| Proposal Number | Subject Category | PI Name | Title |
|---|---|---|---|
| 08200704 | STARS AND WD | Nancy Brickhouse | Accretion or a Corona? Definitive Observations of the Young Accreting Star TW Hydrae |
| 08300134 | WD BINARIES AND CV | Ronnie Hoogerwerf | Testing the Physics of Magnetic Accretion: EX Hydrae from the Shock to the White Dwarf Surface |
| 08500520 | SN, SNR AND ISOLATED NS | Richard McCray | Spatially Resolved LETG Spectrometery of SNR 1987A |
| 08500758 | SN, SNR AND ISOLATED NS | John Hughes | A Deep Chandra Observation of the Tycho Supernova Remnant |
| 08620985 | NORMAL GALAXIES: X-RAY POPULATIONS | You-Hua Chu | Massive Star Formation and Energy Feedback in the Starburst Region N11 |
| 08700512 | ACTIVE GALAXIES AND QUASARS | Ralph Kraft | Jets, Bubbles, Binaries, and Hot Gas: A Deep Observation of Centaurus A |
| 08700551 | ACTIVE GALAXIES AND QUASARS | David Sanders | The Chandra-RBGS Survey of a Complete Sample of Luminous Infrared Galaxie |
| 08700916 | ACTIVE GALAXIES AND QUASARS | Michael Nowak | The Definitive Chandra Observations of NGC 4258 |
| 08800952 | CLUSTERS OF GALAXIES | John Mulchaey | A Complete Baryon Census in a Nearby Galaxy Group |
| 08900073 | EXTRAGALACTIC DIFFUSE EMISSION AND SURVEYS | Martin Elvis | THE Chandra-Cosmos Survey |
| 08900745 | EXTRAGALACTIC DIFFUSE EMISSION AND SURVEYS | David Alexander | The Chandra Deep Proto-cluster Field: Black-Hole Growth and Feedback in Dense Environments |
| 08900784 | EXTRAGALACTIC DIFFUSE EMISSION AND SURVEYS | Tommaso Treu | The Duty Cycle of Supermassive Black Holes: X-raying Virgo |
Subject Category: STARS AND WD
Proposal Number: 08200704
Title: Accretion or a Corona? Definitive Observations of the Young Accreting Star TW Hydrae
PI Name: Nancy Brickhouse
We propose a 500 ks observation of the prototypical accreting young star TW Hydrae to determine whether the X-ray emission is from a hot corona or an accretion shock. In the short archival spectrum, O VII and Ne IX forbidden to intercombination lines signal either extremely high densities that must be associated with a shock, or photoexcitation by UV continuum emission. The definitive measurement for the density is the analogous Mg XI line ratio. We will also measure velocity shifts and line broadening, search for rotational modulation, and determine elemental abundances using standard emission measure distribution techniques. This deep spectrum will probe the density and structure of the magnetic regions associated with the accretion process during star formation.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 11:01:52.00 | -34:42:16.90 | TW Hydrae | ACIS-S | HETG | 20.00 |
| 11:01:52.00 | -34:42:16.90 | TW Hydrae | ACIS-S | HETG | 160.00 |
| 11:01:52.00 | -34:42:16.90 | TW Hydrae | ACIS-S | HETG | 160.00 |
| 11:01:52.00 | -34:42:16.90 | TW Hydrae | ACIS-S | HETG | 160.00 |
Subject Category: WD BINARIES AND CV
Proposal Number: 08300134
Title: Testing the Physics of Magnetic Accretion: EX Hydrae from the Shock to the White Dwarf Surface
PI Name:Ronnie Hoogerwerf
We propose to observe the magnetic Cataclysmic Variable (CV) EX Hydrae with the HETG to make a direct measurement of the temperature and density structure of its accretion columns and study the physics of the shock and subsequent cooling flow. The accretion column structure, crucial to our understanding of accretion physics, remains one of the last unexplored components of CVs and other accreting objects. The accretion columns of EX Hydrae are unobscured and are periodically occulted by the body of the white dwarf, making it the ideal target for this study. We will use high signal-to-noise light curves for individual spectral lines to measure the temperature and density structure. The result will be applicable to a broad range of objects from clusters of galaxies to T Tauri stars.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 12:52:24.20 | -29:14:56.70 | EX Hydrae | ACIS-S | HETG | 20.000 |
| 12:52:24.20 | -29:14:56.70 | EX Hydrae | ACIS-S | HETG | 160.000 |
| 12:52:24.20 | -29:14:56.70 | EX Hydrae | ACIS-S | HETG | 160.000 |
| 12:52:24.20 | -29:14:56.70 | EX Hydrae | ACIS-S | HETG | 160.000 |
Subject Category:SN, SNR AND ISOLATED NS
Proposal Number: 08500520
Title:Spatially Resolved LETG Spectrometry of SNR1987A
PI Name: Richard McCray
We will obtain a spatially resolved LETG spectrum of the newborn supernova remnant SNR1987A. This observation will complement a 270 ks GTO observation of SNR1987A with the HETG. The proposed observations will provide spatial information to interpret the HETG observations and will measure the spectrum at wavelengths > 15 A where the HETG lacks sensitivity. With a projected source > 3 times brighter than it was during our Cycle 5 observation, we will be able to measure for the first time how the temperature distribution and kinematic velocity of the shocked gas has changed and how these parameters vary spatially around the ring-like source. The proposed observation is part of a large multi-wavelength campaign of observations with Spitzer, HST, and ground-based observatories.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 05:35:28.00 | -69:16:11.10 | SNR1987A | ACIS-S | LETG | 140.0000 |
| 05:35:28.00 | -69:16:11.10 | SNR1987A | ACIS-S | LETG | 160.0000 |
Subject Category:SN, SNR AND ISOLATED NS
Proposal Number:08500758
Title:A Deep Chandra Observation of the Tycho Supernova Remnant
PI Name: John Hughes
We propose to obtain a very deep observation of the Tycho supernova remnant. Our observational goals include measuring the angular expansion of the forward shock and contact discontinuity, investigating the nature and origin of Fe-rich ejecta knots, and studying the spectral structure of the forward shock. For the expansion measurement we will compare to an existing Chandra observation taken in cycle 4 that was specifically optimized for subsequent expansion measurements. Tycho is the ideal remnant for studies of cosmic-ray modified dynamics and investigating key features of Type Ia supernova physics.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 00:25:19.00 | +64:08:10.00 | Tycho's SNR | ACIS-I | NONE | 150.0000 |
Subject Category:NORMAL GALAXIES: X-RAY POPULATIONS
Proposal Number: 08620985
Title: Massive Star Formation and Energy Feedback in the Starburst Region N11
PI Name:You-Hua Chu
The starburst region N11 is the second largest star formation complex in the LMC. It contains four OB associations distributed in a central superbubble and dense HII regions along its periphery, indicating sequential star formation. Spitzer observations have revealed hundreds of massive protostars in N11. The relatively simple structure of N11 makes it an ideal starburst region for detailed study. We request a 300 ks ACIS-I observation of N11 to determine the X-ray properties of point sources and diffuse emission at arcsecond resolution. This deep observation will allow us to study (1) discrete X-ray source population and empirical L_x/L_bol, (2) X-ray emission from protostars, (3) bubbles/superbubbles and stellar energy feedback, and (4) physical structure of a starburst region.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 04:56:31.50 | -66:27:47.00 | LHA 120-N 11 | ACIS-I | NONE | 140.0000 |
| 04:56:31.50 | -66:27:47.00 | LHA 120-N 11 | ACIS-I | NONE | 160.0000 |
Subject Category:ACTIVE GALAXIES AND QUASARS
Proposal Number: 08700512
Title: Jets, Bubbles, Binaries, and Hot Gas: A Deep Observation of Centaurus A
PI Name:Ralph Kraft
We propose to observe Centaurus A, the nearest radio galaxy and the nearest massive early-type galaxy, for 1.2 Ms. We will probe the particle acceleration processes of the jet to an unprecedented sensitivity, by measuring its spectrum and morphology on the scale of radiative energy losses. We also will measure the proper motions and velocity shear of X-ray knots. We will measure the temperature and density structure of the shock around the SW radio lobe to study the hydrodynamics of the lobe/ISM interaction to a level previously seen only in Galactic SNRs. We will detect hundreds of X-ray binaries, probe the GC/LMXB link, and investigate their temporal properties. Finally, we will measure the thermodynamic paramters of the gas and the elemental abundance throughout the ISM.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 13:25:33.00 | -43:00:11.00 | Centaurus A Jet | ACIS-I | NONE | 120.0000 |
| 13:25:33.00 | -43:00:11.00 | Centaurus A Jet | ACIS-I | NONE | 160.0000 |
| 13:25:33.00 | -43:00:11.00 | Centaurus A Jet | ACIS-I | NONE | 160.0000 |
| 13:25:33.00 | -43:00:11.00 | Centaurus A Jet | ACIS-I | NONE | 160.0000 |
Subject Category: ACTIVE GALAXIES AND QUASARS
Proposal Number: 08700551
Title: The Chandra-RBGS Survey of a Complete Sample of Luminous Infrared Galaxies
PI Name: David Sanders
We propose a Chandra-ACIS survey of a complete sample of Luminous Infrared Galaxies (LIRGs) with Lir >10^11.5, from the IRAS Revised Bright Galaxy Sample (RBGS). All of these objects are interacting/merging gas-rich spirals. Our new observations will provide a uniform and complete census of AGN and X-ray luminous starbursts in the nearest and brightest LIRGs, and will complement approved Spitzer-IRAC+MIPS, and HST-ACS imaging of the same sample. The results will be used to address the following key questions: are binary AGN a common feature of these LIRGs, and if so, when and at what level is the AGN activity triggered in each nucleus ? and can the fueling and growth of massive black holes be correlated in time with the merger phase ?
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 01:38:52.90 | -10:27:11.40 | IRAS F01364-1042 | ACIS-S | NONE | 15.0000 |
| 04:46:49.50 | -48:33:32.90 | ESO 203-IG001 | ACIS-S | NONE | 15.0000 |
| 05:16:46.40 | +79:40:12.60 | VII Zw 031 | ACIS-S | NONE | 15.0000 |
| 06:27:23.10 | -47:10:47.00 | ESO 255-IG007 | ACIS-S | NONE | 15.0000 |
| 07:27:37.60 | -02:54:54.10 | IRAS 07251-0248 | ACIS-S | NONE | 15.0000 |
| 08:52:29.90 | -69:01:58.00 | ESO 60-IG016 | ACIS-S | NONE | 15.0000 |
| 09:04:12.70 | -36:27:01.10 | IRAS 09022-3615 | ACIS-S | NONE | 15.0000 |
| 09:13:38.80 | -10:19:20.30 | IRAS F09111-1007 | ACIS-S | NONE | 15.0000 |
| 10:06:04.80 | -33:53:15.00 | IC 2545 | ACIS-S | NONE | 15.0000 |
| 10:20:00.20 | +08:13:34.00 | IRAS F10173+0828 | ACIS-S | NONE | 15.0000 |
| 13:15:06.40 | -55:09:22.70 | IRAS 13120-5453 | ACIS-S | NONE | 15.0000 |
| 13:15:35.00 | +62:07:28.80 | VV 250a | ACIS-S | NONE | 15.0000 |
| 13:20:35.30 | +34:08:22.20 | UGC 08387 | ACIS-S | NONE | 15.0000 |
| 14:40:59.00 | -37:04:32.00 | IRAS F14378-3651 | ACIS-S | NONE | 15.0000 |
| 14:57:00.70 | +24:37:02.70 | VV 340a | ACIS-S | NONE | 15.0000 |
| 16:38:13.20 | -68:26:42.80 | ESO 069-IG006 | ACIS-S | NONE | 15.0000 |
| 17:14:20.00 | +53:10:30.00 | IRAS F17132+5313 | ACIS-S | NONE | 15.0000 |
| 18:32:41.10 | -34:11:27.50 | IRAS F18293-3413 | ACIS-S | NONE | 15.0000 |
| 19:14:30.90 | -21:19:07.00 | ESO 593-IG008 | ACIS-S | NONE | 15.0000 |
| 19:32:21.20 | -03:59:56.30 | IRAS F19297-0406 | ACIS-S | NONE | 15.0000 |
| 19:56:35.40 | +11:19:02.60 | IRAS 19542+1110 | ACIS-S | NONE | 15.0000 |
| 20:57:23.30 | +17:07:34.30 | CGCG 448-020 | ACIS-S | NONE | 15.0000 |
| 21:11:30.40 | +58:23:03.20 | IRAS 21101+5810 | ACIS-S | NONE | 15.0000 |
| 22:49:39.90 | -48:50:58.10 | ESO 239-IG002 | ACIS-S | NONE | 15.0000 |
| 22:51:49.30 | -17:52:23.50 | IRAS F22491-1808 | ACIS-S | NONE | 15.0000 |
| 23:21:04.30 | -69:12:54.00 | ESO 077-IG014 | ACIS-S | NONE | 15.0000 |
Subject Category: ACTIVE GALAXIES AND QUASARS
Proposal Number: 08700916
Title: The Definitive Chandra Observations of NGC 4258
PI Name:Michael Nowak
We propose a 320 ksec HETG observation of NGC 4258. This will yield a high S/N nuclear spectra that is uncontaminated by extended emission or pileup. We will measure the fluorescent Kalpha line strength and width, search for low energy emission lines as expected in some ADAF models, and accurately measure the absorbing column. The latter may be probing the warped disk structure. We will search for nuclear flaring, as observed in Sgr A*. The S/N for observations of the `anomalous arms' will be increased over previous observations. The binary population will be surveyed down to an implied isotropic luminosity of 10^36 erg/s. Our observation will be coordinated with the VLA, to further test the "fundamental plane" of black hole radio/X-ray activity.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 12:18:58.00 | +47:18:14.00 | NGC 4258 | ACIS-S | HETG | 160.0000 |
| 12:18:58.00 | +47:18:14.00 | NGC 4258 | ACIS-S | HETG | 160.0000 |
Subject Category:CLUSTERS OF GALAXIES
Proposal Number: 08800952
Title: A Complete Baryon Census in a Nearby Galaxy Group
PI Name: John Mulchaey
We propose an ACIS-I mosaic of the NGC2563 group to study the X-ray properties of the group galaxies out to the virial radius of the system. The proposed observations will provide important observational constraints on the mechanisms that drive galaxy evolution in groups by allowing us to study how the properties of galaxies vary with distance from the group center, IGM and galaxy density. The Chandra data will allow us to study the hot ISM halos of individual galaxies as well as the more extended intragroup medium component, which combined with our existing optical and HI data will provide a complete census of all of the major baryonic components in the group.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 08:20:23.70 | +21:05:00.50 | NGC2563-P1 | ACIS-I | NONE | 50.0000 |
| 08:21:32.10 | +20:49:01.00 | NGC2563-P2 | ACIS-I | NONE | 30.0000 |
| 08:20:23.70 | +20:49:01.60 | NGC2563-P3 | ACIS-I | NONE | 30.0000 |
| 08:21:32.30 | +21:20:57.40 | NGC2563-P4 | ACIS-I | NONE | 30.0000 |
| 08:20:23.70 | +21:20:57.90 | NGC2563-P5 | ACIS-I | NONE | 30.0000 |
| 08:19:15.10 | +21:04:59.40 | NGC2563-P6 | ACIS-I | NONE | 30.0000 |
| 08:19:15.30 | +20:49:00.40 | NGC2563-P7 | ACIS-I | NONE | 30.0000 |
| 08:19:15.00 | +21:20:56.80 | NGC2563-P8 | ACIS-I | NONE | 30.0000 |
| 08:22:40.20 | +21:02:03.90 | NGC2563-P9 | ACIS-I | NONE | 30.0000 |
| 08:21:32.20 | +21:05:00.00 | NGC2563-P10 | ACIS-I | NONE | 30.0000 |
| 08:18:50.80 | +21:42:31.10 | NGC2563-P11 | ACIS-I | NONE | 30.0000 |
| 08:18:00.00 | +20:49:42.20 | NGC2563-P12 | ACIS-I | NONE | 30.0000 |
| 08:19:17.70 | +20:33:33.70 | NGC2563-P13 | ACIS-I | NONE | 30.0000 |
| 08:23:16.40 | +21:23:09.90 | NGC2563-P14 | ACIS-I | NONE | 30.0000 |
Subject Category: EXTRAGALACTIC DIFFUSE EMISSION AND SURVEYS
Proposal Number: 08900073
Title: THE CHANDRA-Cosmos Survey
PI Name: Martin Elvis
We propose the Chandra-COSMOS survey which will provide an unprecedented combination of contiguous area, depth and resolution. 36 densely tiled observations will cover the central 0.7 sq.deg. COSMOS field to a uniform 200ksec depth. COSMOS explores the coupled evolution of galaxies, dark matter halos and AGNs (massive black holes) largely free of cosmic variance. COSMOS is a comprehensive survey including: HST, Spitzer, Subaru, VLT, Magellan, VLA, MAMBO, GALEX, & potentially EVLA & ALMA. Chandra resolution & sensitivity enables the study of large scale phenomena: (1) influence of the surrounding environment; (2) interaction between galaxies; (3) influence of groups and clusters: (4) BH growth and census; (5) star formation and stellar populations; (6) feedback from starbursts and AGNs.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 09:59:08.80 | +01:57:24.10 | C-COSMOS6-6 | ACIS-I | NONE | 50.0000 |
| 09:59:08.80 | +02:05:24.00 | C-COSMOS5-6 | ACIS-I | NONE | 50.0000 |
| 09:59:08.80 | +02:13:23.90 | C-COSMOS4-6 | ACIS-I | NONE | 50.0000 |
| 09:59:08.80 | +02:21:24.10 | C-COSMOS3-6 | ACIS-I | NONE | 50.0000 |
| 09:59:08.80 | +02:29:24.00 | C-COSMOS2-6 | ACIS-I | NONE | 50.0000 |
| 09:59:08.80 | +02:37:23.90 | C-COSMOS1-6 | ACIS-I | NONE | 50.0000 |
| 09:59:40.80 | +01:57:24.10 | C-COSMOS6-5 | ACIS-I | NONE | 50.0000 |
| 09:59:40.80 | +02:05:24.00 | C-COSMOS5-5 | ACIS-I | NONE | 50.0000 |
| 09:59:40.80 | +02:13:23.90 | C-COSMOS4-5 | ACIS-I | NONE | 50.0000 |
| 09:59:40.80 | +02:21:24.10 | C-COSMOS3-5 | ACIS-I | NONE | 50.0000 |
| 09:59:40.80 | +02:29:24.00 | C-COSMOS2-5 | ACIS-I | NONE | 50.0000 |
| 09:59:40.80 | +02:37:23.90 | C-COSMOS1-5 | ACIS-I | NONE | 50.0000 |
| 10:00:12.80 | +01:57:24.10 | C-COSMOS6-4 | ACIS-I | NONE | 50.0000 |
| 10:00:12.80 | +02:05:24.00 | C-COSMOS5-4 | ACIS-I | NONE | 50.0000 |
| 10:00:12.80 | +02:13:23.90 | C-COSMOS4-4 | ACIS-I | NONE | 50.0000 |
| 10:00:12.80 | +02:21:24.10 | C-COSMOS3-4 | ACIS-I | NONE | 50.0000 |
| 10:00:12.80 | +02:29:24.00 | C-COSMOS2-4 | ACIS-I | NONE | 50.0000 |
| 10:00:12.80 | +02:37:23.90 | C-COSMOS1-4 | ACIS-I | NONE | 50.0000 |
| 10:00:44.80 | +01:57:24.10 | C-COSMOS6-3 | ACIS-I | NONE | 50.0000 |
| 10:00:44.80 | +02:05:24.00 | C-COSMOS5-3 | ACIS-I | NONE | 50.0000 |
| 10:00:44.80 | +02:13:23.90 | C-COSMOS4-3 | ACIS-I | NONE | 50.0000 |
| 10:00:44.80 | +02:21:24.10 | C-COSMOS3-3 | ACIS-I | NONE | 50.0000 |
| 10:00:44.80 | +02:29:24.00 | C-COSMOS2-3 | ACIS-I | NONE | 50.0000 |
| 10:00:44.80 | +02:37:23.90 | C-COSMOS1-3 | ACIS-I | NONE | 50.0000 |
| 10:01:16.80 | +01:57:24.10 | C-COSMOS6-2 | ACIS-I | NONE | 50.0000 |
| 10:01:16.80 | +02:05:24.00 | C-COSMOS5-2 | ACIS-I | NONE | 50.0000 |
| 10:01:16.80 | +02:13:23.90 | C-COSMOS4-2 | ACIS-I | NONE | 50.0000 |
| 10:01:16.80 | +02:21:24.10 | C-COSMOS3-2 | ACIS-I | NONE | 50.0000 |
| 10:01:16.80 | +02:29:24.00 | C-COSMOS2-2 | ACIS-I | NONE | 50.0000 |
| 10:01:16.80 | +02:37:23.90 | C-COSMOS1-2 | ACIS-I | NONE | 50.0000 |
| 10:01:48.80 | +01:57:24.10 | C-COSMOS6-1 | ACIS-I | NONE | 50.0000 |
| 10:01:48.80 | +02:05:24.00 | C-COSMOS5-1 | ACIS-I | NONE | 50.0000 |
| 10:01:48.80 | +02:13:23.90 | C-COSMOS4-1 | ACIS-I | NONE | 50.0000 |
| 10:01:48.80 | +02:21:24.10 | C-COSMOS3-1 | ACIS-I | NONE | 50.0000 |
| 10:01:48.80 | +02:29:24.00 | C-COSMOS2-1 | ACIS-I | NONE | 50.0000 |
| 10:01:48.80 | +02:37:23.90 | C-COSMOS1-1 | ACIS-I | NONE | 50.0000 |
Subject Category:EXTRAGALACTIC DIFFUSE EMISSION AND SURVEYS
Proposal Number: 08900745
Title: Tde Chandra Deep Proto-cluster Field: Black-Hole Growtd and Feedback in Dense Environments
PI Name: David Alexander
Deep X-ray surveys have revolutionized our understanding of tde growtd of black holes (SMBH). But tdese surveys only sample low-density regions at high-z due to tdeir limited solid angle. Tdere is no comparably sensitive X-ray census of AGN in high-density regions at high-z. Such environments evolve into tde most massive clusters at z=0, regions which exhibit remarkable trends in galaxy properties - which may reflect early interactions between SMBHs and tdeir host galaxies. A survey of a proto-cluster at high-z would provide a unique view of tde interplay of tde growtd of galaxies and tdeir SMBHs. Here we propose a 400ks survey of tde best-studied proto-cluster at high-z, to enable tde first definitive study of tde growtd of SMBHs and tdeir host galaxies in a dense, young, environment.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 22:17:35.90 | +00:15:58.90 | SSA22 Protocluster | ACIS-I | NONE | 80.0000 |
| 22:17:35.90 | +00:15:58.90 | SSA22 Protocluster | ACIS-I | NONE | 160.0000 |
| 22:17:35.90 | +00:15:58.90 | SSA22 Protocluster | ACIS-I | NONE | 160.0000 |
Subject Category:EXTRAGALACTIC DIFFUSE EMISSION AND SURVEYS
Proposal Number: 08900784
Title: Tde Duty Cycle of Supermassive Black Holes: X-raying Virgo
PI Name: Tommaso Treu
Nuclear accretion on to super-massive black holes (SMBHs) plays a key role in tde evolution of tdeir host galaxies, as inferred from tde ubiquity of SMBHs and tde correlations between BH mass, and host mass and velocity dispersion. A fundamental unadressed issue is tde actual distribution of accretion rates; we propose snapshot observations of an unbiased sample of 84 early-type galaxies in tde Virgo cluster. Togetder witd joint Spitzer 24 um observations, and publicly available HST-ACS and UV data, tdis survey will probe low-level nuclear activity over four orders of magnitude in black hole mass, tdereby delivering tde first unbiased census of tde duty cycle of local SMBHs.
| R.A. | Dec. | Target Name | Det. | Grating | Exp.Time |
|---|---|---|---|---|---|
| 12:09:22.30 | +13:59:33.10 | 9 | ACIS-S | NONE | 5.4000 |
| 12:10:23.20 | +10:11:17.60 | 21 | ACIS-S | NONE | 5.4000 |
| 12:11:07.80 | +14:16:29.80 | 33 | ACIS-S | NONE | 5.4000 |
| 12:15:12.60 | +14:25:59.10 | 140 | ACIS-S | NONE | 5.4000 |
| 12:16:33.70 | +13:01:53.10 | 200 | ACIS-S | NONE | 5.4000 |
| 12:17:19.60 | +11:56:36.20 | 230 | ACIS-S | NONE | 5.4000 |
| 12:19:30.60 | +14:52:41.40 | 355 | ACIS-S | NONE | 5.4000 |
| 12:19:45.40 | +12:47:54.30 | 369 | ACIS-S | NONE | 5.4000 |
| 12:20:48.80 | +17:29:13.40 | 437 | ACIS-S | NONE | 5.4000 |
| 12:22:14.80 | +07:10:00.80 | 538 | ACIS-S | NONE | 5.4000 |
| 12:22:19.50 | +14:45:38.60 | 543 | ACIS-S | NONE | 5.4000 |
| 12:22:41.10 | +07:57:01.10 | 571 | ACIS-S | NONE | 5.4000 |
| 12:22:43.30 | +08:11:53.70 | 575 | ACIS-S | NONE | 5.4000 |
| 12:23:35.30 | +16:43:22.30 | 654 | ACIS-S | NONE | 5.4000 |
| 12:24:05.00 | +11:13:06.00 | 698 | ACIS-S | NONE | 5.4000 |
| 12:24:48.30 | +18:11:42.00 | 751 | ACIS-S | NONE | 5.4000 |
| 12:24:55.50 | +11:42:15.00 | 759 | ACIS-S | NONE | 5.4000 |
| 12:25:12.30 | +14:45:43.80 | 778 | ACIS-S | NONE | 5.4000 |
| 12:25:14.70 | +15:36:27.20 | 784 | ACIS-S | NONE | 5.4000 |
| 12:25:41.70 | +12:48:38.00 | 828 | ACIS-S | NONE | 5.4000 |
| 12:25:57.80 | +10:03:12.80 | 856 | ACIS-S | NONE | 5.4000 |
| 12:26:50.50 | +09:35:02.00 | 944 | ACIS-S | NONE | 5.4000 |
| 12:27:36.70 | +08:09:14.80 | 1025 | ACIS-S | NONE | 5.4000 |
| 12:27:40.50 | +13:04:44.20 | 1030 | ACIS-S | NONE | 5.4000 |
| 12:27:54.90 | +08:05:25.20 | 1049 | ACIS-S | NONE | 5.4000 |
| 12:28:03.90 | +09:48:14.00 | 1062 | ACIS-S | NONE | 5.4000 |
| 12:28:12.30 | +10:17:51.00 | 1075 | ACIS-S | NONE | 5.4000 |
| 12:28:14.90 | +11:47:24.00 | 1087 | ACIS-S | NONE | 5.4000 |
| 12:28:43.40 | +11:45:21.00 | 1125 | ACIS-S | NONE | 5.4000 |
| 12:28:57.60 | +13:14:30.80 | 1146 | ACIS-S | NONE | 5.4000 |
| 12:29:21.30 | +08:09:23.00 | 1178 | ACIS-S | NONE | 5.4000 |
| 12:29:23.40 | +12:27:02.40 | 1185 | ACIS-S | NONE | 5.4000 |
| 12:29:30.20 | +07:59:34.00 | 1192 | ACIS-S | NONE | 5.4000 |
| 12:29:35.00 | +08:03:31.40 | 1199 | ACIS-S | NONE | 5.4000 |
| 12:29:53.50 | +14:04:07.00 | 1242 | ACIS-S | NONE | 5.4000 |
| 12:29:59.10 | +12:20:55.00 | 1250 | ACIS-S | NONE | 5.4000 |
| 12:30:10.40 | +10:46:46.10 | 1261 | ACIS-S | NONE | 5.4000 |
| 12:30:17.40 | +12:19:43.90 | 1279 | ACIS-S | NONE | 5.4000 |
| 12:30:18.40 | +13:34:40.90 | 1283 | ACIS-S | NONE | 5.4000 |
| 12:30:40.60 | +09:00:55.90 | 1303 | ACIS-S | NONE | 5.4000 |
| 12:30:52.20 | +16:45:32.60 | 1321 | ACIS-S | NONE | 5.4000 |
| 12:30:57.60 | +12:16:17.20 | 1327 | ACIS-S | NONE | 5.4000 |
| 12:31:20.00 | +14:06:53.50 | 1355 | ACIS-S | NONE | 5.4000 |
| 12:32:02.70 | +11:53:24.80 | 1407 | ACIS-S | NONE | 5.4000 |
| 12:32:14.20 | +10:15:05.00 | 1422 | ACIS-S | NONE | 5.4000 |
| 12:32:23.40 | +11:15:46.20 | 1431 | ACIS-S | NONE | 5.4000 |
| 12:32:33.40 | +15:24:55.20 | 1440 | ACIS-S | NONE | 5.4000 |
| 12:33:05.00 | +16:15:55.90 | 1475 | ACIS-S | NONE | 5.4000 |
| 12:33:13.40 | +09:23:49.80 | 1488 | ACIS-S | NONE | 5.4000 |
| 12:33:13.80 | +10:55:43.60 | 1489 | ACIS-S | NONE | 5.4000 |
| 12:33:19.80 | +12:51:12.80 | 1499 | ACIS-S | NONE | 5.4000 |
| 12:33:34.60 | +11:15:42.80 | 1512 | ACIS-S | NONE | 5.4000 |
| 12:33:51.60 | +13:19:21.30 | 1528 | ACIS-S | NONE | 5.4000 |
| 12:34:06.10 | +11:19:17.00 | 1537 | ACIS-S | NONE | 5.4000 |
| 12:34:06.80 | +12:44:30.10 | 1539 | ACIS-S | NONE | 5.4000 |
| 12:34:11.50 | +12:02:55.90 | 1545 | ACIS-S | NONE | 5.4000 |
| 12:35:30.60 | +12:13:15.40 | 1619 | ACIS-S | NONE | 5.4000 |
| 12:35:37.30 | +12:22:54.90 | 1627 | ACIS-S | NONE | 5.4000 |
| 12:35:38.00 | +12:15:50.50 | 1630 | ACIS-S | NONE | 5.4000 |
| 12:36:24.80 | +10:23:04.60 | 1661 | ACIS-S | NONE | 5.4000 |
| 12:36:53.40 | +07:14:47.00 | 1692 | ACIS-S | NONE | 5.4000 |
| 12:36:54.90 | +12:31:12.50 | 1695 | ACIS-S | NONE | 5.4000 |
| 12:37:30.60 | +09:33:18.80 | 1720 | ACIS-S | NONE | 5.4000 |
| 12:38:06.80 | +10:04:56.60 | 1743 | ACIS-S | NONE | 5.4000 |
| 12:39:04.70 | +14:43:51.50 | 1779 | ACIS-S | NONE | 5.4000 |
| 12:40:11.20 | +09:53:45.90 | 1826 | ACIS-S | NONE | 5.4000 |
| 12:40:13.40 | +12:52:29.00 | 1828 | ACIS-S | NONE | 5.4000 |
| 12:40:19.60 | +15:56:07.20 | 1833 | ACIS-S | NONE | 5.4000 |
| 12:40:53.10 | +10:28:34.00 | 1857 | ACIS-S | NONE | 5.4000 |
| 12:40:58.50 | +11:11:04.40 | 1861 | ACIS-S | NONE | 5.4000 |
| 12:41:15.70 | +11:23:13.50 | 1871 | ACIS-S | NONE | 5.4000 |
| 12:41:32.70 | +07:18:53.00 | 1883 | ACIS-S | NONE | 5.4000 |
| 12:41:39.40 | +12:14:52.40 | 1886 | ACIS-S | NONE | 5.4000 |
| 12:41:52.00 | +09:24:10.30 | 1895 | ACIS-S | NONE | 5.4000 |
| 12:42:08.70 | +11:45:14.90 | 1910 | ACIS-S | NONE | 5.4000 |
| 12:42:10.70 | +07:40:37.00 | 1913 | ACIS-S | NONE | 5.4000 |
| 12:42:47.40 | +11:26:33.00 | 1938 | ACIS-S | NONE | 5.4000 |
| 12:42:58.00 | +10:40:54.50 | 1948 | ACIS-S | NONE | 5.4000 |
| 12:44:12.00 | +12:56:30.10 | 1993 | ACIS-S | NONE | 5.4000 |
| 12:44:31.90 | +11:11:25.10 | 2000 | ACIS-S | NONE | 5.4000 |
| 12:45:20.40 | +13:41:33.00 | 2019 | ACIS-S | NONE | 5.4000 |
| 12:47:15.30 | +10:12:13.00 | 2048 | ACIS-S | NONE | 5.4000 |
| 12:47:20.70 | +12:09:58.70 | 2050 | ACIS-S | NONE | 5.4000 |
| 12:52:17.50 | +11:18:50.00 | 2092 | ACIS-S | NONE | 5.4000 |