55 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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- Aglietta M
- 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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- 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
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
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- 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
GWTC-2.1: Deep extended catalog of compact binary coalescences observed by LIGO and Virgo during the first half of the third observing run
- Author
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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
All-sky, all-frequency directional search for persistent gravitational waves from Advanced LIGO’s and Advanced Virgo’s first three observing runs
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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
Binary Black Hole Mergers in the first Advanced LIGO Observing Run
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- 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
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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- Yeeles DW
- Yelikar AB
- Ying M
- Yokogawa K
- Yokoyama J
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- Yu H
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- Yuzurihara H
- Zadrozny A
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- Zevin M
- Zhan M
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- Zhou R
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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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- Adame JA
- Adams C
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- Adhikari RX
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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
Cryopreservation of allogeneic PBSC from related and unrelated donors is associated with delayed platelet engraftment but has no impact on survival
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- 'Springer Science and Business Media LLC'
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Business, victimisation and victimology
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- Publication venue
- 'SAGE Publications'
- Publication date
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- …