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Mission Critical Risk-Taking:
The Hubble Deep Field
Robert Williams
Space Telescope Inst/Johns Hopkins U.
GlobForeA)SM1	
  
Kapteyn	
  1922	
  
Hubble	
  1929	
  
Kepler	
  1596	
  
Concepts of the Universe
Digges	
  1576	
  
Kravtsov & Wechsler 2010, U. Chicago
.	
  	
  	
  	
  .	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  .	
  
Springel 2013 Max-Planck-Institut

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Senior_Project
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σT 4 where σ is the Stefan-Boltzmann constant. 1) The document discusses a computer simulation called Starsmasher that astrophysicists use to model binary star mergers like that of V1309 Scorpii. 2) Starsmasher uses smoothed particle hydrodynamics (SPH) which treats fluids as interacting parcels to efficiently simulate gas dynamics in stellar events. 3) The document provides details on how Starsmasher simulations work and the goals of modeling the light curve and visual appearance of V1309 Scorpii's merger event.

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This document discusses three key questions in cosmology: dark matter, inflation, and dark energy. It provides evidence for dark matter from early observations of galaxy rotation curves and clusters. It also summarizes modern evidence from Planck for the matter content of the universe. Regarding inflation, it discusses the generic predictions and open questions about the inflaton field. For dark energy, it reviews evidence from supernovae and Planck and discusses theoretical challenges like the fine-tuning and coincidence problems. It also outlines proposed and ongoing experiments to better understand dark matter, inflation, and dark energy.

HSTLaunch	
  
April	
  1990	
  
HSTSchema8c	
  
Mirror:	
  2.4m	
  diameter	
  
Mass:	
  	
  11,000	
  	
  Kg	
  
Length:	
  	
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Development	
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Opera8ons	
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Asteroseismic constraints on K giants make it possible to infer radii, masses and ages of tens of thousands of field stars. Tests against independent estimates of these properties are however scarce, especially in the metal-poor regime. Here, we report the detection of solar-like oscillations in 8 stars belonging to the red-giant branch and red-horizontal branch of the globular cluster M4. The detections were made in photometric observations from the K2 Mission during its Campaign 2. Making use of independent constraints on the distance, we estimate masses of the 8 stars by utilising different combinations of seismic and non-seismic inputs. When introducing a correction to the Δν scaling relation as suggested by stellar models, for RGB stars we find excellent agreement with the expected masses from isochrone fitting, and with a distance modulus derived using independent methods. The offset with respect to independent masses is lower, or comparable with, the uncertainties on the average RGB mass (4 − 10%, depending on the combination of constraints used). Our results lend confidence to asteroseismic masses in the metal poor regime. We note that a larger sample will be needed to allow more stringent tests to be made of systematic uncertainties in all the observables (both seismic and non-seismic), and to explore the properties of RHB stars, and of different populations in the cluster.

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Studying the atmospheres of a statistically significant number of rocky, terrestrial exoplanets - including the search for habitable and potentially inhabited planets - is one of the major goals of exoplanetary science and possibly the most challenging question in 21st century astrophysics. However, despite being at the top of the agenda of all major space agencies and ground-based observatories, none of the currently planned projects or missions worldwide has the technical capabilities to achieve this goal. In this talk we present new results from the LIFE Mission initiative, which addresses this issue by investigating the scientific potential of a mid infrared nulling interferometer observatory. Here we will focus on the mission's yield estimates, our simulator software as well as various exemplary science cases such as observing Earth- and Venus-twins or searching for phosphine in exoplanetary atmospheres.

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What the Longest Exposures from the
Hubble Space Telescope Will Reveal
JOHN N. BAHCALL, PURAGRA GUHATHAiKURTA,DONALD P. SCHNEIDER
Detailed simulations are presented of the longest expo-
sures on representative fields that will be obtained with
the Hubble Space Telescope, as well as predictions for the
numbers and types of objects that will be recorded with
exposures of different durations. The Hubble Space Tele-
scope will reveal the shapes, sizes, and content of faint,
distant galaxies and could discover a new population of
Galactic stars.
T HE HUBBLESPACETELESCOPE(HST) IS SCHEDULEDTO
be launchedsoon andthefirstscientificobservationsshould
be availablewithin severalmonths. Many authorshave
discussedthe qualitativeadvancesthatmaybe anticipatedwith an
orbitingspacetelescopeinsuchdiverseareasasastrometry,interstel-
larmatter,stellarevolution,galacticstructureandevolution,quasar
research,andcosmology(1,2). Formostobservations,theHSTwill
be pointedat individualobjectsor fieldsof specialinterest.We
discussthe specificset of observationsin whichthe telescopewill
takepicturesof randomfields(devoidof objectsknowna priorito
beof specialinterest)inorderto determinethestatisticalcharacteris-
ticsof faintgalaxiesandstars.
In this articlewe presentquantitativepredictionsof what the
HST imagesof these representativefieldswill show basedupon
whatwe knowfromground-basedtelescopes.The comparisonof
the HST observationswith these predictionswill constitutean
objectivemeasureof what HST discoversaboutthe propertiesof
faintgalaxiesand stars.Our workinghypothesis,which will be
testedbyHSTobservations,isthateverythingin theHST universe
haspreviouslybeenrevealedby ground-basedobservations.Using
V = 19.5 (near-infraredmagnitude I - 18.5); there are approxi-
mately0.1 stars(or galaxies) arcmin-2 mag- I at this magnitude. By
V = 22.5, the galaxies outnumber the stars by a factor of 10, and
there are about 2.5 galaxies arc min-2 mag'l. At V = 25, the
expected number of stars (-0.35 arc min-2 mag-1) is only 1% of
the number of galaxies. The limiting flux level reached by long
exposures on stars or faint, distant galaxies scales approximately
proportional to the inverse square root of the observing time.
We do not expect HST to reveal a new population of galaxies.
Ground-basedobservations can detect galaxiesto avisualmagnitude
limit of about V = 27 (3). This is also the approximate detection
limit for relativelycompact objects (radius -0".2) with HST in the
longest plannedexposures by guaranteedtime observers(GTOs) (4,
5). For a given luminosity, the more compact the object the easierit
is to detect. To escape detection from the ground but still be
observed with HST, the faintest galaxies (V > 27) must have
angular radii of less than -0".2; this seems an unlikely possibility
(see our discussion below of Fig. 4).
In agreementwith previous authors,our analysissuggests that the
major contribution of HST for galaxy researchwill be in revealing
the shapes, sizes, and content of previously unresolved galaxies.
Table1. Thenumberdensityof faintgalaxiesandstars.Thecalculatedtotal
numberofobjectspersquarearcminuteathighGalacticlatitudeswithvisual
magnitudes,V, and near-infraredmagnitudes,I, less than the specified
brightness,m.Alsoshownarethecalculatednumberof starspersquarearc
minute. For specificity,the luminosityfunctionsof faint spheroidand
disk starsare assumedconstantbetweenMv = 12 and Mv = 16.5 No
browndwarfsareincluded.The V galaxycountsareassumedto followa
powerlawbeyondV = 26, andtheI countsareVmagnitude-limitedwith
Vmax= 28 and30 for galaxiesandstars,respectively.The numbersgiven
herereferto the inputdatato thesimulationsandnot to thenumbersthat
wouldbe detected,whichdependuponexposuretime,detectorefficiency,
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Mission Critical Risk Taking: The Hubble Deep Field by Robert Williams
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3C324
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van Dokkum et al. (2023) reported the serendipitous discovery of a thin linear object interpreted as the trail of star-forming regions left behind by a runaway supermassive black hole (SMBH) kicked out from the center of a galaxy. Despite the undeniable interest in the idea, the actual physical interpretation is not devoid of diculty. The wake of a SMBH produces only small perturbations on the external medium, which has to be in exceptional physical conditions to collapse gravitationally and form a long (40 kpc) massive (3  109M ) stellar trace in only 39 Myr. Here we o er a more conventional explanation: the stellar trail is a bulgeless galaxy viewed edge-on. This interpretation is supported by the fact that its position–velocity curve resembles a rotation curve which, together with its stellar mass, puts the object right on top of the Tully-Fisher relation characteristic of disk galaxies. Moreover, the rotation curve (Vmax 110 km s􀀀1), stellar mass, extension, width (z0 1.2 kpc), and surface brightness profile of the object are very much like those of IC 5249, a well-known local bulgeless edge-on galaxy. These observational

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The document summarizes research finding a 17 billion solar mass black hole at the center of the galaxy NGC 1600. Key points: - Orbit modeling found the black hole mass to be 1.7x1010 solar masses, among the most massive found outside rich galaxy clusters. - NGC 1600 has an unusually diffuse, low surface brightness core, indicating a deficit of stars near the center compared to other galaxies. - A strong correlation was found between the black hole's sphere of influence radius and the galaxy's core radius for NGC 1600 and 20 other galaxies, supporting black hole binaries as the cause of core formation. - The black hole in NGC 1600 may be a descendant of the luminous quasars seen

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This study aims to search for ultra-compact dwarf galaxies (UCDs) around local galaxies using photometric and spectroscopic data from surveys like SDSS and Hubble Space Telescope. The researchers discovered a new UCD, VO-UCD1, around the galaxy M59. Spectroscopy of VO-UCD1 found a velocity dispersion of 64 km/s and dynamical mass of 1.0 x 108 solar masses. Further study of newly discovered UCDs could provide insights into their origins, which remain unknown. The researchers plan to use HST to study UCD sizes and shapes and pursue additional data to understand black hole contributions to UCD masses.

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This document summarizes a study that compiled a list of 220 spiral galaxies with quasars at their centers from the Sloan Digital Sky Survey Data Release 7. It analyzed the virial mass estimates of the quasars' supermassive black holes using three different calibration methods/datasets. Histograms of the black hole masses were created and showed a distribution ranging from 10^7 to 10^9 solar masses. Virial mass estimators relate the motion of gas around a black hole to its mass based on measured properties like emission line widths and luminosities.

Observational constraints on mergers creating magnetism in massive stars
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Massive stars (those ≥8 solar masses at birth) have radiative envelopes that cannot sustain the dynamos that produce magnetic fields in lower mass stars. Despite this, ∼7% of massive stars have observed magnetic fields. We use multi-epoch interferometric and spectroscopic observations to characterise a magnetic binary system formed of two massive stars. We find that only one star of the binary is magnetic. Using the non-magnetic star as an independent reference clock to estimate the age of the system, we show that the magnetic star appears younger than its companion. The system properties, and a surrounding bipolar nebula, can be reproduced by a model in which this system was originally a triple within which two of the stars merged, producing the magnetic massive star. Thus, our results provide observational evidence that magnetic fields form in at least some massive stars through stellar mergers.

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A magnetar-powered X-ray transient as the aftermath of a binary neutron-star ...
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Mergers of neutron stars are known to be associated with short γ-ray bursts1–4 . If the neutron-star equation of state is sufficiently stiff (that is, the pressure increases sharply as the density increases), at least some such mergers will leave behind a supramassive or even a stable neutron star that spins rapidly with a strong magnetic field5–8 (that is, a magnetar). Such a magnetar signature may have been observed in the form of the X-ray plateau that follows up to half of observed short γ-ray bursts9,10. However, it has been expected that some X-ray transients powered by binary neutron-star mergers may not be associated with a short γ-ray burst11,12. A fast X-ray transient (CDF-S XT1) was recently found to be associated with a faint host galaxy, the redshift of which is unknown13. Its X-ray and host-galaxy properties allow several possible explanations including a short γ-ray burst seen off-axis, a low-luminosity γ-ray burst at high redshift, or a tidal disruption event involving an intermediatemass black hole and a white dwarf13. Here we report a second X-ray transient, CDF-S XT2, that is associated with a galaxy at redshift z = 0.738 (ref. 14). The measured light curve is fully consistent with the X-ray transient being powered by a millisecond magnetar. More intriguingly, CDF-S XT2 lies in the outskirts of its star-forming host galaxy with a moderate offset from the galaxy centre, as short γ-ray bursts often do15,16. The estimated event-rate density of similar X-ray transients, when corrected to the local value, is consistent with the event-rate density of binary neutron-star mergers that is robustly inferred from the detection of the gravitational-wave event GW170817.

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Mission Critical Risk Taking: The Hubble Deep Field by Robert Williams

  • 1. Mission Critical Risk-Taking: The Hubble Deep Field Robert Williams Space Telescope Inst/Johns Hopkins U.
  • 2. GlobForeA)SM1   Kapteyn  1922   Hubble  1929   Kepler  1596   Concepts of the Universe Digges  1576  
  • 3. Kravtsov & Wechsler 2010, U. Chicago
  • 4. .        .                          .   Springel 2013 Max-Planck-Institut
  • 6. HSTSchema8c   Mirror:  2.4m  diameter   Mass:    11,000    Kg   Length:    13  meters   Development  Cost:    $2.5    billion   Opera8ons  24  yrs:    $5.5  billion  
  • 17. What the Longest Exposures from the Hubble Space Telescope Will Reveal JOHN N. BAHCALL, PURAGRA GUHATHAiKURTA,DONALD P. SCHNEIDER Detailed simulations are presented of the longest expo- sures on representative fields that will be obtained with the Hubble Space Telescope, as well as predictions for the numbers and types of objects that will be recorded with exposures of different durations. The Hubble Space Tele- scope will reveal the shapes, sizes, and content of faint, distant galaxies and could discover a new population of Galactic stars. T HE HUBBLESPACETELESCOPE(HST) IS SCHEDULEDTO be launchedsoon andthefirstscientificobservationsshould be availablewithin severalmonths. Many authorshave discussedthe qualitativeadvancesthatmaybe anticipatedwith an orbitingspacetelescopeinsuchdiverseareasasastrometry,interstel- larmatter,stellarevolution,galacticstructureandevolution,quasar research,andcosmology(1,2). Formostobservations,theHSTwill be pointedat individualobjectsor fieldsof specialinterest.We discussthe specificset of observationsin whichthe telescopewill takepicturesof randomfields(devoidof objectsknowna priorito beof specialinterest)inorderto determinethestatisticalcharacteris- ticsof faintgalaxiesandstars. In this articlewe presentquantitativepredictionsof what the HST imagesof these representativefieldswill show basedupon whatwe knowfromground-basedtelescopes.The comparisonof the HST observationswith these predictionswill constitutean objectivemeasureof what HST discoversaboutthe propertiesof faintgalaxiesand stars.Our workinghypothesis,which will be testedbyHSTobservations,isthateverythingin theHST universe haspreviouslybeenrevealedby ground-basedobservations.Using V = 19.5 (near-infraredmagnitude I - 18.5); there are approxi- mately0.1 stars(or galaxies) arcmin-2 mag- I at this magnitude. By V = 22.5, the galaxies outnumber the stars by a factor of 10, and there are about 2.5 galaxies arc min-2 mag'l. At V = 25, the expected number of stars (-0.35 arc min-2 mag-1) is only 1% of the number of galaxies. The limiting flux level reached by long exposures on stars or faint, distant galaxies scales approximately proportional to the inverse square root of the observing time. We do not expect HST to reveal a new population of galaxies. Ground-basedobservations can detect galaxiesto avisualmagnitude limit of about V = 27 (3). This is also the approximate detection limit for relativelycompact objects (radius -0".2) with HST in the longest plannedexposures by guaranteedtime observers(GTOs) (4, 5). For a given luminosity, the more compact the object the easierit is to detect. To escape detection from the ground but still be observed with HST, the faintest galaxies (V > 27) must have angular radii of less than -0".2; this seems an unlikely possibility (see our discussion below of Fig. 4). In agreementwith previous authors,our analysissuggests that the major contribution of HST for galaxy researchwill be in revealing the shapes, sizes, and content of previously unresolved galaxies. Table1. Thenumberdensityof faintgalaxiesandstars.Thecalculatedtotal numberofobjectspersquarearcminuteathighGalacticlatitudeswithvisual magnitudes,V, and near-infraredmagnitudes,I, less than the specified brightness,m.Alsoshownarethecalculatednumberof starspersquarearc minute. For specificity,the luminosityfunctionsof faint spheroidand disk starsare assumedconstantbetweenMv = 12 and Mv = 16.5 No browndwarfsareincluded.The V galaxycountsareassumedto followa powerlawbeyondV = 26, andtheI countsareVmagnitude-limitedwith Vmax= 28 and30 for galaxiesandstars,respectively.The numbersgiven herereferto the inputdatato thesimulationsandnot to thenumbersthat wouldbe detected,whichdependuponexposuretime,detectorefficiency, Bahcall  et  al.  
  • 21. Nearby Galaxies Nearby Galaxies (Present epoch) Distant Galaxies (8 Byr ago)
  • 22. HDF Spiral Galaxy NGC 3370
  • 23. HDF
  • 25. Palomar Hubble Telescope Hubble Deep Field 10″ Hubble Deep Field − North HST • WFPC2 December 1995
  • 26. HDF 10″ Hubble Deep Field − North HST • WFPC2 December 1995
  • 27. from   Hubble  Deep  Field  
  • 29. HUDF   Black Hole Stars Orbiting Center of the Milky Way Galaxy
  • 31. HDF 10″ Hubble Deep Field − North HST • WFPC2 December 1995
  • 32. History  of  Universe   History  of  the  Universe  
  • 34. HDF