22 research outputs found
Pan-cancer analysis of whole genomes
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- Weisenberger
- Welch
- Wendl M. C. z
- wf Amary
- Whalley
- Wheeler
- wi Futreal
- Wigle
- Wilkerson M. D. v
- Williams
- Wilmott
- Wilson G. W. k
- Wilson R. K. z
- Wintersinger
- Wiznerowicz
- Wolf
- Wong
- Wong
- Woo
- Wood
- Wouters
- Wright
- Wright
- Wright A. J. k
- ws Ang
- Wu
- Wu
- Wu
- wv abg
- wz Hupp
- x Eils
- x Yung
- X. abp
- X. at
- X. bk
- X. cq
- X. ez
- X. ez
- X. fh
- X. fv
- X. fv
- X. fv
- X. fv
- X. k Mbabaali
- X. oi
- X. S. wd
- X. tc
- X. zv
- xb Danilova
- xb Felau
- xc Lovat
- xh Curley
- xh Fulton
- Xi
- Xia
- Xiang
- Xiong
- xo Abeshouse
- xp Benz
- xp Edwards
- xr Ghori
- xs Gundem
- Xue
- xv Luxton
- xw McDermott
- xy Visakorpi
- xz Whitaker
- Y. -E. ot
- Y. -J. k
- Y. -J. xn
- Y. abp
- Y. ae
- Y. ae
- Y. ae
- Y. ae
- Y. ai
- Y. aj
- Y. al
- Y. bk
- Y. dg
- Y. dy
- Y. ef
- Y. ep
- Y. ez
- Y. ff
- Y. fr
- Y. fv
- Y. fv
- Y. gl
- Y. hl
- Y. hq
- Y. hq
- Y. ia
- Y. kq
- Y. lw
- Y. nh
- Y. nk
- Y. nz
- Y. rg
- Y. rj
- Y. rm
- Y. S. jf
- Y. uz
- Y. vr
- Y. wt
- Y. yc
- ya Al-Ahmadie
- Yachida
- Yamaguchi
- Yamaguchi T. N. k
- Yamamoto
- Yamaue
- Yang
- Yang
- Yang
- Yang
- Yang
- Yao
- Yaspo
- Yates
- Yau
- yb Ally
- yd Cherniack
- yd Lai
- yd Schadendorf
- ye Auman
- ye Umbricht
- Yellapantula
- Yellapantula
- yh Bathe
- yj Baylin
- Yoon
- Yu
- Yu
- Yu
- Yuan
- Yugawa
- z ah
- Z. ej
- Z. ep
- Z. fr
- Z. hv
- Z. hy
- Z. jq
- Z. kt
- Z. oe
- Zaikova
- Zapatka
- zd Gershenwald
- Zenklusen
- Zeps
- zf Ghossein
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang H. b
- Zhao
- Zheng
- Zhou
- Zhou
- Zhu
- Zhu
- zi zj
- zm Jayaseelan
- Zou
- Zou
- zt Kim
- zw Lewis
- Ó. A. th
- Ø. sk
- Publication venue
- Publication date
- 11/12/2019
- Field of study
Cancer is driven by genetic change, and the advent of massively parallel sequencing has enabled systematic documentation of this variation at the whole-genome scale(1-3). Here we report the integrative analysis of 2,658 whole-cancer genomes and their matching normal tissues across 38 tumour types from the Pan-Cancer Analysis of Whole Genomes (PCAWG) Consortium of the International Cancer Genome Consortium (ICGC) and The Cancer Genome Atlas (TCGA). We describe the generation of the PCAWG resource, facilitated by international data sharing using compute clouds. On average, cancer genomes contained 4-5 driver mutations when combining coding and non-coding genomic elements; however, in around 5% of cases no drivers were identified, suggesting that cancer driver discovery is not yet complete. Chromothripsis, in which many clustered structural variants arise in a single catastrophic event, is frequently an early event in tumour evolution; in acral melanoma, for example, these events precede most somatic point mutations and affect several cancer-associated genes simultaneously. Cancers with abnormal telomere maintenance often originate from tissues with low replicative activity and show several mechanisms of preventing telomere attrition to critical levels. Common and rare germline variants affect patterns of somatic mutation, including point mutations, structural variants and somatic retrotransposition. A collection of papers from the PCAWG Consortium describes non-coding mutations that drive cancer beyond those in the TERT promoter(4); identifies new signatures of mutational processes that cause base substitutions, small insertions and deletions and structural variation(5,6); analyses timings and patterns of tumour evolution(7); describes the diverse transcriptional consequences of somatic mutation on splicing, expression levels, fusion genes and promoter activity(8,9); and evaluates a range of more-specialized features of cancer genomes(8,10-18).Peer reviewe
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
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- Field of study
Searches for gravitational waves from known pulsars at two harmonics in the second and third LIGO-Virgo observing runs
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- Abbott R
- Abe H
- Acernese F
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- Adhikari N
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- Adkins VK
- Adya VB
- Affeldt C
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- Arellano FEP
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- Haskell B
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- Hathaway JS
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- Hernandez IM
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- Wysocki DM
- Xiao L
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- Yamamoto T
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- Yang Y-C
- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu H
- Yu H
- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeidler S
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- Zendri J-P
- Zevin M
- Zhan M
- Zhang H
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- Zhang R
- Zhang T
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- Zhou R
- Zhou Z
- 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
Search for gravitational waves from Scorpius X-1 with a hidden Markov model in O3 LIGO data
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Alfaidi RA
- Allocca A
- Altin PA
- Amato A
- Anand C
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
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- Andres-Carcasona M
- Andric T
- Angelova SV
- Ansoldi S
- Antelis JM
- Antier S
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- Appavuravther EZ
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- Areeda JS
- Arellano FEP
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- Arnaud N
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- Aronson SM
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- Asali Y
- Ashton G
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- Ballardin G
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- Banerjee B
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- Barsuglia M
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- Barton MA
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- Bayley JC
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- Bedakihale VM
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- Bentley JD
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- Berger BK
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- Bersanetti D
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- Betzwieser J
- Beveridge D
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- Bhardwaj U
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- Bhattacharjee D
- Bhaumik S
- Bianchi A
- Bilenko IA
- Billingsley G
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- Bisht A
- Biswas B
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- Bizouard M-A
- Blackburn JK
- Blair CD
- Blair DG
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- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2022
- Field of study
Results are presented for a semi-coherent search for continuous gravitational waves from the low-mass X-ray binary Scorpius X-1, using a hidden Markov model (HMM) to allow for spin wandering. This search improves on previous HMM-based searches of Laser Interferometer Gravitational-wave Observatory (LIGO) data by including the orbital period in the search template grid, and by analyzing data from the latest (third) observing run (O3). In the frequency range searched, from 60 to 500 Hz, we find no evidence of gravitational radiation. This is the most sensitive search for Scorpius X-1 using a HMM to date. For the most sensitive sub-band, starting at 256.06Hz, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=6.16×10−26, assuming the orbital inclination angle takes its electromagnetically restricted value ι=44∘. The upper limits on gravitational wave strain reported here are on average a factor of ∼3 lower than in the O2 HMM search. This is the first Scorpius X-1 HMM search with upper limits that reach below the indirect torque-balance limit for certain sub-bands, assuming ι=44∘
Search for continuous gravitational wave emission from the Milky Way center in O3 LIGO-Virgo data
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- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
International audienceWe present a directed search for continuous gravitational wave (CW) signals emitted by spinningneutron stars located in the inner parsecs of the Galactic Center (GC). Compelling evidence for the presenceof a numerous population of neutron stars has been reported in the literature, turning this region into a veryinteresting place to look for CWs. In this search, data from the full O3 LIGO-Virgo run in the detectorfrequency band [10, 2000] Hz have been used. No significant detection was found and 95% confidencelevel upper limits on the signal strain amplitude were computed, over the full search band, with the deepestlimit of about 7.6×10−26 at ≃142 Hz. These results are significantly more constraining than those reportedin previous searches. We use these limits to put constraints on the fiducial neutron star ellipticity andr-mode amplitude. These limits can be also translated into constraints in the black hole mass–boson massplane for a hypothetical population of boson clouds around spinning black holes located in the GC
Search for Subsolar-Mass Binaries in the First Half of Advanced LIGO's and Advanced Virgo's Third Observing Run
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- Frasca S
- Frasconi F
- Freed JP
- Frei Z
- Freise A
- Freitas O
- Frey R
- Fritschel P
- Frolov VV
- Fronze GG
- Fujii Y
- Fujikawa Y
- Fujimoto Y
- Fulda P
- Fyffe M
- Gabbard HA
- Gadre BU
- Gair JR
- Gais J
- Galaudage S
- Gamba R
- Ganapathy D
- Ganguly A
- Gao D
- Gaonkar SG
- Garaventa B
- Garcia-Quiros C
- Garufi F
- Gateley B
- Gayathri V
- Ge G-G
- Gemme G
- Gennai A
- George J
- Gerberding O
- Gergely L
- Gewecke P
- Ghonge S
- Ghosh Abhirup
- Ghosh Archisman
- Ghosh Shaon
- Ghosh Shrobana
- Ghosh Tathagata
- Giacomazzo B
- Giacoppo L
- Giaime JA
- Giardina KD
- Gibson DR
- Gier C
- Giesler M
- Giri P
- Gissi F
- Gkaitatzis S
- Glanzer J
- Gleckl AE
- Godwin P
- Goetz E
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- Grignani G
- Grimaldi A
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- Grunewald S
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- Guerra D
- Guidi GM
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- Gupta Anuradha
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- Gustafson R
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- Haegel L
- Haino S
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- Hayakawa H
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- Heidmann A
- Heidt A
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- Holcomb DG
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- Hollows IJ
- Holmes ZJ
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- Hong Q
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- Howell EJ
- Hoy CG
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- Hsieh B-H
- Hsieh H-F
- Hsiung C
- Hsu Y
- Huang H-Y
- Huang P
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- Huang Y-J
- Huang Yiting
- Huang Yiwen
- Hubner MT
- Huddart AD
- Hughey B
- Hui DCY
- Hui V
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- JaberianHamedan V
- Jacqmin T
- Jacquet P-E
- Jadhav SJ
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- James AL
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- Jaranowski P
- Jariwala D
- Jaume R
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- Kajita T
- Kakizaki M
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- Kalogera V
- Kamai B
- Kamiizumi M
- Kanda N
- Kandhasamy S
- Kang G
- Kanner JB
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- Kapadia SJ
- Kapasi DP
- Karathanasis C
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- Kashyap R
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- Kastaun W
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- Katsavounidis E
- Katzman W
- Kaur T
- Kawabe K
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- Kefelian F
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- Khadka S
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- Khazanov EA
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- Knee AM
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- Knyazev E
- Kobayashi Y
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- Koekoek G
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- Kolitsidou P
- Kolstein M
- Komori K
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- Kontos A
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- Korobko M
- Kovalam M
- Koyama N
- Kozak DB
- Kozakai C
- Kringel V
- Krishnendu NV
- Krolak A
- Kuehn G
- Kuei F
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- Kulkarni S
- Kumar A
- Kumar Prayush
- Kumar Rahul
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- Kuromiya Y
- Kuroyanagi S
- Kwak K
- La Rosa I
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- Lazzaro C
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- Lehmann J
- Lemaitre A
- Lenti M
- Leonardi M
- Leonova E
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- Letendre N
- Levesque C
- Levin Y
- Leviton JN
- Leyde K
- Li AKY
- Li B
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- Li TGF
- Li X
- Lin C-Y
- Lin ET
- Lin F-K
- Lin F-L
- Lin HL
- Lin LC-C
- Linde F
- Linker SD
- Linley JN
- Littenberg TB
- Liu GC
- Liu J
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- Liu X
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- 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
- Lucaccioni JF
- Lueuk H
- Lumaca D
- Lundgren AP
- Luo L-W
- Lynam JE
- Ma'arif M
- Macas R
- Machtinger JB
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- Macleod DM
- MacMillan IAO
- Macquet A
- Magazzu C
- Magee RM
- Maggiore R
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- Majorana E
- Maksimovic I
- Maliakal S
- Malik A
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- Mandic V
- Mangano V
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- Marin Pina D
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- Markosyan AS
- Markowitz A
- Maros E
- Marquina A
- Marsat S
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- Martynov DV
- Marx EJ
- Masalehdan H
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- Massera E
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- Mastrogiovanni S
- Matas A
- Mateu-Lucena M
- Matichard F
- Matiushechkina M
- Mavalvala N
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- McWilliams ST
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- Mehmet M
- Mehta AK
- Meijer Q
- Melatos A
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- Melo S Assis de Souza
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- Menendez-Vazquez A
- 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
- Miller A
- Miller AL
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- Millhouse M
- Mills JC
- Milotti E
- Minenkov Y
- Mio N
- Mir Ll M
- 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
- Park J
- 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
- 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 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
- Ray A
- Raymond V
- Raza N
- Razzano M
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- Rees LA
- Regimbau T
- Rei L
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- 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
- Rosinska D
- Ross MP
- Rowan S
- Rowlinson SJ
- Roy S
- Roy Santosh
- Roy Soumen
- 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
- Salces-Carcoba F
- Salconi L
- Saleem M
- Salemi F
- Samajdar A
- San Martin EN Tapia
- Sanchez EJ
- Sanchez JH
- Sanchez LE
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- Sanders JR
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- Sassolas B
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- Schaetzl D
- Scheel M
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- Schiworski MG
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- Schofield RMS
- Schulte BW
- Schutz BF
- Schwartz E
- Scott J
- Scott SM
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- Sekiguchi Y
- Sellers D
- Sengupta AS
- Sentenac D
- Seo EG
- Sequino V
- Sergeev A
- Setyawati Y
- Shaffer T
- Shahriar MS
- Shaikh MA
- Shams B
- Shao L
- Sharma A
- Sharma P
- 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
- Singh N
- Singha A
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- 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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- Sorrentino F
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- Spagnuolo V
- Spencer AP
- Spera M
- Spinicelli P
- Srivastava AK
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- Staats K
- Stachie C
- Stachurski F
- 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 S Chalathadka
- Suchenek M
- Sudhagar S
- Sudhir V
- Sugimoto R
- Suh HG
- Sullivan AG
- Summerscales TZ
- Sun L
- 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
- Takeda H
- Takeda M
- Talbot C
- Talbot CJ
- 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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- 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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- Yeh SW
- Yelikar AB
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- 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
All-sky, all-frequency directional search for persistent gravitational waves from Advanced LIGO’s and Advanced Virgo’s first three observing runs
- Author
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- Ackley K
- Adhikari N
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- Adkins VK
- Adya VB
- Affeldt C
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- Aiello L
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- Albanesi S
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- Anderson SB
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- Yeh S-W
- Yelikar AB
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- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
We present the first results from an all-sky all-frequency (ASAF) search for an anisotropic stochastic gravitational-wave background using the data from the first three observing runs of the Advanced LIGO and Advanced Virgo detectors. Upper limit maps on broadband anisotropies of a persistent stochastic background were published for all observing runs of the LIGO-Virgo detectors. However, a broadband analysis is likely to miss narrowband signals as the signal-to-noise ratio of a narrowband signal can be significantly reduced when combined with detector output from other frequencies. Data folding and the computationally efficient analysis pipeline, PyStoch, enable us to perform the radiometer map-making at every frequency bin. We perform the search at 3072 HEALPix equal area pixels uniformly tiling the sky and in every frequency bin of width 1-32 Hz in the range 20-1726 Hz, except for bins that are likely to contain instrumental artefacts and hence are notched. We do not find any statistically significant evidence for the existence of narrowband gravitational-wave signals in the analyzed frequency bins. Therefore, we place 95\% confidence upper limits on the gravitational-wave strain for each pixel-frequency pair, the limits are in the range (0.030 - 9.6) \times10^{-24}. In addition, we outline a method to identify candidate pixel-frequency pairs that could be followed up by a more sensitive (and potentially computationally expensive) search, e.g., a matched-filtering-based analysis, to look for fainter nearly monochromatic coherent signals. The ASAF analysis is inherently independent of models describing any spectral or spatial distribution of power. We demonstrate that the ASAF results can be appropriately combined over frequencies and sky directions to successfully recover the broadband directional and isotropic results
Recommended from our members
Open Data from the Third Observing Run of LIGO, Virgo, KAGRA, and GEO
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- Zimmerman AB
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- Zweizig J
- 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