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A directed search for gravitational waves from Scorpius X-1 with initial LIGO
J. Aasi, B. P. Abbott, R. Abbott, T. Abbott, M. R. Abernathy, F. Acernese, K. Ackley, C. Adams, T. Adams, P. Addesso, et al.
To cite this version:
J. Aasi, B. P. Abbott, R. Abbott, T. Abbott, M. R. Abernathy, et al.. A directed search for gravi-
tational waves from Scorpius X-1 with initial LIGO. Physical Review D, American Physical Society,
2015, 91 (6), pp.062008. �10.1103/PhysRevD.91.062008�. �in2p3-01091572�
Directed search for gravitational waves from Scorpius X-1 with initial LIGO data
J. Aasi,
1B. P. Abbott,
1R. Abbott,
1T. Abbott,
2M. R. Abernathy,
1F. Acernese,
3,4K. Ackley,
5C. Adams,
6T. Adams,
7,8P. Addesso,
9R. X. Adhikari,
1V. Adya,
10C. Affeldt,
10M. Agathos,
11K. Agatsuma,
11N. Aggarwal,
12O. D. Aguiar,
13A. Ain,
14P. Ajith,
15A. Alemic,
16B. Allen,
17,18A. Allocca,
19,20D. Amariutei,
5S. B. Anderson,
1W. G. Anderson,
18K. Arai,
1M. C. Araya,
1C. Arceneaux,
21J. S. Areeda,
22N. Arnaud,
23G. Ashton,
24S. Ast,
25S. M. Aston,
6P. Astone,
26P. Aufmuth,
25C. Aulbert,
17B. E. Aylott,
27S. Babak,
28P. T. Baker,
29F. Baldaccini,
30,31G. Ballardin,
32S. W. Ballmer,
16J. C. Barayoga,
1M. Barbet,
5S. Barclay,
33B. C. Barish,
1D. Barker,
34F. Barone,
3,4B. Barr,
33L. Barsotti,
12M. Barsuglia,
35J. Bartlett,
34M. A. Barton,
34I. Bartos,
36R. Bassiri,
37A. Basti,
38,20J. C. Batch,
34Th. S. Bauer,
11C. Baune,
10V. Bavigadda,
32B. Behnke,
28M. Bejger,
39C. Belczynski,
40A. S. Bell,
33C. Bell,
33M. Benacquista,
41J. Bergman,
34G. Bergmann,
10C. P. L. Berry,
27D. Bersanetti,
42,43A. Bertolini,
11J. Betzwieser,
6S. Bhagwat,
16R. Bhandare,
44I. A. Bilenko,
45G. Billingsley,
1J. Birch,
6S. Biscans,
12M. Bitossi,
32,20C. Biwer,
16M. A. Bizouard,
23J. K. Blackburn,
1L. Blackburn,
46C. D. Blair,
47D. Blair,
47S. Bloemen,
11,48O. Bock,
17T. P. Bodiya,
12M. Boer,
49G. Bogaert,
49P. Bojtos,
50C. Bond,
27F. Bondu,
51L. Bonelli,
38,20R. Bonnand,
8R. Bork,
1M. Born,
10V. Boschi,
20Sukanta Bose,
14,52C. Bradaschia,
20P. R. Brady,
18V. B. Braginsky,
45M. Branchesi,
53,54J. E. Brau,
55T. Briant,
56D. O. Bridges,
6A. Brillet,
49M. Brinkmann,
10V. Brisson,
23A. F. Brooks,
1D. A. Brown,
16D. D. Brown,
27N. M. Brown,
12S. Buchman,
37A. Buikema,
12T. Bulik,
40H. J. Bulten,
57,11A. Buonanno,
58D. Buskulic,
8C. Buy,
35L. Cadonati,
59G. Cagnoli,
60J. Calderón Bustillo,
61E. Calloni,
62,4J. B. Camp,
46K. C. Cannon,
63J. Cao,
64C. D. Capano,
58E. Capocasa,
35F. Carbognani,
32S. Caride,
65J. Casanueva Diaz,
23S. Caudill,
18M. Cavaglià,
21F. Cavalier,
23R. Cavalieri,
32G. Cella,
20C. Cepeda,
1E. Cesarini,
66R. Chakraborty,
1T. Chalermsongsak,
1S. J. Chamberlin,
18S. Chao,
67P. Charlton,
68E. Chassande-Mottin,
35Y. Chen,
69A. Chincarini,
43A. Chiummo,
32H. S. Cho,
70M. Cho,
58J. H. Chow,
71N. Christensen,
72Q. Chu,
47S. Chua,
56S. Chung,
47G. Ciani,
5F. Clara,
34J. A. Clark,
59F. Cleva,
49E. Coccia,
73,74P.-F. Cohadon,
56A. Colla,
75,26C. Collette,
76M. Colombini,
31L. Cominsky,
77M. Constancio, Jr.,
13A. Conte,
75,26D. Cook,
34T. R. Corbitt,
2N. Cornish,
29A. Corsi,
78C. A. Costa,
13M. W. Coughlin,
72J.-P. Coulon,
49S. Countryman,
36P. Couvares,
16D. M. Coward,
47M. J. Cowart,
6D. C. Coyne,
1R. Coyne,
78K. Craig,
33J. D. E. Creighton,
18T. D. Creighton,
41J. Cripe,
2S. G. Crowder,
79A. Cumming,
33L. Cunningham,
33E. Cuoco,
32C. Cutler,
69K. Dahl,
10T. Dal Canton,
17M. Damjanic,
10S. L. Danilishin,
47S. D ’ Antonio,
66K. Danzmann,
25,10L. Dartez,
41V. Dattilo,
32I. Dave,
44H. Daveloza,
41M. Davier,
23G. S. Davies,
33E. J. Daw,
80R. Day,
32D. DeBra,
37G. Debreczeni,
81J. Degallaix,
60M. De Laurentis,
62,4S. Deléglise,
56W. Del Pozzo,
27T. Denker,
10T. Dent,
17H. Dereli,
49V. Dergachev,
1R. De Rosa,
62,4R. T. DeRosa,
2R. DeSalvo,
9S. Dhurandhar,
14M. Díaz,
41L. Di Fiore,
4A. Di Lieto,
38,20I. Di Palma,
28A. Di Virgilio,
20G. Dojcinoski,
82V. Dolique,
60E. Dominguez,
83F. Donovan,
12K. L. Dooley,
10S. Doravari,
6R. Douglas,
33T. P. Downes,
18M. Drago,
84,85J. C. Driggers,
1Z. Du,
64M. Ducrot,
8S. Dwyer,
34T. Eberle,
10T. Edo,
80M. Edwards,
7M. Edwards,
72A. Effler,
2H.-B. Eggenstein,
17P. Ehrens,
1J. Eichholz,
5S. S. Eikenberry,
5R. Essick,
12T. Etzel,
1M. Evans,
12T. Evans,
6M. Factourovich,
36V. Fafone,
73,66S. Fairhurst,
7X. Fan,
33Q. Fang,
47S. Farinon,
43B. Farr,
86W. M. Farr,
27M. Favata,
82M. Fays,
7H. Fehrmann,
17M. M. Fejer,
37D. Feldbaum,
5,6I. Ferrante,
38,20E. C. Ferreira,
13F. Ferrini,
32F. Fidecaro,
38,20I. Fiori,
32R. P. Fisher,
16R. Flaminio,
60J.-D. Fournier,
49S. Franco,
23S. Frasca,
75,26F. Frasconi,
20Z. Frei,
50A. Freise,
27R. Frey,
55T. T. Fricke,
10P. Fritschel,
12V. V. Frolov,
6S. Fuentes-Tapia,
41P. Fulda,
5M. Fyffe,
6J. R. Gair,
87L. Gammaitoni,
30,31S. Gaonkar,
14F. Garufi,
62,4A. Gatto,
35N. Gehrels,
46G. Gemme,
43B. Gendre,
49E. Genin,
32A. Gennai,
20L. Á. Gergely,
88V. Germain,
8S. Ghosh,
11,48J. A. Giaime,
6,2K. D. Giardina,
6A. Giazotto,
20J. Gleason,
5E. Goetz,
17R. Goetz,
5L. Gondan,
50G. González,
2N. Gordon,
33M. L. Gorodetsky,
45S. Gossan,
69S. Goßler,
10R. Gouaty,
8C. Gräf,
33P. B. Graff,
46M. Granata,
60A. Grant,
33S. Gras,
12C. Gray,
34R. J. S. Greenhalgh,
89A. M. Gretarsson,
90P. Groot,
48H. Grote,
10S. Grunewald,
28G. M. Guidi,
53,54C. J. Guido,
6X. Guo,
64K. Gushwa,
1E. K. Gustafson,
1R. Gustafson,
65J. Hacker,
22E. D. Hall,
1G. Hammond,
33M. Hanke,
10J. Hanks,
34C. Hanna,
91M. D. Hannam,
7J. Hanson,
6T. Hardwick,
55,2J. Harms,
54G. M. Harry,
92I. W. Harry,
28M. Hart,
33M. T. Hartman,
5C.-J. Haster,
27K. Haughian,
33A. Heidmann,
56M. Heintze,
5,6G. Heinzel,
10H. Heitmann,
49P. Hello,
23G. Hemming,
32M. Hendry,
33I. S. Heng,
33A. W. Heptonstall,
1M. Heurs,
10M. Hewitson,
10S. Hild,
33D. Hoak,
59K. A. Hodge,
1D. Hofman,
60S. E. Hollitt,
93K. Holt,
6P. Hopkins,
7D. J. Hosken,
93J. Hough,
33E. Houston,
33E. J. Howell,
47Y. M. Hu,
33E. Huerta,
94B. Hughey,
90S. Husa,
61S. H. Huttner,
33M. Huynh,
18T. Huynh-Dinh,
6A. Idrisy,
91N. Indik,
17D. R. Ingram,
34R. Inta,
91G. Islas,
22J. C. Isler,
16T. Isogai,
12B. R. Iyer,
95K. Izumi,
34M. Jacobson,
1H. Jang,
96P. Jaranowski,
97S. Jawahar,
98Y. Ji,
64F. Jiménez-Forteza,
61W. W. Johnson,
2D. I. Jones,
24R. Jones,
33R. J. G. Jonker,
11L. Ju,
47K. Haris,
99V. Kalogera,
86S. Kandhasamy,
21G. Kang,
96J. B. Kanner,
1M. Kasprzack,
23,32E. Katsavounidis,
12W. Katzman,
6H. Kaufer,
25S. Kaufer,
25T. Kaur,
47K. Kawabe,
34F. Kawazoe,
10F. Kéfélian,
49G. M. Keiser,
37D. Keitel,
17D. B. Kelley,
16W. Kells,
1D. G. Keppel,
17J. S. Key,
41A. Khalaidovski,
10F. Y. Khalili,
45E. A. Khazanov,
100C. Kim,
101,96K. Kim,
102N. G. Kim,
96N. Kim,
37Y.-M. Kim,
70E. J. King,
93P. J. King,
34D. L. Kinzel,
6J. S. Kissel,
34S. Klimenko,
5J. Kline,
18S. Koehlenbeck,
10K. Kokeyama,
2V. Kondrashov,
1M. Korobko,
10PHYSICAL REVIEW D
91,062008 (2015)
W. Z. Korth,
1I. Kowalska,
40D. B. Kozak,
1V. Kringel,
10B. Krishnan,
17A. Królak,
103,104C. Krueger,
25G. Kuehn,
10A. Kumar,
105P. Kumar,
16L. Kuo,
67A. Kutynia,
103M. Landry,
34B. Lantz,
37S. Larson,
86P. D. Lasky,
106A. Lazzarini,
1C. Lazzaro,
107C. Lazzaro,
59J. Le,
86P. Leaci,
28S. Leavey,
33E. Lebigot,
35E. O. Lebigot,
64C. H. Lee,
70H. K. Lee,
102H. M. Lee,
101M. Leonardi,
84,85J. R. Leong,
10N. Leroy,
23N. Letendre,
8Y. Levin,
108B. Levine,
34J. Lewis,
1T. G. F. Li,
1K. Libbrecht,
1A. Libson,
12A. C. Lin,
37T. B. Littenberg,
86N. A. Lockerbie,
98V. Lockett,
22J. Logue,
33A. L. Lombardi,
59M. Lorenzini,
74V. Loriette,
109M. Lormand,
6G. Losurdo,
54J. Lough,
17M. J. Lubinski,
34H. Lück,
25,10A. P. Lundgren,
17R. Lynch,
12Y. Ma,
47J. Macarthur,
33T. MacDonald,
37B. Machenschalk,
17M. MacInnis,
12D. M. Macleod,
2F. Magaña-Sandoval,
16R. Magee,
52M. Mageswaran,
1C. Maglione,
83K. Mailand,
1E. Majorana,
26I. Maksimovic,
109V. Malvezzi,
73,66N. Man,
49I. Mandel,
27V. Mandic,
79V. Mangano,
33V. Mangano,
75,26G. L. Mansell,
71M. Mantovani,
32,20F. Marchesoni,
110,31F. Marion,
8S. Márka,
36Z. Márka,
36A. Markosyan,
37E. Maros,
1F. Martelli,
53,54L. Martellini,
49I. W. Martin,
33R. M. Martin,
5D. Martynov,
1J. N. Marx,
1K. Mason,
12A. Masserot,
8T. J. Massinger,
16F. Matichard,
12L. Matone,
36N. Mavalvala,
12N. Mazumder,
99G. Mazzolo,
17R. McCarthy,
34D. E. McClelland,
71S. McCormick,
6S. C. McGuire,
111G. McIntyre,
1J. McIver,
59K. McLin,
77S. McWilliams,
94D. Meacher,
49G. D. Meadors,
65J. Meidam,
11M. Meinders,
25A. Melatos,
106G. Mendell,
34R. A. Mercer,
18S. Meshkov,
1C. Messenger,
33P. M. Meyers,
79F. Mezzani,
26,75H. Miao,
27C. Michel,
60H. Middleton,
27E. E. Mikhailov,
112L. Milano,
62,4A. Miller,
113J. Miller,
12M. Millhouse,
29Y. Minenkov,
66J. Ming,
28S. Mirshekari,
114C. Mishra,
15S. Mitra,
14V. P. Mitrofanov,
45G. Mitselmakher,
5R. Mittleman,
12B. Moe,
18A. Moggi,
20M. Mohan,
32S. D. Mohanty,
41S. R. P. Mohapatra,
12B. Moore,
82D. Moraru,
34G. Moreno,
34S. R. Morriss,
41K. Mossavi,
10B. Mours,
8C. M. Mow-Lowry,
10C. L. Mueller,
5G. Mueller,
5S. Mukherjee,
41A. Mullavey,
6J. Munch,
93D. Murphy,
36P. G. Murray,
33A. Mytidis,
5M. F. Nagy,
81I. Nardecchia,
73,66T. Nash,
1L. Naticchioni,
75,26R. K. Nayak,
115V. Necula,
5K. Nedkova,
59G. Nelemans,
11,48I. Neri,
30,31M. Neri,
42,43G. Newton,
33T. Nguyen,
71A. B. Nielsen,
17S. Nissanke,
69A. H. Nitz,
16F. Nocera,
32D. Nolting,
6M. E. N. Normandin,
41L. K. Nuttall,
18E. Ochsner,
18J. O ’ Dell,
89E. Oelker,
12G. H. Ogin,
116J. J. Oh,
117S. H. Oh,
117F. Ohme,
7P. Oppermann,
10R. Oram,
6B. O ’ Reilly,
6W. Ortega,
83R. O ’ Shaughnessy,
118C. Osthelder,
1C. D. Ott,
69D. J. Ottaway,
93R. S. Ottens,
5H. Overmier,
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91C. Padilla,
22A. Pai,
99S. Pai,
44O. Palashov,
100C. Palomba,
26A. Pal-Singh,
10H. Pan,
67C. Pankow,
18F. Pannarale,
7B. C. Pant,
44F. Paoletti,
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37A. Pasqualetti,
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32L. Pinard,
60I. M. Pinto,
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33J. Poeld,
10R. Poggiani,
38,20A. Post,
17A. Poteomkin,
100J. Powell,
33J. Prasad,
14V. Predoi,
7S. Premachandra,
108T. Prestegard,
79L. R. Price,
1M. Prijatelj,
32M. Principe,
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17G. A. Prodi,
84,85L. Prokhorov,
45O. Puncken,
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31P. Puppo,
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44G. Rajalakshmi,
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75,26V. Raymond,
1M. Razzano,
38,20V. Re,
73,66C. M. Reed,
34T. Regimbau,
49L. Rei,
43S. Reid,
121D. H. Reitze,
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23A. Rocchi,
66L. Rolland,
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3,4G. Romanov,
112J. H. Romie,
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81R. Vaulin,
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27G. Vedovato,
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53,54R. Vincent-Finley,
111J.-Y. Vinet,
49S. Vitale,
12T. Vo,
34H. Vocca,
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45A. R. Wade,
71L. Wade,
18M. Wade,
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27M. Wang,
27X. Wang,
64R. L. Ward,
71J. Warner,
34M. Was,
10M. Was,
8B. Weaver,
34L.-W. Wei,
49M. Weinert,
10A. J. Weinstein,
1R. Weiss,
12T. Welborn,
6L. Wen,
47P. Wessels,
10T. Westphal,
10K. Wette,
17J. T. Whelan,
118,17D. J. White,
80B. F. Whiting,
5C. Wilkinson,
34L. Williams,
5R. Williams,
1A. R. Williamson,
7J. L. Willis,
113B. Willke,
25,10M. Wimmer,
10W. Winkler,
10C. C. Wipf,
12H. Wittel,
10G. Woan,
33J. Worden,
34S. Xie,
76J. Yablon,
86I. Yakushin,
6W. Yam,
12H. Yamamoto,
1C. C. Yancey,
58Q. Yang,
64M. Yvert,
8A. Zadro ż ny,
103M. Zanolin,
90J.-P. Zendri,
107Fan Zhang,
12,64L. Zhang,
1M. Zhang,
112Y. Zhang,
118C. Zhao,
47M. Zhou,
86X. J. Zhu,
47M. E. Zucker,
12S. Zuraw,
59and J. Zweizig
1(LIGO Scientific Collaboration, Virgo Collaboration)
1
LIGO, California Institute of Technology, Pasadena, California 91125, USA
2
Louisiana State University, Baton Rouge, Louisiana 70803, USA
3
Università di Salerno, Fisciano, I-84084 Salerno, Italy
4
INFN, Sezione di Napoli, Complesso Universitario di Monte Sant
’Angelo, I-80126 Napoli, Italy
5
University of Florida, Gainesville, Florida 32611, USA
6
LIGO Livingston Observatory, Livingston, Louisiana 70754, USA
7
Cardiff University, Cardiff CF24 3AA, United Kingdom
8
Laboratoire d
’Annecy-le-Vieux de Physique des Particules (LAPP), Université de Savoie, CNRS/IN2P3, F-74941 Annecy-le-Vieux, France
9
University of Sannio at Benevento, I-82100 Benevento, Italy and INFN, Sezione di Napoli, I-80100 Napoli, Italy
10
Experimental Group, Albert-Einstein-Institut, Max-Planck-Institut für Gravitationsphysik, D-30167 Hannover, Germany
11
Nikhef, Science Park, 1098 XG Amsterdam, The Netherlands
12
LIGO, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
13
Instituto Nacional de Pesquisas Espaciais, 12227-010 São José dos Campos, São Paulo, Brazil
14
Inter-University Centre for Astronomy and Astrophysics, Pune 411007, India
15
International Centre for Theoretical Sciences, Tata Institute of Fundamental Research, Bangalore 560012, India
16
Syracuse University, Syracuse, New York 13244, USA
17
Data Analysis Group, Albert-Einstein-Institut, Max-Planck-Institut für Gravitationsphysik, D-30167 Hannover, Germany
18
University of Wisconsin
–Milwaukee, Milwaukee, Wisconsin 53201, USA
19
Università di Siena, I-53100 Siena, Italy
20
INFN, Sezione di Pisa, I-56127 Pisa, Italy
21
The University of Mississippi, University, Mississippi 38677, USA
22
California State University Fullerton, Fullerton, California 92831, USA
23
LAL, Université Paris-Sud, IN2P3/CNRS, F-91898 Orsay, France
24
University of Southampton, Southampton SO17 1BJ, United Kingdom
25
Leibniz Universität Hannover, D-30167 Hannover, Germany
26
INFN, Sezione di Roma, I-00185 Roma, Italy
27
University of Birmingham, Birmingham B15 2TT, United Kingdom
28
Albert-Einstein-Institut, Max-Planck-Institut für Gravitationsphysik, D-14476 Golm, Germany
29
Montana State University, Bozeman, Montana 59717, USA
30
Università di Perugia, I-06123 Perugia, Italy
31
INFN, Sezione di Perugia, I-06123 Perugia, Italy
32
European Gravitational Observatory (EGO), I-56021 Cascina, Pisa, Italy
33
SUPA, University of Glasgow, Glasgow G12 8QQ, United Kingdom
34
LIGO Hanford Observatory, Richland, Washington 99352, USA
35
APC, AstroParticule et Cosmologie, Université Paris Diderot, CNRS/IN2P3, CEA/Irfu, Observatoire de Paris, Sorbonne Paris Cité, 10, rue Alice Domon et Léonie Duquet,
F-75205 Paris Cedex 13, France
36
Columbia University, New York, New York 10027, USA
37
Stanford University, Stanford, California 94305, USA
38
Università di Pisa, I-56127 Pisa, Italy
39
CAMK-PAN, 00-716 Warsaw, Poland
40
Astronomical Observatory Warsaw University, 00-478 Warsaw, Poland
41
The University of Texas at Brownsville, Brownsville, Texas 78520, USA
42
Università degli Studi di Genova, I-16146 Genova, Italy
43
INFN, Sezione di Genova, I-16146 Genova, Italy
44
RRCAT, Indore Madhya Pradesh 452013, India
45
Faculty of Physics, Lomonosov Moscow State University, Moscow 119991, Russia
46
NASA/Goddard Space Flight Center, Greenbelt, Maryland 20771, USA
DIRECTED SEARCH FOR GRAVITATIONAL WAVES FROM
…PHYSICAL REVIEW D
91,062008 (2015)
47
University of Western Australia, Crawley, Western Australia 6009, Australia
48
Department of Astrophysics/IMAPP, Radboud University Nijmegen, P.O. Box 9010, 6500 GL Nijmegen, The Netherlands
49
ARTEMIS, Université Nice-Sophia-Antipolis, CNRS and Observatoire de la Côte d
’Azur, F-06304 Nice, France
50
MTA Eötvös University,
‘Lendulet
’Astrophysics Research Group, Budapest 1117, Hungary
51
Institut de Physique de Rennes, CNRS, Université de Rennes 1, F-35042 Rennes, France
52
Washington State University, Pullman, Washington 99164, USA
53
Università degli Studi di Urbino
‘Carlo Bo,
’I-61029 Urbino, Italy
54
INFN, Sezione di Firenze, I-50019 Sesto Fiorentino, Firenze, Italy
55
University of Oregon, Eugene, Oregon 97403, USA
56
Laboratoire Kastler Brossel, ENS, CNRS, UPMC, Université Pierre et Marie Curie, F-75005 Paris, France
57
VU University Amsterdam, 1081 HV Amsterdam, The Netherlands
58
University of Maryland, College Park, Maryland 20742, USA
59
University of Massachusetts Amherst, Amherst, Massachusetts 01003, USA
60
Laboratoire des Matériaux Avancés (LMA), IN2P3/CNRS, Université de Lyon, F-69622 Villeurbanne, Lyon, France
61
Universitat de les Illes Balears
—IEEC, E-07122 Palma de Mallorca, Spain
62
Università di Napoli
‘Federico II,
’Complesso Universitario di Monte Sant
’Angelo, I-80126 Napoli, Italy
63
Canadian Institute for Theoretical Astrophysics, University of Toronto, Toronto, Ontario M5S 3H8, Canada
64
Tsinghua University, Beijing 100084, China
65
University of Michigan, Ann Arbor, Michigan 48109, USA
66
INFN, Sezione di Roma Tor Vergata, I-00133 Roma, Italy
67
National Tsing Hua University, Hsinchu 300, Taiwan
68
Charles Sturt University, Wagga Wagga NSW 2678, Australia
69
Caltech-CaRT, Pasadena, California 91125, USA
70
Pusan National University, Busan 609-735, Korea
71
Australian National University, Canberra ACT 0200, Australia
72
Carleton College, Northfield, Minnesota 55057, USA
73
Università di Roma Tor Vergata, I-00133 Roma, Italy
74
INFN, Gran Sasso Science Institute, I-67100 L
’Aquila, Italy
75
Università di Roma
‘La Sapienza,
’I-00185 Roma, Italy
76
University of Brussels, Brussels 1050, Belgium
77
Sonoma State University, Rohnert Park, California 94928, USA
78
Texas Tech University, Lubbock, Texas 79409, USA
79
University of Minnesota, Minneapolis, Minnesota 55455, USA
80
The University of Sheffield, Sheffield S10 2TN, United Kingdom
81
Wigner RCP, RMKI, H-1121 Budapest, Konkoly Thege Miklós út 29-33, Hungary
82
Montclair State University, Montclair, New Jersey 07043, USA
83
Argentinian Gravitational Wave Group, Cordoba Cordoba 5000, Argentina
84
Università di Trento, I-38123 Povo, Trento, Italy
85
INFN, Trento Institute for Fundamental Physics and Applications, I-38123 Povo, Trento, Italy
86
Northwestern University, Evanston, Illinois 60208, USA
87
University of Cambridge, Cambridge CB2 1TN, United Kingdom
88
University of Szeged, Dóm tér 9, Szeged 6720, Hungary
89
Rutherford Appleton Laboratory, HSIC, Chilton, Didcot, Oxon OX11 0QX, United Kingdom
90
Embry-Riddle Aeronautical University, Prescott, Arizona 86301, USA
91
The Pennsylvania State University, University Park, Pennsylvania 16802, USA
92
American University, Washington DC 20016, USA
93
University of Adelaide, Adelaide, SA 5005, Australia
94
West Virginia University, Morgantown, West Virginia 26506, USA
95
Raman Research Institute, Bangalore, Karnataka 560080, India
96
Korea Institute of Science and Technology Information, Daejeon 305-806, Korea
97
University of Bia
łystok, 15-424 Bia
łystok, Poland
98
SUPA, University of Strathclyde, Glasgow G1 1XQ, United Kingdom
99
IISER-TVM, CET Campus, Trivandrum, Kerala 695016, India
100
Institute of Applied Physics, Nizhny Novgorod, 603950, Russia
101
Seoul National University, Seoul 151-742, Korea
102
Hanyang University, Seoul 133-791, Korea
103
NCBJ, 05-400
Świerk-Otwock, Poland
104
IM-PAN, 00-956 Warsaw, Poland
105
Institute for Plasma Research, Bhat, Gandhinagar 382428, India
106
The University of Melbourne, Parkville VIC 3010, Australia
107
INFN, Sezione di Padova, I-35131 Padova, Italy
108
Monash University, Victoria 3800, Australia
109
ESPCI, CNRS, F-75005 Paris, France
110
Università di Camerino, Dipartimento di Fisica, I-62032 Camerino, Italy
111
Southern University and A&M College, Baton Rouge, Louisiana 70813, USA
112
College of William and Mary, Williamsburg, Virginia 23187, USA
113
Abilene Christian University, Abilene, Texas 79699, USA
114
Instituto de Física Teórica, University Estadual Paulista/ICTP South American Institute for Fundamental Research, São Paulo, São Paulo 01140-070, Brazil
115
IISER-Kolkata, Mohanpur, West Bengal 741252, India
116
Whitman College, 280 Boyer Avenue, Walla Walla, Washington 99362, USA
117
National Institute for Mathematical Sciences, Daejeon 305-390, Korea
118
Rochester Institute of Technology, Rochester, New York 14623, USA
119
Hobart and William Smith Colleges, Geneva, New York 14456, USA
120
Tata Institute for Fundamental Research, Mumbai 400005, India
121
SUPA, University of the West of Scotland, Paisley PA1 2BE, United Kingdom
122
Institute of Astronomy, 65-265 Zielona Góra, Poland
123
Universität Hamburg, D-22761 Hamburg, Germany
124
Indian Institute of Technology, Gandhinagar, Ahmedabad, Gujarat 382424, India
125
Andrews University, Berrien Springs, Michigan 49104, USA
126
Trinity University, San Antonio, Texas 78212, USA
127
University of Washington, Seattle, Washington 98195, USA (Received 3 December 2014; published 26 March 2015)
We present results of a search for continuously emitted gravitational radiation, directed at the brightest low-mass x-ray binary, Scorpius X-1. Our semicoherent analysis covers 10 days of LIGO S5 data ranging from 50
–550 Hz, and performs an incoherent sum of coherent
F-statistic power distributed amongst frequency-modulated orbital sidebands. All candidates not removed at the veto stage were found to be consistent with noise at a 1% false alarm rate. We present Bayesian 95% confidence upper limits on gravitational-wave strain amplitude using two different prior distributions: a standard one, with no a priori assumptions about the orientation of Scorpius X-1; and an angle-restricted one, using a prior derived from electromagnetic observations. Median strain upper limits of
1.
3×
10−24and
8×
10−25are reported at 150 Hz for the standard and angle-restricted searches respectively. This proof-of-principle analysis was limited to a short observation time by unknown effects of accretion on the intrinsic spin frequency of the neutron star, but improves upon previous upper limits by factors of
∼1.
4for the standard, and 2.3 for the angle-restricted search at the sensitive region of the detector.
DOI:10.1103/PhysRevD.91.062008 PACS numbers: 95.85.Sz, 97.60.Jd, 97.80.Jp
I. INTRODUCTION
Recycled neutron stars are a likely source of persistent, quasimonochromatic gravitational waves detectable by ground-based interferometric detectors. Emission mecha- nisms include thermocompositional and magnetic moun- tains [1–6], unstable oscillation modes [7] and free precession [8]. If the angular momentum lost to gravita- tional radiation is balanced by the spin-up torque from accretion, the gravitational-wave strain h
0can be estimated independently of the microphysical origin of the quadrupole and is proportional to the observable x-ray flux F
xand spin frequency ν
s[9,10] via h
0∝ ðF
X=ν
sÞ
1=2. Given the assumption of torque balance, the strongest
gravitational-wave sources are those that are most proxi- mate with the highest accretion rate and hence x-ray flux, such as low-mass x-ray binary (LMXB) systems. In this sense the most luminous gravitational-wave LMXB source is Scorpius X-1 (Sco X-1).
The plausibility of the torque-balance scenario is strengthened by observations of the spin frequencies ν
sof pulsating or bursting LMXBs, which show them
clustered in a relatively narrow band from 270 ≤ ν
s≤
620 Hz [11], even though their ages and accretions rates
imply that they should have accreted enough matter to
reach the centrifugal break-up limit ν
max∼ 1400 Hz [12] of
the neutron star. The gravitational-wave spin-down torque
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91,062008 (2015)
scales as ν
5s, mapping a wide range of accretion rates into a narrow range of equilibrium spins, so far conforming with observations. Alternative explanations for the clustering of LMXB spin periods involving disc accretion physics have been proposed [13]. Although this explanation suggests that gravitational radiation is not required to brake the spin- up of the neutron star, it does not rule out gravitational emission from these systems. The gravitational-wave torque-balance argument is used here as an approximate bound.
The initial instruments installed in the Laser Interferometer Gravitational Wave Observatory (LIGO) consisted of three Michelson interferometers, one with 4-km orthogonal arms at Livingston, LA, and two collo- cated at Hanford, CA, with 4-km and 2-km arms. Initial LIGO achieved its design sensitivity during its fifth science run (between November 2005 and October 2007) [14,15]
and is currently being upgraded to the next-generation Advanced LIGO configuration, which is expected to improve its sensitivity tenfold in strain [16].
Three types of searches have previously been con- ducted with LIGO data for Sco X-1. The first, a coherent analysis using data from LIGO’s second science run (S2), was computationally limited to six-hour data segments. It placed a wave-strain upper limit at 95% confidence of h
950≈ 2 × 10
−22for two 20 Hz bands between 464 – 484 Hz and 604 – 626 Hz [17]. The second, employing a radiom- eter technique [18], was conducted using all 20 days of LIGO S4 data [19]. It improved the upper limits on the previous (S2) search by an order of magnitude in the relevant frequency bands but did not yield a detection. The same method was later applied to S5 data and reported roughly a fivefold sensitivity improvement over the S4 results [20]. The S5 analysis returned a median 90%
confidence root-mean-square strain upper limit of h
90rms¼ 7 × 10
−25at 150 Hz, the most sensitive detector frequency (this converts to h
950≈ 2 × 10
−24[21 – 23]). Thirdly, an all-sky search for continuous gravitational waves from sources in binary systems, which looks for patterns caused by binary orbital motion doubly Fourier-transformed data (TwoSpect), was adapted to search the Sco X-1 sky position, and returned results in the low frequency band from 20 – 57.25 Hz [24].
Here we implement a new search for gravitational waves from sources in known binary systems, with unknown spin frequency, initially directed at Sco X-1 on LIGO S5 data to demonstrate feasibility. Values of the coherent, matched- filtered F -statistic [25] are incoherently summed at the locations of frequency-modulated sidebands. This multi- stage, semicoherent, analysis yields a new detection sta- tistic, denoted the C -statistic [26,27]. A similar technique was first employed in electromagnetic searches for radio pulsars [28]. We utilize this technique to efficiently deal with the large parameter space introduced by the orbital motion of a source in a binary system.
A brief description of the search is given in Sec. II, while the astrophysical target source and its associated parameter space are discussed in Sec. III. Section IV outlines the search method, reviews the pipeline, discusses the selection and preprocessing of LIGO S5 data, and explains the postprocessing procedure. Results of the search, including upper limits of gravitational-wave strain, are presented and discussed in Sections V and VI, respectively and restated in Sec. VII.
II. SEARCH METHOD
For a gravitational-wave source in a binary system, the frequency of the signal is Doppler modulated by the orbital motion of the source with respect to the Earth [26 – 28]. The semicoherent sideband search method involves the inco- herent summation of frequency-modulated sidebands of the coherent F -statistic [25–27].
The first step in the sideband search is to calculate the coherent F -statistic as a function of frequency, assuming only a fixed sky position. Knowing the sky position, one can account for the phase evolution due to the motion of the detector. For sources in binary systems, the orbital motion splits the signal contribution to the F -statistic into approximately M ¼ 2m þ 1 sidebands separated by 1=P in frequency, where m ¼ ceiling ð2πf
0a
0Þ [29], f
0is the intrinsic gravitational-wave frequency, a
0is the light travel time across the semimajor axis of the orbit, and P is the orbital period. Knowledge of P and a
0allows us to construct an F -statistic sideband template.
The second stage of the sideband pipeline is the calculation of the C -statistic, where we convolve the side- band template with the coherent F -statistic. The result is an incoherent sum of the signal power at each of the potential sidebands as a function of intrinsic gravitational-wave frequency. For our template we use a flat comb function with equal amplitude teeth (see Fig. 1 of [27]), and hence, for a discrete frequency bin f
k, the template is given by
T ðf
kÞ ¼ X
m0j¼−m0
δ
kl½j; ð1Þ
where m
0¼ ceiling ð2πf
0a
0Þ depends on search frequency f
0and the semimajor axis a
0used to construct the template (see Sec. III D) [30]. The index l
½jof the Kronecker delta function is defined as
l
½j≡ round j
P
0Δ
f; ð2Þ
for a frequency bin width Δf , where round ðÞ returns
the closest integer, and P
0denotes our best guess at the
orbital period. The following convolution then yields the
C -statistic:
Cðf
kÞ ¼ ð2F T Þðf
kÞ ð 3 Þ
¼ X
m0j¼−m0