281 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â 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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- 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 fbâ1 of â 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
Measurement of VH, H â b b ÂŻ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
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- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
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- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
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- Araque JP
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- Arduh FA
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- Argyropoulos S
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- Armadans RC
- Armbruster AJ
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- Arnold H
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- Artamonov A
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- Zobernig G
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- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fbâ1 of proton-proton collision data at âs =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.âsyst.). The phase ÎŽ â between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be â0.014Ï Â± 0.036Ï (stat.âsyst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] â [â0.36, 0.10] and Im[g R /V L] â [â0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
- Author
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- Zhemchugov A
- Zheng Z
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fbâ1 of sâ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015â2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z â 4â branching fraction is extracted, giving a value of (4.41 ± 0.30) Ă 10â6. Constraints on effective field theory parameters and a model based on a spontaneously broken B â L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Measurement of the transverse polarization of Î and ÎÂŻ hyperons produced in proton-proton collisions at âs=7ââTeV using the ATLAS detector
- Author
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- Merritt FS
- Merritt H
- Messina A
- Metcalfe J
- Mete AS
- Meyer C
- Meyer C
- Meyer J
- Meyer J-P
- Middleton RP
- Migas S
- Miglioranzi S
- Mijovic L
- Mikenberg G
- Mikestikova M
- Mikuz M
- Milic A
- Miller DW
- Mills C
- Milosavljevic MV
- Milov A
- Milstead DA
- Minaenko AA
- Minami Y
- Minashvili IA
- Mincer AI
- Mindur B
- Mineev M
- Ming Y
- Miotto GL
- Mir LM
- Mirabelli G
- Mitani T
- Mitrevski J
- Mitsou VA
- Miucci A
- Miyagawa PS
- Mjornmark JU
- Moa T
- Mochizuki K
- Moenig K
- Mohapatra S
- Mohr W
- Molander S
- Moles-Valls R
- Monini C
- Monk J
- Monnier E
- Monticelli F
- Monzani S
- Moore RW
- Morange N
- Moreno D
- Morettini P
- Morgenstern M
- Morii M
- Morisbak V
- Moritz S
- Morley AK
- Mornacchi G
- Morris JD
- Morton A
- Morvaj L
- Moser HG
- Mosidze M
- Moss J
- Motohashi K
- Mount R
- Mountricha E
- Mouraviev SV
- Moyse EJW
- Muanza S
- Mudd RD
- Mueller F
- Mueller J
- Mueller K
- Mueller T
- Muenstermann D
- Mullen P
- Munwes Y
- Murray WJ
- Musheghyan H
- Musto E
- Myagkov AG
- Myska M
- Nackenhorst O
- Nadal J
- Nagai K
- Nagai R
- Nagai Y
- Nagano K
- Nagarkar A
- Nagasaka Y
- Nagata K
- Nagel M
- Nairz AM
- Nakahama Y
- Nakamura K
- Nakamura T
- Nakano I
- Namasivayam H
- Nanava G
- Narayan R
- Nattermann T
- Naumann T
- Navarro G
- Navarro JEG
- Nayyar R
- Neal HA
- Nechaeva PY
- Nedden MZ
- Neep TJ
- Nef PD
- Negri A
- Negri G
- Negrini M
- Nektarijevic S
- Nellist C
- Nelson A
- Nelson TK
- Nemecek S
- Nemethy P
- Nepomuceno AA
- Nessi M
- Neubauer MS
- Neumann M
- Neves RM
- Nevski P
- Newman PR
- Nguyen DH
- Nickerson RB
- Nicolaidou R
- Nicquevert B
- Nielsen J
- Nikiforou N
- Nikiforov A
- Nikolaenko V
- Nikolic-Audit I
- Nikolics K
- Nikolopoulos K
- Nilsson P
- Ninomiya Y
- Nisati A
- Nisius R
- Nobe T
- Noccioli EB
- Nomachi M
- Nomidis I
- Norberg S
- Nordberg M
- Novgorodova O
- Nowak S
- Nozaki M
- Nozka L
- Ntekas K
- Nunnemann T
- Nurse E
- Nuti F
- O'Brien BJ
- O'grady F
- O'Neil DC
- O'Shea V
- Oakham FG
- Oberlack H
- Obermann T
- Ocariz J
- Ochi A
- Ochoa I
- Oda S
- Odaka S
- Ogren H
- Oh A
- Oh SH
- Ohm CC
- Ohman H
- Oide H
- Okamura W
- Okawa H
- Okumura Y
- Okuyama T
- Olariu A
- Olchevski AG
- Olszewski A
- Olszowska J
- Onofre A
- Onyisi PUE
- Oram CJ
- Oreglia MJ
- Oren Y
- Orestano D
- Orlando N
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- Ortiz NGG
- Ortuzar MC
- Osculati B
- Ospanov R
- Otono H
- Ouchrif M
- Ouellette EA
- Ould-Saada F
- Ouraou A
- Oussoren KP
- Ouyang Q
- Ovcharova A
- Owen M
- Ozcan VE
- Ozturk N
- Pachal K
- Pagacova M
- Paganis E
- Pages AP
- Pahl C
- Paige F
- Pais P
- Pajchel K
- Palacino G
- Palestini S
- Palka M
- Pallin D
- Palma A
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- Pan YB
- Panagiotopoulou E
- Pani P
- Panikashvili N
- Panitkin S
- Pantea D
- Paolozzi L
- Papadopoulou TD
- Papageorgiou K
- Paramonov A
- Paredes BL
- Parker MA
- Parodi AF
- Parodi F
- Parra GG
- Parsons JA
- Parzefall U
- Pasqualucci E
- Passaggio S
- Passeri A
- Pastor ET
- Pastore F
- Pastore F
- Pasztor G
- Pataraia S
- Patel ND
- Pater JR
- Patricelli S
- Pauly T
- Paz IL
- Pearce J
- Pedersen LE
- Pedersen M
- Pedro R
- Peleganchuk SV
- Pelikan D
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- Perepelitsa DV
- Perez MV
- Perez SF
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- Pernegger H
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- Peschke R
- Peshekhonov VD
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
- Petit E
- Petridis A
- Petridou C
- Petrolo E
- Petrucci F
- Pettersson NE
- Pezoa R
- Phillips PW
- Piacquadio G
- Pianori E
- Picazio A
- Piccaro E
- Piccinini M
- Pickering MA
- Piegaia R
- Pignotti DT
- Pilcher JE
- Pilkington AD
- Pina J
- Pinamonti M
- Pinder A
- Pinfold JL
- Pingel A
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- Pinto B
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- Pitt M
- Pizio C
- Plazak L
- Pleier M-A
- Pleskot V
- Plotnikova E
- Plucinski P
- Pluth D
- Poddar S
- Podlyski F
- Poettgen R
- Poggioli L
- Pohl D
- Pohl M
- Polesello G
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Pommes K
- Ponce JMI
- Pontecorvo L
- Pope BG
- Popeneciu GA
- Popovic DS
- Poppleton A
- Pospisil S
- Potamianos K
- Potrap IN
- Potter CJ
- Potter CT
- Poulard G
- Poveda J
- Pozdnyakov V
- Pralavorio P
- Pranko A
- Prasad S
- Prell S
- Price D
- Price J
- Price LE
- Prieur D
- Primavera M
- Prince S
- Proissl M
- Prokofiev K
- Prokoshin F
- Protopapadaki E
- Protopopescu S
- Proudfoot J
- Przybycien M
- Przysiezniak H
- Ptacek E
- Puddu D
- Pueschel E
- Puldon D
- Purohit M
- Puzo P
- Qian J
- Qin G
- Qin Y
- Quadt A
- Quarrie DR
- Quayle WB
- Queitsch-Maitland M
- Quijada JAM
- Quiles AI
- Quilty D
- Qureshi A
- Radeka V
- Radescu V
- Radhakrishnan SK
- Radloff P
- Rados P
- Ragusa F
- Rahal G
- Rajagopalan S
- Rammensee M
- Ramos JAM
- Rangel-Smith C
- Rao K
- Rauscher F
- Rave S
- Rave TC
- Ravenscroft T
- Raymond M
- Read AL
- Readioff NP
- Rebuzzi DM
- Redelbach A
- Redlinger G
- Reece R
- Reeves K
- Rehnisch L
- Reisin H
- Relich M
- Rembser C
- Ren H
- Ren ZL
- Renaud A
- Rescigno M
- Resconi S
- Rezanova OL
- Reznicek P
- Rezvani R
- Richter R
- Richter-Was E
- Ridel M
- Rieck P
- Rieger J
- Rijssenbeek M
- Rimoldi A
- Rinaldi L
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
- Robertson SH
- Robichaud-Veronneau A
- Robinson D
- Robinson JEM
- Robson A
- Roda C
- Rodrigues L
- Roe S
- Rohne O
- Rolli S
- Romaniouk A
- Romano M
- Rompotis N
- Ronzani M
- Roos L
- Ros E
- Rosati S
- Rosbach K
- Rose M
- Rose P
- Rosendahl PL
- Rosenthal O
- Rossetti V
- Rossi E
- Rossi LP
- Rosten R
- Rotaru M
- Roth I
- Rothberg J
- Rousseau D
- Royon CR
- Rozanov A
- Rozen Y
- Ruan X
- Rubbo F
- Rubinskiy I
- Rud VI
- Rudolph C
- Rudolph MS
- Ruehr F
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich NA
- Ruschke A
- Russell HL
- Rutherfoord JP
- Ruthmann N
- Ryabov YF
- Rybar M
- Rybkin G
- Ryder NC
- Saadi DS
- Saavedra AF
- Sabato G
- Sacerdoti S
- Saddique A
- Sadrozinski HF-W
- Sadykov R
- Sakamoto H
- Sakurai Y
- Salamanna G
- Salamon A
- Saleem M
- Salek D
- Salihagic D
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Sampsonidis D
- Sanchez A
- Sanchez J
- Sandaker H
- Sandbach RL
- Sander HG
- Sanders MP
- Sandhoff M
- Sandoval C
- Sandoval T
- Sandstroem R
- Sankey DPC
- Sansoni A
- Santoni C
- Santonico R
- Santos H
- Sapp K
- Sapronov A
- Saraiva JG
- Sarrazin B
- Sartisohn G
- Sasaki O
- Sasaki Y
- Sato K
- Sauvage G
- Sauvan E
- Savage G
- Savard P
- Sawyer C
- Sawyer L
- Saxon DH
- Saxon J
- Sbarra C
- Sbrizzi A
- Scanlon T
- Scannicchio DA
- Scarcella M
- Scarfone V
- Schaarschmidt J
- Schacht P
- Schaefer D
- Schaefer R
- Schaefer U
- Schaepe S
- Schaetzel S
- Schaffer AC
- Schaile D
- Schamberger RD
- Scharf V
- Schegelsky VA
- Scheirich D
- Schernau M
- Schiavi C
- Schieck J
- Schillo C
- Schioppa M
- Schlenker S
- Schmidt E
- Schmieden K
- Schmitt C
- Schmitt S
- Schneider B
- Schnellbach YJ
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schorlemmer ALS
- Schott M
- Schouten D
- Schovancova J
- Schramm S
- Schreyer M
- Schroeder C
- Schroeder TV
- Schuh N
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwanenberger C
- Schwartzman A
- Schwarz TA
- Schwegler P
- Schwemling P
- Schwienhorst R
- Schwindling J
- Schwindt T
- Schwoerer M
- Sciacca FG
- Scifo E
- Sciolla G
- Scuri F
- Scutti F
- Searcy J
- Sedov G
- Sedykh E
- Seema P
- Seidel SC
- Seiden A
- Seifert F
- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Selbach KE
- Seliverstov DM
- Sellers G
- Semprini-Cesari N
- Serfon C
- Serin L
- Serkin L
- Serre T
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shamim M
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Shatalov PB
- Shaw K
- Shcherbakova A
- Shehu CY
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shiyakova M
- Shmeleva A
- Shochet MJ
- Shojaii S
- Short D
- Shrestha S
- Shulga E
- Shupe MA
- Shushkevich S
- Sicho P
- Sidiropoulou O
- Sidorov D
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silver Y
- Silverstein D
- Silverstein SB
- Simak V
- Simard O
- Simic L
- Simion S
- Simioni E
- Simmons B
- Simon D
- Simoniello R
- Sinervo P
- Sinev NB
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjolin J
- Sjursen TB
- Skottowe HP
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith KM
- Smith M
- Smizanska M
- Smolek K
- Snesarev AA
- Snidero G
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Solans CA
- Solar M
- Solc J
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Song HY
- Soni N
- Sood A
- Sopczak A
- Sopko B
- Sopko V
- Sorin V
- Sosa D
- Sosebee M
- Soualah R
- Soueid P
- Soukharev AM
- South D
- Spagnolo S
- Spano F
- Spearman WR
- Spettel F
- Spighi R
- Spigo G
- Spiller LA
- Spousta M
- Spreitzer T
- St Denis RD
- Staerz S
- Stahlman J
- Stamen R
- Stamm S
- Stanecka E
- Stanescu C
- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Stavina P
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stern S
- Stewart GA
- Stillings JA
- Stockton MC
- Stoebe M
- Stoicea G
- Stolte P
- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strandlie A
- Strauss E
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Svatos M
- Swedish S
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
- Taccini C
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tam JYC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tannenwald BB
- Tannoury N
- Tapprogge S
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor FE
- Taylor GN
- Taylor W
- Tehrani FS
- Teischinger FA
- Teixeira-Dias P
- Temming KK
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson RJ
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisserant S
- Todorov T
- Todorova-Nova S
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
- Tolley E
- Tomlinson L
- Tomoto M
- Tompkins L
- Toms K
- Topilin ND
- Toro RC
- Torregrosa EF
- Torrence E
- Torres H
- Toth J
- Touchard F
- Tovey DR
- Tran HL
- Trefzger T
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- True P
- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turra R
- Turvey AJ
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Ueda I
- Ueno R
- Ughetto M
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urban J
- Urbaniec D
- Urquijo P
- Usai G
- Usanova A
- Vacavant L
- Vacek V
- Vachon B
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallecorsa S
- Van den Wollenberg W
- Van der Deijl PC
- Van der Geer R
- Van der Graaf H
- Van der Leeuw R
- Van der Ster D
- Van Eldik N
- Van Gemmeren P
- Van Huysduynen LH
- Van Nieuwkoop J
- Van Vulpen I
- Van Woerden MC
- Vanadia M
- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloso F
- Velz T
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Verzini MJA
- Vest A
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigne R
- Villa M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Virzi J
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- Von der Schmitt H
- Von Radziewski H
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
- Walker R
- Walkowiak W
- Wall R
- Waller P
- Walls FMG
- Walsh B
- Wang C
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang X
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watkins PM
- Watson AT
- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb S
- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Wessels M
- Wetter J
- Whalen K
- White A
- White MJ
- White R
- White S
- Whiteson D
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson A
- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wright M
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xiao M
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamada M
- Yamaguchi H
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2014
- Field of study
The transverse polarization of Î and ÎÂŻ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760ââÎŒbâ1 of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5Ă10â5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is â0.010±0.005(stat)±0.004(syst) for Î and 0.002±0.006(stat)±0.004(syst) for ÎÂŻ. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement
Measurement of the W±Z boson pair-production cross section in pp collisions at âs=13TeV with the ATLAS detector
- Author
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- Youssef S
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- Yusuff I
- Zabinski B
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- Zakharchuk N
- Zalieckas J
- Zaman A
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- Zanzi D
- Zeitnitz C
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- Zemla A
- Zeng JC
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- Zenin O
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- Zerwas D
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou M
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- Zhu CG
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- Netherlands
- Publication date
- 01/01/2016
- Field of study
published_or_final_versio
Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
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- Acharya BS
- Adam ER
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- Akesson TP
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- Alberghi GL
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- Alconada Verzini MJ
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- Aleksandrov IN
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- Allbrooke BMM
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- Antonaki A
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- Arce ATH
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- Ashkenazi A
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- Astalos R
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
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- Azuelos G
- Azuma Y
- Baak MA
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- Bacci C
- Bachacou H
- Bachas K
- Backes M
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- Badescu E
- Bagiacchi P
- Bagnaia P
- Bai Y
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- Baker OK
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- Chalupkova I
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
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- Chen C
- Chen H
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- Chen X
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- Cheng HC
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- Cheplakov A
- Chernyatin V
- Cheu E
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- Chiarella V
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- Childers JT
- Chilingarov A
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- Czyczula Z
- D'Auria S
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Via C
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- Dafinca A
- Dai T
- Dale O
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- Dam M
- Damazio DO
- Daniells AC
- Dao V
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- de Andrade Filho LM
- de Asmundis R
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- De Groot N
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- De la Torre H
- de Lima DEF
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- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
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- Dearnaley WJ
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- Deliot F
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- Delmastro M
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- Deviveiros PO
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- Zanzi D
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- Zhemchugov A
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- Zibell A
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- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5ââfb[superscript â1] of proton-proton collisions data at âs=7ââTeV and 20.3ââfb[superscript â1] at âs=8ââTeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be ÎŒ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4ââGeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be ÎŒ[subscript ggF]=1.32±0.38, ÎŒ[subscript VBF]=0.8±0.7, ÎŒ[subscript WH]=1.0±1.6, ÎŒ[subscript ZH]=0.1[superscript +3.7 subscript â0.1], and ÎŒ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript â1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Search for pair production of third-generation scalar leptoquarks decaying into a top quark and a Ï-lepton in pp collisions at sâ = 13 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
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- 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
- Akbiyik M
- 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
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- Ali B
- Ali S
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- Allaire C
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- Allen BW
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- Yildiz HD
- Yin P
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- Yoshihara K
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- Yue X
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- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- 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
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- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 30/06/2021
- Field of study
A search for pair production of third-generation scalar leptoquarks decaying into a top quark and a Ï-lepton is presented. The search is based on a dataset of pp collisions at sâ = 13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fbâ1. Events are selected if they have one light lepton (electron or muon) and at least one hadronically decaying Ï -lepton, or at least two light leptons. In addition, two or more jets, at least one of which must be identified as containing b-hadrons, are required. Six final states, defined by the multiplicity and flavour of lepton candidates, are considered in the analysis. Each of them is split into multiple event categories to simultaneously search for the signal and constrain several leading backgrounds. The signal-rich event categories require at least one hadronically decaying Ï-lepton candidate and exploit the presence of energetic final-state objects, which is characteristic of signal events. No significant excess above the Standard Model expectation is observed in any of the considered event categories, and 95% CL upper limits are set on the production cross section as a function of the leptoquark mass, for different assumptions about the branching fractions into tÏ and bÎœ. Scalar leptoquarks decaying exclusively into tÏ are excluded up to masses of 1.43 TeV while, for a branching fraction of 50% into tÏ, the lower mass limit is 1.22 TeV
Measurement of the ttÌW and ttÌZ production cross sections in pp collisions at âs = 8 TeV with the ATLAS detector
- Author
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
The production cross sections of top-quark pairs in association with massive vector bosons have been measured using data from pp collisions at sâ = 8 TeV. The dataset corresponds to an integrated luminosity of 20.3 fbâÂč collected by the ATLAS detector in 2012 at the LHC. Final states with two, three or four leptons are considered. A fit to the data considering the ttÌW and ttÌZ processes simultaneously yields a significance of 5.0Ï (4.2Ï) over the background-only hypothesis for ttÂŻWttÂŻW (ttÌZ) production. The measured cross sections are ÏttÌW = 369 + 100â91 fb and ÏttÌZ = 176 + 58â52 fb. The background-only hypothesis with neither ttÌW nor ttÌZ production is excluded at 7.1Ï. All measurements are consistent with next-to-leading-order calculations for the ttÌW and ttÌZ processes
Measurement of the inelastic proton-proton cross section at âs=13 TeV with the ATLAS detector at the LHC
- Author
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
This Letter presents a measurement of the inelastic proton-proton cross section using 60ââÎŒb â1 of pp collisions at a center-of-mass energy âs of 13 TeV with the ATLAS detector at the LHC. Inelastic interactions are selected using rings of plastic scintillators in the forward region (2.0710 â6 , where M X is the larger invariant mass of the two hadronic systems separated by the largest rapidity gap in the event. In this Ο range the scintillators are highly efficient. For diffractive events this corresponds to cases where at least one proton dissociates to a system with M X >13ââGeV . The measured cross section is compared with a range of theoretical predictions. When extrapolated to the full phase space, a cross section of 78.1±2.9ââmb is measured, consistent with the inelastic cross section increasing with center-of-mass energy
- âŠ