133 research outputs found
Conformal radiotherapy for lung cancer: interobservers' variability in the definition of gross tumor volume between radiologists and radiotherapists
- Author
- [ICRU] International Commission on Radiation Units and Measurements
- [ICRU] International Commission on Radiation Units and Measurements
- [ICRU] International Commission on Radiation Units and Measurements
- A Van Baardwijk
- Almir GV Bitencourt
- B Emami
- B Emami
- B Emami
- C Greco
- C Rasch
- CA Perez
- CA Perez
- Chiang J Tyng
- CS Hamilton
- DA Jaffray
- Douglas G Castro
- G Leunens
- GS Sibley
- J Armstrong
- J Armstrong
- J Armstrong
- J Armstrong
- JA Antolak
- JD Bradley
- JF Valley
- JM Robertson
- JP Logue
- JVan de Steene
- JVan de Steene
- K Satoh
- L Ekberg
- LF Cazzaniga
- Marcelle A Borba
- MV Graham
- MV Graham
- MV Graham
- P Giraud
- P Tai
- Paula NV Pinto
- Paulo E Novaes
- Ph Giraud
- Ph Giraud
- R Oozeer
- Ricardo C Fogaroli
- Rubens Chojniak
- S Senan
- S Sundar
- S Vijayakumar
- SG McNee
- SL Faria
- V Beckendorf
- Publication venue
- BioMed Central
- Publication date
- 01/01/2009
- Field of study
Circadian Clock Genes Contribute to the Regulation of Hair Follicle Cycling
- Author
- A Grechez-Cassiau
- AA Panteleyev
- Alexander T. Ihler
- BH Miller
- BH Miller
- Bogi Andersen
- C Bertolucci
- Darya Chudova
- DJ Veis
- DP King
- E Fuchs
- F Guillaumond
- G Cotsarelis
- G Dennis Jr
- G Kaya
- GA Bjarnason
- GA Bjarnason
- HR Ueda
- JA Ripperger
- Joseph S. Takahashi
- K Kume
- Kevin K. Lin
- KK Lin
- KS Stenn
- LS Hansen
- M Geyfman
- M Ito
- M Reick
- M Schneider
- M Tanioka
- MH Vitaterna
- Mikhail Geyfman
- MK Bunger
- MV Plikus
- N Gekakis
- N Nakao
- N Preitner
- ND Pruett
- NV Botchkareva
- P Baldi
- Padhraic Smyth
- PL Lowrey
- R Jordan
- R Paus
- R Paus
- Ralf Paus
- RV Kondratov
- S Chib
- S Kawara
- S Muller-Rover
- S Panda
- S Yamazaki
- Sarah E. Millar
- SB Zanello
- SE Millar
- SH Yoo
- SM Reppert
- T Hunt
- T Matsuo
- V Greco
- V Jaks
- VA Botchkarev
- Vivek Kumar
- Publication venue
- Public Library of Science
- Publication date
- 01/07/2009
- Field of study
Hair follicles undergo recurrent cycling of controlled growth (anagen), regression (catagen), and relative quiescence (telogen) with a defined periodicity. Taking a genomics approach to study gene expression during synchronized mouse hair follicle cycling, we discovered that, in addition to circadian fluctuation, CLOCK–regulated genes are also modulated in phase with the hair growth cycle. During telogen and early anagen, circadian clock genes are prominently expressed in the secondary hair germ, which contains precursor cells for the growing follicle. Analysis of Clock and Bmal1 mutant mice reveals a delay in anagen progression, and the secondary hair germ cells show decreased levels of phosphorylated Rb and lack mitotic cells, suggesting that circadian clock genes regulate anagen progression via their effect on the cell cycle. Consistent with a block at the G1 phase of the cell cycle, we show a significant upregulation of p21 in Bmal1 mutant skin. While circadian clock mechanisms have been implicated in a variety of diurnal biological processes, our findings indicate that circadian clock genes may be utilized to modulate the progression of non-diurnal cyclic processes
Multi-messenger observations of a binary neutron star merger
- Author
- Aab A
- Aartsen MG
- Abbott BP
- Abbott R
- Abbott TD
- Abbott TMC
- Abdalla H
- Abe F
- Abeysekara AU
- Abramo LR
- Abramowski A
- Abreu P
- Acernese F
- Acero F
- Ackermann M
- Ackley K
- Ackley K
- Adams C
- Adams J
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- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Afrough M
- Agarwal B
- Agathos M
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- Aglietta M
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- Aguilar JA
- Aharonian F
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- Ahrens M
- Aiello L
- Ain A
- Ajith P
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- Al Samarai I
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- Albuquerque IFM
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- Alighieri S Di Serego
- Allam S
- Allekotte I
- Allen B
- Allen G
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- Almela A
- Altin PA
- Altmann D
- Alvarez C
- Alvarez JD
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- Alvarez-Muiz J
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- Ananyeva A
- Anastasi GA
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- Anupama GC
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- Araya MC
- Arcavi I
- Arceo R
- Ardid M
- Areeda JS
- Aresu G
- Argan A
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- Array LWA Long Wavelength
- Array MWA Murchison Widefield
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- Zhang Y-H
- Zhang YF
- Zhang YJ
- Zhang Z
- Zhang ZL
- Zhao C
- Zhao HS
- Zhao JL
- Zhao W
- Zhao XF
- Zheng SJ
- Zhou H
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- Zhou M
- Zhou Z
- Zhu SJ
- Zhu XJ
- Zhu Y
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- Zhu Z
- Ziegler A
- Zimmerman AB
- Zimmermann B
- Zimnukhov DS
- Ziolkowski M
- Zoll M
- Zong Z
- Zorn J
- Zornoza JD
- Zou CL
- Zuccarello F
- Zucker ME
- Zuniga J
- Zweizig J
- Zywucka N
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- Wu Ds
- Wysocki Dm
- Xiao S
- Xu R
- Yamamoto H
- Yancey Cc
- Yang L
- Yang Y
- Yang Z
- Yap Mj
- Yazback M
- Yeeles Dw
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- Yu Hc
- Yuen Shr
- Zadrozny A
- Zadrozny Ak
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- Zelenova T
- Zendri Jp
- Zevin M
- Zhang J
- Zhang L
- Zhang T
- Zhao C
- Zhao G
- Zhou M
- Zhou Z
- Zhu Xj
- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- College Park, MD : American Physical Society
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO's second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=3.47×10-25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering. © 2019 American Physical Society
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- van den Brand Jfj
- Van Den Broeck C
- van der Schaaf L
- van Veggel Aa
- Vander-Hyde Dc
- VanHeijningen Jv
- Vardaro M
- Varma V
- Vass S
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- Vecchio A
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- Wade M
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- Walker M
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- Wang H
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- Wang S
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- Wang Yf
- Ward Rl
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- Warner J
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- Watchi J
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- Wei Lw
- Weinert M
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- Wellmann F
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- Westhouse Jw
- Wette K
- Whelan Jt
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- Williams D
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- Willke B
- Winkler W
- Wipf Cc
- Wittel H
- Woan G
- Woehler J
- Wofford Jk
- Wright Jl
- Wu Ds
- Wysocki Dm
- Xiao S
- Xu R
- Yamamoto H
- Yancey Cc
- Yang L
- Yang Y
- Yang Z
- Yap Mj
- Yazback M
- Yeeles Dw
- Yu H
- Yu Hc
- Yuen Shr
- Zadrozny A
- Zadrozny Ak
- Zanolin M
- Zelenova T
- Zendri Jp
- Zevin M
- Zhang J
- Zhang L
- Zhang T
- Zhao C
- Zhao G
- Zhou M
- Zhou Z
- Zhu Xj
- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO’s second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h95%0=3.47×10−25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering
Corrigendum to "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at √s=13 TeV" (Physics Letters B, 842 (2023), 137379)
- Author
- Aad G
- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- Abidi Sh
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman Ac
- Acharya Bs
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Addepalli Sv
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder Aa
- Afik Y
- Agaras Mn
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra Ja
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- Cherkaoui El Moursli R
- Cheu E
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- Herrmann T
- Herten G
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- Iguchi R
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- Ikegami Y
- Ilg A
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- Issever C
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- Ketabchi Haghighat S
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- Koletsou I
- Komarek T
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- Lari T
- Lasagni Manghi F
- Lassnig M
- Latonova V
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- Laudrain A
- Laurier A
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- Lawrence Z
- Lazzaroni M
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- Lebedev A
- Leblanc M
- Lecompte T
- Ledroit-Guillon F
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- Ponomarenko D
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- Seitz C
- Seixas Jm
- Sekhniaidze G
- Sekula Sj
- Selem L
- Semprini-Cesari N
- Sen S
- Senthilkumar V
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sevova S
- Sforza F
- Sfyrla A
- Shabalina E
- Shaheen R
- Shahinian Jd
- Shaikh Nw
- Shaked Renous D
- Shan Ly
- Shapiro M
- Sharma A
- Sharma As
- Sharma P
- Sharma S
- Shatalov Pb
- Shaw K
- Shaw Sm
- Sherwood P
- Shi L
- Shimmin Co
- Shimogama Y
- Shinner Jd
- Shipsey Ipj
- Shirabe S
- Shiyakova M
- Shlomi J
- Shochet Mj
- Shojaii J
- Shope Dr
- Shrestha S
- Shrif Em
- Shroff Mj
- Sicho P
- Sickles Am
- Sideras Haddad E
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Sikora R
- Sili F
- Silva Oliveira Mv
- Silva Jm
- Silverstein Sb
- Simion S
- Simoniello R
- Simpson El
- Simpson Nd
- Simsek S
- Sindhu S
- Sinervo P
- Sinetckii V
- Singh S
- Singh S
- Sinha S
- Sinha S
- Sioli M
- Siral I
- Sivoklokov Sy
- Sjölin J
- Skaf A
- Skorda E
- Skubic P
- Slawinska M
- Smakhtin V
- Smart Bh
- Smiesko J
- Smirnov Sy
- Smirnov Y
- Smirnova Ln
- Smirnova O
- Smith Ea
- Smith Ha
- Smith Jl
- Smith R
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev Aa
- Snoek Hl
- Snyder S
- Sobie R
- Soffer A
- Solans Sanchez Ca
- Soldatov Ey
- Soldevila U
- Solodkov Aa
- Solomon S
- Soloshenko A
- Solovieva K
- Solovyanov Ov
- Solovyev V
- Sommer P
- Sonay A
- Song Wy
- Sopczak A
- Sopio Al
- Sopkova F
- Sothilingam V
- Sottocornola S
- Soualah R
- Soumaimi Z
- South D
- Spagnolo S
- Spalla M
- Spanò F
- Sperlich D
- Spigo G
- Spina M
- Spinali S
- Spiteri Dp
- Spousta M
- Staats Ej
- Stabile A
- Stamen R
- Stamenkovic M
- Stampekis A
- Standke M
- Stanecka E
- Stanislaus B
- Stanitzki Mm
- Stankaityte M
- Stapf B
- Starchenko Ea
- Stark Gh
- Stark J
- Starko Dm
- Staroba P
- Starovoitov P
- Staszewski R
- Stavropoulos G
- Stärz S
- Steentoft J
- Steinberg P
- Steinhebel Al
- Stelzer B
- Stelzer Hj
- Stelzer-Chilton O
- Stenzel H
- Stevenson Tj
- Stewart Ga
- Stockton Mc
- Stoicea G
- Stolarski M
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strebler T
- Strizenec P
- Strom Dm
- Strom Lr
- Stroynowski R
- Ströhmer R
- Strubig A
- Stucci Sa
- Stugu B
- Stupak J
- Styles Na
- Su D
- Su S
- Su W
- Su X
- Sugizaki K
- Sulin Vv
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- Sultan Dms
- Sultanaliyeva L
- Sultansoy S
- Sumida T
- Sun S
- Sun S
- Sunneborn Gudnadottir O
- Sutton Mr
- Svatos M
- Swiatlowski M
- Swirski T
- Sykora I
- Sykora M
- Sykora T
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Tafoya Vargas Js
- Taibah Rhm
- Takashima R
- Takeda K
- Takeva Ep
- Takubo Y
- Talby M
- Talyshev Aa
- Tam Kc
- Tamir Nm
- Tanaka A
- Tanaka J
- Tanaka R
- Tanasini M
- Tang J
- Tao Z
- Tapia Araya S
- Tapprogge S
- Tarek Abouelfadl Mohamed A
- Tarem S
- Tariq K
- Tarna G
- Tartarelli Gf
- Tas P
- Tasevsky M
- Tassi E
- Tate Ac
- Tateno G
- Tayalati Y
- Taylor Gn
- Taylor W
- Teagle H
- Tee As
- Teixeira De Lima R
- Teixeira-Dias P
- Teoh Jj
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher Rj
- Themistokleous N
- Theveneaux-Pelzer T
- Thielmann O
- Thomas Dw
- Thomas Jp
- Thompson Ea
- Thompson Pd
- Thomson E
- Thorpe Ej
- Tian Y
- Tikhomirov V
- Tikhonov Ya
- Timoshenko S
- Ting Exl
- Tipton P
- Tisserant S
- Tlou Sh
- Tnourji A
- Todome K
- Todorova-Nova S
- Todt S
- Togawa M
- Tojo J
- Tokár S
- Tokushuku K
- Tombs R
- Tomoto M
- Tompkins L
- Tornambe P
- Torrence E
- Torres H
- Torró Pastor E
- Toscani M
- Tosciri C
- Tovey Dr
- Traeet A
- Trandafir Is
- Trefzger T
- Tricoli A
- Trigger Im
- Trincaz-Duvoid S
- Trischuk Da
- Trocmé B
- Trofymov A
- Troncon C
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tsai M
- Tsiamis A
- Tsiareshka Pv
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze Eg
- Tsopoulou M
- Tsujikawa Y
- Tsukerman Ii
- Tsulaia V
- Tsuno S
- Tsur O
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna An
- Turchikhin S
- Turk Cakir I
- Turra R
- Tuts Pm
- Tzamarias S
- Tzanis P
- Tzovara E
- Uchida K
- Ukegawa F
- Ulloa Poblete Pa
- Unal G
- Unal M
- Undrus A
- Unel G
- Uno K
- Urban J
- Urquijo P
- Usai G
- Ushioda R
- Usman M
- Uysal Z
- Vacek V
- Vachon B
- Vadla Koh
- Vafeiadis T
- Valderanis C
- Valdes Santurio E
- Valente M
- Valentinetti S
- Valero A
- Vallier A
- Valls Ferrer Ja
- Van Daalen Tr
- Van Gemmeren P
- Van Stroud S
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall Er
- Vannicola D
- Vannoli L
- Vari R
- Varnes Ew
- Varni C
- Varol T
- Varouchas D
- Varriale L
- Varvell Ke
- Vasile Me
- Vaslin L
- Vasquez Ga
- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veen Mj
- Veliscek I
- Veloce Lm
- Veloso F
- Veneziano S
- Ventura A
- Verbytskyi A
- Verducci M
- Vergis C
- Verissimo De Araujo M
- Verkerke W
- Vermeulen Jc
- Vernieri C
- Verschuuren Pj
- Vessella M
- Vesterbacka Ml
- Vetterli Mc
- Vgenopoulos A
- Viaux Maira N
- Vickey Boeriu Oe
- Vickey T
- Viehhauser Gha
- Vigani L
- Villa M
- Villaplana Perez M
- Villhauer Em
- Vilucchi E
- Vincter Mg
- Virdee Gs
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vladimirov V
- Voevodina E
- Vogel F
- Vokac P
- Von Ahnen J
- Von Toerne E
- Vormwald B
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld Jh
- Vozak M
- Vozdecky L
- Vranjes Milosavljevic M
- Vranjes N
- Vreeswijk M
- Vuillermet R
- Vujinovic O
- Vukotic I
- Wada S
- Wagner C
- Wagner W
- Wahdan S
- Wahlberg H
- Wakasa R
- Wakida M
- Walbrecht Vm
- Walder J
- Walker R
- Walkowiak W
- Wang Am
- Wang Az
- Wang C
- Wang C
- Wang H
- Wang J
- Wang P
- Wang R
- Wang R
- Wang R-
- Wang S
- Wang Sm
- Wang T
- Wang Wt
- Wang Wx
- Wang X
- Wang X
- Wang X
- Wang Y
- Wang Y
- Wang Z
- Wang Z
- Wang Z
- Warburton A
- Ward Rj
- Warrack N
- Watson At
- Watson Mf
- Watts G
- Waugh Bm
- Webb Af
- Weber C
- Weber Ms
- Weber Sa
- Weber Sm
- Wei C
- Wei Y
- Weidberg Ar
- Weingarten J
- Weirich M
- Weiser C
- Wells Cj
- Wenaus T
- Wendland B
- Wengler T
- Wenke Ns
- Wermes N
- Wessels M
- Whalen K
- Wharton Am
- White A
- White As
- White Mj
- Whiteson D
- Wickremasinghe L
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs Lam
- Wilbern Dj
- Wilkens Hg
- Williams Dm
- Williams Hh
- Williams S
- Willocq S
- Windischhofer Pj
- Winklmeier F
- Winter Bt
- Wittgen M
- Wobisch M
- Wolf A
- Wollrath J
- Wolter Mw
- Wolters H
- Wong Vws
- Wongel Af
- Worm Sd
- Wosiek Bk
- Woźniak Kw
- Wölker R
- Wraight K
- Wu J
- Wu M
- Wu Sl
- Wu X
- Wu Y
- Wu Z
- Wuerzinger J
- Wyatt Tr
- Wynne Bm
- Xella S
- Xia L
- Xia M
- Xiang J
- Xiao X
- Xie M
- Xie X
- Xiotidis I
- Xu D
- Xu H
- Xu H
- Xu L
- Xu R
- Xu T
- Xu W
- Xu Y
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yamaguchi N
- Yamaguchi Y
- Yamauchi H
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan S
- Yan Z
- Yang Hj
- Yang Ht
- Yang S
- Yang T
- Yang X
- Yang X
- Yang Y
- Yang Z
- Yao W
- Yap Yc
- Ye H
- Ye J
- Ye S
- Ye X
- Yeletskikh I
- Yexley Mr
- Yin P
- Yorita K
- Young C
- Young Cjs
- Yuan M
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeißner Sv
- Zeng Jc
- Zenger Dt
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang Df
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu C
- Zhu Cg
- Zhu H
- Zhu Hl
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine Ni
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas Tg
- Zormpa O
- Zou W
- Zwalinski L
- Ženiš T
- Živković L
- Publication venue
- ELSEVIER
- Publication date
- 01/01/2023
- Field of study
Binary Black Hole Mergers in the first Advanced LIGO Observing Run
- Author
- a DTO
- a MC
- Abbott BP
- Abbott R
- Abbott TD
- Abernathy MR
- Acernese F
- Ackley K
- Adams C
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Allen B
- Allocca A
- Altin PA
- Anderson SB
- Anderson WG
- Arai K
- Araya MC
- Arceneaux CC
- Areeda JS
- Arnaud N
- Arun KG
- Ascenzi S
- Ashton G
- Ast M
- Aston SM
- Astone P
- Aufmuth P
- Aulbert C
- Babak S
- Bacon P
- Bader MKM
- Baiardi LC
- Bakel NV
- Baker PT
- Baldaccini F
- Ballardin G
- Ballmer SW
- Barayoga JC
- Barclay SE
- Barish BC
- Barker D
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Bartos I
- Bassiri R
- Basti A
- Batch JC
- Baune C
- Bavigadda V
- Bazzan M
- Bejger M
- Bell AS
- Berger BK
- Bergmann G
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Beuzekom MV
- Bhagwat S
- Bhandare R
- Bilenko IA
- Billingsley G
- Birch J
- Birney R
- Birnholtz O
- Biscans S
- Bisht A
- Bitossi M
- Biwer C
- Bizouard MA
- Blackburn JK
- Blair CD
- Blair DG
- Blair RM
- Bloemen S
- Bock O
- Boer M
- Bogaert G
- Bogan C
- Bohe A
- Bond C
- Bondu F
- Bonnand R
- Boom BA
- Bork R
- Boschi V
- Bose S
- Bouffanais Y
- Bozzi A
- Bradaschia C
- Brady PR
- Braginsky VB
- Branchesi M
- Brand JFJVD
- Brau JE
- Briant T
- Brillet A
- Brinkmann M
- Brisson V
- Brockill P
- Broeck CVD
- Broida JE
- Brooks AF
- Brown DA
- Brown DD
- Brown NM
- Brunett S
- Buchanan CC
- Buikema A
- Bulik T
- Bulten HJ
- Buonanno A
- Buskulic D
- Bustillo JC
- Buy C
- Byer RL
- Cabero M
- Cadonati L
- Cagnoli G
- Cahillane C
- Callister T
- Calloni E
- Camp JB
- Cannon KC
- Canton TD
- Cao J
- Capano CD
- Capocasa E
- Carbognani F
- Caride S
- Casentini C
- Castro JMG
- Caudill S
- Cavalier F
- Cavalieri R
- Cella G
- Cepeda CB
- Cerretani G
- Cesarini E
- Chamberlin SJ
- Chan M
- Chao S
- Charlton P
- Chassande-Mottin E
- Cheeseboro BD
- Chen HY
- Chen Y
- Cheng C
- Chincarini A
- Chiummo A
- Cho HS
- Cho M
- Chow JH
- Christensen N
- Chu Q
- Chua S
- Chung S
- Ciani G
- Clara F
- Clark JA
- Cleva F
- Coccia E
- Cohadon P-F
- Colla A
- Collaboration TLIGOS
- Collaboration TV
- Collette CG
- Cominsky L
- Conte A
- Conti L
- Cook D
- Corbitt TR
- Cornish N
- Corsi A
- Cortese S
- Costa CA
- Costa CFDS
- Coughlin MW
- Coughlin SB
- Coulon J-P
- Countryman ST
- Couvares P
- Cowan EE
- Coward DM
- Cowart MJ
- Coyne DC
- Coyne R
- Craig K
- Creighton JDE
- Cripe J
- Crowder SG
- Cumming A
- Cunningham L
- Cuoco E
- D'Antonio S
- D'iaz MC
- Danilishin SL
- Danzmann K
- Darman NS
- Dasgupta A
- Dattilo V
- Dave I
- Davier M
- Davies GS
- Daw EJ
- Day R
- De S
- DeBra D
- Debreczeni G
- Degallaix J
- Del'eglise S
- Denker T
- Dent T
- Dergachev V
- DeRosa RT
- DeSalvo R
- Devine RC
- Dhurandhar S
- Diaz JC
- Dolique V
- Donovan F
- Dooley KL
- Doravari S
- Douglas R
- Downes TP
- Drago M
- Drever RWP
- Driggers JC
- Ducrot M
- Dwyer SE
- Edo TB
- Edwards MC
- Effler A
- Eggenstein H-B
- Ehrens P
- Eichholz J
- Eikenberry SS
- Engels W
- Essick RC
- Etzel T
- Evans M
- Evans TM
- Everett R
- Factourovich M
- Fafone V
- Fair H
- Fairhurst S
- Fan X
- Fang Q
- Farinon S
- Farr B
- Farr WM
- Favata M
- Fays M
- Fehrmann H
- Fejer MM
- Fenyvesi E
- Ferrante I
- Ferreira EC
- Ferrini F
- Fidecaro F
- Fiore LD
- Fiori I
- Fiorucci D
- Fisher RP
- Flaminio R
- Fletcher M
- Fong H
- Fournier J-D
- Frasca S
- Frasconi F
- Frei Z
- Freise A
- Frey R
- Frey V
- Fritschel P
- Frolov VV
- Fulda P
- Fyffe M
- Gabbard HAG
- Gaebel S
- Gair JR
- Gammaitoni L
- Gaonkar SG
- Garufi F
- Gaur G
- Gehrels N
- Gemme G
- Geng P
- Genin E
- Gennai A
- George J
- Gergely L
- Germain V
- Ghosh A
- Ghosh A
- Ghosh S
- Giaime JA
- Giardina KD
- Giazotto A
- Gill K
- Giovanni MD
- Girolamo TD
- Glaefke A
- Goetz E
- Goetz R
- Gondan L
- Gonz'alez G
- Gopakumar A
- Gordon NA
- Gorodetsky ML
- Gossan SE
- Gosselin M
- Gouaty R
- Grado A
- Graef C
- Graff PB
- Granata M
- Grant A
- Gras S
- Gray C
- Greco G
- Green AC
- Groot P
- Grote H
- Grunewald S
- Guidi GM
- Guo X
- Gupta A
- Gupta MK
- Gushwa KE
- Gustafson EK
- Gustafson R
- Hacker JJ
- Hall BR
- Hall ED
- Hamilton H
- Hammond G
- Haney M
- Hanke MM
- Hanks J
- Hanna C
- Hannam MD
- Hanson J
- Hardwick T
- Haris K
- Harms J
- Harry GM
- Harry IW
- Hart MJ
- Hartman MT
- Haster C-J
- Haughian K
- Healy J
- Heidmann A
- Heijningen JVV
- Heintze MC
- Heitmann H
- Hello P
- Hemming G
- Hendry M
- Heng IS
- Hennig J
- Henry J
- Heptonstall AW
- Heurs M
- Hild S
- Hoak D
- Hofman D
- Holt K
- Holz DE
- Hopkins P
- Hough J
- Houston EA
- Howell EJ
- Hu YM
- Huang S
- Huerta EA
- Huet D
- Hughey B
- Husa S
- Huttner SH
- Huynh-Dinh T
- Indik N
- Ingram DR
- Inta R
- Isa HN
- Isac J-M
- Isi M
- Isogai T
- Iyer BR
- Izumi K
- Jacqmin T
- Jang H
- Jani K
- Jaranowski P
- Jawahar S
- Jian L
- Jim'enez-Forteza F
- Johnson WW
- Johnson-McDaniel N
- Jones DI
- Jones R
- Jonker RJG
- Jr MC
- Ju L
- K'ef'elian F
- Kalaghatgi CV
- Kalogera V
- Kandhasamy S
- Kang G
- Kanner JB
- Kapadia SJ
- Karki S
- Karvinen KS
- Kasprzack M
- Katsavounidis E
- Katzman W
- Kaufer S
- Kaur T
- Kawabe K
- Kehl MS
- Keitel D
- Kelley DB
- Kells W
- Kennedy R
- Key JS
- Khalili FY
- Khan I
- Khan S
- Khan Z
- Khazanov EA
- Kijbunchoo N
- Kim C
- Kim C-W
- Kim J
- Kim K
- Kim N
- Kim W
- Kim Y-M
- Kimbrell SJ
- King EJ
- King PJ
- Kissel JS
- Klein B
- Kleybolte L
- Klimenko S
- Koehlenbeck SM
- Koley S
- Kondrashov V
- Kontos A
- Korobko M
- Korth WZ
- Kowalska I
- Kozak DB
- Kr'olak A
- Kringel V
- Krishnan B
- Krueger C
- Kuehn G
- Kumar P
- Kumar R
- Kuo L
- Kutynia A
- Lackey BD
- Landry M
- Lange J
- Lantz B
- Lasky PD
- Laurentis MD
- Laxen M
- Lazzarini A
- Lazzaro C
- Leaci P
- Leavey S
- Lebigot EO
- Lee CH
- Lee HK
- Lee HM
- Lee K
- Lenon A
- Leonardi M
- Leong JR
- Leroy N
- Letendre N
- Levin Y
- Lewis JB
- Li TGF
- Libson A
- Lieto AD
- Littenberg TB
- Lockerbie NA
- Lombardi AL
- London LT
- Lord JE
- Lorenzini M
- Loriette V
- Lormand M
- Losurdo G
- Lough JD
- Lousto C
- Lundgren AP
- Lynch R
- M'arka S
- M'arka Z
- Ma Y
- Machenschalk B
- MacInnis M
- Macleod DM
- Magana-Sandoval F
- Magee RM
- Majorana E
- Maksimovic I
- Malvezzi V
- Man N
- Mandel I
- Mandic V
- Mangano V
- Mansell GL
- Manske M
- Mantovani M
- Marchesoni F
- Marion F
- Markosyan AS
- Maros E
- Martelli F
- Martellini L
- Martin IW
- Martynov DV
- Marx JN
- Mason K
- Masserot A
- Massinger TJ
- Masso-Reid M
- Mastrogiovanni S
- Matichard F
- Matone L
- Mavalvala N
- Mazumder N
- McCarthy R
- McClelland DE
- McCormick S
- McGuire SC
- McIntyre G
- McIver J
- McManus DJ
- McRae T
- McWilliams ST
- Meacher D
- Meadors GD
- Meidam J
- Melatos A
- Mendell G
- Mercer RA
- Merilh EL
- Merzougui M
- Meshkov S
- Messenger C
- Messick C
- Metzdorff R
- Meyers PM
- Mezzani F
- Miao H
- Michel C
- Middleton H
- Mikhailov EE
- Milano L
- Miller A
- Miller AL
- Miller BB
- Miller J
- Millhouse M
- Minenkov Y
- Ming J
- Mirshekari S
- Mishra C
- Mitra S
- Mitrofanov VP
- Mitselmakher G
- Mittleman R
- Moggi A
- Mohan M
- Mohapatra SRP
- Montani M
- Moore BC
- Moore CJ
- Moraru D
- Moreno G
- Morriss SR
- Mossavi K
- Mours B
- Mow-Lowry CM
- Mueller G
- Muir AW
- Mukherjee A
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- zny AZ
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- Zuraw SE
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2016
- Field of study
The first observational run of the Advanced LIGO detectors, from September 12, 2015 to January 19, 2016, saw the first detections of gravitational waves from binary black hole mergers. In this paper we present full results from a search for binary black hole merger signals with total masses up to 100M⊙ and detailed implications from our observations of these systems. Our search, based on general-relativistic models of gravitational wave signals from binary black hole systems, unambiguously identified two signals, GW150914 and GW151226, with a significance of greater than 5σ over the observing period. It also identified a third possible signal, LVT151012, with substantially lower significance, which has a 87% probability of being of astrophysical origin. We provide detailed estimates of the parameters of the observed systems. Both GW150914 and GW151226 provide an unprecedented opportunity to study the two-body motion of a compact-object binary in the large velocity, highly nonlinear regime. We do not observe any deviations from general relativity, and place improved empirical bounds on several high-order post-Newtonian coefficients. From our observations we infer stellar-mass binary black hole merger rates lying in the range 9−240Gpc−3yr−1. These observations are beginning to inform astrophysical predictions of binary black hole formation rates, and indicate that future observing runs of the Advanced detector network will yield many more gravitational wave detections
Search for gravitational waves associated with gamma-ray bursts detected by Fermi and Swift during the LIGO–Virgo run O3b
- Author
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- Yelikar AB
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- Yuzurihara H
- Zadrozny A
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- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2022
- Field of study
We search for gravitational-wave signals associated with gamma-ray bursts (GRBs) detected by the Fermi and Swift satellites during the second half of the third observing run of Advanced LIGO and Advanced Virgo (2019 November 1 15:00 UTC–2020 March 27 17:00 UTC). We conduct two independent searches: a generic gravitational-wave transients search to analyze 86 GRBs and an analysis to target binary mergers with at least one neutron star as short GRB progenitors for 17 events. We find no significant evidence for gravitational-wave signals associated with any of these GRBs. A weighted binomial test of the combined results finds no evidence for subthreshold gravitational-wave signals associated with this GRB ensemble either. We use several source types and signal morphologies during the searches, resulting in lower bounds on the estimated distance to each GRB. Finally, we constrain the population of low-luminosity short GRBs using results from the first to the third observing runs of Advanced LIGO and Advanced Virgo. The resulting population is in accordance with the local binary neutron star merger rate
Localization and broadband follow-up of the gravitational-wave transient GW150914
- Author
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- Abbott FTBOOTESCTMC
- Abdalla FB
- Abe FTINF
- Ackermann FTFGBMCM
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- Publication venue
- IOP PUBLISHING LTD
- Publication date
- Field of study
A gravitational-wave transient was identified in data recorded by the Advanced LIGO detectors on 2015 September 14. The event candidate, initially designated G184098 and later given the name GW150914, is described in detail elsewhere. By prior arrangement, preliminary estimates of the time, significance, and sky location of the event were shared with 63 teams of observers covering radio, optical, near-infrared, X-ray, and gamma-ray wavelengths with ground- and space-based facilities. In this Letter we describe the low-latency analysis of the gravitational wave data and present the sky localization of the first observed compact binary merger. We summarize the follow-up observations reported by 25 teams via private Gamma-ray Coordinates Network Circulars, giving an overview of the participating facilities, the gravitational wave sky localization coverage, the timeline and depth of the observations. As this event turned out to be a binary black hole merger, there is little expectation of a detectable electromagnetic signature. Nevertheless, this first broadband campaign to search for a counterpart of an Advanced LIGO source represents a milestone and highlights the broad capabilities of the transient astronomy community and the observing strategies that have been developed to pursue neutron star binary merger events. Detailed investigations of the electromagnetic data and results of the electromagnetic follow-up campaign will be disseminated in the papers of the individual teams
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