J/ApJ/795/105      Electromagnetic follow-up with LIGO/Virgo     (Singer+, 2014)
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The first two years of electromagnetic follow-up with advanced LIGO and Virgo.
    Singer L.P., Price L.R., Farr B., Urban A.L., Pankow C., Vitale S.,
    Veitch J., Farr W.M., Hanna C., Cannon K., Downes T., Graff P.,
    Haster C.-J., Mandel I., Sidery T., Vecchio A.
   <Astrophys. J., 795, 105 (2014)>
   =2014ApJ...795..105S    (SIMBAD/NED BibCode)
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ADC_Keywords: Stars, double and multiple ; Polarization ; Stars, distances ;
              Stars, masses ; Surveys ; Interferometry
Keywords: gravitational waves - stars: neutron - surveys

Abstract:
    We anticipate the first direct detections of gravitational waves (GWs)
    with Advanced LIGO and Virgo later this decade. Though this
    groundbreaking technical achievement will be its own reward, a still
    greater prize could be observations of compact binary mergers in both
    gravitational and electromagnetic channels simultaneously. During
    Advanced LIGO and Virgo's first two years of operation, 2015 through
    2016, we expect the global GW detector array to improve in sensitivity
    and livetime and expand from two to three detectors. We model the
    detection rate and the sky localization accuracy for binary neutron
    star (BNS) mergers across this transition. We have analyzed a large,
    astrophysically motivated source population using real-time detection
    and sky localization codes and higher-latency parameter estimation
    codes that have been expressly built for operation in the Advanced
    LIGO/Virgo era. We show that for most BNS events, the rapid sky
    localization, available about a minute after a detection, is as
    accurate as the full parameter estimation. We demonstrate that
    Advanced Virgo will play an important role in sky localization, even
    though it is anticipated to come online with only one-third as much
    sensitivity as the Advanced LIGO detectors. We find that the median
    90% confidence region shrinks from ~500 deg^2^ in 2015 to ~200 deg^2^
    in 2016. A few distinct scenarios for the first LIGO/Virgo detections
    emerge from our simulations.

Description:
    Aasi et al. (2013, arXiv:1304.0670) outline five observing scenarios
    representing the evolving configuration and capability of the Advanced
    GW detector array, from the first observing run in 2015, to achieving
    final design sensitivity in 2019, to adding a fourth detector at
    design sensitivity by 2022. In this study, we focus on the first two
    epochs. The first, in 2015, is envisioned as a three-month science
    run. LIGO Hanford (H) and LIGO Livingston (L) Observatories are
    operating with an averaged (1.4, 1.4) M_{sun}_ BNS range between 40 and
    80 Mpc. The second, in 2016-2017, is a six-month run with H and L
    operating between 80 and 120 Mpc and the addition of Advanced Virgo (V)
    with a range between 20 and 60 Mpc.

File Summary:
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 FileName      Lrecl  Records   Explanations
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ReadMe            80        .   This file
table2.dat        99      630   Simulated BNS signals for 2015 scenario
table3.dat       103      630   Detections and sky localization areas
                                for 2015 scenario
table4.dat        99      475   Simulated BNS signals for 2016 scenario
table5.dat       103      475   Detections and sky localization areas
                                for 2016 scenario
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See also:
 J/ApJ/760/12  : LIGO/Virgo gravitational-wave (GW) bursts with GRBs
                                                                 (Abadie+, 2012)
 J/ApJ/804/114 : Parameter-estimation performance with LIGO (Berry+, 2015)
 J/ApJ/813/39  : LIGO gravitational-wave (GW) searches from SNRs (Aasi+, 2015)

Byte-by-byte Description of file: table2.dat table4.dat
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   Bytes Format Units  Label    Explanations
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   1-  7  A7    ---    dID      Detection ID (G1)
   9- 13  I5    ---    sID      Simulation ID (G2)
  15- 25  F11.5 d      MJD      MJD of simulated signal (3)
  27- 31  F5.1  deg    RAdeg    Right Ascension; decimal degrees (J2000)
  33- 37  F5.1  deg    DEdeg    Declination; decimal degrees (J2000)
  39- 41  I3    deg    Inc      Binary orbital inclination angle
  43- 45  I3    deg    PA       [] Polarization angle (4)
  47- 49  I3    deg    Phase    Orbital phase at coalescence
  51- 53  I3    Mpc    Dist     Distance
  55- 58  F4.2  Msun   Mass1    Mass of binary component 1
  60- 63  F4.2  Msun   Mass2    Mass of binary component 2
  65- 69  F5.2  ---    Spin1x   Spin of binary component 1, x-axis
  71- 75  F5.2  ---    Spin1y   Spin of binary component 1, y-axis
  77- 81  F5.2  ---    Spin1z   Spin of binary component 1, z-axis
  83- 87  F5.2  ---    Spin2x   Spin of binary component 2, x-axis
  89- 93  F5.2  ---    Spin2y   Spin of binary component 2, y-axis
  95- 99  F5.2  ---    Spin2z   Spin of binary component 2, z-axis
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Note (3): Time of arrival at geocenter of gravitational waves from last stable
          orbit.
Note (4): According to convention in Appendix B of Anderson et al.
          (2001PhRvD..63d2003A).
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Byte-by-byte Description of file: table3.dat table5.dat
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   Bytes Format Units Label      Explanations
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   1-  7  A7    ---   dID        Detection ID (G1)
   9- 13  I5    ---   sID        Simulation ID (G2)
  15- 17  A3    ---   network    Detector network
  19- 23  F5.1  ---   SNR-net    Network signal-to-noise ratio
  25- 28  F4.1  ---   SNR-H      ? Signal-to-noise ratio in H (3)
  30- 33  F4.1  ---   SNR-L      ? Signal-to-noise ratio in L (3)
  35- 38  F4.1  ---   SNR-V      ? Signal-to-noise ratio in V
                                  (only in table5.dat) (3)
  40- 43  F4.2  Msun  Mass1      Recovered mass 1
  45- 48  F4.2  Msun  Mass2      Recovered mass 2
  50- 56  F7.3  deg2  Area50     50% area, BAYESTAR
  58- 64  F7.2  deg2  Area90     90% area, BAYESTAR
  66- 76  F11.5 deg2  Area       Searched area, BAYESTAR
  78- 84  F7.3  deg2  pe-area50  ? 50% area, LALINFERENCE_NEST
  86- 93  F8.3  deg2  pe-area90  ? 90% area, LALINFERENCE_NEST
  95-103  F9.4  deg2  pe-area    ? Searched area, LALINFERENCE_NEST
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Note (3): Blank if SNR<4 or detector is not online.
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Global notes:
Note (G1): Identifier for detection candidate. This is the same value as the
           coinc_event_id column in the GSTLAL output database and the OBJECT
           cards in sky map FITS headers, with the 'coinc_event:coinc_event_id:'
           prefix stripped.
Note (G2): Identifier for simulated signal. This is the same value as the
           simulation_id column in the GSTLAL output database, with the
           'sim_inspiral:simulation_id:' prefix stripped.
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History:
    From electronic version of the journal

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(End)             Prepared by [AAS], Tiphaine Pouvreau [CDS]         22-May-2017
