achieved by a spaceborne VLBI system. We consider the preliminary mission
design of such a system, specifically focused on the detection and analysis
of photon rings, an intrinsic feature of supermassive black holes. Optimised
Earth, Sun-Earth L2 and Earth-Moon L2 orbit configurations for the space
interferometer system are presented, all of which provide an order of magnitude improvement in resolution compared to the EHT. Such a space-borne
1. Structural Evolution of Galaxies from Cosmic Assembly Near-
infrared Deep Extragalactic Legacy Survey and Cosmological
Simulations
Vivian Tang1, Yicheng Guo2, Joel Primack3
1 Department of Astronomy and Astrophysics, University of California, Santa Cruz
2 UCO/Lick Observatory, Dept. of Astronomy and Astrophysics, University of California, Santa Cruz
3 Department of Physics, University of California, Santa Cruz
Introduction Methods
Results
Conclusion
Future Work
Acknowledgement
The main motivation for this project is to systematically compare projected axis ratio distributions under random
viewing angles in simulated galaxies to those of the observed galaxies which have unknown viewing angles. In
particular, we focus on galaxies in the range of redshift 1 to 3 in both simulation and observation.
In both observations and simulations, wealth of data allow us to do statistical studies. By looking at how the
distributions change over cosmic time, we can statistically determine how the shape and formation of galaxies
evolve.
Study done previously by van der Wel et al. have shown that observed galaxies in the lower-mass range from
CANDELS are elongated, rather than disk-like or spheroidal, and the axial ratio is skewed for higher redshift
galaxies.
To investigate this observation, we obtain the axis ratio distributions from simulated galaxies as a function of
redshift, stellar mass, size, and Sersic index with and without RP feedback and compare to those found by van
der Wel et al.
We suspect that simulated galaxies with RP feedback represent observation more correctly, thus we will also
compare the axis ratio distributions of simulated galaxies with and without RP feedback to see how RP feedback
affect each of the parameters. A subset of 35 different simulations with and without RP feedback is used for
analysis.
III. The Project: Observations vs. Simulations
T o u n d e r s t a n d
s t r u c t u r a l a n d
m o r p h o l o g i c a l
e v o l u t i o n o f
galaxies, we need to
look far back in time
and compare the
differences between
older and younger
galaxies.
Early star forming
g a l a x i e s h a v e
distorted, irregular
appearance while
present day star
forming galaxies
tend be flat disks
a n d h a v e s p i r a l
arms.
I. Observation: CANDELS
II. Cosmological Simulations: With and without
Radiative Pressure (RP) Feedback
References
I. CANDELization
High resolution images of simulated galaxies need to go
through a process called CANDELization before the analysis.
To CANDELized an image, the Sunrise radiative transfer code
is applied, as well as the Point Spread Function for the
relevant Hubble Space Telescope observations. Noise is also
added and the end result is an image with the same resolution
to those of the observed galaxies from Hubble Space
Telescope.
It is necessary for simulated images to be CANDELized since
in reality we do not observe distant galaxies with high
resolution.
II. GALFIT
After CANDELizing images, GALFIT, a data analysis algorithm that fits
2D analytic functions to galaxies, is used for image analysis. Each
function in GALFIT corresponds to a component that creates a model
for image fitting. For this project we have chosen to use a single
component fit.
Output from GALFIT contains best fit parameters which can be used
for statistical studies. These include the Sersic index, axis ratio, and
effective radius.
The Sersic index describes radial distribution of light; the effective
radius is defined as containing half of the total luminosity from the
galaxy, and the axis ratio is simply the minor axis divided by major
axis.
FIGURE 3: Model shape parameter defined by colour [4]
Determine whether simulations with RF is a more accurate representation
than those without RF by comparing findings to the axis ratio distributions
obtained previously by van der Wel et al.
To obtain axis ratio as a function of stellar mass and redshift of simulated
galaxies, in those that have been analyzed for this project as well as other
simulations by Daniel Ceverino et al. to see whether lower-mass galaxies
are elongated as observed by CANDELS.
Galaxies used for this project were selected based on acceptable
uncertainties from GALFIT. We will compare those uncertainties for the face-
on and edge-on galaxies to determine whether it has an effect on our
previous selections.
CANDLES is the largest project in history of Hubble Space Telescope with 902
assigned orbits of observing time. Equivalent to observing 4 months
consecutively, it captures images of galaxies far in deep space at high redshifts
as well as those in the local universe.
In astronomy, redshift is used to determine how far objects are in the skies. By
measuring the wavelength of emitted light from stars and galaxies, astronomer
can determine their ages, speeds, and distances away from us. The higher the
redshift, the further away they are from us.
From observation, galaxies from early epochs were smaller than present day.
They were bluer than older galaxies as the stars were younger and hotter than
older galaxies, which tend to be redder.
All simulated galaxies with and without RP feedback by Daniel Ceverino et al. [3] were done using the ART code
with resolution of 17-34 pc. In these simulations, all the input physics are known and galaxies can be viewed
under different orientations.
In galaxy simulations, an effect of RP feedback is to suppress star formation. Those that were simulated without
the mechanism of RP feedback tend to overproduce stars, which does not match well with observations. And
those that were simulated using RP feedback produced less stars, by about a factor of 2 at all redshifts.
FIGURE 1: Hubble Sequence; dividing galaxies into groups based on visual appearance. [1]
FIGURE 2: Relationship between
redshift and age of galaxies. [2]
FIGURE 4: van der Wel et al. have shown that lower-mass galaxies at higher
redshift are more elongated [4]
FIGURE 5: Before (left) and after (right) CANDELization
FIGURE6: Elliptical like
structure corresponds to a
Sersic index value of n=4.
Spiral, bulgeless disk like
structure corresponds to a
Sersic index value of n=1. [5]
FIGURE7: Axis ratio=b/a. [6]
I. Comparing Simulation with and without RP feedback
II. Face-on viewing angle
VELA04 VELA04MRP
We have chosen images of galaxies with face-on orientation which
would yield a higher axis ratio if they are disk-like or spherical, and a
lower axis ratio if they are elongated.
Images of face-on galaxies (VLEA04 and VELA04MRP) where the
axis ratios were measured to be the lowest.
For the effective radius, each of the three pairs of simulations (with and
without radiative pressure feedback) provides different indications as to
how the size evolves over time.
The axis ratios are generally lower for the RP simulations for z > 1.5; this
might be relevant to comparison with the van der Wel et al. observations.
For the face-on viewing angle, axis ratios decrease towards higher
redshifts. Although this is similar to van der Wel et al. observations, more
analysis are needed for verification.
More data analysis between simulations with and without RP are required
in order to determine how much RF changes the structure and morphology
of galaxies.
FIGURE 8: Axis ratio distributions of star forming galaxies from CANDELS. [4]
0 0.5 1 1.5 2 2.5
0
1
2
3
4
5
6
7
VELA04
VELA04MRP
Z
SersicIndex
0 0.5 1 1.5 2 2.5
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
VELA04
VELA04MRP
Z
AxisRatio
0 0.5 1 1.5 2 2.5
0
2
4
6
8
10
12
14
VELA04
VELA04MRP
Z
EffectiveRadius
0 0.5 1 1.5 2 2.5 3 3.5 4
0
1
2
3
4
VELA15
VELA15MRP
Z
SersicIndex
0 0.5 1 1.5 2 2.5 3 3.5 4
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
VELA15
VELA15MRP
Z
AxisRatio
0 0.5 1 1.5 2 2.5 3 3.5 4
0
2
4
6
8
10
12
VELA15
VELA15MRP
Z
EffectiveRadius
0 0.5 1 1.5 2 2.5 3 3.5 4
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Face-on
VELA02
VELA02MRP
Z
AxisRatio
0 0.5 1 1.5 2 2.5
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Face-onVELA04
VELA04MRP
Z
AxisRatio
0 0.5 1 1.5 2 2.5 3 3.5
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Face-on
VELA15
VELA15MRP
Z
AxisRatio
0 0.5 1 1.5 2 2.5 3
0
1
2
3
4
5
6
VELA02
VELA02MRP
Z
SersicIndex
0 0.5 1 1.5 2 2.5 3
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
VELA02
VELA02MRP
Z
AxisRatio
0 0.5 1 1.5 2 2.5 3
0
1
2
3
4
5
6
7
8
9
VELA02
VELA02MRP
Z
EffectiveRadius
[1] “CANDELS galaxies reveal the Hubble Sequence throughout the Universe's
history”. August 2013. ESA/Hubble Press Release (http://spacetelescope.org/
images/heic1315e/).
[2] Sandra M. Faber, Henry C. Ferguson, David C. Koo, Joel R. Primack & Trudy E.
Bell. “Staring Back to Cosmic Dawn”. June 2014. Sky & Telescope (http://
hipacc.ucsc.edu/NewsArchive/June2014-S&T-CANDELS-CoverStory.pdf).
[3] Daniel Ceverino et al. 2014, Radiative feedback and the low efficiency of
galaxy formation in low-mass haloes at high redshift, MNRAS 442, 1545.
[4] A. van der Wel 2014, Geometry of Star-forming Galaxies from SDSS, 3D-HST,
and CANDELS, arXiv:1407.4233.
[5] Chien Y. Peng. August 2003. GALFIT User’s Manual (http://
users.obs.carnegiescience.edu/peng/work/galfit/README.pdf).
[6] Amit6. “Ellipse axis.svg”. April 2009. Wikimedia Commons (http://
commons.wikimedia.org/wiki/File:Ellipse_axis.svg).
This research is supported by the Julie Packard Summer Scholarship and the
Ron Ruby Memorial Scholarship. Special thanks to postdoc Yicheng Guo
here at UCSC for his great assistance with GALFIT and also to Professor
Primack for his invaluable advice and support.
VELA simulations do not have RP feedback. VELAMRP simulations have RP feedback.
Sunday, January 18, 2015