Slides from 1-hour talk about ongoing research on stellar activity with data from NASA's Kepler space telescope. Stellar flares and starspots are the subject of investigation here.
Applications Of Computer Science in AstronomyAhmed Abuzuraiq
A presentations I did for an Astronomy course about the role that computer science plays in in astronomy , Examples included are
Adaptive Optics,Automated Ground Observatory,Galaxies Classifications and Simulations.
The Square Kilometre Array (SKA), even in its first phase (SKA Phase 1, or SKA1) will be the largest ground-based astronomical facility ever built, with unprecedented sensitivity in the frequency ranges for local to highly redshifted HI, and future expansion up to 25 GHz. The range of science cases that the SKA telescopes will cater for will also be the largest of any research facility, from the Epoch of Reionization (EoR) and the Cosmic Down (CD), to tests of Einstein’s General Relativity, to finding all detectable pulsars in the Milky Way, and helping with the Cradle of Life case for Astrobiology. In this talk we will go through the different science cases, with emphasis in those with the most cosmological significance, such as EoR, CD, and probing General Relativity. (Talk presented at CosmoAndes 2018.)
Applications Of Computer Science in AstronomyAhmed Abuzuraiq
A presentations I did for an Astronomy course about the role that computer science plays in in astronomy , Examples included are
Adaptive Optics,Automated Ground Observatory,Galaxies Classifications and Simulations.
The Square Kilometre Array (SKA), even in its first phase (SKA Phase 1, or SKA1) will be the largest ground-based astronomical facility ever built, with unprecedented sensitivity in the frequency ranges for local to highly redshifted HI, and future expansion up to 25 GHz. The range of science cases that the SKA telescopes will cater for will also be the largest of any research facility, from the Epoch of Reionization (EoR) and the Cosmic Down (CD), to tests of Einstein’s General Relativity, to finding all detectable pulsars in the Milky Way, and helping with the Cradle of Life case for Astrobiology. In this talk we will go through the different science cases, with emphasis in those with the most cosmological significance, such as EoR, CD, and probing General Relativity. (Talk presented at CosmoAndes 2018.)
Evidence for reflected_lightfrom_the_most_eccentric_exoplanet_knownSérgio Sacani
Planets in highly eccentric orbits form a class of objects not seen within our Solar System. The most extreme case known amongst these objects is the planet orbiting HD 20782, with an orbital period of 597 days and an eccentricity of 0.96. Here we present new data and analysis for this system as part of the Transit Ephemeris Refinement and Monitoring Survey (TERMS). We obtained CHIRON spectra to perform an independent estimation of the fundamental stellar parameters. New radial velocities from AAT and PARAS observations during periastron passage greatly improve our knowledge of the eccentric nature of the orbit. The combined analysis of our Keplerian orbital and Hipparcos astrometry show that the inclination of the planetary orbit is > 1.22◦, ruling out stellar masses for the companion. Our long-term robotic photometry show that the star is extremely stable over long timescales. Photometric monitoring of the star during predicted transit and periastron times using MOST rule out a transit of the planet and reveal evidence of phase variations during periastron. These possible photometric phase variations may be caused by reflected light from the planet’s atmosphere and the dramatic change in star–planet separation surrounding the periastron passage.
Orbit design for exoplanet discovery spacecraft dr dora musielak 1 april 2019Dora Musielak, Ph.D.
Most exoplanets have been discovered with space telescopes. Starting with an overview of rocket propulsion, this presentation introduces spacecraft trajectories in the Sun-Earth-Moon System, focusing especially on those appropriate for exoplanet detection spacecraft. It reviews past, present, and future exoplanet discovery missions.
Beyond the Kuiper Belt Edge: New High Perihelion Trans-Neptunian Objects With...Sérgio Sacani
We are conducting a survey for distant solar system objects beyond the Kuiper
Belt edge ( 50 AU) with new wide-field cameras on the Subaru and CTIO tele-
scopes. We are interested in the orbits of objects that are decoupled from the
giant planet region in order to understand the structure of the outer solar sys-
tem, including whether a massive planet exists beyond a few hundred AU as first
reported in Trujillo and Sheppard (2014). In addition to discovering extreme
trans-Neptunian objects detailed elsewhere, we have found several objects with
high perihelia (q > 40 AU) that differ from the extreme and inner Oort cloud
objects due to their moderate semi-major axes (50 < a < 100 AU) and eccen-
tricities (e . 0.3). Newly discovered objects 2014 FZ71 and 2015 FJ345 have
the third and fourth highest perihelia known after Sedna and 2012 VP113, yet
their orbits are not nearly as eccentric or distant. We found several of these high
perihelion but moderate orbit objects and observe that they are mostly near Nep-
tune mean motion resonances and have significant inclinations (i > 20 degrees).
These moderate objects likely obtained their unusual orbits through combined
interactions with Neptune’s mean motion resonances and the Kozai resonance,
similar to the origin scenarios for 2004 XR190. We also find the distant 2008
ST291 has likely been modified by the MMR+KR mechanism through the 6:1
Neptune resonance. We discuss these moderately eccentric, distant objects along
with some other interesting low inclination outer classical belt objects like 2012
FH84 discovered in our ongoing survey.
We report the discovery of a new Kepler transiting circumbinary planet (CBP).
This latest addition to the still-small family of CBPs defies the current trend of known
short-period planets orbiting near the stability limit of binary stars. Unlike the previous
discoveries, the planet revolving around the eclipsing binary system Kepler-1647 has
a very long orbital period ( 1100 days) and was at conjunction only twice during
the Kepler mission lifetime. Due to the singular configuration of the system, Kepler-
1647b is not only the longest-period transiting CBP at the time of writing, but also one
of the longest-period transiting planets. With a radius of 1:060:01 RJup it is also the
largest CBP to date. The planet produced three transits in the light-curve of Kepler-
1647 (one of them during an eclipse, creating a syzygy) and measurably perturbed the
times of the stellar eclipses, allowing us to measure its mass to be 1:520:65 MJup.
The planet revolves around an 11-day period eclipsing binary consisting of two Solarmass
stars on a slightly inclined, mildly eccentric (ebin = 0:16), spin-synchronized
orbit. Despite having an orbital period three times longer than Earth’s, Kepler-1647b is
in the conservative habitable zone of the binary star throughout its orbit.
Seismic data Interpretation On Dhodak field PakistanJamal Ahmad
I (Jamal Ahmad) presented this on 21 Feb, 2009 to defend my M.Phil dissertation in Geophysics at QAU, Islamabad, Pakistan. For more information about this, you may contact me directly at jamal.qau@gmail.com.
Large turbulent reservoirs of cold molecular gas around high-redshift starbur...Sérgio Sacani
Starburst galaxies at the peak of cosmic star formation1
are among
the most extreme star-forming engines in the Universe, producing
stars over about 100 million years (ref. 2). The star-formation
rates of these galaxies, which exceed 100 solar masses per year,
require large reservoirs of cold molecular gas3
to be delivered to
their cores, despite strong feedback from stars or active galactic
nuclei4,5
. Consequently, starburst galaxies are ideal for studying the
interplay between this feedback and the growth of a galaxy6
. The
methylidyne cation, CH+, is a most useful molecule for such studies
because it cannot form in cold gas without suprathermal energy
input, so its presence indicates dissipation of mechanical energy7–9
or strong ultraviolet irradiation10,11. Here we report the detection of
CH+ (J=1–0) emission and absorption lines in the spectra of six
lensed starburst galaxies12–15 at redshifts near 2.5. This line has
such a high critical density for excitation that it is emitted only in
very dense gas, and is absorbed in low-density gas10. We find that
the CH+ emission lines, which are broader than 1,000 kilometres
per second, originate in dense shock waves powered by hot galactic
winds. The CH+ absorption lines reveal highly turbulent reservoirs
of cool (about 100 kelvin), low-density gas, extending far (more than
10 kiloparsecs) outside the starburst galaxies (which have radii of
less than 1 kiloparsec). We show that the galactic winds sustain
turbulence in the 10-kiloparsec-scale environments of the galaxies,
processing these environments into multiphase, gravitationally
bound reservoirs. However, the mass outflow rates are found to be
insufficient to balance the star-formation rates. Another mass input
is therefore required for these reservoirs, which could be provided by
ongoing mergers16 or cold-stream accretion17,18. Our results suggest
that galactic feedback, coupled jointly to turbulence and gravity,
extends the starburst phase of a galaxy instead of quenching it
Evidence for reflected_lightfrom_the_most_eccentric_exoplanet_knownSérgio Sacani
Planets in highly eccentric orbits form a class of objects not seen within our Solar System. The most extreme case known amongst these objects is the planet orbiting HD 20782, with an orbital period of 597 days and an eccentricity of 0.96. Here we present new data and analysis for this system as part of the Transit Ephemeris Refinement and Monitoring Survey (TERMS). We obtained CHIRON spectra to perform an independent estimation of the fundamental stellar parameters. New radial velocities from AAT and PARAS observations during periastron passage greatly improve our knowledge of the eccentric nature of the orbit. The combined analysis of our Keplerian orbital and Hipparcos astrometry show that the inclination of the planetary orbit is > 1.22◦, ruling out stellar masses for the companion. Our long-term robotic photometry show that the star is extremely stable over long timescales. Photometric monitoring of the star during predicted transit and periastron times using MOST rule out a transit of the planet and reveal evidence of phase variations during periastron. These possible photometric phase variations may be caused by reflected light from the planet’s atmosphere and the dramatic change in star–planet separation surrounding the periastron passage.
Orbit design for exoplanet discovery spacecraft dr dora musielak 1 april 2019Dora Musielak, Ph.D.
Most exoplanets have been discovered with space telescopes. Starting with an overview of rocket propulsion, this presentation introduces spacecraft trajectories in the Sun-Earth-Moon System, focusing especially on those appropriate for exoplanet detection spacecraft. It reviews past, present, and future exoplanet discovery missions.
Beyond the Kuiper Belt Edge: New High Perihelion Trans-Neptunian Objects With...Sérgio Sacani
We are conducting a survey for distant solar system objects beyond the Kuiper
Belt edge ( 50 AU) with new wide-field cameras on the Subaru and CTIO tele-
scopes. We are interested in the orbits of objects that are decoupled from the
giant planet region in order to understand the structure of the outer solar sys-
tem, including whether a massive planet exists beyond a few hundred AU as first
reported in Trujillo and Sheppard (2014). In addition to discovering extreme
trans-Neptunian objects detailed elsewhere, we have found several objects with
high perihelia (q > 40 AU) that differ from the extreme and inner Oort cloud
objects due to their moderate semi-major axes (50 < a < 100 AU) and eccen-
tricities (e . 0.3). Newly discovered objects 2014 FZ71 and 2015 FJ345 have
the third and fourth highest perihelia known after Sedna and 2012 VP113, yet
their orbits are not nearly as eccentric or distant. We found several of these high
perihelion but moderate orbit objects and observe that they are mostly near Nep-
tune mean motion resonances and have significant inclinations (i > 20 degrees).
These moderate objects likely obtained their unusual orbits through combined
interactions with Neptune’s mean motion resonances and the Kozai resonance,
similar to the origin scenarios for 2004 XR190. We also find the distant 2008
ST291 has likely been modified by the MMR+KR mechanism through the 6:1
Neptune resonance. We discuss these moderately eccentric, distant objects along
with some other interesting low inclination outer classical belt objects like 2012
FH84 discovered in our ongoing survey.
We report the discovery of a new Kepler transiting circumbinary planet (CBP).
This latest addition to the still-small family of CBPs defies the current trend of known
short-period planets orbiting near the stability limit of binary stars. Unlike the previous
discoveries, the planet revolving around the eclipsing binary system Kepler-1647 has
a very long orbital period ( 1100 days) and was at conjunction only twice during
the Kepler mission lifetime. Due to the singular configuration of the system, Kepler-
1647b is not only the longest-period transiting CBP at the time of writing, but also one
of the longest-period transiting planets. With a radius of 1:060:01 RJup it is also the
largest CBP to date. The planet produced three transits in the light-curve of Kepler-
1647 (one of them during an eclipse, creating a syzygy) and measurably perturbed the
times of the stellar eclipses, allowing us to measure its mass to be 1:520:65 MJup.
The planet revolves around an 11-day period eclipsing binary consisting of two Solarmass
stars on a slightly inclined, mildly eccentric (ebin = 0:16), spin-synchronized
orbit. Despite having an orbital period three times longer than Earth’s, Kepler-1647b is
in the conservative habitable zone of the binary star throughout its orbit.
Seismic data Interpretation On Dhodak field PakistanJamal Ahmad
I (Jamal Ahmad) presented this on 21 Feb, 2009 to defend my M.Phil dissertation in Geophysics at QAU, Islamabad, Pakistan. For more information about this, you may contact me directly at jamal.qau@gmail.com.
Large turbulent reservoirs of cold molecular gas around high-redshift starbur...Sérgio Sacani
Starburst galaxies at the peak of cosmic star formation1
are among
the most extreme star-forming engines in the Universe, producing
stars over about 100 million years (ref. 2). The star-formation
rates of these galaxies, which exceed 100 solar masses per year,
require large reservoirs of cold molecular gas3
to be delivered to
their cores, despite strong feedback from stars or active galactic
nuclei4,5
. Consequently, starburst galaxies are ideal for studying the
interplay between this feedback and the growth of a galaxy6
. The
methylidyne cation, CH+, is a most useful molecule for such studies
because it cannot form in cold gas without suprathermal energy
input, so its presence indicates dissipation of mechanical energy7–9
or strong ultraviolet irradiation10,11. Here we report the detection of
CH+ (J=1–0) emission and absorption lines in the spectra of six
lensed starburst galaxies12–15 at redshifts near 2.5. This line has
such a high critical density for excitation that it is emitted only in
very dense gas, and is absorbed in low-density gas10. We find that
the CH+ emission lines, which are broader than 1,000 kilometres
per second, originate in dense shock waves powered by hot galactic
winds. The CH+ absorption lines reveal highly turbulent reservoirs
of cool (about 100 kelvin), low-density gas, extending far (more than
10 kiloparsecs) outside the starburst galaxies (which have radii of
less than 1 kiloparsec). We show that the galactic winds sustain
turbulence in the 10-kiloparsec-scale environments of the galaxies,
processing these environments into multiphase, gravitationally
bound reservoirs. However, the mass outflow rates are found to be
insufficient to balance the star-formation rates. Another mass input
is therefore required for these reservoirs, which could be provided by
ongoing mergers16 or cold-stream accretion17,18. Our results suggest
that galactic feedback, coupled jointly to turbulence and gravity,
extends the starburst phase of a galaxy instead of quenching it
Line Spectra and Doppler Shifts One way that astronomers detect exopla.pdfatexsalem
Line Spectra and Doppler Shifts One way that astronomers detect exoplanets is by observing the
wobble of their host stars via doppler shifts. This is known as the radial velocity technique. The
simulated spectra provided on the last page show the position of a 1-solar-mass star's hydrogen-
alpha absorption line over time. In the laboratory (at rest), this absorption line occurs 656
nanometers. 4) Calculate the star's radial velocity from each spectrum using the doppler
equation, and fill in the table provided. Then, sketch the associated graph. 5) Estimate the period
of this system's orbit based on your graph. (Measure the time between two peaks or two troughs.)
Convert your answer to years. 6) Calculate the semi-major axis of this exoplanet's orbit using
Kepler's law. How does this compare to the orbit of Mercury? (This exoplanet is known as a "hot
Jupiter." Does the nickname make sense?) Data.
In this deck from DOE CSGF 2019, Chelsea Harris from the University of Michigan presents: Making Supernovae with Jets.
"Supernovae are the explosions of stars. One reason they are fundamentally important is they create and disperse elements heavier than carbon throughout the universe. Different stars explode in different ways, but the most common supernova type is from massive stars (greater than 10 times the mass of the sun) whose cores collapse to form a neutron star or black hole – "core collapse supernovae" or CC SNe. Even among massive stars, though, there are differences that can affect the outcome of core collapse. I am specifically interested in progenitors whose cores are rotating and magnetic (magnetorotational). Such cores may experience instabilities after collapse that launch a fast jet, which could rescue r-process elements formed near the proto-neutron star from destruction. The instabilities can also add power to the explosion and relieve tension between observations and theory. In addition to running simulations with existing FLASH code modules, I am developing a FLASH hydrodynamics module, SparkJoy, to perform these simulations at high order. These projects are part of a DOE INCITE project to explore progenitor effects on CC SNe and of the DOE SciDAC program "Towards Exascale Astrophysics of Mergers and Supernovae," a nationwide collaboration of supernova theorists unprecedented in its collaborative scale. Research like mine is made much easier at Michigan State University through the Department of Computational Mathematics, Science, and Engineering which, like the DOE CSGF, brings together members from different areas to share knowledge and strengthen each other's research."
Watch the video: https://wp.me/p3RLHQ-lr0
Learn more: https://www.krellinst.org/csgf/conf/2019/video/charris
Sign up for our insideHPC Newsletter: http://insidehpc.com/newsletter
Be sure to show work for 4-6- One way that astronomers detect exopla.pdfrdzire2014
Be sure to show work for 4-6.
One way that astronomers detect exoplanets is by observing the wobble of their host stars via
doppler shifts. This is known as the radial velocity technique. The simulated spectra provided on
the last page show the position of a 1-solar-mass star's hydrogen-alpha absorption line over time.
In the laboratory (at rest), this absorption line occurs 656 nanometers. 4) Calculate the star's
radial velocity from each spectrum using the doppler equation, and fill in the table provided.
Then, sketch the associated graph. 5) Estimate the period of this system's orbit based on your
graph. (Measure the time between two peaks or two troughs.) Convert your answer to years. 6)
Calculate the semi-major axis of this exoplanet's orbit using Kepler's law. How does this
compare to the orbit of Mercury? (This exoplanet is known as a "hot Jupiter." Does the nickname
make sense?) Data Ti.
The James Webb Space Telescope is NASA's next flagship mission. Webb will revolutionize astronomy in the infrared like the Hubble Space Telescope has done for the visible portion of the spectrum over the last 22 years. Webb will reveal the story of the formation of the first starts and galaxies, investigate the processes of planet formation, and trace the origins of life.
Combining special relativity, general relativity and quantum mechanics.pdfEran Akiva Sinbar
This presentation combines the surprising non-local features in physics
quantum entanglement in space (“spooky action at a distance” – Albert Einstein, EPR paradox ).
The delayed choice quantum eraser, the delayed particle/wave choice in the double slit experiment.
Special relativity – for a photon, all spacetime is concentrated to a singular infinitely small point.
General relativity – for a gravitational wave, all spacetime is concentrated to a singular infinitely small point.
Schrodinger's wave equation predicts that a particle can be located throughout spacetime until it is measured, and general relativity predicts non-local worm holes through spacetime.
American Astronautical Society, Astronauts and Robots: Partners in Space Exploration, May 12-13, 2015 - http://astronautical.org/event/astronauts-robots
Unit 8 - Information and Communication Technology (Paper I).pdfThiyagu K
This slides describes the basic concepts of ICT, basics of Email, Emerging Technology and Digital Initiatives in Education. This presentations aligns with the UGC Paper I syllabus.
Embracing GenAI - A Strategic ImperativePeter Windle
Artificial Intelligence (AI) technologies such as Generative AI, Image Generators and Large Language Models have had a dramatic impact on teaching, learning and assessment over the past 18 months. The most immediate threat AI posed was to Academic Integrity with Higher Education Institutes (HEIs) focusing their efforts on combating the use of GenAI in assessment. Guidelines were developed for staff and students, policies put in place too. Innovative educators have forged paths in the use of Generative AI for teaching, learning and assessments leading to pockets of transformation springing up across HEIs, often with little or no top-down guidance, support or direction.
This Gasta posits a strategic approach to integrating AI into HEIs to prepare staff, students and the curriculum for an evolving world and workplace. We will highlight the advantages of working with these technologies beyond the realm of teaching, learning and assessment by considering prompt engineering skills, industry impact, curriculum changes, and the need for staff upskilling. In contrast, not engaging strategically with Generative AI poses risks, including falling behind peers, missed opportunities and failing to ensure our graduates remain employable. The rapid evolution of AI technologies necessitates a proactive and strategic approach if we are to remain relevant.
Macroeconomics- Movie Location
This will be used as part of your Personal Professional Portfolio once graded.
Objective:
Prepare a presentation or a paper using research, basic comparative analysis, data organization and application of economic information. You will make an informed assessment of an economic climate outside of the United States to accomplish an entertainment industry objective.
How to Make a Field invisible in Odoo 17Celine George
It is possible to hide or invisible some fields in odoo. Commonly using “invisible” attribute in the field definition to invisible the fields. This slide will show how to make a field invisible in odoo 17.
The French Revolution, which began in 1789, was a period of radical social and political upheaval in France. It marked the decline of absolute monarchies, the rise of secular and democratic republics, and the eventual rise of Napoleon Bonaparte. This revolutionary period is crucial in understanding the transition from feudalism to modernity in Europe.
For more information, visit-www.vavaclasses.com
2024.06.01 Introducing a competency framework for languag learning materials ...Sandy Millin
http://sandymillin.wordpress.com/iateflwebinar2024
Published classroom materials form the basis of syllabuses, drive teacher professional development, and have a potentially huge influence on learners, teachers and education systems. All teachers also create their own materials, whether a few sentences on a blackboard, a highly-structured fully-realised online course, or anything in between. Despite this, the knowledge and skills needed to create effective language learning materials are rarely part of teacher training, and are mostly learnt by trial and error.
Knowledge and skills frameworks, generally called competency frameworks, for ELT teachers, trainers and managers have existed for a few years now. However, until I created one for my MA dissertation, there wasn’t one drawing together what we need to know and do to be able to effectively produce language learning materials.
This webinar will introduce you to my framework, highlighting the key competencies I identified from my research. It will also show how anybody involved in language teaching (any language, not just English!), teacher training, managing schools or developing language learning materials can benefit from using the framework.
Spots and Flares, Stellar Activity with Kepler (James R. A. Davenport, 2014)
1. Spots & Flares
Stellar Activity with Kepler
Leslie Hebb (Hobart & William Smith)
James R. A. Davenport (University of Washington)
!1
Suzanne L. Hawley (University of Washington)
Boston University — 2014 February 25
2. Spots & Flares
Observable byproducts of magnetic fields
"If the Sun did not have a magnetic field,
it would be as uninteresting a star
as most astronomers believe it to be."
-R.B. Leighton (or E. Parker)
!2
8. Flares - why we care?
A few reasons…
• Insight into properties of stellar dynamo/interior
• Habitability (of our planet, and others)
• Potential age-tracer for stars
!8
19. Massive Flare Sample!
• 6107 flares, spanning 300 days
• most of any star besides the Sun!
• 15% complex
• energy range: Log E = 27-33 erg
• complete to Log E ~31
!19
26. RelativeFlux
Some flares not well fit by template
Davenport in prep
Caused by different physical
morphology (e.g. arcade)?
Active region rolling off limb? !26
27. Hawley in prep
No correlation between flares & spot
1 month short cadence
!27
28. Big questions still await us!
• Dependence of morphology
on stellar properties?
• Does decay rate depend on
total flare energy?
• Can we resolve peak shape?
• More detailed understanding
of complex events
!28
29. GJ 1245 AB(C):
a novel system for spots & flares
2 distinct periods
Lurie in prep!29
30. GJ 1245 AB(C):
a novel system for spots & flares
2 distinct periods
!30
31. GJ 1245 AB(C):
a novel system for spots & flares
HST
2”
Kepler Pixel
!31
32. GJ 1245 AB(C):
a novel system for spots & flares
HST
2”
Kepler Pixel
!32
36. Strassmeier (1999)
• Observed across range of
mass, evolutionary phase
• Trace B field geometry,
rotation, differential rotation
!
• Evolve on timescales from
days to years (perhaps longer!)
Starspots
a generic result of B fields
SDO
Carroll (2012)
!36
37. – Stellar rotation rate
– Spot sizes
– Differential rotation rate
– Spot Lifetimes
– Spot evolution over stellar cycles
– Evolution with stellar age
Starspots:
Parameters/Physics of Interest
!37
38. Davenport in prep
GJ 1243: M4, Prot=0.59 days,
300days1-min data, 13 Quarters 30-min data
!38
44. Phase
Davenport in prep
GJ 1243 Differential Rotation!
“Equator-Lap-Pole” time of
700-1200 days
(assume Solar-like diff. rot.)
!44
45. Phase
Davenport in prep
GJ 1243 Differential Rotation!
Spot lifetimes: 150-500 days for 2nd spot
>4 years for 1st spot
!45
46. Davenport in prep
GJ 1243 2-spot lightcurve model
Phase
1-spot model preferredunclear
!46
47. Time
Time
Phase
Phase
Some other M dwarfs
with Prot<2 day
!
A wide range of starspot-
phase evolution!
~20 other short P dM’s
in Kepler 30-min data
!47
54. Kepler 63: 40-80 days ! ! (G2, P=5d)!
Sun: 115 days !! ! ! ! (G2, P=25d)!
!
AB Dor: 110 days ! ! ! ! (K0, P=0.5d)!
Speedy Mic: 191 days ! ! (K3, P=0.4d)!
!
GJ 1243: 700-1200 days ! (M4, P=0.6d)!
HK Aqr: [-1449-449] days ! (M0, P=0.4d)
Expectation: lap times increase with
later spectral type
e.g. Kueker (2011), Barnes (2005)
See excellent recent paper by
Timo Reinhold et al. (2013)
Equator-Lap-Pole time comparisons
!54
65. Fitting
challenges…
• MCMC very expensive
• Parameter space “target” very small
• Need to run over many “windows” of time
• Spots can evolve on few-transit
(or few rotation) timescales
!65
66. The future: measure contrast
from umbra & penumbra?
NewSolarTelescope(2010)
!66
68. The future: compare detailed spot
properties with gyrochronology
• Spot timescales
• Spot contrast(s)
• Differential rotation rate
& direction
(Prot spin down with stellar age)
!68
69. The future: find flares in every Kepler
target, learn about B fields en masse
• Comparable to transit-finding
(just inverted)
• Tackle flare physics questions
(e.g. dependence on star properties)
• Include gyrochronology, flares as age indicator?
(viable for LSST?)
!69
71. Summary
Thanks!
• Largest sample of flares on any star,
create flare template
• One of slowest differential rotation
rates ever measured
• Detailed starspot properties
observable in transiting systems
• Kepler opening door to statistical
understanding of stellar activity!
!71