131 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
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- Achkar B
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- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at root s=13 TeV with the ATLAS detector
- Author
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- Zaripovas DR
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- Zenin O
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- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou M
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- Zhou N
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- Zhu CG
- Zhu H
- Zhu HL
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 13/08/2020
- Field of study
A search for heavy neutral Higgs bosons produced in association with one or two
b
-quarks and decaying to
b
-quark pairs is presented using
27.8
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross section times its branching ratio to
b
¯
b
are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the minimal supersymmetric Standard Model
Measurement of single top-quark production in association with a W boson in the single-lepton channel at \sqrt{s} = 8\,\text {TeV} with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
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- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
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- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
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- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
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- Alviggi MG
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- Amelung C
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- Anders JK
- Andreazza A
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- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
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- Anthony MT
- Antipov E
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- Antrim DJA
- Anulli F
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- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
The production cross-section of a top quark in association with a W boson is measured using proton–proton collisions at \sqrt{s} = 8\,\text {TeV}. The dataset corresponds to an integrated luminosity of 20.2\,\text {fb}^{-1}, and was collected in 2012 by the ATLAS detector at the Large Hadron Collider at CERN. The analysis is performed in the single-lepton channel. Events are selected by requiring one isolated lepton (electron or muon) and at least three jets. A neural network is trained to separate the tW signal from the dominant t{\bar{t}} background. The cross-section is extracted from a binned profile maximum-likelihood fit to a two-dimensional discriminant built from the neural-network output and the invariant mass of the hadronically decaying W boson. The measured cross-section is \sigma _{tW} = 26 \pm 7\,\text {pb}, in good agreement with the Standard Model expectation
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
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- Zhemchugov A
- Zheng Z
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
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- 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
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Acharya BS
- Achkar B
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- Adelman J
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- Metcalfe J
- Mete AS
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- Michetti M
- Middleton RP
- Miguens JM
- Mijovic L
- Mikenberg G
- Mikestikova M
- Mikuz M
- Mildner H
- Milic A
- Milke CD
- Miller DW
- Miller LS
- Milosavljevic MV
- Milov A
- Milstead DA
- Minaenko AA
- Minashvili IA
- Mince L
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- Mindur B
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- Minegishi Y
- Mino Y
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- Mir LM
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- Mitani T
- Mitrevski J
- Mitsou VA
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- Miu O
- Miucci A
- Miyagawa PS
- Mizukami A
- Mjoernmark JU
- Mkrtchyan T
- Mlynarikova M
- Moa T
- Mobius S
- Mochizuki K
- Moder P
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- Mohapatra S
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- Morgenstern S
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- Morii M
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- Morisbak V
- Morley AK
- Mornacchi G
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- Moschovakos P
- Moser B
- Mosidze M
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- Moskvitina P
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- Mueller RSP
- Muenstermann D
- Muino PC
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- Mungo DP
- Munoz DC
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- Murrone A
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- Muskinja M
- Mwewa C
- Myagkov AG
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- Myers G
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- Nanjo H
- Napolitano F
- Narayan R
- Naryshkin I
- Naseri M
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- Navarro G
- Navarro JEG
- Navarro LB
- Nechaeva PY
- Nechansky F
- Neep TJ
- Negri A
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- Nellist C
- Nelson C
- Nelson ME
- Nemecek S
- Nessi M
- Neubauer MS
- Neuhaus F
- Neumann M
- Newhouse R
- Newman PR
- Ng CW
- Ng YS
- Ng YWY
- Ngair B
- Nguyen HDN
- Nibigira E
- Nickerson RB
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- Nielsen J
- Niemeyer M
- Nikiforou N
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Nindhito HR
- Nisati A
- Nishu N
- Nisius R
- Nitsche I
- Nitta T
- Nobe T
- Noel DL
- Noguchi Y
- Nomidis I
- Nomura MA
- Nordberg M
- Novak J
- Novak T
- Novgorodova O
- Novotny R
- Nozka L
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- Nurse E
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- O'neill AP
- O'Shea V
- Oakham FG
- Ocariz J
- Ochi A
- Ochoa I
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- Oda S
- Odaka S
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- Oishi R
- Ojeda ML
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- Okazaki Y
- Okumura Y
- Olariu A
- Oliveira MVS
- Oliver JL
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- Onofre A
- Onyisi PUE
- Oppen H
- Oreglia MJ
- Orellana GE
- Orestano D
- Orlando N
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- Otero y Garzon G
- Otono H
- Ott PS
- Ottino GJ
- Ouchrif M
- Ouellette J
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- Outschoorn VIM
- Ouyang Q
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- Pages AP
- Palacino G
- Palazzo S
- Palestini S
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- Palni P
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- Panizzo G
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- Papadatos C
- Papageorgiou K
- Parajuli S
- Paramonov A
- Paraskevopoulos C
- Pardos CD
- Parida B
- Park TH
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- Parker MA
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- Parrish EW
- Parsons JA
- Parzefall U
- Pascual JAG
- Pascuzzi VR
- Pasner JMP
- Pasquali F
- Pasqualucci E
- Passaggio S
- Pastor ET
- Pastor OE
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- Pasuwan P
- Pataraia S
- Pater JR
- Pathak A
- Patton J
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- Paz IL
- Pearkes J
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- Peiffer T
- Peixoto APP
- Peleganchuk SV
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- Peralva BS
- Perego MM
- Pereira RA
- Perepelitsa DV
- Perez MV
- Perini L
- Pernegger H
- Perrella S
- Perrevoort A
- Peso JD
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
- Petit E
- Petousis V
- Petridou C
- Petrucci F
- Pettee M
- Pettersson NE
- Petukhova K
- Peyaud A
- Pezoa R
- Pezzotti L
- Pham T
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- Phipps MW
- Piacquadio G
- Pianori E
- Picazio A
- Pickles RH
- Piegaia R
- Pietreanu D
- Pilcher JE
- Pilkington AD
- Pinamonti M
- Pineda AS
- Pinfold JL
- Pino SAO
- Pitt M
- Pizzimento L
- Pizzini A
- Pleier M-A
- Plesanovs V
- Pleskot V
- Plotnikova E
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Ponce JMI
- Ponomarenko D
- Pontecorvo L
- Popa S
- Popeneciu GA
- Portales L
- Pospisil S
- Potamianos K
- Potrap IN
- Potter CJ
- Potti H
- Poulsen T
- Poveda J
- Powell TD
- Pownall G
- Pozo JAA
- Pralavorio P
- Prapa MM
- Pree TAD
- Prell S
- Price D
- Primavera M
- Proffitt ML
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Pudzha D
- Puri A
- Puzo P
- Pyatiizbyantseva D
- Qian J
- Qin Y
- Quadt A
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- Quintero DMP
- Racko M
- Ragusa F
- Rahal G
- Raine JA
- Rajagopalan S
- Ramos JM
- Ran K
- Rassloff DF
- Rauch DM
- Rauscher F
- Rave S
- Ravina B
- Ravinovich I
- Rawling JH
- Raymond M
- Read AL
- Readioff NP
- Reale M
- Rebuzzi DM
- Redlinger G
- Reeves K
- Reikher D
- Reiss A
- Rej A
- Rembser C
- Renardi A
- Renda M
- Rendel MB
- Rennie AG
- Renous DS
- Renteria CG
- Resconi S
- Resseguie ED
- Rettie S
- Reynolds B
- Reynolds E
- Rezanova OL
- Reznicek P
- Ricci E
- Richter R
- Richter S
- Richter-Was E
- Ridel M
- Rieck P
- Rifki O
- Rijssenbeek M
- Rimoldi A
- Rimoldi M
- Rinaldi L
- Rinn TT
- Ripellino G
- Riu I
- Rivadeneira P
- Rizatdinova F
- Rizvi E
- Rizzi C
- Robertson SH
- Robin M
- Robinson D
- Robson A
- Rocchi A
- Roda C
- Rodriguez AR
- Rodriguez GRG
- Roe S
- Roehrig R
- Roggel J
- Rohne O
- Rojas JGRG
- Rojas RA
- Roland B
- Roland CPA
- Roloff J
- Romaniouk A
- Romano M
- Rompotis N
- Ronzani M
- Roos L
- Rosati S
- Rosin G
- Rosser BJ
- Rossi E
- Rossi E
- Rossi E
- Rossi LP
- Rossini L
- Rosten R
- Rotaru M
- Rottler B
- Rousseau D
- Rovelli G
- Roy A
- Roy D
- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Ruehr F
- Ruettinger EM
- Ruggeri TA
- Ruiz-Martinez A
- Rummler A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rustige L
- Rutherfoord JP
- Rybar M
- Rybkin G
- Rye EB
- Ryzhov A
- Sabatini P
- Sabetta L
- Sacerdoti S
- Sadrozinski HF-W
- Sadykov R
- Saenz SRP
- Safdari M
- Saha P
- Saha S
- Sahinsoy M
- Sahu A
- Saimpert M
- Saito M
- Saito T
- Sakamoto H
- Salamani D
- Salamanna G
- Salas AS
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Samani BS
- Samarati J
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez CAS
- Sanchez FJM
- Sanchez J
- Sanchez LP
- Sandaker H
- Sander CO
- Sanderswood IG
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sano Y
- Sansoni A
- Santoni C
- Santos H
- Santos SPAD
- Santpur SN
- Santra A
- Santurio EV
- Saoucha KA
- Sapronov A
- Saraiva JG
- Sasaki O
- Sato K
- Sauerburger F
- Sauvan E
- Savard P
- Sawada R
- Sawyer C
- Sawyer L
- Sbarra C
- Sbrizzi A
- Scanlon T
- Schaarschmidt J
- Schacht P
- Schaefer D
- Schaefer L
- Schaefer U
- Schaffer AC
- Schaile D
- Schamberger RD
- Schanet E
- Scharf C
- Scharmberg N
- Schegelsky VA
- Scheirich D
- Schenck F
- Schernau M
- Schiavi C
- Schildgen LK
- Schillaci ZM
- Schioppa EJ
- Schioppa M
- Schleicher KE
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schoeffel L
- Schoening A
- Scholer PG
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder F
- Schroeder TV
- Schulte A
- Schultz-Coulon H-C
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Scyboz LM
- Seabra LFO
- Sebastiani CD
- Sedlaczek K
- Seema P
- Seidel SC
- Seiden A
- Seidlitz BD
- Seiss T
- Seitz C
- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Semprini-Cesari N
- Sen S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sevova S
- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian JD
- Shaikh NW
- Shan LY
- Shapiro M
- Sharma A
- Sharma AS
- Shatalov PB
- Shaw K
- Shaw SM
- Shehade M
- Shen Y
- Sherman AD
- Sherwood P
- Shi L
- Shimmin CO
- Shimogama Y
- Shimojima M
- Shinner JD
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet MJ
- Shojaii J
- Shope DR
- Shrestha S
- Shrif EM
- Shroff MJ
- Shulga E
- Sicho P
- Sickles AM
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva MJ
- Silverstein SB
- Simion S
- Simoniello R
- Simpson-allsop CJ
- Simsek S
- Sinervo P
- Sinetckii V
- Singh S
- Sinha S
- Sioli M
- Siral I
- Sivoklokov SY
- Sjoelin J
- Skaf A
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith EA
- Smith HA
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev AA
- Snoek HL
- Snyder IM
- Snyder S
- Sobie R
- Soffer A
- Sogaard A
- Sohns F
- Sola JDB
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sonay A
- Song W
- Song WY
- Sopczak A
- Sopio AL
- Sopkova F
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spieker TM
- Spigo G
- Spina M
- Spiteri DP
- Spousta M
- Stabile A
- Staerz S
- Stamas BL
- Stamen R
- Stamenkovic M
- Stampekis A
- Stanecka E
- Stanislaus B
- Stanitzki MM
- Stankaityte M
- Stapf B
- Starchenko EA
- Stark GH
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Stavropoulos G
- Stegler M
- Steinberg P
- Steinhebel AL
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stevenson TJ
- Stewart GA
- Stockton MC
- Stoicea G
- Stolarski M
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strebler T
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
- Su W
- Su X
- Suarez NB
- Suarez RG
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suster CJE
- Sutton MR
- Suzuki S
- svatos M
- Swiatlowski M
- Swift SP
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Tagiev E
- Taibah RHM
- Takashima R
- Takeda K
- Takeshita T
- Takeva EP
- Takubo Y
- Talby M
- Talyshev AA
- Tam KC
- Tame ZPA
- Tamir NM
- Tanaka J
- Tanaka R
- Tapprogge S
- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tateno G
- Tayalati Y
- Taylor AJ
- Taylor GN
- Taylor W
- Teagle H
- Tee AS
- Tehrani FS
- Teixeira-Dias P
- Teoh JJ
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Themistokleous N
- Theveneaux-Pelzer T
- Thomas DW
- Thomas JP
- Thompson EA
- Thompson PD
- Thomson E
- Thorpe EJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Todome K
- Todorova-Nova S
- Todt S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
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- Tomiwa KG
- Tomoto M
- Tompkins L
- Tornambe P
- Toro RC
- Torregrosa EF
- Torrence E
- Torres H
- Toscani M
- Tosciri C
- Toth J
- Tovey DR
- Traeet A
- Treado CJ
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trischuk DA
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tsiareshka PV
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
- Turra R
- Tuts PM
- Tzamarias S
- Tzovara E
- Uchida K
- Ukegawa F
- Unal G
- Unal M
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urban SC
- Urquijo P
- Usai G
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vafeiadis T
- Vaidya A
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Van Daalen TR
- Van Gemmeren P
- Van Stroud S
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vazeille F
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Vera AMR
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vernieri C
- Verschuuren PJ
- Verzini MJA
- Vetterli MC
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vu NK
- Vuillermet R
- Vukotic I
- Wada S
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Wakasa R
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Walls FMG
- Wang AM
- Wang AZ
- Wang C
- Wang C
- Wang H
- Wang H
- Wang J
- Wang P
- Wang Q
- Wang R
- Wang R
- Wang R-J
- Wang SM
- Wang W
- Wang WT
- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Ward RJ
- Warrack N
- Watson AT
- Watson MF
- Watts G
- Waugh BM
- Webb AF
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Wei Y
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wendland B
- Wengler T
- Wenig S
- Wermes N
- Wessels M
- Weston TD
- Whalen K
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams DM
- Williams HH
- Williams S
- Willocq S
- Windischhofer PJ
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winter BT
- Wittgen M
- Wobisch M
- Woelker R
- Wolf A
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Wongel AF
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wuerzinger J
- Wyatt TR
- Wynne BM
- Xella S
- Xiang J
- Xiao X
- Xie X
- Xiotidis I
- Xu D
- Xu H
- Xu H
- Xu L
- Xu R
- Xu T
- Xu W
- Xu Y
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang X
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb−1 of s√ = 13 TeV pp collision data with the ATLAS detector
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- Zemaityte G
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
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- Zorbas TG
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 17/02/2021
- Field of study
A search for the supersymmetric partners of quarks and gluons (squarks and gluinos) in final states containing jets and missing transverse momentum, but no electrons or muons, is presented. The data used in this search were recorded by the ATLAS experiment in proton-proton collisions at a centre-of-mass energy of s√ = 13 TeV during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. The results are interpreted in the context of various R-parity-conserving models where squarks and gluinos are produced in pairs or in association and a neutralino is the lightest supersymmetric particle. An exclusion limit at the 95% confidence level on the mass of the gluino is set at 2.30 TeV for a simplified model containing only a gluino and the lightest neutralino, assuming the latter is massless. For a simplified model involving the strong production of mass-degenerate first- and second-generation squarks, squark masses below 1.85 TeV are excluded if the lightest neutralino is massless. These limits extend substantially beyond the region of supersymmetric parameter space excluded previously by similar searches with the ATLAS detector
Measurement of Azimuthal Anisotropy of Muons from Charm and Bottom Hadrons in pp Collisions at √s = 13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
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- Cardillo FC
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- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 28/02/2020
- Field of study
The elliptic flow of muons from the decay of charm and bottom hadrons is measured in
p
p
collisions at
√
s
=
13
TeV
using a data sample with an integrated luminosity of
150
pb
−
1
recorded by the ATLAS detector at the LHC. The muons from heavy-flavor decay are separated from light-hadron decay muons using momentum imbalance between the tracking and muon spectrometers. The heavy-flavor decay muons are further separated into those from charm decay and those from bottom decay using the distance-of-closest-approach to the collision vertex. The measurement is performed for muons in the transverse momentum range 4–7 GeV and pseudorapidity range
|
η
|
<
2.4
. A significant nonzero elliptic anisotropy coefficient
v
2
is observed for muons from charm decays, while the
v
2
value for muons from bottom decays is consistent with zero within uncertainties
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
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- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
Properties of jet fragmentation using charged particles measured with the ATLAS detector in pp collisions at root s=13 TeV
- Author
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- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/09/2019
- Field of study
This paper presents a measurement of quantities related to the formation of jets from high-energy quarks and gluons (fragmentation). Jets with transverse momentum 100 GeV 500 MeV and |η| < 2.5 are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the two leading jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons with parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark and gluon extractions using input from simulation. The simulations provide a reasonable description of the quark-like data across the jet
Pt range presented in -this measurement, but the gluon-like data have systematically fewer charged particles than the simulation
Identification of boosted Higgs bosons decaying into b-quark pairs with the ATLAS detector at 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
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- Aleksa M
- Aleksandrov IN
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- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
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- Bonilla JS
- Boonekamp M
- Borecka-Bielska HM
- Borisov A
- Borissov G
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- Brau B
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- Briglin DL
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- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
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- Bryngemark L
- Bscher V
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- Buchholz P
- Buckley AG
- Budagov IA
- Bugge MK
- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burka K
- Burr JTP
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
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- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
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- Camincher C
- Campana S
- Campanelli M
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- Campoverde A
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- Canesse A
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- Cao T
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- Cardillo FC
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carter JWS
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
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- Cerri A
- Cerrito L
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- Cervelli A
- Cetin SA
- Chakraborty D
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- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chau CC
- Che S
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- Chekanov S
- Chekulaev S
- Chelkov GA
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- Chen B
- Chen C
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- Cheng HC
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- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevaleier L
- Chevalrias TJA
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
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- Chow YS
- Chu MC
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- Cinca D
- Cindro V
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- Cornell SD
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- Da Fonseca Pinto J
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- de Jong P
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- De Maria A
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
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- Del Gaudio M
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- Denysiuk D
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- Deviveiros PO
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- Di Ciaccio A
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- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Gregorio G
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- Fleck I
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- Flierl BM
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- Laurier A
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- Le Dortz O
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- von Buddenbrock SE
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- Yexley MR
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- Yildiz HD
- Yorita K
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- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zinonos Z
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2019
- Field of study
This paper describes a study of techniques for identifying Higgs bosons at high transverse momenta decaying into bottom-quark pairs, H→bb¯ , for proton–proton collision data collected by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy s√=13 TeV . These decays are reconstructed from calorimeter jets found with the anti- kt R=1.0 jet algorithm. To tag Higgs bosons, a combination of requirements is used: b-tagging of R=0.2 track-jets matched to the large-R calorimeter jet, and requirements on the jet mass and other jet substructure variables. The Higgs boson tagging efficiency and corresponding multijet and hadronic top-quark background rejections are evaluated using Monte Carlo simulation. Several benchmark tagging selections are defined for different signal efficiency targets. The modelling of the relevant input distributions used to tag Higgs bosons is studied in 36 fb −1 of data collected in 2015 and 2016 using g→bb¯ and Z(→bb¯)γ event selections in data. Both processes are found to be well modelled within the statistical and systematic uncertainties
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