66 research outputs found
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
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- Ackley K
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- Agathos M
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- Aglietta M
- Agliozzo C
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- Aguilar JA
- Aharonian F
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- Ahrens M
- Aiello L
- Ain A
- Ajith P
- Akras S
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- Allen G
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- Allison JR
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- Alvarez JD
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- Arceo R
- Ardid M
- Areeda JS
- Aresu G
- Argan A
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- Array LWA Long Wavelength
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- Asakura Y
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- Peiffer P
- Peixoto CJ Todero
- Pekeur NW
- Pekowsky L
- Pelayo R
- Pele A
- Pellegrino C
- Pelletier G
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- Penacchioni AV
- Penn S
- Penuela T
- Pepper JA
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- Perennes C
- Perez CJ
- Perez-Perez EG
- Perley DA
- Perlin M
- Perreca A
- Perri LM
- Perri M
- Perrina C
- Perrodin D
- Perrone L
- Pescalli A
- Pesce-Rollins M
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- Petrera S
- Petrucci P-O
- Peyaud B
- Pfeiffer HP
- Phelps M
- Phlhofer G
- Phuntsok J
- Pian E
- Piano G
- Piattelli P
- Piccinni OJ
- Pichot M
- Picozza P
- Piel Q
- Pieloth D
- Piergiovanni F
- Pierog T
- Pierro V
- Pignata G
- Pike S
- Pilia M
- Pillant G
- Pimenta M
- Pinard L
- Pinat E
- Pinto IM
- Piotrowski LW
- Piran T
- Piran T
- Piranomonte S
- Pirello M
- Piro AL
- Piro L
- Piron F
- Pirronello V
- Pisanu T
- Pita S
- Pitkin M
- Pittori C
- Placco VM
- Platino M
- Plazas AA
- Plum M
- Podesta F
- Podesta RC
- Podsiadlowski P
- Poe M
- Poggiani R
- Poh J
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- Pollmann A Obertacke
- Poolakkil S
- Poon H
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- Popolizio P
- Poppi S
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- Porter EK
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- Possenti A
- Post A
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- Powell J
- Pozanenko AS
- Poznanski D
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- Prado RR
- Prasad J
- Pratt JWW
- Pratten G
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- Prestegard T
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- Price PB
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- Principe G
- Principe M
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- Privitera P
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- Prochaska JX
- Prodi GA
- Prokhorov D
- Prokhorov LG
- Prokoph H
- Prouza M
- Prrer M
- Przybylski GT
- Pulone L
- Pumo ML
- Punch M
- Puncken O
- Punturo M
- Puppo P
- Qi H
- Qi H
- Qu JL
- Quataert E
- Quel EJ
- Querchfeld S
- Querel R
- Quetschke V
- Quimby RM
- Quinn L
- Quinn S
- Quinones C
- Quintero EA
- Quirrenbach A
- Quispe ID Vergara
- Quitzow-James R
- Raab C
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- Rabeling DS
- Rabus M
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- Raffai P
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- Raja S
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- Rameez M
- Ramirez KE
- Ramirez-Ruiz E
- Ramos-Buades A
- Ramos-Pollan R
- Rana J
- Rando R
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- Rappoldi A
- RATIR RIMAS
- Rau A
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- Rauth R
- Ravignani D
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- Raymond V
- Razza A
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- Razzaque S
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- Rdiger A
- Rea IC
- Read J
- Rebolo R
- Regimbau T
- Rei L
- Reichart DE
- Reid S
- Reimann R
- Reimer A
- Reimer A
- Reimer O
- Reimer O
- Reitze DH
- Relethford B
- Relich M
- Ren W
- Ren Z
- Renaud M
- Renzi V
- Reposeur T
- Resconi E
- Resmi L
- Rest A
- Reva IV
- Reyes R De Los
- Reyes SD
- Reynolds T
- Rho CD
- Rhode W
- Ribeiro T
- Ricci F
- Ricci R
- Ricciarini S
- Riccobene G
- Richman M
- Ricker PM
- Ridden-Harper R
- Ridky J
- Rieger F
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- Riehn F
- Righini S
- Riguccini L
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- Rinchiuso L
- Rios-Lopez E
- Risse M
- Ristori P
- Rivera A Ramirez
- Riviere C
- Rizi V
- Rizzo M
- Roberts OJ
- Robertson NA
- Robertson S
- Robie R
- Robinet F
- Rocchi A
- Rochester LS
- Rodi J
- Rodriguez H
- Rojas D Avila
- Rojas-Bravo C
- Rojo J Rodriguez
- Rol E
- Rolland L
- Rollins JG
- Roma VJ
- Romano R
- Romel CL
- Romer AK
- Romero M Dominguez
- Romie JH
- Romoli C
- Roncoroni MJ
- Rongen M
- Roodman A
- Roques J-P
- Rosa-Gonzlez D
- Rosell A Carnero
- Rosenberg M
- Rosetti S
- Rosinska D
- Ross MP
- Rossi A
- Rosswog S
- Rosswog S
- Roth M
- Rott C
- Roulet E
- Rovero AC
- Rowan S
- Rowell G
- Rowlinson A
- Rowlinson A
- Roy R
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- Rudak B
- Ruehl P
- Ruggi P
- Ruhe T
- Ruiter AJ
- Ruiz R Gracia
- Ruiz-Velasco E
- Rulten CB
- Rumyantsev VV
- Rusu F
- Rutins G
- Ryan K
- Rybicki KA
- Ryckbosch D
- Rykoff ES
- Rysewyk D
- Saba A
- Sachdev S
- Sadecki T
- Sadeghian L
- Sadler EM
- Sadler EM
- Saffe C
- Saffi SJ
- Saftoiu A
- Sahakian V
- Sai N
- Saito S
- Saito T
- Saito Y
- Sakamaki A
- Sakamoto T
- Sakellariadou M
- Sako M
- Sako S
- Salafia OS
- Salamida F
- Salazar H
- Salazar H
- Salconi L
- Saldaa M
- Saleem M
- Saleh A
- Salemi F
- Salina G
- Salmon L
- Salvadori I
- Salvaterra R
- Samajdar A
- Sammut L
- Sampedro L
- Sampson LM
- Samtleben DFE
- Sanchez B
- Sanchez DA
- Sanchez E
- Sanchez EJ
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- Sanchez LE
- Sanchez-Losa A
- Sanchez-Lucas P
- Sanchez-Ramirez R
- Sanchis-Gual N
- Sand DJ
- Sandberg V
- Sanders JR
- Sandoval A
- Sandrock A
- Sandroos J
- Sanguineti M
- Sansom EK
- Santander M
- Santangelo A
- Santos E
- Santos EM
- Sapienza P
- Sarazin F
- Sarkar S
- Sarkar S
- Sarmento R
- Sarmiento-Cano C
- Sasaki M
- Sasaki R
- Sassolas B
- Satalecka K
- Sathyaprakash BS
- Sato R
- Saulson PR
- Sauseda M
- Sauter O
- Savage RL
- Savchenko V
- Sawadsky A
- Sbarufatti B
- Scalzo RA
- Scarpine V
- Schady P
- Schale P
- Schauer M
- Scheel M
- Scherini V
- Scheuer J
- Schieler H
- Schimp M
- Schindler R
- Schipani P
- Schlegel DJ
- Schlickeiser R
- Schlunder P
- Schmalz SE
- Schmidt BP
- Schmidt D
- Schmidt J
- Schmidt P
- Schmidt T
- Schnabel R
- Schneider A
- Schneider M
- Schneiter M
- Schoenell W
- Schoenen S
- Schofield RMS
- Scholten O
- Schonbeck A
- Schoneberg S
- Schoorlemmer H
- Schovnek P
- Schreiber E
- Schroder FG
- Schroder S
- Schroder SL
- Schssler F
- Schubnell M
- Schuette D
- Schulte BW
- Schultz ASB
- Schulz A
- Schulz A
- Schulze S
- Schumacher J
- Schumacher L
- Schutz BF
- Schwalbe SG
- Schwanke U
- Schwemmer S
- Schweyer T
- Sciutto SJ
- Scolnic D
- Scott J
- Scott SM
- Secco LF
- Seckel D
- Seglar-Arroyo M
- Segreto A
- Seidel E
- Seitenzahl IR
- Sekiguchi Y
- Sellers D
- Selsing J
- Sengupta AS
- Sentenac D
- Sequino V
- Sergeev A
- Sergienko Yu P
- Serino M
- Serra G
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- Serrau M
- Settimo M
- Seunarine S
- Sevilla-Noarbe I
- Seyffert AS
- Sgro C
- Shaddock DA
- Shadkam A
- Shaffer TJ
- Shafi N
- Shah AA
- Shahriar MS
- Shaner MB
- Shang Z
- Shannon RM
- Shao L
- Shapiro B
- Shappee BJ
- Shara MM
- Sharma I
- Sharp RG
- Shawhan P
- Sheldon E
- Shellard RC
- Sheperd A
- Shidatsu M
- Shilon I
- Shimizu Y
- Shimomukai R
- Shingles LJ
- Shiningayamwe K
- Shoemaker DH
- Shoemaker DM
- Shulevski A
- Siebert MR
- Siegel MH
- Sieger C
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- Siemens X
- Sieniawska M
- Sigg D
- Sigl G
- Silli G
- Silva AD
- Sim SA
- Simon JD
- Simonetti JH
- Simoni R
- Singer LP
- Singh A
- Singhal A
- Sinnis G
- Sintes AM
- Siskind EJ
- Slagmolen BJJ
- Slzer T
- Smartt SJ
- Smida R
- Smirnov OM
- Smith AJ
- Smith B
- Smith JR
- Smith KW
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- Smith M
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- Snow GR
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- Sobreira F
- Sodre L
- Soedingrekso J
- Soffitta P
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- Sollerman J
- Sollerman J
- Somala S
- Sommers P
- Son EJ
- Song LM
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- Sonnenberg JA
- Sonntag S
- Sorazu B
- Soriano JF
- Sorrentino F
- Souradeep T
- Spada F
- Spandre G
- Spanier F
- Spencer AP
- Spera M
- Spiczak GM
- Spiering C
- Spir-Jacob M
- Springer RW
- Spurio M
- Squartini R
- Srivastava AK
- Staats K
- Stachurska J
- Staff J
- Stagni M
- Stalder B
- Staley A
- Stamatikos M
- Stamerra A
- Stanbro M
- Stanca D
- Stanev T
- Stanic S
- Stanway ER
- Starck M
- Starling RLC
- Stasielak J
- Stasik A
- Stassi P
- Stawarz L
- Stebbins A
- Steeghs DTH
- Steele I
- Steele K
- Steenkamp R
- Stegmann C
- Steinke M
- Steinlechner J
- Steinlechner S
- Steinmeyer D
- Stella L
- Steppa C
- Stettner J
- Steuer A
- Stevenson SP
- Stewart AJ
- Stezelberger T
- Stokstad RG
- Stolarczyk Th
- Stolpovskiy M
- Stone R
- Stops DJ
- Stosl A
- Strafella F
- Strain KA
- Stratta G
- Streich A
- Strigin SE
- Strotjohann NL
- Strunk A
- Stubbs CW
- Sturani R
- Stuttard T
- Stuver AL
- Suarez F
- Suarez-Duran M
- Suchyta E
- Sudholz T
- Sugawara Y
- Sugita S
- Sugizaki M
- Sullivan GW
- Sullivan M
- Sumi T
- Summerscales TZ
- Sun L
- Sun L
- Sun T
- Sunil S
- Suntzeff NB
- Sunyaev R
- Suomijarvi T
- Supanitsky AD
- Supik J
- Surajbali P
- Surcis G
- Suresh J
- Sushch I
- Suson DJ
- Sutherland M
- Sutton PJ
- Svinkin DS
- Swain J
- Swanson MEC
- Swinkels BL
- Szadkowski Z
- Szczepanczyk MJ
- Szegedi H
- Szomoru A
- Taboada A
- Taboada I
- Taborda OA
- Tacca M
- Tachibana Y
- Taddia F
- Tagliaferri G
- Tait SC
- Taiuti M
- Tajitsu A
- Takahashi I
- Takahashi J
- Takahashi M
- Takahashi T
- Takao Y
- Takayama M
- Talbot C
- Talukder D
- Tamura T
- Tamura Y
- Tan Y
- Tanaka I
- Tanaka M
- Tanaka Y
- Tanimoto A
- Tanner DB
- Tanvir NR
- Tao C
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- Tao WH
- Taracchini A
- Tarle G
- Tartaglia L
- Tasson JD
- Tatar J
- Taubenberger S
- Tavani M
- Tavernet J-P
- Tavernier T
- Tayalati Y
- Taylor AM
- Taylor GB
- Taylor JA
- Taylor R
- Team AGILE
- Team Euro VLBI
- Team MAXI
- Team The 1M2H
- Telescope ATCA Australia
- Telescope Fermi Large Area
- Telescope Nordic Optical
- Tello JC
- Telluride AstroSat Cadmium Zinc
- Tenholt F
- Ter Veen S
- Ter-Antonyan S
- Terai T
- Terliuk A
- Terreran G
- Terrier R
- Tesic G
- Testa V
- Tewari SV
- Thayer JB
- Thayer JG
- Theeg T
- Thene CC
- Thierry P
- Thierry P
- Thies F
- Thomas EG
- Thomas M
- Thomas P
- Thomas RC
- Thompson DJ
- Thorne KA
- Thorne KS
- Thrane E
- Tibaldo L
- Tibaldo L
- Tibolla O
- Tilav S
- Timmermans C
- Tingay SJ
- Tiwari S
- Tiwari V
- Tiziani D
- Tjus J Becker
- Tjus J Becker
- Tlatov AG
- Tluczykont M
- Toale PA
- Tobin MN
- Tohuvavohu A
- Tokmakov KV
- Toland K
- Tollefson K
- Toma K
- Tomankova L
- Tomasella L
- Tome B
- Tomida H
- Tominaga N
- Tonelli M
- Tonnis C
- Tonry J
- Torii S
- Tornasi Z
- Tornatore M
- Torres DF
- Torres I
- Torres-Flores S
- Torres-Forn A
- Torresi E
- Torrie CI
- Toscano S
- Tosi D
- Towner MC
- Toyr D
- Tpai M
- Travasso F
- Travnicek P
- Traylor G
- Trichard C
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- Trinastic J
- Tringali MC
- Trini M
- Tristram PJ
- Trois A
- Troja E
- Troja E
- Trott CM
- Trovato A
- Troxel MA
- Trozzo L
- Tsai J
- Tsang KW
- Tse M
- Tselengidou M
- Tsirou M
- Tso R
- Tsuboi Y
- Tsuji N
- Tsukada L
- Tsuna D
- Tsunemi H
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- Tungalag N
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- Turpin D
- Turpin D
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- Ty B
- Tyurina NV
- Ubertini P
- Uchiyama Y
- Ueda Y
- Uemura M
- Ueno K
- Ueno S
- Ugolini D
- Ukwatta TN
- Ulaczyk K
- Ulanov MV
- Ulloa N
- Ulrich R
- Unger E
- Unger M
- Univ Chandra Team McGill
- Univ Texas Tech
- Universe High Time Resolution
- Unnikrishnan CS
- Urban AL
- Urban M
- Ursi A
- Usman SA
- Usner M
- Utsumi Y
- Vacca V
- Vadawale SV
- Vahlbruch H
- Vaisanen P
- Vajente G
- Valdes G
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- Valio I
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- Van der Walt DJ
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- Vander-Hyde DC
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- Vergani D
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- Verkindt D
- Verrecchia F
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- Vibhute A
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- Viets AD
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- Vink J
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- Vitale PF Gomez
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- Vivolo D
- Vizzoca A
- Vladimirov VV
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- Vo T
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- Vogel E
- Voisin F
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- Vorobiov S
- Vorvick C
- Vos J
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- Wainscoat RJ
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- Walz D
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- Wave GRAWITA GRAvitational
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- Weiland H
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- Wessel EK
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- Wiebusch CH
- Wiedenski M
- Wiencke L
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- Wiersema K
- Wierzcholska A
- Wijers RAMJ
- Wijers RAMJ
- Wilczynski H
- Wilken D
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- Williams PKG
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- Wilms J
- Wilson-Hodge CA
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- Worden J
- Woschnagg K
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- Wrochna G
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- Wundheiler B
- Wyrzykowski L
- Wysocki DM
- Xiao GC
- Xiao S
- Xiong SL
- Xu D
- Xu DL
- Xu H
- Xu XW
- Xu Y
- Xu Y
- Xu YP
- Yamada S
- Yamaguchi MS
- Yamamoto H
- Yamaoka K
- Yamaoka K
- Yamauchi M
- Yan L
- Yan LL
- Yancey CC
- Yanez JP
- Yang J
- Yang J
- Yang JW
- Yang L
- Yang L
- Yang R
- Yang S
- Yang S
- Yang YJ
- Yanny B
- Yap MJ
- Yapici T
- Yaron O
- Yasuda N
- Yatabe F
- Yatsu Y
- Yazback M
- Yock PC
- Yodh G
- Yodh GB
- Yoneyama T
- Yoon Y
- Yoshida A
- Yoshida M
- Yoshida S
- Yoshii T
- Young DR
- Younk PW
- Yu Hang
- Yu Haocun
- Yu P-C
- Yuan T
- Yuan X
- Yurkov VV
- Yushkov A
- Yvert M
- Zaborov D
- Zacharias M
- Zadrozny A
- Zadrozny A
- Zaharijas G
- Zaltzman M
- Zanin R
- Zanolin M
- Zaremba M
- Zarnecki AF
- Zas E
- Zavrtanik D
- Zavrtanik M
- Zdziarski AA
- Zech A
- Zefi F
- Zelenova T
- Zendri J-P
- Zenko T
- Zenteno A
- Zepeda A
- Zertuche L Magaa
- Zevin M
- Zhang AM
- Zhang B-B
- Zhang C
- Zhang CL
- Zhang CM
- Zhang F
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- Zhang HM
- Zhang J
- Zhang L
- Zhang M
- Zhang Q
- Zhang S
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- Zhang T
- Zhang W
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- Zhang Y
- Zhang Y
- Zhang Y
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- Zhang YF
- Zhang YJ
- Zhang Z
- Zhang ZL
- Zhao C
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- Zhao JL
- Zhao W
- Zhao XF
- Zheng SJ
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- Zhu SJ
- Zhu XJ
- Zhu Y
- Zhu YX
- 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
GWTC-2.1: Deep extended catalog of compact binary coalescences observed by LIGO and Virgo during the first half of the third observing run
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- Zhu XJ
- Zimmerman AB
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- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 15/01/2024
- Field of study
The second Gravitational-Wave Transient Catalog, GWTC-2, reported on 39 compact binary coalescences observed by the Advanced LIGO and Advanced Virgo detectors between 1 April 2019 15 ∶ 00 UTC and 1 October 2019 15 ∶ 00 UTC. Here, we present GWTC-2.1, which reports on a deeper list of candidate events observed over the same period. We analyze the final version of the strain data over this period with improved calibration and better subtraction of excess noise, which has been publicly released. We employ three matched-filter search pipelines for candidate identification, and estimate the probability of astrophysical origin for each candidate event. While GWTC-2 used a false alarm rate threshold of 2 per year, we include in GWTC-2.1, 1201 candidates that pass a false alarm rate threshold of 2 per day. We calculate the source properties of a subset of 44 high-significance candidates that have a probability of astrophysical origin greater than 0.5. Of these candidates, 36 have been reported in GWTC-2. We also calculate updated source properties for all binary black hole events previously reported in GWTC-1. If the eight additional high-significance candidates presented here are astrophysical, the mass range of events that are unambiguously identified as binary black holes (both objects ≥ 3 M⊙ ) is increased compared to GWTC-2, with total masses from ∼ 14 M ⊙ for GW190924_021846 to ∼ 182 M⊙ for GW190426_190642. Source properties calculated using our default prior suggest that the primary components of two new candidate events (GW190403_051519 and GW190426_190642) fall in the mass gap predicted by pair-instability supernova theory. We also expand the population of binaries with significantly asymmetric mass ratios reported in GWTC-2 by an additional two events (the mass ratio is less than 0.65 and 0.44 at 90% probability for GW190403_051519 and GW190917_114630 respectively), and find that two of the eight new events have effective inspiral spins χeff > 0 (at 90% credibility), while no binary is consistent with χeff < 0 at the same significance. We provide updated estimates for rates of binary black hole and binary neutron star coalescence in the local Universe
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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- 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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- 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
All-sky search for continuous gravitational waves from isolated neutron stars in the early O3 LIGO data
- Author
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- Zweizig J
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 15/10/2021
- Field of study
We report on an all-sky search for continuous gravitational waves in the frequency band 20-2000 Hz and with a frequency time derivative in the range of [-1.0,+0.1]×10-8 Hz/s. Such a signal could be produced by a nearby, spinning and slightly nonaxisymmetric isolated neutron star in our Galaxy. This search uses the LIGO data from the first six months of Advanced LIGO's and Advanced Virgo's third observational run, O3. No periodic gravitational wave signals are observed, and 95% confidence-level (C.L.) frequentist upper limits are placed on their strengths. The lowest upper limits on worst-case (linearly polarized) strain amplitude h0 are ∼1.7×10-25 near 200 Hz. For a circularly polarized source (most favorable orientation), the lowest upper limits are ∼6.3×10-26. These strict frequentist upper limits refer to all sky locations and the entire range of frequency derivative values. For a population-averaged ensemble of sky locations and stellar orientations, the lowest 95% C.L. upper limits on the strain amplitude are ∼1.4×10-25. These upper limits improve upon our previously published all-sky results, with the greatest improvement (factor of ∼2) seen at higher frequencies, in part because quantum squeezing has dramatically improved the detector noise level relative to the second observational run, O2. These limits are the most constraining to date over most of the parameter space searched
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A
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- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17, the gravitational-wave event GW170817 was observed by the Advanced LIGO and Virgo detectors, and the gamma-ray burst (GRB) GRB 170817A was observed independently by the Fermi Gamma-ray Burst Monitor, and the Anti-Coincidence Shield for the Spectrometer for the International Gamma-Ray Astrophysics Laboratory. The probability of the near-simultaneous temporal and spatial observation of GRB 170817A and GW170817 occurring by chance is 5.0×10−8. We therefore confirm binary neutron star mergers as a progenitor of short GRBs. The association of GW170817 and GRB 170817A provides new insight into fundamental physics and the origin of short GRBs. We use the observed time delay of (+1.74±0.05)s between GRB 170817A and GW170817 to: (i) constrain the difference between the speed of gravity and the speed of light to be between −3×10−15 and +7×10−16 times the speed of light, (ii) place new bounds on the violation of Lorentz invariance, (iii) present a new test of the equivalence principle by constraining the Shapiro delay between gravitational and electromagnetic radiation. We also use the time delay to constrain the size and bulk Lorentz factor of the region emitting the gamma-rays. GRB 170817A is the closest short GRB with a known distance, but is between 2 and 6 orders of magnitude less energetic than other bursts with measured redshift. A new generation of gamma-ray detectors, and subthreshold searches in existing detectors, will be essential to detect similar short bursts at greater distances. Finally, we predict a joint detection rate for the Fermi Gamma-ray Burst Monitor and the Advanced LIGO and Virgo detectors of 0.1-1.4 per year during the 2018-2019 observing run and 0.3-1.7 per year at design sensitivity
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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- Zhu Z-H
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 03/06/2022
- 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, {\tt PyStoch}, enable us to
perform the radiometer map-making at every frequency bin. We perform the search
at 3072 {\tt{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)×10−24. 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
All-sky search for gravitational-wave bursts in the second joint LIGO-Virgo run
- Author
- Abadie J
- Abbott BP
- Abbott R
- Abbott TD
- Abernathy M
- Accadia T
- Acernese F
- Adams C
- Adhikari R
- Affeldt C
- Agathos M
- Agatsuma K
- Ajith P
- Allen B
- Amariutei D
- Anderson SB
- Anderson WG
- Arai K
- Arain MA
- Araya MC
- Aston SM
- Astone P
- Atkinson D
- Aufmuth P
- Aulbert C
- Aylott BE
- Babak S
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- Ballardin G
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- Barayoga JCB
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- Barone F
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- Barrera C. Oropeza
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- Barsuglia M
- Barton MA
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- Bassiri R
- Bastarrika M
- Basti A
- Batch J
- Bauchrowitz J
- Bauer TS
- Bebronne M
- Beck D
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- Vitale S
- Vocca H
- Vorvick C
- Vyatchanin SP
- Wade A
- Wade L
- Wade M
- Waldman SJ
- Wallace L
- Wan Y
- Wang M
- Wang X
- Wang Z
- Wanner A
- Ward RL
- Was M
- Weinert M
- Weinstein AJ
- Weiss R
- Wen L
- Wessels P
- West M
- Westphal T
- Wette K
- Whelan JT
- Whitcomb SE
- White DJ
- Whiting BF
- Wilkinson C
- Willems PA
- Williams L
- Williams R
- Willke B
- Winkelmann L
- Winkler W
- Wipf CC
- Wiseman AG
- Wittel H
- Woan G
- Wooley R
- Worden J
- Yakushin I
- Yamamoto H
- Yamamoto K
- Yancey CC
- Yang H
- Yeaton-Massey D
- Yeaton-Massey D
- Yoshida S
- Yoshida S
- Yu P
- Yvert M
- Yvert M
- Zadrozny A
- Zadrozny A
- Zanolin M
- Zanolin M
- Zendri JP
- Zendri JP
- Zhang F
- Zhang F
- Zhang L
- Zhang L
- Zhang W
- Zhao C
- Zhao C
- Zotov N
- Zotov N
- Zucker ME
- Zucker ME
- Zweizig Jang H
- Zweizig Jkiforov A.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We present results from a search for gravitational-wave bursts in the data
collected by the LIGO and Virgo detectors between July 7, 2009 and October 20,
2010: data are analyzed when at least two of the three LIGO-Virgo detectors are
in coincident operation, with a total observation time of 207 days. The
analysis searches for transients of duration < 1 s over the frequency band
64-5000 Hz, without other assumptions on the signal waveform, polarization,
direction or occurrence time. All identified events are consistent with the
expected accidental background. We set frequentist upper limits on the rate of
gravitational-wave bursts by combining this search with the previous LIGO-Virgo
search on the data collected between November 2005 and October 2007. The upper
limit on the rate of strong gravitational-wave bursts at the Earth is 1.3
events per year at 90% confidence. We also present upper limits on source rate
density per year and Mpc^3 for sample populations of standard-candle sources.
As in the previous joint run, typical sensitivities of the search in terms of
the root-sum-squared strain amplitude for these waveforms lie in the range 5
10^-22 Hz^-1/2 to 1 10^-20 Hz^-1/2. The combination of the two joint runs
entails the most sensitive all-sky search for generic gravitational-wave bursts
and synthesizes the results achieved by the initial generation of
interferometric detectors.Comment: 15 pages, 7 figures: data for plots and archived public version at
https://dcc.ligo.org/cgi-bin/DocDB/ShowDocument?docid=70814&version=19, see
also the public announcement at
http://www.ligo.org/science/Publication-S6BurstAllSky
Recommended from our members
Prospects for Observing and Localizing Gravitational-Wave Transients with Advanced LIGO and Advanced Virgo.
- Author
- 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
- Ain A
- Ajith P
- Allen B
- Allocca A
- Altin PA
- Amariutei DV
- Anderson SB
- Anderson WG
- Arai K
- Araya MC
- Arceneaux CC
- Areeda JS
- Arnaud N
- Arun KG
- Ashton G
- Ast M
- Aston SM
- Astone P
- Aufmuth P
- Aulbert C
- Babak S
- 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
- Behnke B
- Bejger M
- Belczynski C
- Bell AS
- Bell CJ
- Berger BK
- Bergman J
- Bergmann G
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Bhagwat S
- Bhandare R
- Bilenko IA
- Billingsley G
- Birch J
- Birney R
- Biscans S
- Bisht A
- Bitossi M
- Biwer C
- Bizouard MA
- Blackburn JK
- Blair CD
- Blair D
- Blair RM
- Bloemen S
- Bock O
- Bodiya TP
- Boer M
- Bogaert G
- Bogan C
- Bohe A
- Bojtos P
- Bond C
- Bondu F
- Bonnand R
- Bork R
- Boschi V
- Bose S
- Bozzi A
- Bradaschia C
- Brady PR
- Braginsky VB
- Branchesi M
- Brau JE
- Briant T
- Brillet A
- Brinkmann M
- Brisson V
- Brockill P
- Brooks AF
- Brown DA
- Brown DD
- Brown NM
- Buchanan CC
- Buikema A
- Bulik T
- Bulten HJ
- Buonanno A
- Buskulic D
- Buy C
- Byer RL
- Cadonati L
- Cagnoli G
- Cahillane C
- Calderón Bustillo J
- Callister T
- Calloni E
- Camp JB
- Cannon KC
- Cao J
- Capano CD
- Capocasa E
- Carbognani F
- Caride S
- Casanueva Diaz J
- Casentini C
- Castro JM Gonzalez
- Caudill S
- Cavaglià M
- Cavalier F
- Cavalieri R
- Cella G
- Cepeda C
- Cerboni Baiardi L
- Cerretani G
- Cesarini E
- Chakraborty R
- Chalermsongsak T
- Chamberlin SJ
- Chan M
- Chao S
- Charlton P
- Chassande-Mottin E
- 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
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- Clark JA
- Cleva F
- Coccia E
- Cohadon P-F
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- Collette CG
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- Conte A
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- Cook D
- Corbitt TR
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- Corsi A
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- Costa CA
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- Drever RWP
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- Jiménez-Forteza F
- Johnson WW
- Jones DI
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- Jonker RJG
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- Kang G
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- Katzman W
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- Kawazoe F
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- Kondrashov V
- Kontos A
- Korobko M
- Korth WZ
- Kowalska I
- Kozak DB
- Kringel V
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- LIGO Scientific Collaboration
- Littenberg TB
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- McClelland DE
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- Meadors GD
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- Merzougui M
- Meshkov S
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- Middleton H
- Mikhailov EE
- Milano L
- 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
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- Mueller G
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- Mullavey A
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- Murray PG
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- Márka Z
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- Naticchioni L
- Nayak RK
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- Nedkova K
- Nelemans G
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- Nissanke S
- Nitz A
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- Nolting D
- Normandin MEN
- Nuttall LK
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- Oelker E
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- Oh SH
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- Oram RJ
- Ott CD
- Ottaway DJ
- Ottens RS
- Overmier H
- Owen BJ
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- Pai SA
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- Palamos JR
- Palashov O
- Palomba C
- Pan H
- Pankow C
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- Paoletti F
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- Pascucci D
- Pasqualetti A
- Passaquieti R
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- Pedurand R
- Pekowsky L
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- Premachandra SS
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- Price LR
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- Prodi GA
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- Punturo M
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- Qin J
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- Quintero EA
- Quitzow-James R
- Raab FJ
- Rabeling DS
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- Raffai P
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- Romano JD
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- Romie JH
- Rosińska D
- Rowan S
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- Sadecki T
- Sadeghian L
- Saleem M
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- Samajdar A
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- Sandberg V
- Sandeen B
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- Saulson PR
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- Savage RL
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- Schofield RMS
- Schreiber E
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- Sequino V
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- Shao Z
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- Shawhan P
- Sheperd A
- Shoemaker DH
- Shoemaker DM
- Siellez K
- Siemens X
- Sigg D
- Silva AD
- Simakov D
- Singer A
- Singer LP
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- Singh R
- Sintes AM
- Slagmolen BJJ
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- Smith RJE
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- Sorrentino F
- Souradeep T
- Srivastava AK
- Staley A
- Steinke M
- Steinlechner J
- Steinlechner S
- Steinmeyer D
- Stephens BC
- Stone R
- Strain KA
- Straniero N
- Stratta G
- Strauss NA
- Strigin S
- Sturani R
- Stuver AL
- Summerscales TZ
- Sun L
- Sutton PJ
- Swinkels BL
- Szczepanczyk MJ
- Tacca M
- Talukder D
- Tanner DB
- Tarabrin SP
- Taracchini A
- Taylor R
- Theeg T
- Thirugnanasambandam MP
- Thomas EG
- Thomas M
- Thomas P
- Thorne KA
- Thorne KS
- Thrane E
- Tiwari S
- Tiwari V
- Tokmakov KV
- Tomlinson C
- Tonelli M
- Torres CV
- Torrie CI
- Travasso F
- Traylor G
- Trifirò D
- Tringali MC
- Trozzo L
- Tse M
- Turconi M
- Tuyenbayev D
- Tápai M
- Töyrä D
- Ugolini D
- Unnikrishnan CS
- Urban AL
- Usman SA
- Vahlbruch H
- Vajente G
- Valdes G
- van Bakel N
- van Beuzekom M
- van den Brand JFJ
- van den Broeck C
- van der Schaaf L
- van der Sluys MV
- van Heijningen JV
- van Veggel AA
- Vander-Hyde DC
- Vardaro M
- Vass S
- Vasúth M
- Vaulin R
- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Venkateswara K
- Verkindt D
- Vetrano F
- Viceré A
- Vinciguerra S
- Vine DJ
- Vinet J-Y
- Virgo Collaboration
- Vitale S
- Vo T
- Vocca H
- Vorvick C
- Vousden WD
- Vyatchanin SP
- Wade AR
- Wade LE
- Wade M
- Walker M
- Wallace L
- Walsh S
- Wang G
- Wang H
- Wang M
- Wang X
- Wang Y
- Ward RL
- Warner J
- Was M
- Weaver B
- Wei L-W
- Weinert M
- Weinstein AJ
- Weiss R
- Welborn T
- Wen L
- Westphal T
- Wette K
- Weßels P
- Whelan JT
- White DJ
- Whiting BF
- Williams RD
- Williamson AR
- Willis JL
- Willke B
- Wimmer MH
- Winkler W
- Wipf CC
- Wittel H
- Woan G
- Worden J
- Wright JL
- Wu G
- Yablon J
- Yam W
- Yamamoto H
- Yancey CC
- Yap MJ
- Yu H
- Yvert M
- Zadrożny A
- Zangrando L
- Zanolin M
- Zendri J-P
- Zevin M
- Zhang F
- Zhang L
- Zhang M
- Zhang Y
- Zhao C
- Zhou M
- Zhou Z
- Zhu XJ
- Zucker ME
- Zuraw SE
- Zweizig J
- Publication venue
- Living Rev Relativ
- Publication date
- 28/09/2021
- Field of study
We present a possible observing scenario for the Advanced LIGO and Advanced Virgo gravitational-wave detectors over the next decade, with the intention of providing information to the astronomy community to facilitate planning for multi-messenger astronomy with gravitational waves. We determine the expected sensitivity of the network to transient gravitational-wave signals, and study the capability of the network to determine the sky location of the source. We report our findings for gravitational-wave transients, with particular focus on gravitational-wave signals from the inspiral of binary neutron-star systems, which are considered the most promising for multi-messenger astronomy. The ability to localize the sources of the detected signals depends on the geographical distribution of the detectors and their relative sensitivity, and 90% credible regions can be as large as thousands of square degrees when only two sensitive detectors are operational. Determining the sky position of a significant fraction of detected signals to areas of 5 deg2 to 20 deg2 will require at least three detectors of sensitivity within a factor of ∼ 2 of each other and with a broad frequency bandwidth. Should the third LIGO detector be relocated to India as expected, a significant fraction of gravitational-wave signals will be localized to a few square degrees by gravitational-wave observations alone
Observation of Gravitational Waves from a Binary Black Hole Merger
- Author
- 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
- Arain MA
- 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
- 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
- Barton MA
- Bartos I
- Bassiri R
- Basti A
- Batch JC
- Baune C
- Bavigadda V
- Bazzan M
- Behnke B
- Bejger M
- Belczynski C
- Bell AS
- Bell CJ
- Berger BK
- Bergman J
- Bergmann G
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- 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
- Bodiya TP
- Boer M
- Bogaert G
- Bogan C
- Bohe A
- Bojtos P
- 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
- Brau JE
- Briant T
- Brillet A
- Brinkmann M
- Brisson V
- Brockill P
- Brooks AF
- Brown DA
- Brown DD
- Brown NM
- Buchanan CC
- Buikema A
- Bulik T
- Bulten HJ
- Buonanno A
- Buskulic D
- Bustillo JC
- Buy C
- Byer RL
- Cabero M
- Cadonati L
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- Zweizig J
- Publication venue
- American Physical Society
- Publication date
- 01/01/2016
- Field of study
On September 14, 2015 at 09:50:45 UTC the two detectors of the Laser Interferometer Gravitational-Wave
Observatory simultaneously observed a transient gravitational-wave signal. The signal sweeps upwards in
frequency from 35 to 250 Hz with a peak gravitational-wave strain of 1.0 × 10−21. It matches the waveform
predicted by general relativity for the inspiral and merger of a pair of black holes and the ringdown of the
resulting single black hole. The signal was observed with a matched-filter signal-to-noise ratio of 24 and a
false alarm rate estimated to be less than 1 event per 203 000 years, equivalent to a significance greater
than 5.1σ. The source lies at a luminosity distance of 410þ160
−180 Mpc corresponding to a redshift z ¼ 0.09þ0.03 −0.04 .
In the source frame, the initial black hole masses are 36þ5
−4M⊙ and 29þ4
−4M⊙, and the final black hole mass is
62þ4
−4M⊙, with 3.0þ0.5 −0.5M⊙c2 radiated in gravitational waves. All uncertainties define 90% credible intervals.
These observations demonstrate the existence of binary stellar-mass black hole systems. This is the first direct
detection of gravitational waves and the first observation of a binary black hole merger
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