21 research outputs found
Astrometric effects of gravitational wave backgrounds with non-Einsteinian polarizations
- Publication venue
- Physical Review D - Particles, Fields, Gravitation and Cosmology
- Publication date
- 02/04/2018
- Field of study
The Gaia mission offers a new opportunity to search for the low-frequency gravitational wave background using astrometric measurements. In this paper, the astrometric effect of gravitational waves is reviewed, with a particular focus on the effect of non-Einsteinian gravitational wave polarizations. A stochastic gravitational wave background generates a correlated vector field of astrometric deflections on the sky. A convenient decomposition for the correlation matrix is introduced, enabling it to be calculated for all possible gravitational wave polarizations and compared to the redshift correlations from the pulsar-timing literature; in the case of a general relativity background of transverse traceless gravitational waves, this also allows us to identify an astrometric analog of the famous Hellings-Downs curve. Finally, the cross correlation between the redshift and astrometric signal is also calculated; this may form the basis for future joint pulsar-timing and astrometry searches for arbitrarily polarized gravitational wave backgrounds.D.âM. is funded by the STFC. C.âM. acknowledges financial support provided under the European Unionâs H2020 ERC Consolidator Grant âMatter and strong-field gravity: New frontiers in Einsteins theoryâ grant agreement no. MaGRaTh646597. This project has received funding from the European Unionâs Horizon 2020 research and innovation programme under the Marie Sklodowska-Curie grant agreement No. 690904 and C.âM. would like to acknowledge networking support by the COST Action CA16104
Determining 'need' for a Removable Partial Denture: a qualitative study of factors that influence dentist provision and patient use
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
The Changing Landscapes in DCD Liver Transplantation
- Author
- A Casavilla
- A Rojas-Peña
- A Schlegel
- A Schlegel
- AA Rabinstein
- AI Skaro
- AJ Hessheimer
- AK Mathur
- AM DâAlessandro
- C Jay
- C Moers
- CB Taner
- CB Taner
- CJE Watson
- CJE Watson
- D Kollmann
- D Nasralla
- DD Lee
- DE Schaubel
- DJ Reich
- DP Foley
- H Bohorquez
- H Sharma
- HM Wadei
- HW Lee
- J Lewis
- JC Hong
- JC LaMattina
- JD van der Bilt
- JL Bernat
- JR Montgomery
- JV Guarrera
- K Doi
- KJ Giesbrandt
- KJ Ho
- KM Olthoff
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- KP Croome
- L Matsuoka
- ME de Vera
- MJ Hobeika
- MT Perera
- O van Leeuwen
- P Dutkowski
- P Mihaylov
- R De Carlis
- R Mateo
- R van Rijn
- RM Chadha
- RW Laing
- S Khorsandi
- S Khorsandi
- SA Karangwa
- SG Farid
- T Alhamad
- T Ishaque
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Searches for Gravitational Waves from Known Pulsars at Two Harmonics in the Second and Third LIGO-Virgo Observing Runs
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
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- 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
- Andres N
- Andres-Carcasona M
- Andric T
- Angelova SV
- Ansoldi S
- Antelis JM
- Antier S
- Antonopoulou D
- Apostolatos T
- Appavuravther EZ
- Appert S
- Apple SK
- Arai K
- Araya A
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- Areeda JS
- Arellano FEP
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- Aritomi N
- Arnaud N
- Arogeti M
- Aronson SM
- Arun KG
- Arzoumanian Z
- Asada H
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- 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
Recommended from our members
Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGOâVirgo Network
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- Wysocki DM
- Xiao L
- Yadav N
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- Yamashita K
- Yamazaki R
- Yang FW
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- Yap MJ
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- Yeh S-W
- Yelikar AB
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- ZadroĆŒny A
- Zanolin M
- Zeidler S
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- Zevin M
- Zhan M
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- Zhao Yue
- 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
Searches for gravitational waves from known pulsars at two harmonics in the second and third LIGO-Virgo observing runs
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
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- 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 Δ. 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 J0437â4715 and J0711â6830, 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 âŒ100 and âŒ20 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
Model-based Cross-correlation Search for Gravitational Waves from the Low-mass X-Ray Binary Scorpius X-1 in LIGO O3 Data
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- 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 10â25 when marginalized isotropically over the unknown inclination angle of the neutron star's rotation axis, or less than 4 Ă 10â26 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 LIGOâVirgo Network
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- Wysocki DM
- Xiao L
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- Yamazaki R
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- Yang Yang
- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- ZadroĆŒny A
- Zanolin M
- Zeidler S
- Zelenova T
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- Zevin M
- Zhan M
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- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- 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
- Abbott R
- Abe H
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- Ackley K
- Adhikari N
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- 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 qâ„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 fPBHÏPBH/ÏDM6%. This improves existing constraints on primordial black hole abundance by a factor of âŒ3. 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 fDBHÏDBH/ÏDM0.003%. These are the first constraints placed on dissipative dark models by subsolar-mass analyses
Search for subsolar-mass black hole binaries in the second part of Advanced LIGOâs and Advanced Virgoâs third observing run
- Author
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- Abe H
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- Griggs HL
- Grignani G
- Grimaldi A
- Grimm SJ
- Grote H
- Grunewald S
- Gruson AS
- Guerra D
- Guidi GM
- Guimaraes AR
- Gulati HK
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- Howell D
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- Jariwala D
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- Kozak DB
- Kozakai C
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- Kringel V
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- LemaĂźtre A
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- Leonardi M
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- Leviton JN
- Leyde K
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- Li TGF
- Li X
- Lin C-Y
- Lin ET
- Lin F-K
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- Linde F
- Linker SD
- Littenberg TB
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- London LT
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- Loriette V
- Lormand M
- Losurdo G
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- Lough JD
- Lousto CO
- Lovelace G
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- Lundgren AP
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- Luo L-W
- Lussier AW
- Lynam JE
- LĂŒck H
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- Macleod DM
- MacMillan IAO
- Macquet A
- MagazzĂč C
- Magee RM
- Maggiore R
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- Mahesh S
- Majorana E
- Makarem CN
- Maksimovic I
- Maliakal S
- Malik A
- Man N
- Mandic V
- Mangano V
- Mannix BR
- Mansell GL
- Mansingh G
- Manske M
- Mantovani M
- Mapelli M
- Marchesoni F
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- Mark Z
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- Markosyan AS
- Markowitz A
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- Mehmet M
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- Melo ITE
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- Menendez-Vazquez A
- Menoni CS
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- Merilh EL
- Merritt JD
- Merzougui M
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- Messick C
- Meyers PM
- Meylahn F
- Mhaske A
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- Miao H
- Michaloliakos I
- Michel C
- Michimura Y
- Middleton H
- Mihaylov DP
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- Miller AL
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- Milotti E
- Minenkov Y
- Mio N
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- Miravet-Tenés M
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- Mishra C
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- Mitchell AL
- Mitra S
- Mitrofanov VP
- Mitselmakher G
- Mittleman R
- Miyakawa O
- Miyo K
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- Mo G
- Modafferi LM
- Moguel E
- Mogushi K
- Mohapatra SRP
- Mohite SR
- Molina-Ruiz M
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- Mondin M
- Montani M
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- Moragues J
- Morales ER
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- Morawski F
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- Moreno C
- Moreno G
- Mori Y
- Morisaki S
- Morisue N
- Moriwaki Y
- Morras G
- Mours B
- Mow-Lowry CM
- Mozzon S
- Mu niz EA
- Muciaccia F
- Mukherjee D
- Mukherjee S
- Mukherjee S
- Mukherjee S
- Mukund N
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- Munch J
- Murray PG
- Muusse S
- MĂĄrka S
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- Nadji SL
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- Nakayama Y
- Napolano V
- Nardecchia I
- Narola H
- Naticchioni L
- Nayak RK
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- Neilson J
- Nelson A
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- Nery M
- Neubauer P
- Neunzert A
- Ng KY
- Ng SWS
- Nguyen C
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- Ni J
- Ni W-T
- Nichols SA
- Nieradka G
- Nishimoto T
- Nishizawa A
- Nissanke S
- Nitoglia E
- Niu W
- Nocera F
- Norman M
- North C
- Notte J
- Novak J
- Nozaki S
- Nurbek G
- Nuttall LK
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- Oberling J
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- Oganesyan G
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- Ohashi T
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- Olivetto C
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- Ormsby ND
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- Ossokine S
- Osthelder C
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- OâBrien BD
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- OâHanlon T
- OâReilly B
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- OâShea E
- Pace AE
- Pagano G
- Pagano R
- Pagliaroli G
- Pai A
- Pai SA
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- Palamos JR
- Palashov O
- Palomba C
- Pan K-C
- Panda PK
- Pang PTH
- Pannarale F
- Pant BC
- Panther FH
- Paoletti F
- Paoli A
- Paolone A
- Pappas G
- Parisi A
- Park J
- Parker W
- Pascucci D
- Pasqualetti A
- Passaquieti R
- Passuello D
- Patel M
- Patel NR
- Pathak M
- Patricelli B
- Patron AS
- Paul S
- Payne E
- Pedraza M
- Pedurand R
- Pegna R
- Pegoraro M
- Pele A
- Penano S
- Penn S
- Perego A
- Pereira A
- Pereira T
- Perez CJ
- Perkins CC
- Perreca A
- PerriĂšs S
- Perry JW
- Pesios D
- Petermann J
- Pfeiffer HP
- Pham H
- Pham KA
- Phukon KS
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- Pichot M
- Piendibene M
- Piergiovanni F
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- 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
- Poggiani R
- Polini E
- Pong DYT
- Ponrathnam S
- Porter EK
- Portilla ML
- Posnansky C
- Poulton R
- 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
- PĂ©rigois C
- PĂŒrrer M
- Qi H
- Quartey N
- Quetschke V
- Quinonez PJ
- Quitzow-James R
- Quynh LN
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- Raaijmakers G
- Radkins H
- Radulesco N
- Raffai P
- Rail SX
- Raja S
- Rajan C
- Ramirez KE
- Ramirez TD
- Ramos-Buades A
- Rana D
- Rana J
- Rangnekar PR
- Rapagnani P
- Ray A
- Raymond V
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- Razzano M
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- Reinhard M
- Reitze DH
- Relton P
- Renzini A
- Rettegno P
- Revenu B
- Reyes J
- Reza A
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- Rezaei AS
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- Richards D
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- Robertson C
- Robertson NA
- Robie R
- Robinet F
- Rocchi A
- Rodriguez S
- Rolland L
- Rollins JG
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- Romano R
- Romel CL
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- Romie JH
- Ronchini S
- Roocke TJ
- Rosa IL
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- Rowlinson SJ
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- Ruggi P
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- Sadecki T
- Sadiq J
- Saffarieh P
- Saha S
- Saito Y
- Sakai K
- Sakellariadou M
- Sakon S
- Salafia OS
- Salces-Carcoba F
- Salconi L
- Saleem M
- Salemi F
- Sallé M
- Samajdar A
- San MartĂn ENT
- Sanchez EJ
- Sanchez JH
- Sanchez LE
- Sanchis-Gual N
- Sanders JR
- Sanuy A
- Saravanan TR
- Sarin N
- Sasli A
- Sassolas B
- Satari H
- Sathyaprakash BS
- Sauter O
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- Savant V
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- Sawant HL
- Sayah S
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- Schiworski MG
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- Sellers D
- Sengupta AS
- Sentenac D
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- Sequino V
- Sergeev A
- Servignat G
- Shaffer YST
- Shahriar MS
- Shaikh MA
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- Shao L
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- Shcheblanov NS
- Sheela A
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- Shikano Y
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- Shimode K
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- Shishido T
- Shoda A
- Shoemaker DH
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- Sieniawska M
- Sigg D
- Silenzi L
- Siles JFN
- Singer LP
- Singh D
- Singh MK
- Singh N
- Singha A
- Sintes AM
- Sipala V
- Skliris V
- Slagmolen BJJ
- Slaven-Blair TJ
- Smetana J
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- Somala SN
- Somiya K
- Song I
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- Sorrentino N
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- Spagnuolo V
- Spencer AP
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- Srivastava AK
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- Stachie C
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- Steer DA
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- Steinlechner S
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- Stops DJ
- Strain KA
- Strang LC
- Stratta G
- Strong MD
- Strunk A
- Sturani R
- Stuver AL
- Subrahmanya SC
- Suchenek M
- Sudhagar S
- 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
- Syx A
- SzczepaĆczyk MJ
- Szewczyk P
- Tacca M
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- Tait SC
- Takahashi H
- Takahashi R
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- Tanaka T
- Tanasijczuk AJ
- Tanioka S
- Tanner DB
- Tao D
- Tao L
- Tapia RD
- Taranto C
- Taruya A
- Tasson JD
- Tenorio R
- Terhune JES
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- Themann H
- Thirugnanasambandam MP
- Thomas M
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- Thompson EE
- Thompson JE
- Thondapu SR
- Thorne KA
- Thrane E
- Tiwari S
- Tiwari S
- Tiwari V
- Toivonen AM
- Tolley AE
- Tomaru T
- Tomura T
- Tonelli M
- Torres-Forné A
- Torrie CI
- Tournefier E
- Trapananti A
- Travasso F
- Traylor G
- Trenado J
- Trevor M
- Tringali MC
- Tripathee A
- Troiano L
- Trovato A
- Trozzo L
- Trudeau RJ
- Tsai D
- Tsang KW
- Tsang T
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- Tsuchida S
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- Tsuna D
- Tsutsui T
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- Turconi M
- Turski C
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- Ubach H
- Ubhi AS
- Uchiyama T
- Udall RP
- Ueda A
- Uehara T
- Ueno K
- Ueshima G
- Unnikrishnan CS
- Urban AL
- Ushiba T
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- Vajente G
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- Valdes G
- Valentini M
- Vallero S
- Valsan V
- van Bakel N
- van Beuzekom M
- van Dael M
- Van de Walle A
- van den Brand JFJ
- Van Den Broeck C
- van Dongen J
- van Haevermaet H
- van Heijningen JV
- van Putten MHPM
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- van Remortel N
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- Vanosky J
- Vardaro M
- Vargas AF
- Varma V
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- Veitch PJ
- Venneberg J
- Venugopalan G
- Verdier P
- Verkindt D
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- Vermeulen SM
- Veske D
- Vetrano F
- Viceré A
- Vidyant S
- Viets AD
- Vijaykumar A
- Villa-Ortega V
- Vinet J-Y
- 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
- Wang JZ
- Wang WH
- Ward RL
- Warner J
- Was M
- Washimi T
- Washington NY
- Watada K
- Watarai D
- Watchi J
- Wayt KE
- Weaver B
- Weaving CR
- Webster SA
- Weinert M
- Weinstein AJ
- Weiss R
- Weller CM
- Weller RA
- Wellmann F
- Wen L
- Wette K
- WeĂels P
- Whelan JT
- White DD
- Whiting BF
- Whittle C
- Wilk OS
- Wilken D
- Williams CE
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- Williams MJ
- Williamson AR
- Willis JL
- Willke B
- Wipf CC
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- Woehler J
- Wofford JK
- Wojtowicz IA
- Wong D
- Wong ICF
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- Wu C
- Wu DS
- Wu H
- Wysocki DM
- Xiao L
- Yadav N
- Yamada T
- Yamamoto H
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- Yamamoto T
- Yamashita K
- Yamazaki R
- Yang FW
- Yang KZ
- Yang L
- Yang Y
- Yang Y
- Yang Y-C
- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu H
- Yu H
- Yuzurihara H
- ZadroĆŒny 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 Y
- Zheng Y
- Zhou R
- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 28/02/2023
- Field of study