18 research outputs found
Smart systems related to polypeptide sequences
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- Zhao Y
- Zhao Y
- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2016
- Field of study
Recommended from our members
Open Data from the Third Observing Run of LIGO, Virgo, KAGRA, and GEO
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhicary S
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Al-Jodah A
- Albanesi S
- Alfaidi RA
- Allocca A
- Alléné C
- Almualla M
- Altin PA
- Amato A
- Amez-Droz L
- Amorosi A
- Anand S
- Ananyeva A
- Andersen R
- Anderson SB
- Anderson WG
- Andia M
- Ando M
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- Antelis JM
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- Publication venue
- The Astrophysical Journal Supplement Series
- Publication date
- 22/08/2023
- Field of study
Abstract
The global network of gravitational-wave observatories now includes five detectors, namely LIGO Hanford, LIGO Livingston, Virgo, KAGRA, and GEO 600. These detectors collected data during their third observing run, O3, composed of three phases: O3a starting in 2019 April and lasting six months, O3b starting in 2019 November and lasting five months, and O3GK starting in 2020 April and lasting two weeks. In this paper we describe these data and various other science products that can be freely accessed through the Gravitational Wave Open Science Center at https://gwosc.org. The main data set, consisting of the gravitational-wave strain time series that contains the astrophysical signals, is released together with supporting data useful for their analysis and documentation, tutorials, as well as analysis software packages.</jats:p
Searches for Gravitational Waves from Known Pulsars at Two Harmonics in the Second and Third LIGO-Virgo Observing Runs
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- Enomoto Y
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- Ferrante I
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- Fiumara V
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- Forsyth PWF
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- Freed JP
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- Fujii Y
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- Gayathri V
- Ge GG
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- Gennai A
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- Giacomazzo B
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- Hsieh BH
- Hsieh HF
- Hsiung C
- Hsu Y
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- Huang YT
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- Hubner MT
- Huddart AD
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- Hui V
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- Krishnendu NV
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- Lee HM
- Lee HW
- Lee K
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- Lehmann J
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- Leonardi M
- Leonova E
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- Levesque C
- Levin Y
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- Leyde K
- Li AKY
- Li B
- Li J
- Li KL
- Li P
- Li TGF
- Li X
- Lin CY
- Lin ET
- Lin FK
- Lin FL
- Lin HL
- Lin LCC
- Linde F
- Linker SD
- Linley JN
- Littenberg TB
- Liu GC
- Liu J
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- Liu X
- Llamas F
- Lo RKL
- Lo T
- London LT
- Longo A
- Lopez D
- Lorenzini M
- Loriette V
- Lormand M
- Losurdo G
- Lott TP
- Lough JD
- Lousto CO
- Lovelace G
- Lower ME
- Lucaccioni JF
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- Lumaca D
- Lundgren AP
- Luo LW
- Lynam JE
- Lyne AG
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- Machtinger JB
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- Macleod DM
- MacMillan IAO
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- Maksimovic I
- Maliakal S
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- Markowitz A
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- Mateu-Lucena M
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- Melo ITE
- Melo SAD
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- Menendez-Vazquez A
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- Mercer RA
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- Merfeld K
- Merilh EL
- Merritt JD
- Merzougui M
- Meshkov S
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- Messick C
- Meyers BW
- Meyers PM
- Meylahn F
- Mhaske A
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- Miao H
- Michaloliakos I
- Michel C
- Michimura Y
- Middleton H
- Mihaylov DP
- Milano L
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- Miller AL
- Miller B
- Millhouse M
- Mills JC
- Milotti E
- Minenkov Y
- Mio N
- Mir LM
- Miravet-Tenes M
- Mishkin A
- Mishra C
- Mishra T
- Mistry T
- Mitra S
- Mitrofanov VP
- Mitselmakher G
- Mittleman R
- Miyakawa O
- Miyo K
- Miyoki S
- Mo G
- Modafferi LM
- Moguel E
- Mogushi K
- Mohapatra SRP
- Mohite SR
- Molina I
- Molina-Ruiz M
- Mondin M
- Montani M
- Moore CJ
- Moragues J
- Moraru D
- Morawski F
- More A
- Moreno C
- Moreno G
- Mori Y
- Morisaki S
- Morisue N
- Moriwaki Y
- Mours B
- Mow-Lowry CM
- Mozzon S
- Muciaccia F
- Mukherjee A
- Mukherjee D
- Mukherjee S
- Mukherjee S
- Mukherjee S
- Mukund N
- Mullavey A
- Munch J
- Muniz EA
- Murray PG
- Musenich R
- Muusse S
- Nadji SL
- Nagano K
- Nagar A
- Nakamura K
- Nakano H
- Nakano M
- Nakayama Y
- Napolano V
- Nardecchia I
- Narikawa T
- Narola H
- Naticchioni L
- Nayak B
- Nayak RK
- Neil BF
- Neilson J
- Nelson A
- Nelson TJN
- Nery M
- Neubauer P
- Neunzert A
- Ng KY
- Ng SWS
- Nguyen C
- Nguyen P
- Nguyen T
- Ni J
- Ni WT
- Nichols SA
- Nishimoto T
- Nishizawa A
- Nissanke S
- Nitoglia E
- Nocera F
- Norman M
- North C
- Nozaki S
- Nunez CG
- Nurbek G
- Nuttall LK
- O'Brien BD
- O'Dell J
- O'Reilly B
- O'Shaughnessy R
- O'Shea E
- Obayashi Y
- Oberling J
- Oelker E
- Ogaki W
- Oganesyan G
- Oh JJ
- Oh K
- Oh SH
- Ohashi M
- Ohashi T
- Ohkawa M
- Ohme F
- Ohta H
- Okada MA
- Okutani Y
- Olivetto C
- Oohara K
- Oram R
- Ormiston RG
- Ormsby ND
- Oshino S
- Ossokine S
- Osthelder C
- Otabe S
- Ottaway DJ
- Overmier H
- Pace AE
- Pagano G
- Pagano R
- Page MA
- Pagliaroli G
- Pai A
- Pai SA
- Pal S
- Palamos JR
- Palashov O
- Palfreyman JL
- Palomba C
- Pan H
- Pan KC
- Panda PK
- Pang PTH
- Pankow C
- Pannarale F
- Pant BC
- Panther FH
- Paoletti F
- Paoli A
- Paolone A
- Pappas G
- Parisi A
- Park H
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- Parker W
- Pascucci D
- Pasqualetti A
- Passaquieti R
- Passuello D
- Patel M
- Pathak M
- Patricelli B
- Patron AS
- Paul S
- Payne E
- Pedraza M
- Pedurand R
- Pegoraro M
- Pele A
- Penano S
- Penn S
- Perego A
- Pereira A
- Pereira T
- Perez CJ
- Perigois C
- Perkins CC
- Perreca A
- Perries S
- Pesios D
- Petermann J
- Petterson D
- Pfeiffer HP
- Pham H
- Pham KA
- Phukon KS
- Phurailatpam H
- Piccinni OJ
- Pichot M
- Piendibene M
- Piergiovanni F
- Pierini L
- Pierro V
- Pillant G
- Pillas M
- Pilo F
- Pina DM
- Pinard L
- Pineda-Bosque C
- Pinto IM
- Pinto M
- Piotrzkowski BJ
- Piotrzkowski K
- Pirello M
- Pitkin MD
- Placidi A
- Placidi E
- Planas ML
- Plastino W
- Pluchar C
- Poggiani R
- Polini E
- Pong DYT
- Ponrathnam S
- Porter EK
- Portilla ML
- Poulton R
- Poverman A
- Powell J
- Pracchia M
- Pradier T
- Prajapati AK
- Prasai K
- Prasanna R
- Pratten G
- Principe M
- Prodi GA
- Prokhorov L
- Prosposito P
- Prudenzi L
- Puecher A
- Punturo M
- Puosi F
- Puppo P
- Purrer M
- Qi H
- Quartey N
- Quetschke V
- Quinonez PJ
- Quitzow-James R
- Quynh LN
- Raab FJ
- Raaijmakers G
- Radkins H
- Radulesco N
- Raffai P
- Rail SX
- Raja S
- Rajan C
- Ramirez KE
- Ramirez TD
- Ramos-Buades A
- Rana J
- Rapagnani P
- Ray A
- Raymond V
- Raza N
- Razzano M
- Read J
- Rees LA
- Regimbau T
- Rei L
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- Reid SW
- Reitze DH
- Relton P
- Renzini A
- Rettegno P
- Revenu B
- Reza A
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- Riemenschneider G
- Riles K
- Rinaldi S
- Rink K
- Robertson NA
- Robie R
- Robinet F
- Rocchi A
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- Rolland L
- Rollins JG
- Romanelli M
- Romano R
- Romel CL
- Romero A
- Romero-Shaw IM
- Romie JH
- Ronchini S
- Rosa L
- Rose CA
- Ross MP
- Rowan S
- Rowlinson SJ
- Roy S
- Roy S
- Roy S
- Rozza D
- Ruggi P
- Ruiz-Rocha K
- Ryan K
- Sachdev S
- Sadecki T
- Sadiq J
- Saha S
- Saito Y
- Sakai K
- Sakellariadou M
- Sakon S
- Salafia OS
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- Salconi L
- Saleem M
- Salemi F
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- Sanchez JH
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- Saravanan TR
- Sarin N
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- Sayah S
- Schaetzl D
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- Schofield RMS
- Schonbeck A
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- Sekiguchi Y
- Sellers D
- Sengupta AS
- Sentenac D
- Seo EG
- Sequino V
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- Setyawati Y
- Shaffer T
- Shahriar MS
- Shaikh MA
- Shams B
- Shannon RM
- Shao L
- Sharma A
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- Shaw B
- Shawhan P
- Shcheblanov NS
- Sheela A
- Shikano Y
- Shikauchi M
- Shimizu H
- Shimode K
- Shinkai H
- Shishido T
- Shoda A
- Shoemaker DH
- Shoemaker DM
- ShyamSundar S
- Sieniawska M
- Sigg D
- Silenzi L
- Singer LP
- Singh D
- Singh MK
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- Singha A
- Sintes AM
- Sipala V
- Skliris V
- Slagmolen BJJ
- Slaven-Blair TJ
- Smetana J
- Smith JR
- Smith L
- Smith RJE
- Soldateschi J
- Somala SN
- Somiya K
- Song I
- Soni K
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- Soulard R
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- Sowell E
- Spagnuolo V
- Spencer AP
- Spera M
- Spinicelli P
- Srivastava AK
- Srivastava V
- Staats K
- Stachie C
- Stachurski F
- Stairs IH
- Stappers BW
- Steer DA
- Steinlechner J
- Steinlechner S
- Stergioulas N
- Stops DJ
- Stover M
- Strain KA
- Strang LC
- Stratta G
- Strong MD
- Strunk A
- Sturani R
- Stuver AL
- Subrahmanya SC
- Suchenek M
- Sudhagar S
- Sudhir V
- Sugimoto R
- Suh HG
- Sullivan AG
- Summerscales TZ
- Sun L
- Sunil S
- Sur A
- Suresh J
- Sutton PJ
- Suzuki T
- Suzuki T
- Suzuki T
- Swinkels BL
- Szczepanczyk MJ
- Szewczyk P
- Tacca M
- Tagoshi H
- Tait SC
- Takahashi H
- Takahashi R
- Takano S
- Takeda H
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- Talbot C
- Talbot CJ
- Tan CM
- Tanaka K
- Tanaka T
- Tanaka T
- Tanasijczuk AJ
- Tanioka S
- Tanner DB
- Tao D
- Tao L
- Tapia RD
- Taranto C
- Taruya A
- Tasson JD
- Tenorio R
- Terhune JES
- Terkowski L
- Theureau G
- Thirugnanasambandam MP
- Thomas M
- Thomas P
- Thompson EE
- Thompson JE
- Thondapu SR
- Thorne KA
- Thrane E
- Tiwari S
- Tiwari S
- Tiwari V
- Toivonen AM
- Tolley AE
- Tomaru T
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- Tonelli M
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- Torres-Forne A
- Torrie CI
- Toyra D
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- Tripathee A
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- Trovato A
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- Ubhi AS
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- Uchiyama T
- Udall RP
- Ueda A
- Uehara T
- Ueno K
- Ueshima G
- Unnikrishnan CS
- Urban AL
- Ushiba T
- Utina A
- Vajente G
- Vajpeyi A
- Valdes G
- Valentini M
- Valsan V
- van Bakel N
- van Beuzekom M
- van Dael M
- van den Brand JFJ
- Van den Broeck C
- van Haevermaet H
- van Heijningen JV
- van Putten MHPM
- van Remortel N
- Vander-Hyde DC
- Vardaro M
- Vargas AF
- Varma V
- Vasuth M
- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Venneberg J
- Venugopalan G
- Verkindt D
- Verma P
- Verma Y
- Vermeulen SM
- Veske D
- Vetrano F
- Vicere A
- Vidyant S
- Viets AD
- Vijaykumar A
- Villa-Ortega V
- Vinet JY
- Virtuoso A
- Vitale S
- Vivanco FH
- Vocca H
- von Reis ERG
- von Wrangel JSA
- Vorvick C
- Vyatchanin SP
- Wade LE
- Wade M
- Wagner KJ
- Walet RC
- Walker M
- Wallace GS
- Wallace L
- Wang J
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- Wang WH
- Ward RL
- Warner J
- Was M
- Washimi T
- Washington NY
- Watchi J
- Weaver B
- Weaving CR
- Webster SA
- Weinert M
- Weinstein AJ
- Weiss R
- Weller CM
- Weller RA
- Wellmann F
- Weltevrede P
- Wen L
- Wessels P
- Wette K
- Whelan JT
- White DD
- Whiting BF
- Whittle C
- Wilken D
- Williams D
- Williams MJ
- Williamson AR
- Willis JL
- Willke B
- Wilson DJ
- Wipf CC
- Wlodarczyk T
- Woan G
- Woehler J
- Wofford JK
- Wong D
- Wong ICF
- Wright M
- Wu C
- Wu DS
- Wu H
- Wysocki DM
- Xiao L
- Yamada T
- Yamamoto H
- Yamamoto K
- Yamamoto T
- Yamashita K
- Yamazaki R
- Yang FW
- Yang KZ
- Yang L
- Yang Y
- Yang Y
- Yang YC
- Yap MJ
- Yeeles DW
- Yeh SW
- Yelikar AB
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu H
- Yu HC
- Yuzurihara H
- Zanolin M
- Zeidler S
- Zelenova T
- Zendri JP
- Zevin M
- Zhan M
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang T
- Zhang Y
- Zhao C
- Zhao G
- Zhao Y
- Zhao Y
- Zhou R
- Zhou Z
- Zhu XJ
- Zhu ZH
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2022
- Field of study
We present a targeted search for continuous gravitational waves (GWs) from 236 pulsars using data from the third observing run of LIGO and Virgo (O3) combined with data from the second observing run (O2). Searches were for emission from the l = m = 2 mass quadrupole mode with a frequency at only twice the pulsar rotation frequency (single harmonic) and the l = 2, m = 1, 2 modes with a frequency of both once and twice the rotation frequency (dual harmonic). No evidence of GWs was found, so we present 95% credible upper limits on the strain amplitudes h (0) for the single-harmonic search along with limits on the pulsars' mass quadrupole moments Q (22) and ellipticities epsilon. Of the pulsars studied, 23 have strain amplitudes that are lower than the limits calculated from their electromagnetically measured spin-down rates. These pulsars include the millisecond pulsars J0437-4715 and J0711-6830, which have spin-down ratios of 0.87 and 0.57, respectively. For nine pulsars, their spin-down limits have been surpassed for the first time. For the Crab and Vela pulsars, our limits are factors of similar to 100 and similar to 20 more constraining than their spin-down limits, respectively. For the dual-harmonic searches, new limits are placed on the strain amplitudes C (21) and C (22). For 23 pulsars, we also present limits on the emission amplitude assuming dipole radiation as predicted by Brans-Dicke theory
Search for subsolar-mass black hole binaries in the second part of Advanced LIGO’s and Advanced Virgo’s third observing run
- Author
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- Wysocki DM
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- Yeh S-W
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- Yokoyama J
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- Yoshioka T
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- Zadrożny A
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- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 28/02/2023
- Field of study
Model-based Cross-correlation Search for Gravitational Waves from the Low-mass X-Ray Binary Scorpius X-1 in LIGO O3 Data
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhicary S
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Alfaidi RA
- Allocca A
- Alléné C
- Altin PA
- Amato A
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
- Andres N
- Andrić T
- Andrés-Carcasona M
- Ansoldi S
- Antelis JM
- Antier S
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- Appavuravther EZ
- Appert S
- Apple SK
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- Araya A
- Araya MC
- Areeda JS
- Aritomi N
- Arnaud N
- Arogeti M
- Aronson SM
- Arène M
- Asada H
- Ashton G
- Aso Y
- Assiduo M
- Aston SM
- Astone P
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- Babak S
- Badaracco F
- Badger C
- Bae S
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- Bagnasco S
- Bai Y
- Baier JG
- Baird J
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- Barish BC
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- Barsuglia M
- Barta D
- Bartlett J
- Barton MA
- Bartos I
- Basak S
- Bassiri R
- Basti A
- Bawaj M
- Bayley JC
- Bazzan M
- Bedakihale VM
- Beirnaert F
- Bejger M
- Belahcene I
- Bell AS
- Benedetto V
- Beniwal D
- Benoit W
- Bentley JD
- BenYaala M
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- Berbel M
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- Bersanetti D
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- Danzmann K
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- Dasgupta A
- Datrier LEH
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- Dattilo V
- Dave I
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- Ewing BE
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- Fan PC
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- Fenyvesi E
- Ferguson DL
- Fernandez-Galiana A
- Ferrante I
- Ferreira TA
- Fidecaro F
- Figura P
- Fiore LD
- Fiori A
- Fiori I
- Fishbach M
- Fisher RP
- Fittipaldi R
- Fiumara V
- Flaminio R
- Floden E
- Fong HK
- Font JA
- Fornal B
- Forsyth PWF
- Franke A
- Frasca S
- Frasconi F
- Freed JP
- Frei Z
- Freise A
- Freitas O
- Frey R
- Fritschel P
- Frolov VV
- Fronzo CD
- Fronzé GG
- Fujii Y
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- Gadre BU
- Gair JR
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- Yelikar AB
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- Zadrożny A
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- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2022
- Field of study
We present the results of a model-based search for continuous gravitational waves from the low-mass X-ray binary Scorpius X-1 using LIGO detector data from the third observing run of Advanced LIGO and Advanced Virgo. This is a semicoherent search that uses details of the signal model to coherently combine data separated by less than a specified coherence time, which can be adjusted to balance sensitivity with computing cost. The search covered a range of gravitational-wave frequencies from 25 to 1600 Hz, as well as ranges in orbital speed, frequency, and phase determined from observational constraints. No significant detection candidates were found, and upper limits were set as a function of frequency. The most stringent limits, between 100 and 200 Hz, correspond to an amplitude h0 of about 10−25 when marginalized isotropically over the unknown inclination angle of the neutron star's rotation axis, or less than 4 × 10−26 assuming the optimal orientation. The sensitivity of this search is now probing amplitudes predicted by models of torque balance equilibrium. For the usual conservative model assuming accretion at the surface of the neutron star, our isotropically marginalized upper limits are close to the predicted amplitude from about 70 to 100 Hz; the limits assuming that the neutron star spin is aligned with the most likely orbital angular momentum are below the conservative torque balance predictions from 40 to 200 Hz. Assuming a broader range of accretion models, our direct limits on gravitational-wave amplitude delve into the relevant parameter space over a wide range of frequencies, to 500 Hz or more
Recommended from our members
Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGO–Virgo Network
- Author
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- Wysocki DM
- Xiao L
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- Yamashita K
- Yamazaki R
- Yang FW
- Yang KZ
- Yang L
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- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Yokoyama J
- Yokozawa T
- Yoo J
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- Yu Hang
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- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeidler S
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- Zhan M
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- Zheng Y
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- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- The Astrophysical Journal
- Publication date
- 05/08/2024
- Field of study
Abstract
Gravitational lensing by massive objects along the line of sight to the source causes distortions to gravitational wave (GW) signals; such distortions may reveal information about fundamental physics, cosmology, and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO-Virgo network. We search for repeated signals from strong lensing by (1) performing targeted searches for subthreshold signals, (2) calculating the degree of overlap among the intrinsic parameters and sky location of pairs of signals, (3) comparing the similarities of the spectrograms among pairs of signals, and (4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by (1) frequency-independent phase shifts in strongly lensed images, and (2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the nondetection of GW lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects.</jats:p
Recommended from our members
Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGO–Virgo Network
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- Zweizig J
- Publication venue
- The Astrophysical Journal
- Publication date
- 01/08/2024
- Field of study
Abstract
Gravitational lensing by massive objects along the line of sight to the source causes distortions to gravitational wave (GW) signals; such distortions may reveal information about fundamental physics, cosmology, and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO-Virgo network. We search for repeated signals from strong lensing by (1) performing targeted searches for subthreshold signals, (2) calculating the degree of overlap among the intrinsic parameters and sky location of pairs of signals, (3) comparing the similarities of the spectrograms among pairs of signals, and (4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by (1) frequency-independent phase shifts in strongly lensed images, and (2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the nondetection of GW lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects.</jats:p
Search for Subsolar-Mass Binaries in the First Half of Advanced LIGO's and Advanced Virgo's Third Observing Run
- Author
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- Abe H
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- Ackley K
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- Ferrante I
- Ferreira TA
- Fidecaro F
- Figura P
- Fiori A
- Fiori I
- Fishbach M
- Fisher RP
- Fittipaldi R
- Fiumara V
- Flaminio R
- Floden E
- Fong HK
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- Forsyth PWF
- Franke A
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- Freed JP
- Frei Z
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- Fronze GG
- Fujii Y
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- Fujimoto Y
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- Gamba R
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- Ganguly A
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- Gateley B
- Gayathri V
- Ge G-G
- Gemme G
- Gennai A
- George J
- Gerberding O
- Gergely L
- Gewecke P
- Ghonge S
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- Giacomazzo B
- Giacoppo L
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- Glanzer J
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- Guidi GM
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- Haegel L
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- Holmes ZJ
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- Howell EJ
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- Hsieh B-H
- Hsieh H-F
- Hsiung C
- Hsu Y
- Huang H-Y
- Huang P
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- Huang Yiting
- Huang Yiwen
- Hubner MT
- Huddart AD
- Hughey B
- Hui DCY
- Hui V
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- Jadhav SJ
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- Jaranowski P
- Jariwala D
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- Kamai B
- Kamiizumi M
- Kanda N
- Kandhasamy S
- Kang G
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- Kobayashi Y
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- Koekoek G
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- Kontos A
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- Kovalam M
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- Krishnendu NV
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- Leonardi M
- Leonova E
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- Li X
- Lin C-Y
- Lin ET
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- Linde F
- Linker SD
- Linley JN
- Littenberg TB
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- Longo A
- Lopez D
- Lorenzini M
- Loriette V
- Lormand M
- Losurdo G
- Lott TP
- Lough JD
- Lousto CO
- Lovelace G
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- Lundgren AP
- Luo L-W
- Lynam JE
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- Macleod DM
- MacMillan IAO
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- Maksimovic I
- Maliakal S
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- Martynov DV
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- McWilliams ST
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- Mehmet M
- Mehta AK
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- Menoni CS
- Mercer RA
- Mereni L
- Merfeld K
- Merilh EL
- Merritt JD
- Merzougui M
- Meshkov S
- Messenger C
- Messick C
- Meyers PM
- Meylahn F
- Mhaske A
- Miani A
- Miao H
- Michaloliakos I
- Michel C
- Michimura Y
- Middleton H
- Mihaylov DP
- Milano L
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- Mills JC
- Milotti E
- Minenkov Y
- Mio N
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- Miravet-Tenes M
- Mishkin A
- Mishra C
- Mishra T
- Mistry T
- Mitra S
- Mitrofanov VP
- Mitselmakher G
- Mittleman R
- Miyakawa O
- Miyo K
- Miyoki S
- Mo Geoffrey
- Modafferi LM
- Moguel E
- Mogushi K
- Mohapatra SRP
- Mohite SR
- Molina I
- Molina-Ruiz M
- Mondin M
- Montani M
- Moore CJ
- Moragues J
- Moraru D
- Morawski F
- More A
- Moreno C
- Moreno G
- Mori Y
- Morisaki S
- Morisue N
- Moriwaki Y
- Mours B
- Mow-Lowry CM
- Mozzon S
- Muciaccia F
- Mukherjee Arunava
- Mukherjee D
- Mukherjee Soma
- Mukherjee Subroto
- Mukherjee Suvodip
- Mukund N
- Mullavey A
- Munch J
- Muniz EA
- Murray PG
- Musenich R
- Muusse S
- Nadji SL
- Nagano K
- Nagar A
- Nakamura K
- Nakano H
- Nakano M
- Nakayama Y
- Napolano V
- Nardecchia I
- Narikawa T
- Narola H
- Naticchioni L
- Nayak B
- Nayak RK
- Neil BF
- Neilson J
- Nelson A
- Nelson TJN
- Nery M
- Neubauer P
- Neunzert A
- Ng KY
- Ng SWS
- Nguyen C
- Nguyen P
- Nguyen T
- Ni J
- Ni W-T
- Nichols SA
- Nishimoto T
- Nishizawa A
- Nissanke S
- Nitoglia E
- Nocera F
- Norman M
- North C
- Nozaki S
- Nunez C Garcia
- Nurbek G
- Nuttall LK
- O'Brien BD
- O'Dell J
- O'Reilly B
- O'Shaughnessy R
- O'Shea E
- Obayashi Y
- Oberling J
- Oelker E
- Ogaki W
- Oganesyan G
- Oh JJ
- Oh K
- Oh SH
- Ohashi M
- Ohashi T
- Ohkawa M
- Ohme F
- Ohta H
- Okada MA
- Okutani Y
- Olivetto C
- Oohara K
- Oram R
- Ormiston RG
- Ormsby ND
- Oshino S
- Ossokine S
- Osthelder C
- Otabe S
- Ottaway DJ
- Overmier H
- Pace AE
- Pagano G
- Pagano R
- Page MA
- Pagliaroli G
- Pai A
- Pai SA
- Pal S
- Palamos JR
- Palashov O
- Palomba C
- Pan H
- Pan K-C
- Panda PK
- Pang PTH
- Pankow C
- Pannarale F
- Pant BC
- Panther FH
- Paoletti F
- Paoli A
- Paolone A
- Pappas G
- Parisi A
- Park H
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- Pascucci D
- Pasqualetti A
- Passaquieti R
- Passuello D
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- Pathak M
- Patricelli B
- Patron AS
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- Pedraza M
- Pedurand R
- Pegoraro M
- Pele A
- Penano S
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- Perego A
- Pereira A
- Pereira T
- Perez CJ
- Perigois C
- Perkins CC
- Perreca A
- Perries S
- Pesios D
- Petermann J
- Petterson D
- Pfeiffer HP
- Pham H
- Pham KA
- Phukon KS
- Phurailatpam H
- Piccinni OJ
- Pichot M
- Piendibene M
- Piergiovanni F
- Pierini L
- Pierro V
- Pillant G
- Pillas M
- Pilo F
- Pinard L
- Pineda-Bosque C
- Pinto IM
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- Piotrzkowski BJ
- Piotrzkowski K
- Pirello M
- Pitkin MD
- Placidi A
- Placidi E
- Planas ML
- Plastino W
- Pluchar C
- Poggiani R
- Polini E
- Pong DYT
- Ponrathnam S
- Porter EK
- Portilla M Lopez
- Poulton R
- Poverman A
- Powell J
- Pracchia M
- Pradier T
- Prajapati AK
- Prasai K
- Prasanna R
- Pratten G
- Principe M
- Prodi GA
- Prokhorov L
- Prosposito P
- Prudenzi L
- Puecher A
- Puerrer M
- Punturo M
- Puosi F
- Puppo P
- Qi H
- Quartey N
- Quetschke V
- Quinonez PJ
- Quitzow-James R
- Quynh L Nguyen
- Raab FJ
- Raaijmakers G
- Radkins H
- Radulesco N
- Raffai P
- Rail SX
- Raja S
- Rajan C
- Ramirez KE
- Ramirez TD
- Ramos-Buades A
- Rana J
- Rapagnani P
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- Raza N
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- Rees LA
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- Rei L
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- Reitze DH
- Relton P
- Renzini A
- Rettegno P
- Revenu B
- Reza A
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- Robertson NA
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- Rocchi A
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- Rollins JG
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- Romano R
- Romel CL
- Romero A
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- Romie JH
- Ronchini S
- Rosa L
- Rose CA
- Rosinska D
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- Rowan S
- Rowlinson SJ
- Roy S
- Roy Santosh
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- Rozza D
- Ruggi P
- Ruiz-Rocha K
- Ryan K
- Sachdev S
- Sadecki T
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- Sakon S
- Salafia OS
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- Sanchez JH
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- Schulte BW
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- Sellers D
- Sengupta AS
- Sentenac D
- Seo EG
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- Sergeev A
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- Shaffer T
- Shahriar MS
- Shaikh MA
- Shams B
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- Shawhan P
- Shcheblanov NS
- Sheela A
- Shikano Y
- Shikauchi M
- Shimizu H
- Shimode K
- Shinkai H
- Shishido T
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- Shoemaker DH
- Shoemaker DM
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- Silenzi L
- Singer LP
- Singh D
- Singh MK
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- Slagmolen BJJ
- Slaven-Blair TJ
- Smetana J
- Smith JR
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- Smith RJE
- Soldateschi J
- Somala SN
- Somiya K
- Song I
- Soni K
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- Spagnuolo V
- Spencer AP
- Spera M
- Spinicelli P
- Srivastava AK
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- Staats K
- Stachie C
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- Steer DA
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- Steinlechner S
- Stergioulas N
- Stops DJ
- Stover M
- Strain KA
- Strang LC
- Stratta G
- Strong MD
- Strunk A
- Sturani R
- Stuver AL
- Subrahmanya S Chalathadka
- Suchenek M
- Sudhagar S
- Sudhir V
- Sugimoto R
- Suh HG
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- Summerscales TZ
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- Sunil S
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- Suzuki Takamasa
- Suzuki Takanori
- Suzuki Toshikazu
- Swinkels BL
- Szczepanczyk MJ
- Szewczyk P
- Tacca M
- Tagoshi H
- Tait SC
- Takahashi H
- Takahashi R
- Takano S
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- Tanaka K
- Tanaka Taiki
- Tanaka Takahiro
- Tanasijczuk AJ
- Tanioka S
- Tanner DB
- Tao D
- Tao L
- Tapia RD
- Taranto C
- Taruya A
- Tasson JD
- Tenorio R
- Terhune JES
- Terkowski L
- Thirugnanasambandam MP
- Thomas M
- Thomas P
- Thompson EE
- Thompson JE
- Thondapu SR
- Thorne KA
- Thrane E
- Tiwari Shubhanshu
- Tiwari Srishti
- Tiwari V
- Toivonen AM
- Tolley AE
- Tomaru T
- Tomura T
- Tonelli M
- Tornasi Z
- Torres-Forne A
- Torrie CI
- Tosta e Melo I
- Toyra D
- Trapananti A
- Travasso F
- Traylor G
- Trevor M
- Tringali MC
- Tripathee A
- Troiano L
- Trovato A
- Trozzo L
- Trudeau RJ
- Tsai D
- Tsang KW
- Tsang T
- Tsao J-S
- Tse M
- Tso R
- Tsuchida S
- Tsukada L
- Tsuna D
- Tsutsui T
- Turbang K
- Turconi M
- Tuyenbayev D
- Ubhi AS
- Uchikata N
- Uchiyama T
- Udall RP
- Ueda A
- Uehara T
- Ueno K
- Ueshima G
- Unnikrishnan CS
- Urban AL
- Ushiba T
- Utina A
- Vajente G
- Vajpeyi A
- Valdes G
- Valentini M
- Valsan V
- van Bakel N
- van Beuzekom M
- van Dael M
- van den Brand JFJ
- Van den Broeck C
- van Haevermaet H
- van Heijningen JV
- van Putten MHPM
- van Remortel N
- Vander-Hyde DC
- Vardaro M
- Vargas AF
- Varma V
- Vasuth M
- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Venneberg J
- Venugopalan G
- Verkindt D
- Verma P
- Verma Y
- Vermeulen SM
- Veske D
- Vetrano F
- Vicere A
- Vidyant S
- Viets AD
- Vijaykumar A
- Villa-Ortega V
- Vinet J-Y
- Virtuoso A
- Vitale S
- Vivanco F Hernandez
- Vocca H
- von Reis ERG
- von Wrangel JSA
- Vorvick C
- Vyatchanin SP
- Wade LE
- Wade M
- Wagner KJ
- Walet RC
- Walker M
- Wallace GS
- Wallace L
- Wang J
- Wang JZ
- Wang WH
- Ward RL
- Warner J
- Was M
- Washimi T
- Washington NY
- Watchi J
- Weaver B
- Weaving CR
- Webster SA
- Weinert M
- Weinstein AJ
- Weiss R
- Weller CM
- Weller RA
- Wellmann F
- Wen L
- Wessels P
- Wette K
- Whelan JT
- White DD
- Whiting BF
- Whittle C
- Wilken D
- Williams D
- Williams MJ
- Williamson AR
- Willis JL
- Willke B
- Wilson DJ
- Wipf CC
- Wlodarczyk T
- Woan G
- Woehler J
- Wofford JK
- Wong D
- Wong ICF
- Wright M
- Wu C
- Wu DS
- Wu H
- Wysocki DM
- Xiao L
- Yamada T
- Yamamoto H
- Yamamoto K
- Yamamoto T
- Yamashita K
- Yamazaki R
- Yang FW
- Yang KZ
- Yang L
- Yang Y
- Yang Y-C
- Yang Yang
- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- Zadrozny A
- Zanolin M
- Zeidler S
- Zelenova T
- Zendri J-P
- Zevin M
- Zhan M
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang T
- Zhang Y
- Zhao C
- Zhao G
- Zhao Y
- Zhao Yue
- Zhou R
- Zhou Z
- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
We report on a search for compact binary coalescences where at least one binary component has a mass between 0.2 M and 1.0 M in Advanced LIGO and Advanced Virgo data collected between 1 April 2019 1500 UTC and 1 October 2019 1500 UTC. We extend our previous analyses in two main ways: we include data from the Virgo detector and we allow for more unequal mass systems, with mass ratio q≥0.1. We do not report any gravitational-wave candidates. The most significant trigger has a false alarm rate of 0.14 yr-1. This implies an upper limit on the merger rate of subsolar binaries in the range [220-24200] Gpc-3 yr-1, depending on the chirp mass of the binary. We use this upper limit to derive astrophysical constraints on two phenomenological models that could produce subsolar-mass compact objects. One is an isotropic distribution of equal-mass primordial black holes. Using this model, we find that the fraction of dark matter in primordial black holes in the mass range 0.2 M<1.0 M is fPBHωPBH/ωDM6%. This improves existing constraints on primordial black hole abundance by a factor of ∼3. The other is a dissipative dark matter model, in which fermionic dark matter can collapse and form black holes. The upper limit on the fraction of dark matter black holes depends on the minimum mass of the black holes that can be formed: the most constraining result is obtained at Mmin=1 M, where fDBHωDBH/ωDM0.003%. These are the first constraints placed on dissipative dark models by subsolar-mass analyses
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- Author
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- Ying M
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- Yuzurihara H
- Zadrożny A
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- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- The Astrophysical Journal
- Publication date
- 07/06/2023
- Field of study
Abstract
We use 47 gravitational wave sources from the Third LIGO–Virgo–Kamioka Gravitational Wave Detector Gravitational Wave Transient Catalog (GWTC–3) to estimate the Hubble parameter H(z), including its current value, the Hubble constant H
0. Each gravitational wave (GW) signal provides the luminosity distance to the source, and we estimate the corresponding redshift using two methods: the redshifted masses and a galaxy catalog. Using the binary black hole (BBH) redshifted masses, we simultaneously infer the source mass distribution and H(z). The source mass distribution displays a peak around 34 M
⊙, followed by a drop-off. Assuming this mass scale does not evolve with the redshift results in a H(z) measurement, yielding
H
0
=
68
−
8
+
12
km
s
−
1
Mpc
−
1
(68% credible interval) when combined with the H
0 measurement from GW170817 and its electromagnetic counterpart. This represents an improvement of 17% with respect to the H
0 estimate from GWTC–1. The second method associates each GW event with its probable host galaxy in the catalog GLADE+, statistically marginalizing over the redshifts of each event’s potential hosts. Assuming a fixed BBH population, we estimate a value of
H
0
=
68
−
6
+
8
km
s
−
1
Mpc
−
1
with the galaxy catalog method, an improvement of 42% with respect to our GWTC–1 result and 20% with respect to recent H
0 studies using GWTC–2 events. However, we show that this result is strongly impacted by assumptions about the BBH source mass distribution; the only event which is not strongly impacted by such assumptions (and is thus informative about H
0) is the well-localized event GW190814.</jats:p
Searches for gravitational waves from known pulsars at two harmonics in the second and third LIGO-Virgo observing runs
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- Zhu XJ
- Zhu Z-H
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 25/05/2022
- Field of study
We present a targeted search for continuous gravitational waves (GWs) from 236 pulsars using data from the third observing run of LIGO and Virgo (O3) combined with data from the second observing run (O2). Searches were for emission from the l = m = 2 mass quadrupole mode with a frequency at only twice the pulsar rotation frequency (single harmonic) and the l = 2, m = 1, 2 modes with a frequency of both once and twice the rotation frequency (dual harmonic). No evidence of GWs was found, so we present 95% credible upper limits on the strain amplitudes h0 for the single-harmonic search along with limits on the pulsars' mass quadrupole moments Q22 and ellipticities ε. Of the pulsars studied, 23 have strain amplitudes that are lower than the limits calculated from their electromagnetically measured spin-down rates. These pulsars include the millisecond pulsars J0437−4715 and J0711−6830, which have spin-down ratios of 0.87 and 0.57, respectively. For nine pulsars, their spin-down limits have been surpassed for the first time. For the Crab and Vela pulsars, our limits are factors of ∼100 and ∼20 more constraining than their spin-down limits, respectively. For the dual-harmonic searches, new limits are placed on the strain amplitudes C21 and C22. For 23 pulsars, we also present limits on the emission amplitude assuming dipole radiation as predicted by Brans-Dicke theory