58 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
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- Agliozzo C
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- Aguilar JA
- Aharonian F
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- Aiello L
- Ain A
- Ajith P
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- Areeda JS
- Aresu G
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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
Localization and broadband follow-up of the gravitational-wave transient GW150914
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- Zimmer S
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- Zweizig J
- Publication venue
- Astrophysical Journal Letters
- Publication date
- 01/01/2016
- Field of study
A gravitational-wave (GW) transient was identified in data recorded by the Advanced Laser Interferometer Gravitational-wave Observatory (LIGO) detectors on 2015 September 14. The event, 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 GW 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 GW 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 (EM) 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 EM data and results of the EM follow-up campaign are being disseminated in papers by the individual teams
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
- 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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- Yamamoto Kazuhiro
- Yamamoto Kohei
- Yamamoto T
- Yamashita K
- Yamazaki R
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- Yang Yang
- Yang Yi
- Yang Z
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- Yelikar AB
- Ying M
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- Zhu Z-H
- Zucker ME
- 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
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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- 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
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
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- Chamberlin SJ
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- Chen HY
- Chen Y
- Cheng C
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- Chiummo A
- Cho HS
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- Christensen N
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- Virgo Collaboration
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- Weßels P
- Whelan JT
- White DJ
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- Willke B
- Wimmer MH
- Winkler W
- Wipf CC
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- Worden J
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- Wu G
- Yablon J
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- Yamamoto H
- Yancey CC
- Yap MJ
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- 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
- Cagnoli G
- Cahillane C
- Callister T
- Calloni E
- Camp JB
- Cannon KC
- Cao J
- Capano CD
- Capocasa E
- Carbognani F
- Caride S
- Casentini C
- Castro JMG
- Caudill S
- Cavaglia M
- Cavalier F
- Cavalieri R
- Cella G
- Cepeda CB
- 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
- Clara F
- Clark JA
- Cleva F
- Coccia E
- Cohadon P-F
- Colla A
- Collaboration LIGOS
- Collaboration V
- Collette CG
- Cominsky L
- Constancio M
- Conte A
- Conti L
- Cook D
- Corbitt TR
- Cornish N
- Corsi A
- Cortese S
- Costa CA
- 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
- Creighton TD
- Cripe J
- Crowder SG
- Cruise AM
- Cumming A
- Cunningham L
- Cuoco E
- D'Antonio S
- Da Silva Costa CF
- Dal Canton T
- Danilishin SL
- Danzmann K
- Darman NS
- Dattilo V
- Dave I
- Daveloza HP
- Davier M
- Davies GS
- Daw EJ
- Day R
- De laurentis M
- De Rosa R
- De S
- DeBra D
- Debreczeni G
- Degallaix J
- Del Pozzo W
- Deleglise S
- Denker T
- Dent T
- Dereli H
- Dergachev V
- DeRosa RT
- DeSalvo R
- Dhurandhar S
- Di Fiore L
- Di Giovanni M
- Di Lieto A
- Di Pace S
- Di Palma I
- Di Virgilio A
- Diaz JC
- Diaz MC
- Dojcinoski G
- Dolique V
- Donovan F
- Dooley KL
- Doravari S
- Douglas R
- Downes TP
- Drago M
- Drever RWP
- Driggers JC
- Du Z
- 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
- Feldbaum D
- Ferrante I
- Ferreira EC
- Ferrini F
- Fidecaro F
- Finn LS
- Fiori I
- Fiorucci D
- Fisher RP
- Flaminio R
- Fletcher M
- Fong H
- Fournier J-D
- Franco S
- Frasca S
- Frasconi F
- Frede M
- Frei Z
- Freise A
- Frey R
- Frey V
- Fricke TT
- Fritschel P
- Frolov VV
- Fulda P
- Fyffe M
- Gabbard HAG
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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
Search for Gravitational Waves Associated with Gamma-Ray Bursts during the First Advanced LIGO Observing Run and Implications for the Origin of GRB 150906B
- Author
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- Worden J
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- Zangrando L
- Zanolin M
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- Zevin M
- Zhang L
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- Zhang X
- Zhang Y
- Zhao C
- Zhou M
- Zhou Z
- Zhu XJ
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 29/11/2016
- Field of study
We present the results of the search for gravitational waves (GWs) associated with γ-ray bursts detected during the first observing run of the Advanced Laser Interferometer Gravitational-Wave Observatory (LIGO). We find no evidence of a GW signal for any of the 41 γ-ray bursts for which LIGO data are available with sufficient duration. For all γ-ray bursts, we place lower bounds on the distance to the source using the optimistic assumption that GWs with an energy of 10−2M⊙c2 were emitted within the 16–500 Hz band, and we find a median 90% confidence limit of 71 Mpc at 150 Hz. For the subset of 19 short/hard γ-ray bursts, we place lower bounds on distance with a median 90% confidence limit of 90 Mpc for binary neutron star (BNS) coalescences, and 150 and 139 Mpc for neutron star–black hole coalescences with spins aligned to the orbital angular momentum and in a generic configuration, respectively. These are the highest distance limits ever achieved by GW searches. We also discuss in detail the results of the search for GWs associated with GRB 150906B, an event that was localized by the InterPlanetary Network near the local galaxy NGC 3313, which is at a luminosity distance of 54 Mpc (z = 0.0124). Assuming the γ-ray emission is beamed with a jet half-opening angle ⩽30∘, we exclude a BNS and a neutron star–black hole in NGC 3313 as the progenitor of this event with confidence >99%. Further, we exclude such progenitors up to a distance of 102 Mpc and 170 Mpc, respectively
Binary Black Hole Mergers in the first Advanced LIGO Observing Run
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- Abbott TD
- Abernathy MR
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- Jr MC
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- Kalaghatgi CV
- Kalogera V
- Kandhasamy S
- Kang G
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- Kapadia SJ
- Karki S
- Karvinen KS
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- Katzman W
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- Kehl MS
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- Kowalska I
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- Nuttall LK
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- O'Reilly B
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- o DT
- Oberling J
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- Oliver M
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- Oppermann P
- Oram RJ
- Ottaway DJ
- Overmier H
- Owen BJ
- Pace SD
- Pai A
- Pai SA
- Pal-Singh A
- Palamos JR
- Palashov O
- Palma ID
- Palomba C
- Pan H
- Pan Y
- Pankow C
- Pannarale F
- Pant BC
- Paoletti F
- Paoli A
- Papa MA
- Paris HR
- Parker W
- Pascucci D
- Pasqualetti A
- Passaquieti R
- Passuello D
- Patricelli B
- Patrick Z
- Pearlstone BL
- Pedraza M
- Pedurand R
- Pekowsky L
- Pele A
- Penn S
- Perreca A
- Perri LM
- Pfeiffer H
- Phelps M
- Piccinni OJ
- Pichot M
- Piergiovanni F
- Pierro V
- Pillant G
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- Pinto IM
- Pitkin M
- Poe M
- Poggiani R
- Popolizio P
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- Zertuche LM
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- Zhu XJ
- zny AZ
- Zucker ME
- 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
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