J/ApJ/760/12 LIGO/Virgo gravitational-wave (GW) bursts with GRBs (Abadie+, 2012)

Search for gravitational waves associated with gamma-ray bursts during LIGO science run 6 and Virgo science runs 2 and 3. Abadie J., Abbott B.P., Abbott R., Abbott T.D., Abernathy M., Accadia T., Acernese F., Adams C., Adhikari R.X., Affeldt C., Agathos M., Agatsuma K., Ajith P., Allen B., Ceron E.A., Amariutei D., Anderson S.B., Anderson W.G., Arai K., Arain M.A., Araya M.C., Aston S.M., Astone P., Atkinson D., Aufmuth P., Aulbert C., Aylott B.E., Babak S., Baker P., Ballardin G., Ballmer S., Barayoga J.C.B., Barker D., Barone F., Barr B., Barsotti L., Barsuglia M., Barton M.A., Bartos I., Bassiri R., Bastarrika M., Basti A., Batch J., Bauchrowitz J., Bauer TH.S., Bebronne M., Beck D., Behnke B., Bejger M., Beker M.G., Bell A.S., Belopolski I., Benacquista M., Berliner J.M., Bertolini A., Betzwieser J., Beveridge N., Beyersdorf P.T., Bilenko I.A., Billingsley G., Birch J., Biswas R., Bitossi M., Bizouard M.A., Black E., Blackburn J.K., Blackburn L., Blair D., Bland B., Blom M., Bock O., Bodiya T.P., Bogan C., Bondarescu R., Bondu F., Bonelli L., Bonnand R., Bork R., Born M., Boschi V., Bose S., Bosi L., 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V., Hewitson M., Hild S., Hoak D., Hodge K.A., Holt K., Holtrop M., Hong T., Hooper S., Hosken D.J., Hough J., Howell E.J., Hughey B., Husa S., Huttner S.H., Huynh-dinh T., Ingram D.R., Inta R., Isogai T., Ivanov A., Izumi K., Jacobson M., James E., Jang Y.J., Jaranowski P., Jesse E., Johnson W.W., Jones D.I., Jones G., Jones R., Jonker R.J.G., Ju L., Kalmus P., Kalogera V., Kandhasamy S., Kang G., Kanner J.B., Kasturi R., Katsavounidis E., Katzman W., Kaufer H., Kawabe K., Kawamura S., Kawazoe F., Kelley D., Kells W., Keppel D.G., Keresztes Z., Khalaidovski A., Khalili F.Y., Khazanov E.A., Kim B.K., Kim C., Kim H., Kim K., Kim N., Kim Y.M., King P.J., Kinzel D.L., Kissel J.S., Klimenko S., Kokeyama K., Kondrashov V., Koranda S., Korth W.Z., Kowalska I., Kozak D., Kranz O., Kringel V., Krishnamurthy S., Krishnan B., Krolak A., Kuehn G., Kumar P., Kumar R., Kwee P., Lam P.K., Landry M., Lantz B., Lastzka N., Lawrie C., Lazzarini A., Leaci P., Lee C.H., Lee H.K., Lee H.M., Leong J.R., 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J., 760, 12 (2012)> =2012ApJ...760...12A 2012ApJ...760...12A (SIMBAD/NED BibCode)
ADC_Keywords: Gamma rays ; Interferometry Keywords: binaries: close; gamma-ray burst: general; gravitational waves Abstract: We present the results of a search for gravitational waves associated with 154 gamma-ray bursts (GRBs) that were detected by satellite-based gamma-ray experiments in 2009-2010, during the sixth LIGO science run and the second and third Virgo science runs. We perform two distinct searches: a modeled search for coalescences of either two neutron stars or a neutron star and black hole, and a search for generic, unmodeled gravitational-wave bursts. We find no evidence for gravitational-wave counterparts, either with any individual GRB in this sample or with the population as a whole. For all GRBs we place lower bounds on the distance to the progenitor, under the optimistic assumption of a gravitational-wave emission energy of 10-2Mc2 at 150Hz, with a median limit of 17Mpc. For short-hard GRBs we place exclusion distances on binary neutron star and neutron-star-black-hole progenitors, using astrophysically motivated priors on the source parameters, with median values of 16Mpc and 28Mpc, respectively. These distance limits, while significantly larger than for a search that is not aided by GRB satellite observations, are not large enough to expect a coincidence with a GRB. However, projecting these exclusions to the sensitivities of Advanced LIGO and Virgo, which should begin operation in 2015, we find that the detection of gravitational waves associated with GRBs will become quite possible. Description: The LIGO and Virgo detectors are kilometer-scale, power-recycled Michelson interferometers with orthogonal Fabry-Perot arms. They are designed to detect gravitational waves (GWs) with frequencies ranging from ∼40Hz to several kHz, with maximum sensitivity near 150Hz. There are two LIGO observatories: one located at Hanford, WA and the other at Livingston, LA. The Hanford site houses two interferometers: one with 4km arms (H1) and the other with 2km arms (H2). The Livingston observatory has one 4km interferometer (L1). The Virgo detector (V1) is in Cascina near Pisa, Italy. The sixth LIGO science run was held from 2009 July 07 to 2010 October 20. The second Virgo science run was held from 2009 July 7 to 2010 January 8 with an improvement in sensitivity by roughly a factor of two over Virgo's first science run. The third Virgo science run was held from 2010 August 11 to October 20. The overall Virgo duty cycle over these two science runs was 78% (See Figure 1). File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table1.dat 76 26 *Short GRB sample and search results table2.dat 74 128 *Long GRB sample and search results -------------------------------------------------------------------------------- Note on table1.dat and table2.dat: Information and limits on associated gravitational wave (GW) emission for each of the analyzed GRBs that were classified by us as short or long, respectively. -------------------------------------------------------------------------------- See also: VII/267 : Gravitational Wave Galaxy Catalogue (White+ 2011) J/ApJS/199/18 : The Fermi GBM catalog (Paciesas+, 2012) J/ApJ/715/1438 : Gravitational-wave bursts with GRBs (Abbott+, 2010) J/ApJ/713/671 : Gravitational waves from pulsars (Abbott+, 2010) http://gcn.gsfc.nasa.gov/ : The Gamma-ray Coordinates Network homepage http://heasarc.gsfc.nasa.gov/W3Browse/fermi/fermigbrst.html : Fermi GBM burst catalog Byte-by-byte Description of file: table[12].dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- GRB GRB name (YYMMDDA or YYMMDDNNN for the Fermi/GBM trigger ID) (1) 10 A1 --- f_GRB [Ds] GRB was assigned as short one (2) 12- 19 A8 "h:m:s" Time UTC trigger time 21- 22 I2 s Shift ? Time by which the trigger was shifted for the coalescence search (only for table 1) (3) 24- 25 I2 h RAh Hour of right ascension (J2000) (4) 27- 28 I2 min RAm Minute of right ascension (J2000) 30- 31 I2 s RAs Second of right ascension (J2000) 33 A1 --- DE- Sign of declination (J2000) (4) 34- 35 I2 deg DEd Degree of declination (J2000) (4) 37- 38 I2 arcmin DEm Arcminute of declination (J2000) 40- 45 A6 --- Nw [H1H2L1V1 ] Gravitational wave detector network used (5) 46- 48 A3 --- f_Nw [*dg, ] Observation peculiarity (6) 50- 53 F4.1 Mpc D150 [2.7/47.3]? Median exclusion distance for the GW burst at 150Hz (7) 55- 58 F4.1 Mpc D300 [0.4/18.2]? Median exclusion distance for the GW burst at 300Hz (7) 60- 63 F4.1 Mpc DNS-NS [2.1/37.1]? Median exclusion distance for two neutron stars (NS-NS) (only for table1) (7) 65- 68 F4.1 Mpc DNS-BH [3.7/64.5]? median exclusion distance for neutron star with a black hole (NS-BH) (only for table 1) (7) 70- 76 A7 --- Det γ-ray detector(s) (8) -------------------------------------------------------------------------------- Note (1): The GRB name in YYMMDD format or the Fermi/GBM trigger ID for GBM triggers classified as a GRB without an available GRB name (see http://heasarc.gsfc.nasa.gov/W3Browse/fermi/fermigbrst.html and Paciesas et al. 2012, Cat. J/ApJS/199/18) Note (2): Both a "s" and a "D" indicate that, although the formal duration of this GRB is longer than 4s ("D"), or unavailable ("s"), the GRB was analyzed as a short GRB because of a prominent short spike at the beginning of the light curve (see Section 4). Note (3): The time in seconds by which the trigger was shifted for the coalescence search following visual inspection of the light curve. Note (4): The sky position used for the GW search. Note (5): Detectors: H1 = LIGO Hanford interferometer with 4km arms (WA) H2 = LIGO Hanford interferometer with 2km arms (WA) L1 = LIGO Livingston 4km interferometer (LA) V1 = Virgo detector (Italy) Note (6): Flag as follows: * = when the shorter on-source window starting 120s before the trigger is used for the GW burst search, g = when the on-source window is extended to cover the GRB duration (T90>60s). d = use of only H1L1 data for the burst search, because of data-quality requirements. Note (7): The result of the search: the 90% confidence lower limits on the distance to the GRB for different waveform models. A standard siren energy emission of EGW=10-2Mc2 is assumed for the circular sine-Gaussian GW burst models; these limits are not available for four short GRBs which were not analyzed by GW burst search. See section 7.1. Note (8): The γ-ray detector that provided the sky location used for the search: AGILE, BAT, GBM, IBIS, IPN or LAT. For GRB 090802, IPN triangulation from Konus-WIND, INTEGRAL, and Fermi was used to further constrain the sky position. The intersection of the IPN and Fermi error regions was used to place search points using the method described in Predoi & Hurley (2012JPhCS.363a2034P 2012JPhCS.363a2034P). For this GRB, the quoted right ascension and declination correspond to the center of the Fermi error region. For IPN localizations a complete list of detectors can be found on the project trigger page, http://www.ssl.berkeley.edu/ipn3/masterli.txt. -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Emmanuelle Perret [CDS] 17-Jul-2014
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