381 research outputs found
Detour technique, Dipping technique, or IIeal bladder flap technique for surgical correction of uretero-ileal anastomotic stricture in orthotopic ileal neobladder
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- 'FapUNIFESP (SciELO)'
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- Field of study
Multi-messenger observations of a binary neutron star merger
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- Aab A
- Aartsen MG
- Abbott BP
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- Patil M
- Patricelli B
- Paul T
- Pavalas GE
- Pavana M
- Paxman J
- Paz-Chinchn F
- Pea-Rodriguez J
- Pearlstone BL
- Pech M
- Pedraza M
- Pedreira F
- Pedurand R
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- Peixoto CJ Todero
- Pekeur NW
- Pekowsky L
- Pelayo R
- Pele A
- Pellegrino C
- Pelletier G
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- Penacchioni AV
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- Perennes C
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- Perez-Perez EG
- Perley DA
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- Perri LM
- Perri M
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- Perrodin D
- Perrone L
- Pescalli A
- Pesce-Rollins M
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- Petrera S
- Petrucci P-O
- Peyaud B
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- Phelps M
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- Phuntsok J
- Pian E
- Piano G
- Piattelli P
- Piccinni OJ
- Pichot M
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- 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
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- Pollmann A Obertacke
- Poolakkil S
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- Poppi S
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- Possenti A
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- Principe G
- Principe M
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- Prodi GA
- Prokhorov D
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- Prokoph H
- Prouza M
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- Przybylski GT
- Pulone L
- Pumo ML
- Punch M
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- Qi H
- Qi H
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- Quataert E
- Quel EJ
- Querchfeld S
- Querel R
- Quetschke V
- Quimby RM
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- Quinones C
- Quintero EA
- Quirrenbach A
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- Rabeling DS
- Rabus M
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- Ramirez-Ruiz E
- Ramos-Buades A
- Ramos-Pollan R
- Rana J
- Rando R
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- RATIR RIMAS
- Rau A
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- Rebolo R
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- Rei L
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- Reimer A
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- Reimer O
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- Relethford B
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- 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
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- Ricci F
- Ricci R
- Ricciarini S
- Riccobene G
- Richman M
- Ricker PM
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- 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
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- Rudak B
- Ruehl P
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- Ruhe T
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- 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
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- 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
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- Sengupta AS
- Sentenac D
- Sequino V
- Sergeev A
- Sergienko Yu P
- Serino M
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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
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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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- Snow GR
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- Sobreira F
- Sodre L
- Soedingrekso J
- Soffitta P
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- Somala S
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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
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- Tao C
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- Tao WH
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- 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
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- 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
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- 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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- Tung CF
- Tungalag N
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- Turley CF
- 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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- Vergani D
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- 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
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- Vos J
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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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- Westphal T
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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
- Zhang Y-H
- 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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- Zhou Z
- 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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- 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
Impact of SNPs on methylation readouts by Illumina Infinium HumanMethylation450 BeadChip Array: implications for comparative population studies
- Author
- A Majchrzak-Celińska
- A Meissner
- AB Brinkman
- Aleksandra Pfeifer
- Aleksandra Szybińska
- Barbara Jarząb
- Dagmara Rusinek
- E Szmida
- EL Dempster
- Ewa Ziętkiewicz
- F Eckhardt
- F Marabita
- H Heyn
- H Naeem
- HM Byun
- J Maksimovic
- J Sandoval
- Jadwiga Żebracka-Gala
- JD Storey
- JD Storey
- KD Hansen
- M Bibikova
- MD Kraszewska
- ME Price
- Michał Witt
- MJ Aryee
- N Touleimat
- P Du
- Patrycja Daca-Roszak
- PW Laird
- R Edgar
- R Gupta
- RA Irizarry
- S Biswas
- S Dedeurwaerder
- S Dedeurwaerder
- T Zuo
- YA Chen
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of the Ratio of b Quark Production Cross Sections in Antiproton-Proton Collisions at 630 GeV and 1800 GeV
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- Yun JC
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- Zhang J
- Zhu RY
- Zito M
- Zucchelli Stison TS
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2002
- Field of study
We report a measurement of the ratio of the bottom quark production cross
section in antiproton-proton collisions at 630 GeV to 1800 GeV using bottom
quarks with transverse momenta greater than 10.75 GeV identified through their
semileptonic decays and long lifetimes. The measured ratio
sigma(630)/sigma(1800) = 0.171 +/- .024 +/- .012 is in good agreement with
next-to-leading order (NLO) quantum chromodynamics (QCD)
The impact of viral mutations on recognition by SARS-CoV-2 specific T cells.
- Author
- Aanensen DM
- Abudahab K
- Adams A
- Adams H
- Adeniji K
- Afifi S
- Aggarwal D
- Agranoff D
- Agwuh K
- Ahmad SSY
- Ahmed KA
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- Ail D
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- Aldera EL
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- Ariani CV
- Armstrong JA
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- Asiimwe IG
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- Zamudio ME
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- Zhang JE
- Zhang P
- Publication venue
- iScience
- Publication date
- 01/01/2021
- Field of study
We identify amino acid variants within dominant SARS-CoV-2 T cell epitopes by interrogating global sequence data. Several variants within nucleocapsid and ORF3a epitopes have arisen independently in multiple lineages and result in loss of recognition by epitope-specific T cells assessed by IFN-γ and cytotoxic killing assays. Complete loss of T cell responsiveness was seen due to Q213K in the A∗01:01-restricted CD8+ ORF3a epitope FTSDYYQLY207-215; due to P13L, P13S, and P13T in the B∗27:05-restricted CD8+ nucleocapsid epitope QRNAPRITF9-17; and due to T362I and P365S in the A∗03:01/A∗11:01-restricted CD8+ nucleocapsid epitope KTFPPTEPK361-369. CD8+ T cell lines unable to recognize variant epitopes have diverse T cell receptor repertoires. These data demonstrate the potential for T cell evasion and highlight the need for ongoing surveillance for variants capable of escaping T cell as well as humoral immunity.This work is supported by the UK Medical Research Council (MRC); Chinese Academy of Medical Sciences(CAMS) Innovation Fund for Medical Sciences (CIFMS), China; National Institute for Health Research (NIHR)Oxford Biomedical Research Centre, and UK Researchand Innovation (UKRI)/NIHR through the UK Coro-navirus Immunology Consortium (UK-CIC). Sequencing of SARS-CoV-2 samples and collation of data wasundertaken by the COG-UK CONSORTIUM. COG-UK is supported by funding from the Medical ResearchCouncil (MRC) part of UK Research & Innovation (UKRI),the National Institute of Health Research (NIHR),and Genome Research Limited, operating as the Wellcome Sanger Institute. T.I.d.S. is supported by a Well-come Trust Intermediate Clinical Fellowship (110058/Z/15/Z). L.T. is supported by the Wellcome Trust(grant number 205228/Z/16/Z) and by theUniversity of Liverpool Centre for Excellence in Infectious DiseaseResearch (CEIDR). S.D. is funded by an NIHR GlobalResearch Professorship (NIHR300791). L.T. and S.C.M.are also supported by the U.S. Food and Drug Administration Medical Countermeasures Initiative contract75F40120C00085 and the National Institute for Health Research Health Protection Research Unit (HPRU) inEmerging and Zoonotic Infections (NIHR200907) at University of Liverpool inpartnership with Public HealthEngland (PHE), in collaboration with Liverpool School of Tropical Medicine and the University of Oxford.L.T. is based at the University of Liverpool. M.D.P. is funded by the NIHR Sheffield Biomedical ResearchCentre (BRC – IS-BRC-1215-20017). ISARIC4C is supported by the MRC (grant no MC_PC_19059). J.C.K.is a Wellcome Investigator (WT204969/Z/16/Z) and supported by NIHR Oxford Biomedical Research Centreand CIFMS. The views expressed are those of the authors and not necessarily those of the NIHR or MRC
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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- Williams D
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- Willis Jl
- Willke B
- Winkler W
- Wipf Cc
- Wittel H
- Woan G
- Woehler J
- Wofford Jk
- Wright Jl
- Wu Ds
- Wysocki Dm
- Xiao S
- Xu R
- Yamamoto H
- Yancey Cc
- Yang L
- Yang Y
- Yang Z
- Yap Mj
- Yazback M
- Yeeles Dw
- Yu H
- Yu Hc
- Yuen Shr
- Zadrozny A
- Zadrozny Ak
- Zanolin M
- Zelenova T
- Zendri Jp
- Zevin M
- Zhang J
- Zhang L
- Zhang T
- Zhao C
- Zhao G
- Zhou M
- Zhou Z
- Zhu Xj
- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- 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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- Zhao G
- Zhou M
- Zhou Z
- Zhu Xj
- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO’s second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h95%0=3.47×10−25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A
- Author
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- Zhang Y-H
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- Zhou M
- Zhou Z
- Zhu SJ
- Zhu XJ
- 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
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
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- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
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- Addepalli SV
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- Zhemchugov A
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
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