442 research outputs found
Clinical experience with integrase inhibitors in HIV-2-infected individuals in Spain.
- Author
- Aguilera A.
- Aldamiz T.
- Barreiro P.
- BENITO R.
- Benítez-Gutiérrez L.
- Caballero E.
- Caballero E.
- Cabrera J.
- Cifuentes C.
- Cilla G.
- Cuervas-Mons V.
- de Lejarazu, RO.
- de Mendoza, C.
- de Mendoza, C.
- Del Romero, J.
- Diz J.
- Eirós JM.
- Fernández JM.
- Fernández JM.
- Fernández-Fuertes E.
- Fernández-Pereira L.
- Force L.
- García F.
- García J.
- García-Bermejo I.
- García-Campello M.
- Gaspar G.
- Gimeno A.
- González-Praetorius A.
- Gómez-Hernando C.
- Gómez-Sirvent JL.
- Górgolas M.
- Hernández M.
- Hernández-Betancor A.
- HIV-2 Spanish Study Group
- Lozano AB.
- Lozano AB.
- López-Lirola AM.
- Marcaida G.
- Margall N.
- Martín AM.
- Martín-Carbonero L.
- Miralles P.
- Miralles P.
- Montejo JM.
- Morano L.
- Nieto MC.
- Nieto MC.
- Niubó J.
- Ocete MD.
- Paz I.
- Peñaranda M.
- Pérez L.
- Pérez S.
- Pérez-Trallero E.
- Ramos C.
- Ramos JM.
- Raya C.
- Requena S.
- Requena S.
- Roc L.
- Rodríguez C.
- Rodríguez-Avial I.
- Rodríguez-Avial I.
- Rodríguez-Iglesias M.
- Rojo S.
- Soriano V.
- Soriano V.
- Suárez A.
- Sánchez V.
- Trigo M.
- Trigo M.
- Téllez R.
- Téllez R.
- Valeiro M.
- Vera M.
- Viciana I.
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/01/2019
- Field of study
Background: HIV-2 is a neglected virus despite estimates of 1–2 million people being infected worldwide. The virus is naturally resistant to some antiretrovirals used to treat HIV-1 and therapeutic options are limited for patients with HIV-2.
Methods: In this retrospective observational study, we analysed all HIV-2-infected individuals treated with inte- grase strand transfer inhibitors (INSTIs) recorded in the Spanish HIV-2 cohort. Demographics, treatment modal- ities, laboratory values, quantitative HIV-2 RNA and CD4 counts as well as drug resistance were analysed.
Results: From a total of 354 HIV-2-infected patients recruited by the Spanish HIV-2 cohort as of December 2017, INSTIs had been given to 44, in 18 as first-line therapy and in 26 after failing other antiretroviral regimens. After a median follow-up of 13 months of INSTI-based therapy, undetectable viraemia for HIV-2 was achieved in 89% of treatment-naive and in 65.4% of treatment-experienced patients. In parallel, CD4 gains were 82 and 126cells/mm3, respectively. Treatment failure occurred in 15 patients, 2 being treatment-naive and 13 treatment-experienced. INSTI resistance changes were recognized in 12 patients: N155H (5), Q148H/R (3), Y143C/G (3) and R263K (1).
Conclusions: Combinations based on INSTIs are effective and safe treatment options for HIV-2-infected individ- uals. However, resistance mutations to INSTIs are selected frequently in failing patients, reducing the already limited treatment options
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
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- Angelozzi I
- Angerami A
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- Argyropoulos S
- Armbruster AJ
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- Zhemchugov A
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- Zibell A
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- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
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- Zobernig G
- Zoccoli A
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- Zorbas TG
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- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for supersymmetry in events with four or more leptons in √s =13 TeV pp collisions with ATLAS
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
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- Minami Y
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- Mizukami A
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- Sadrozinski HF
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- Sanchez Pineda A
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- Santoyo Castillo I
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- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schuh N
- Schulte A
- Schultens MJ
- Schultz-Coulon H
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
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- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
- Schäfer U
- Sciandra A
- Sciolla G
- Scornajenghi M
- Scuri F
- Scutti F
- Searcy J
- Seema P
- Seidel SC
- Seiden A
- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Semprini-Cesari N
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Seuster R
- Severini H
- Sforza F
- Sfyrla A
- Shabalina E
- Shaikh NW
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shehu CY
- Shen Y
- Sherafati N
- Sherman AD
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shoaleh Saadi D
- Shochet MJ
- Shojaii S
- Shope DR
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
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- Sidebo PE
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- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
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- Silverstein SB
- Simak V
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- Sinev NB
- Sioli M
- Siragusa G
- Siral I
- Sivoklokov SY
- Sjölin J
- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Sokhrannyi G
- Solans Sanchez CA
- Solar M
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sopczak A
- Sosa D
- Sotiropoulou CL
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spanò F
- Sperlich D
- Spettel F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spousta M
- St. Denis RD
- St. Panagiotopoulou E
- Stabile A
- Stamen R
- Stamm S
- Stanecka E
- Stanek RW
- Stanescu C
- Stanitzki MM
- Stapf BS
- Stapnes S
- Starchenko EA
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- Staroba P
- Starovoitov P
- Staszewski R
- Stegler M
- Steinberg P
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- Stelzer-Chilton O
- Stenzel H
- Sterzo FL
- Stevenson TJ
- Stewart GA
- Stockton MC
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- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Strom DM
- Stroynowski R
- Strubig A
- Ströhmer R
- Stucci SA
- Stugu B
- Styles NA
- Stärz S
- Su D
- Su J
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- Sugaya Y
- Suk M
- Sulin VV
- Sultan D
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Sykora I
- Sykora T
- Sánchez J
- Søgaard A
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Tahirovic E
- Taiblum N
- Takai H
- Takashima R
- Takasugi EH
- Takeda K
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tanaka J
- Tanaka M
- Tanaka R
- Tanaka S
- Tanioka R
- Tannenwald BB
- Tapia Araya S
- Tapprogge S
- Tarem S
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
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- Taylor AJ
- Taylor GN
- Taylor PTE
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- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Thais SJ
- Theveneaux-Pelzer T
- Thiele F
- Thomas JP
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- Thompson AS
- Thompson PD
- Thomsen LA
- Thomson E
- Tian Y
- Tibbetts MJ
- Ticse Torres RE
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
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- Tricoli A
- Trigger IM
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- Tripiana MF
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- Trocmé B
- Trofymov A
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- Truong L
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- Trzupek A
- Tsang KW
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- Tsiareshka PV
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
- Turk Cakir I
- Turra R
- Tuts PM
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Unverdorben C
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valdes Santurio E
- Valente M
- Valentinetti S
- Valero A
- Valkar S
- Vallier A
- Valls Ferrer JA
- Valéry L
- Van Den Wollenberg W
- van der Graaf H
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Veatch J
- Veeraraghavan V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Venturini A
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- Verducci M
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vetterli MC
- Viaux Maira N
- Viazlo O
- Vichou I
- Vickey Boeriu OE
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
- Vokac P
- Volpi G
- von der Schmitt H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes Milosavljevic M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakamiya K
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Wang C
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- Wang Q
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- Wang SM
- Wang T
- Wang W
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
- Watkins PM
- Watson AT
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb AF
- Webb S
- Weber MS
- Weber SA
- Weber SM
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Werner P
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wotschack J
- Wozniak KW
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu L
- Xu T
- Xu W
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang Y
- Yang Z
- Yao W
- Yap YC
- Yasu Y
- Yatsenko E
- Yau Wong KH
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
Results from a search for supersymmetry in events with four or more charged leptons (electrons, muons and taus) are presented. The analysis uses a data sample corresponding to 36.1 fb −1 of proton-proton collisions delivered by the Large Hadron Collider at s √ =13 TeV and recorded by the ATLAS detector. Four-lepton signal regions with up to two hadronically decaying taus are designed to target a range of supersymmetric scenarios that can be either enriched in or depleted of events involving the production and decay of a Z boson. Data yields are consistent with Standard Model expectations and results are used to set upper limits on the event yields from processes beyond the Standard Model. Exclusion limits are set at the 95% confidence level in simplified models of General Gauge Mediated supersymmetry, where higgsino masses are excluded up to 295 GeV. In R -parity-violating simplified models with decays of the lightest supersymmetric particle to charged leptons, lower limits of 1.46 TeV, 1.06 TeV, and 2.25 TeV are placed on wino, slepton and gluino masses, respectively
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Zobernig G
- Zoccoli A
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- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Cognitive impairment in COPD: a systematic review
- Author
- Allen SC
- Antonelli Incalzi R
- Antonelli-Incalzi R
- Antonelli-Incalzi R
- Antonelli-Incalzi R
- Bolton CE
- Borson S
- Chang SS
- Corsonello A
- Corsonello A
- de Batlle J
- de Oliveira JC
- Dodd JW
- Dodd JW
- Dodd JW
- Elisabeth Rodríguez-Alzueta
- Gasquoine PG
- Grant I
- Heaton RK
- Hung WW
- Irene Cabrera-Martos
- Irene Torres-Sánchez
- Isabel López-Torres
- Jemal A
- Klein M
- Landi F
- Lezak MD
- Lima OM
- Mannino DM
- Maria Paz Moreno-Ramírez
- Marie Carmen Valenza
- Martin SE
- Miravitlles M
- Orth M
- Pereira ED
- Salik Y
- Schillerstrom JE
- Schou L
- Sin DD
- Thakur N
- Villeneuve S
- Wasswa-Kintu S
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Performance of the ATLAS muon trigger in pp collisions at [Formula: see text] TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdinov O
- Aben R
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- Aleksandrov IN
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- Allbrooke BM
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- ATLAS Collaboration
- Atlay NB
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- Åkesson TP
- Åsman B
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- Publication venue
- Publication date
- 01/03/2015
- Field of study
The performance of the ATLAS muon trigger system is evaluated with proton-proton collision data collected in 2012 at the Large Hadron Collider at a centre-of-mass energy of 8 TeV. It is primarily evaluated using events containing a pair of muons from the decay of [Formula: see text] bosons. The efficiency of the single-muon trigger is measured for muons with transverse momentum [Formula: see text] GeV, with a statistical uncertainty of less than 0.01 % and a systematic uncertainty of 0.6 %. The [Formula: see text] range for efficiency determination is extended by using muons from decays of [Formula: see text] mesons, [Formula: see text] bosons, and top quarks. The muon trigger shows highly uniform and stable performance. The performance is compared to the prediction of a detailed simulation
Search for excited electrons singly produced in proton–proton collisions at \sqrt{s} = 13 TeV with the ALAS experiment at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
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- Zhemchugov A
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- Zobernig G
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- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2019
- Field of study
A search for excited electrons produced in pp collisions at s√ = 13 TeV via a contact interaction qq¯→ee∗ is presented. The search uses 36.1 fb −1 of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( eqq¯ ) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a W boson ( νW ) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying W boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the pp→ee∗→eeqq¯ and pp→ee∗→eνW production cross sections as a function of the excited electron mass me∗ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Λ of the model as a function of me∗ . For me∗<0.5 TeV , the lower bound for Λ is 11 TeV . In the special case of me∗=Λ , the values of me∗<4.8 TeV are excluded. The presented limits on Λ are more stringent than those obtained in previous searches
Recommended from our members
Search for Dark Matter Produced in Association with a Higgs Boson Decaying to bb[over ¯] Using 36 fb^{-1} of pp Collisions at sqrt[s]=13 TeV with the ATLAS Detector.
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
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- Adelman J
- Adersberger M
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- Agatonovic-Jovin T
- Agheorghiesei C
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- Ahlen SP
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- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
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- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Ženiš T
- Živković L
- Publication venue
- Phys Rev Lett
- Publication date
- 03/11/2017
- Field of study
Several extensions of the standard model predict associated production of dark-matter particles with a Higgs boson. Such processes are searched for in final states with missing transverse momentum and a Higgs boson decaying to a bb[over ¯] pair with the ATLAS detector using 36.1 fb^{-1} of pp collisions at a center-of-mass energy of 13 TeV at the LHC. The observed data are in agreement with the standard model predictions and limits are placed on the associated production of dark-matter particles and a Higgs boson
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
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- Acharya BS
- Achkar B
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- Adamek L
- Adelman J
- Adiguzel A
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- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
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- Akatsuka S
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- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
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- Alfonsi A
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- Andrean SY
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- Angerami A
- Anisenkov AV
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- Borbély AG
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortoletto D
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- Bosman M
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- Buddenbrock SEV
- Bugge MK
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- Bullard BA
- Burch TJ
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- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Büscher V
- Cabras G
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
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- Calace N
- Calafiura P
- Calderini G
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- Caloba LP
- Caltabiano A
- Calvet D
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- Camerlingo MT
- Cameron D
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- Camplani A
- Canale V
- Canesse A
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- Cao Y
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- Capua M
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- Cheremushkina E
- Cheu E
- Cheung K
- Chevalier L
- Chevalérias TJA
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
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- Christopher LD
- Chu MC
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- Ciaccio AD
- Ciaccio LD
- Cieri D
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- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
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- Citterio M
- Ciubotaru DA
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- da Costa JBG
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Daalen TRV
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- Doglioni C
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- Donato CD
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- Gkialas I
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- Yallup DP
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- Zemaityte G
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou H
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- Zhu C
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- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
Search for flavour-changing neutral current top-quark decays t → qZ in proton-proton collisions at \sqrt{s} = 13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Abulaiti Y
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- Šfiligoj T
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- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/07/2018
- Field of study
A search for flavour-changing neutral-current processes in top-quark decays is presented. Data collected with the ATLAS detector from proton-proton collisions at the Large Hadron Collider at a centre-of-mass energy of s√=13 TeV, corresponding to an integrated luminosity of 36.1 fb−1, are analysed. The search is performed using top-quark pair events, with one top quark decaying through the t → qZ (q = u, c) flavour-changing neutral-current channel, and the other through the dominant Standard Model mode t → bW. Only Z boson decays into charged leptons and leptonic W boson decays are considered as signal. Consequently, the final-state topology is characterized by the presence of three isolated charged leptons (electrons or muons), at least two jets, one of the jets originating from a b-quark, and missing transverse momentum from the undetected neutrino. The data are consistent with Standard Model background contributions, and at 95% confidence level the search sets observed (expected) upper limits of 1.7 × 10−4 (2.4 × 10−4) on the t → uZ branching ratio and 2.4 × 10−4 (3.2 × 10−4) on the t → cZ branching ratio, constituting the most stringent limits to date.
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