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Searches for Gravitational Waves from Known Pulsars at Two Harmonics in 2015–2017 LIGO Data
B. P. Abbott1, R. Abbott1, T. D. Abbott2, S. Abraham3, F. Acernese4,5, K. Ackley6, C. Adams7, R. X. Adhikari1, V. B. Adya8,9, C. Affeldt8,9Show full author list
Published 2019 June 26 • © 2019. The American Astronomical Society. All rights reserved.
The Astrophysical Journal, Volume 879, Number 1
Citation B. P. Abbott et al 2019 ApJ 879 10
DOI 10.3847/1538-4357/ab20cb
DownloadArticle PDF DownloadArticle ePub
This article is corrected by 2019 ApJ 882 73
This article is corrected by 2020 ApJ 899 170
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Abstract
We present a search for gravitational waves from 222 pulsars with rotation frequencies ≳10 Hz. We use advanced LIGO data from its first and second observing runs spanning 2015–2017, which provides the highest-sensitivity gravitational-wave data so far obtained. In this search we target emission from both the l = m = 2 mass quadrupole mode, with a frequency at twice that of the pulsar's rotation, and the l = 2, m = 1 mode, with a frequency at the pulsar rotation frequency. The search finds no evidence for gravitational-wave emission from any pulsar at either frequency. For the l = m = 2 mode search, we provide updated upper limits on the gravitational-wave amplitude, mass quadrupole moment, and fiducial ellipticity for 167 pulsars, and the first such limits for a further 55. For 20 young pulsars these results give limits that are below those inferred from the pulsars' spin-down. For the Crab and Vela pulsars our results constrain gravitational-wave emission to account for less than 0.017% and 0.18% of the spin-down luminosity, respectively. For the recycled millisecond pulsar J0711−6830 our limits are only a factor of 1.3 above the spin-down limit, assuming the canonical value of 1038 kg m2 for the star's moment of inertia, and imply a gravitational-wave-derived upper limit on the star's ellipticity of 1.2 × 10−8. We also place new limits on the emission amplitude at the rotation frequency of the pulsars.
Abbott, B.p., Abbott, R., Abbott, T.d., Abraham, S., Acernese, F., Ackley, K., et al. (2019). Searches for Gravitational Waves from Known Pulsars at Two Harmonics in 2015-2017 LIGO Data. THE ASTROPHYSICAL JOURNAL, 882(1), 10-37 [10.3847/1538-4357/ab3231].
Searches for Gravitational Waves from Known Pulsars at Two Harmonics in 2015-2017 LIGO Data
Abbott BP; Abbott R; Abbott TD; Abraham S; Acernese F; Ackley K; Adams C; Adhikari RX; Adya VB; Affeldt C; Agathos M; Agatsuma K; Aggarwal N; Aguiar OD; Aiello L; Ain A; Ajith P; Allen G; Allocca A; Aloy MA; Altin PA; Amato A; Anand S; Ananyeva A; Anderson SB; Anderson WG; Angelova SV; Antier S; Appert S; Arai K; Araya MC; Areeda JS; Arene M; Arnaud N; Aronson SM; Ascenzi S; Ashton G; Aston SM; Astone P; Aubin F; Aufmuth P; AultONeal K; Austin C; Avendano V; Avila-Alvarez A; Babak S; Bacon P; Badaracco F; Bader MKM; Bae S; Baird J; Baker PT; Baldaccini F; Ballardin G; Ballmer SW; Bals A; Banagiri S; Barayoga JC; Barbieri C; Barclay SE; Barish BC; Barker D; Barkett K; Barnum S; Barone F; Barr B; Barsotti L; Barsuglia M; Barta D; Bartlett J; Bartos I; Bassiri R; Basti A; Bawaj M; Bayley JC; Bazzan M; Becsy B; Bejger M; Belahcene I; Bell AS; Beniwal D; Benjamin MG; Berger BK; Bergmann G; Bernuzzi S; Berry CPL; Bersanetti D; Bertolini A; Betzwieser J; Bhandare R; Bidler J; Biggs E; Bilenko IA; Bilgili SA; Billingsley G; Birney R; Birnholtz O; Biscans S; Bischi M; Biscoveanu S; Bisht A; Bitossi M; Bizouard MA; Blackburn JK; Blackman J; Blair CD; Blair DG; Blair RM; Bloemen S; Bobba F; Bode N; Boer M; Boetzel Y; Bogaert G; Bondu F; Bonnand R; Booker P; Boom BA; Bork R; Boschi V; Bose S; Bossilkov V; Bosveld J; Bouffanais Y; Bozzi A; Bradaschia C; Brady PR; Bramley A; Branchesi M; Brau JE; Breschi M; Briant T; Briggs JH; Brighenti F; Brillet A; Brinkmann M; Brockill P; Brooks AF; Brooks J; Brown DD; Brunett S; Buikema A; Bulik T; Bulten HJ; Buonanno A; Buskulic D; Buy C; Byer RL; Cabero M; Cadonati L; Cagnoli G; Cahillane C; Bustillo JC; Callister TA; Calloni E; Camp JB; Campbell WA; Cannon KC; Cao H; Cao J; Carapella G; Carbognani F; Caride S; Carney MF; Carullo G; Diaz JC; Casentini C; Caudill S; Cavaglia M; Cavalier F; Cavalieri R; Cella G; Cerda-Duran P; Cesarini E; Chaibi O; Chakravarti K; Chamberlin SJ; Chan M; Chao S; Charlton P; Chase EA; Chassande-Mottin E; Chatterjee D; Chaturvedi M; Cheeseboro BD; Chen HY; Chen X; Chen Y; Cheng HP; Cheong CK; Chia HY; Chiadini F; Chincarini A; Chiummo A; Cho G; Cho HS; Cho M; Christensen N; Chu Q; Chua S; Chung KW; Chung S; Ciani G; Cieslar M; Ciobanu AA; Ciolfi R; Cipriano F; Cirone A; Clara F; Clark JA; Clearwater P; Cleva F; Coccia E; Cohadon PF; Cohen D; Colleoni M; Collette CG; Collins C; Colpi M; Cominsky LR; Constancio M; Conti L; Cooper SJ; Corban P; Corbitt TR; Cordero-Carrion I; Corley KR; Cornish N; Corre D; Corsi A; Cortese S; Costa CA; Cotesta R; Coughlin MW; Coughlin SB; Coulon JP; Countryman ST; Couvares P; Covas PB; Cowan EE; Coward DM; Cowart MJ; Coyne DC; Coyne R; Creighton JDE; Creighton TD; Cripe J; Croquette M; Crowder SG; Cullen TJ; Cumming A; Cunningham L; Cuoco E ;Dal Canton T; Dalya G; D'Angelo B; Danilishin SL; D'Antonio S; Danzmann K; Dasgupta A; Costa CFD; Datrier LEH; Dattilo V; Dave I; Davier M; Davis D; Daw EJ; DeBra D; Deenadayalan M; Degallaix J; De Laurentis M; Deleglise S; Del Pozzo W; DeMarchi LM; Demos N; Dent T; De Pietri R; De Rosa R; De Rossi C; DeSalvo R; de Varona O; Dhurandhar S; Diaz MC; Dietrich T; Di Fiore L; DiFronzo C; Di Giorgio C; Di Giovanni F; Di Giovanni M; Di Girolamo T; Di Lieto A; Ding B; Di Pace S; Di Palma I; Di Renzo F; Divakarla AK; Dmitriev A; Doctor Z; Donovan F; Dooley KL; Doravari S; Dorrington I; Downes TP; Drago M; Driggers JC; Du Z; Ducoin JG; Dupej P; Durante O; Dwyer SE; Easter PJ; Eddolls G; Edo TB; Effler A; Ehrens P; Eichholz J; Eikenberry SS; Eisenmann M; Eisenstein RA; Errico L; Essick RC; Estelles H; Estevez D; Etienne ZB; Etzel T; Evans M; Evans TM; Fafone V; Fairhurst S; Fan X; Farinon S; Farr B; Farr WM; Fauchon-Jones EJ; Favata M; Fays M; Fazio M; Fee C; Feicht J; Fejer MM; Feng F; Fernandez-Galiana A; Ferrante I; Ferreira EC; Ferreira TA; Fidecaro F; Fiori I; Fiorucci D; Fishbach M; Fisher RP; Fishner JM; Fittipaldi R; Fitz-Axen M; Fiumara V; Flaminio R; Fletcher M; Floden E; Flynn E; Fong H; Font JA; Forsyth PWF; Fournier JD; 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Haster CJ; Haughian K; Hayes FJ; Healy J; Heidmann A; Heintze MC; Heitmann H; Hellman F; Hello P; Hemming G; Hendry M; Heng IS; Hennig J; Heurs M; Hild S; Hinderer T; Hochheim S; Hofman D; Holgado AM; Holland NA; Holt K; Holz DE; Hopkins P; Horst C; Hough J; Howell EJ; Hoy CG; Huang Y; Hubner MT; Huerta EA; Huet D; Hughey B; Hui V; Husa S; Huttner SH; Huynh-Dinh T; Idzkowski B; Iess A; Inchauspe H; Ingram C; Inta R; Intini G; Irwin B; Isa HN; Isac JM; Isi M; Iyer BR; Jacqmin T; Jadhav SJ; Jani K; Janthalur NN; Jaranowski P; Jariwala D; Jenkins AC; Jiang J; Johnson DS; Jones AW; Jones DI; Jones JD; Jones R; Jonker RJG; Ju L; Junker J; Kalaghatgi CV; Kalogera V; Kamai B; Kandhasamy S; Kang G; Kanner JB; Kapadia SJ; Karki S; Kashyap R; Kasprzack M; Katsanevas S; Katsavounidis E; Katzman W; Kaufer S; Kawabe K; Keerthana NV; Kefelian F; Keitel D; Kennedy R; Key JS; Khalili FY; Khan I; Khan S; Khazanov EA; Khetan N; Khursheed M; Kijbunchoo N; Kim C; Kim JC; Kim K; Kim W; Kim WS; Kim YM; Kimball C; King PJ; Kinley-Hanlon M; Kirchhoff R; Kissel JS; Kleybolte L; Klika JH; Klimenko S; Knowles TD; Koch P; Koehlenbeck SM; Koekoek G; Koley S; Kondrashov V; Kontos A; Koper N; Korobko M; Korth WZ; Kovalam M; Kozak DB; Kramer C; Kringel V; Krishnendu N; Krolak A; Krupinski N; Kuehn G; Kumar A; Kumar P; Kumar R; Kumar R; Kuo L; Kutynia A; Kwang S; Lackey BD; Laghi D; Lai KH; Lam TL; Landry M; Lane BB; Lang RN; Lange J; Lantz B; Lanza RK; Lartaux-Vollard A; Lasky PD; Laxen M; Lazzarini A; Lazzaro C; Leaci P; Leavey S; Lecoeuche K; Lee CH; Lee HK; Lee HM; Lee HW; Lee J; Lee K; Lehmann J; Lenon AK; Leroy N; Letendre N; Levin Y; Li A; Li J; Li KJL; Li TGF; Li X; Lin F; Linde F; Linker SD; Littenberg TB; Liu J; Liu X; Llorens-Monteagudo M; Lo RKL; London LT; Longo A; Lorenzini M; Loriette V; Lormand M; Losurdo G; Lough JD; Lousto CO; Lovelace G; Lower ME; Luck H; Lumaca D; Lundgren AP; Lynch R; Ma Y; Macas R; Macfoy S; MacInnis M; Macleod DM; Macquet A; Hernandez IM; Magana-Sandoval F; Magee RM; Majorana E; Maksimovic I; Malik A; Man N; Mandic V; Mangano V; Mansell GL; Manske M; Mantovani M; Mapelli M; Marchesoni F; Marion F; Marka S; Marka Z; Markakis C; Markosyan AS; Markowitz A; Maros E; Marquina A; Marsat S; Martelli F; Martin IW; Martin RM; Martinez V; Martynov DV; Masalehdan H; Mason K; Massera E; Masserot A; Massinger TJ; Masso-Reid M; Mastrogiovanni S; Matas A; Matichard F; Matone L; Mavalvala N; McCann JJ; McCarthy R; McClelland DE; McCormick S; McCuller L; McGuire SC; McIsaac C; McIver J; McManus DJ; McRae T; McWilliams ST; Meacher D; Meadors GD; Mehmet M; Mehta AK; Meidam J; Villa EM; Melatos A; Mendell G; Mercer RA; Mereni L; Merfeld K; Merilh EL; Merzougui M; Meshkov S; Messenger C; Messick C; Messina F; Metzdorff R; Meyers PM; Meylahn F; Miani A; Miao H; Michel C; Middleton H; Milano L; Miller L; Millhouse M; Mills JC; Milovich-Goff MC; Minazzoli O; Minenkov Y; Mishkin A; Mishra C; Mistry T; Mitra S; Mitrofanov VP; Mitselmakher G; Mittleman R; Mo G; Moffa D; Mogushi K; 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2019
Abstract
The Astrophysical Journal
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The Institute of Physics, find out more.
A publishing partnership
Searches for Gravitational Waves from Known Pulsars at Two Harmonics in 2015–2017 LIGO Data
B. P. Abbott1, R. Abbott1, T. D. Abbott2, S. Abraham3, F. Acernese4,5, K. Ackley6, C. Adams7, R. X. Adhikari1, V. B. Adya8,9, C. Affeldt8,9Show full author list
Published 2019 June 26 • © 2019. The American Astronomical Society. All rights reserved.
The Astrophysical Journal, Volume 879, Number 1
Citation B. P. Abbott et al 2019 ApJ 879 10
DOI 10.3847/1538-4357/ab20cb
DownloadArticle PDF DownloadArticle ePub
This article is corrected by 2019 ApJ 882 73
This article is corrected by 2020 ApJ 899 170
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Abstract
We present a search for gravitational waves from 222 pulsars with rotation frequencies ≳10 Hz. We use advanced LIGO data from its first and second observing runs spanning 2015–2017, which provides the highest-sensitivity gravitational-wave data so far obtained. In this search we target emission from both the l = m = 2 mass quadrupole mode, with a frequency at twice that of the pulsar's rotation, and the l = 2, m = 1 mode, with a frequency at the pulsar rotation frequency. The search finds no evidence for gravitational-wave emission from any pulsar at either frequency. For the l = m = 2 mode search, we provide updated upper limits on the gravitational-wave amplitude, mass quadrupole moment, and fiducial ellipticity for 167 pulsars, and the first such limits for a further 55. For 20 young pulsars these results give limits that are below those inferred from the pulsars' spin-down. For the Crab and Vela pulsars our results constrain gravitational-wave emission to account for less than 0.017% and 0.18% of the spin-down luminosity, respectively. For the recycled millisecond pulsar J0711−6830 our limits are only a factor of 1.3 above the spin-down limit, assuming the canonical value of 1038 kg m2 for the star's moment of inertia, and imply a gravitational-wave-derived upper limit on the star's ellipticity of 1.2 × 10−8. We also place new limits on the emission amplitude at the rotation frequency of the pulsars.
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande. La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.