Detecting and Measuring the Masses of Isolated Black Holes and Neutron Stars through Astrometric Microlensing
We propose a 3-year program of monitoring of 12 fields in the Galactic bulge, containing a total of ~1.5 million stars down to V=28. Our primary aim is to detect microlensing events caused by non-luminous isolated black holes (BHs) and neutron stars (NSs) in the Galactic disk and bulge.
The unique capability of HST imaging for microlensing observations is the addition of high-precision astrometry, allowing detection of the astrometric shift of the source during the event. Combined with the lens parallax, provided by the HST event light curve, the astrometric shift provides a direct measurement of the lens mass. We will detect ~120 microlensing events, of which 45% will show astrometric deflections, leading to direct determinations of the lens masses. Of these, about 18 lenses are expected to be BHs and 14 of them NSs, along with about 22 events due to main-sequence stars.
To date, BH and NS masses have been directly measured only in binaries; no isolated BH has been detected unambiguously within our Galaxy. A survey of the scope proposed here is the only means available at present for measuring the mass function of isolated BHs and NSs, and moreover one that is normalized to that of luminous stars. The results will provide a quantitative estimate of the mass content in the form of stellar remnants in the young Galactic disk and old bulge, and important constraints on SN/GRB explosion mechanisms that produce NSs and BHs.
Our data will also be useful for other investigations, including a more accurate determination of the microlensing optical depth, faint variable stars, bulge proper motions and kinematics, and a deep luminosity function of the disk and bulge stars.
Our observing strategy has been designed to yield the maximum number of microlensing events over a wide range of event timescales, building upon the strong heritage of microlens- ing surveys in the Galactic bulge from the ground. To both optimize our observing strategy and accurately predict the distribution of microlensing events such a program would charac- terize, we performed an extensive set of Monte-Carlo simulations, where the intrinsic rates of microlensing events on various timescales were scaled from the OGLE survey (e.g., Udal- ski et al. 2002). The most efficient strategy is to observe 4 fields with ACS as the prime instrument, and 8 fields with WFC3 as the parallel instrument. These 12 fields would be monitored over the course of a three-year period, with a total of 48 epochs in each of the 4 ACS fields and 24 epochs in each of the 8 WFC3 fields.
For the Galactic bulge, we can use just two telescope roll orientations (90◦ and 270◦) throughout the 8-month yearly observing window, with each orientation available for a con- tinuous 4-month interval per year. Our three-year program would thus image the 4 ACS fields for 8 months per year, along with 4 parallel WFC3 fields for 4 months per year, and a second set of another 4 parallel WFC3 fields for the other 4 months per year. A probable layout for these fields is shown in Fig. 7. Because of the abundant observing opportunities, our program does not present a scheduling burden.
Our goal is to characterize the population producing microlensing events on three timescales: short (less than 40 days; bulge lens mass 1 M⊙, dominated by dwarf stars), medium (40 to 70 days; bulge lens mass of 1–3 M⊙, dominated by NSs), and long (longer than 70 days; stellar-mass BHs). An individual microlensing event can be accurately charac- terized if it has at least 12 photometric samples, with at least 4 photometric samples outside of the event (providing a baseline) and at least 8 photometric samples during the event. Each photometric sample must be in two bands, to ensure the events are achromatic.
Each epoch of observation in each individual field will take one HST single orbit. During that orbit, we will obtain four dithered ACS/WFC images and four parallel WFC3/UVIS images, with each camera’s exposures split between F606W and F814W. We have verified that the orbits can be packed in this manner using the APT.
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true
1
0
Timing link suitability includes constraints ([35 After 34 by at most 0.1 days] [36 After 35 by at most 0.1 days])
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true
1
0
Timing link suitability includes constraints ([36 After 35 by at most 0.1 days])
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true
1
0
Timing link suitability includes constraints ([38 After 37 by at most 0.1 days])
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false
1
0
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false
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false
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false
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false
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false
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false
1
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false
1
0
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false
1
0
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false
1
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false
1
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false
1
0
Timing link suitability includes constraints ([50 After 49 by at most 0.1 days])
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false
1
0
Timing link suitability includes constraints ([50 After 49 by at most 0.1 days] [51 After 50 by at most 0.1 days])
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false
1
0
Timing link suitability includes constraints ([51 After 50 by at most 0.1 days] [52 After 51 by at most 0.1 days])
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false
1
0
Timing link suitability includes constraints ([52 After 51 by at most 0.1 days])
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(Tic-Visit
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false
1
0
Timing link suitability includes constraints ([54 After 53 by at most 0.1 days])
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false
1
0
Timing link suitability includes constraints ([54 After 53 by at most 0.1 days] [55 After 54 by at most 0.1 days])
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