65 research outputs found
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
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- Bellagamba L
- Bellerive A
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- Beltramello O
- Belyaev NL
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- Benchekroun D
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- Bendtz K
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- Benitez J
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- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particle–hole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Performance of the ATLAS Transition Radiation Tracker in Run 1 of the LHC: tracker properties
- Author
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- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- Abidi SH
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2017
- Field of study
he tracking performance parameters of the ATLAS Transition Radiation Tracker (TRT) as part of the ATLAS inner detector are described in this paper for different data-taking conditions in proton-proton, proton-lead and lead-lead collisions at the Large Hadron Collider (LHC). The performance is studied using data collected during the first period of LHC operation (Run 1) and is compared with Monte Carlo simulations. The performance of the TRT, operating with two different gas mixtures (xenon-based and argon-based) and its dependence on the TRT occupancy is presented. These studies show that the tracking performance of the TRT is similar for the two gas mixtures and that a significant contribution to the particle momentum resolution is made by the TRT up to high particle densities.We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently.info:eu-repo/semantics/publishedVersio
Search for resonances in diphoton events at √s = 13 TeV with the ATLAS detector
- Author
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- Aad G
- Abbott B
- Abdallah J
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- Mccarthy Tg
- Mcclymont Li
- Mcdonald Ef
- Mcfayden Ja
- Mchedlidze G
- Mcmahon Sj
- Mcpherson Ra
- Medinnis M
- Meehan S
- Mehlhase S
- Mehta A
- Meideck T
- Meier K
- Meineck C
- Meirose B
- Melini D
- Mellado Garcia Br
- Melo M
- Meloni F
- Mengarelli A
- Menke S
- Meoni E
- Mergelmeyer S
- Mermod P
- Merola L
- Meroni C
- Merritt Fs
- Messina A
- Metcalfe J
- Mete As
- Meyer Zu Theenhausen H
- Meyer C
- Meyer C
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- Meyer J-
- Miano F
- Middleton Rp
- Miglioranzi S
- Mijovic L
- Mikenberg G
- Mikestikova M
- Mikuz M
- Milesi M
- Milic A
- Miller Dw
- Mills C
- Milov A
- Milstead Da
- Minaenko Aa
- Minami Y
- Minashvili Ia
- Mincer Ai
- Mindur B
- Mineev M
- Ming Y
- Mir Lm
- Mistry Kp
- Mitani T
- Mitrevski J
- Mitsou Va
- Miucci A
- Miyagawa Ps
- Mjornmark Ju
- Moa T
- Mochizuki K
- Mohapatra S
- Molander S
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- Monden R
- Mondragon Mc
- Monig K
- Monk J
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- Montejo Berlingen J
- Monticelli F
- Monzani S
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- Moreno Llacer M
- Moreno D
- Morettini P
- Mori D
- Mori T
- Morii M
- Morinaga M
- Morisbak V
- Moritz S
- Morley Ak
- Mornacchi G
- Morris Jd
- Mortensen Ss
- Morvaj L
- Mosidze M
- Moss J
- Motohashi K
- Mount R
- Mountricha E
- Mouraviev Sv
- Moyse Ejw
- Muanza S
- Mudd Rd
- Mueller F
- Mueller J
- Mueller Rsp
- Mueller T
- Muenstermann D
- Mullen P
- Mullier Ga
- Munoz Sanchez Fj
- Murillo Quijada Ja
- Murray Wj
- Musheghyan H
- Muskinja M
- Myagkov Ag
- Myska M
- Nachman Bp
- Nackenhorst O
- Nagai K
- Nagai R
- Nagano K
- Nagasaka Y
- Nagata K
- Nagel M
- Nagy E
- Nairz Am
- Nakahama Y
- Nakamura K
- Nakamura T
- Nakano I
- Namasivayam H
- Naranjo Garcia Rf
- Narayan R
- Narrias Villar Di
- Naryshkin I
- Naumann T
- Navarro G
- Nayyar R
- Neal Ha
- Nechaeva Py
- Neep Tj
- Negri A
- Negrini M
- Nektarijevic S
- Nellist C
- Nelson A
- Nemecek S
- Nemethy P
- Nepomuceno Aa
- Nessi M
- Neubauer Ms
- Neumann M
- Neves Rm
- Nevski P
- Newman Pr
- Nguyen Manh T
- Nguyen Dh
- Nickerson Rb
- Nicolaidou R
- Nielsen J
- Nikiforov A
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsen Jk
- Nilsson P
- Ninomiya Y
- Nisati A
- Nisius R
- Nobe T
- Nomachi M
- Nomidis I
- Nooney T
- Norberg S
- Nordberg M
- Norjoharuddeen N
- Novgorodova O
- Nowak S
- Nozaki M
- Nozka L
- Ntekas K
- Nurse E
- Nuti F
- O'Grady F
- O'Neil Dc
- O'Rourke Aa
- O'Shea V
- Oakham Fg
- Oberlack H
- Obermann T
- Ocariz J
- Ochi A
- Ochoa I
- Ochoa-Ricoux Jp
- Oda S
- Odaka S
- Ogren H
- Oh A
- Oh Sh
- Ohm Cc
- Ohman H
- Oide H
- Okawa H
- Okumura Y
- Okuyama T
- Olariu A
- Oleiro Seabra Lf
- Olivares Pino Sa
- Oliveira Damazio D
- Olszewski A
- Olszowska J
- Onofre A
- Onogi K
- Onyisi Pue
- Oreglia Mj
- Oren Y
- Orestano D
- Orlando N
- Orr Rs
- Osculati B
- Ospanov R
- Otero Ygg
- Otono H
- Ouchrif M
- Ould-Saada F
- Ouraou A
- Oussoren Kp
- Ouyang Q
- Owen M
- Owen Re
- Ozcan Ve
- Ozturk N
- Pachal K
- Pacheco Pages A
- Pacheco Rodriguez L
- Padilla Aranda C
- Pagacova M
- Pagan Griso S
- Paige F
- Pais P
- Pajchel K
- Palacino G
- Palazzo S
- Palestini S
- Palka M
- Pallin D
- Pandini Ce
- Panduro Vazquez Jg
- Pani P
- Panitkin S
- Pantea D
- Paolozzi L
- Papadopoulou Td
- Papageorgiou K
- Paramonov A
- Paredes Hernandez D
- Parker Aj
- Parker Ka
- Parker Ma
- Parodi F
- Parsons Ja
- Parzefall U
- Pascuzzi Vr
- Pasqualucci E
- Passaggio S
- Pastore F
- Pasztor G
- Pataraia S
- Pater Jr
- Pauly T
- Pearce J
- Pearson B
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- Pedersen M
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- Penc O
- Peng C
- Peng H
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- Peralva Bs
- Perego Mm
- Perepelitsa Dv
- Perez Codina E
- Perini L
- Pernegger H
- Perrella S
- Peschke R
- Peshekhonov Vd
- Peters K
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- Petersen Ba
- Petersen Tc
- Petit E
- Petridis A
- Petridou C
- Petroff P
- Petrolo E
- Petrov M
- Petrucci F
- Pettersson Ne
- Peyaud A
- Pezoa R
- Phillips Pw
- Piacquadio G
- Pianori E
- Picazio A
- Piccaro E
- Piccinini M
- Pickering Ma
- Piegaia R
- Pilcher Je
- Pilkington Ad
- Pin Awj
- Pinamonti M
- Pinfold Jl
- Pingel A
- Pires S
- Pirumov H
- Pitt M
- Plazak L
- Pleier M-
- Pleskot V
- Plotnikova E
- Plucinski P
- Pluth D
- Poettgen R
- Poggioli L
- Pohl D
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard Cs
- Polychronakos V
- Pommes K
- 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
- Pozo Astigarraga Me
- Pralavorio P
- Pranko A
- Prell S
- Price D
- Price Le
- Primavera M
- Prince S
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Puddu D
- Purohit M
- Puzo P
- Qian J
- Qin G
- Qin Y
- Quadt A
- Quayle Wb
- Queitsch-Maitland M
- Quilty D
- Raddum S
- Radeka V
- Radescu V
- Radhakrishnan Sk
- Radloff P
- Rados P
- Ragusa F
- Rahal G
- Raine Ja
- Rajagopalan S
- Rammensee M
- Rangel-Smith C
- Ratti Mg
- Rauscher F
- Rave S
- Ravenscroft T
- Ravinovich I
- Raymond M
- Read Al
- Readioff Np
- Reale M
- Rebuzzi Dm
- Redelbach A
- Redlinger G
- Reece R
- Reeves K
- Rehnisch L
- Reichert J
- Reisin H
- Rembser C
- Ren H
- Rescigno M
- Resconi S
- Rezanova Ol
- Reznicek P
- Rezvani R
- Richter R
- Richter S
- Richter-Was E
- Ricken O
- Ridel M
- Rieck P
- Riegel Cj
- Rieger J
- Rifki O
- Rijssenbeek M
- Rimoldi A
- Rimoldi M
- Rinaldi L
- Ristic B
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
- Rizzi C
- Robertson Sh
- Robichaud-Veronneau A
- Robinson D
- Robinson Jem
- Robson A
- Roda C
- Rodina Y
- Rodriguez Perez A
- Rodriguez Rodriguez D
- Roe S
- Rogan Cs
- Rohne O
- Romaniouk A
- Romano Saez Sm
- Romano M
- Romero Adam E
- Rompotis N
- Ronzani M
- Roos L
- Ros E
- Rosati S
- Rosbach K
- Rose P
- Rosenthal O
- Rosien N-
- Rossetti V
- Rossi E
- Rossi Lp
- Rosten Jhn
- Rosten R
- Rotaru M
- Roth I
- Rothberg J
- Rousseau D
- Royon Cr
- Rozanov A
- Rozen Y
- Ruan X
- Rubbo F
- Rudolph Ms
- Ruhr F
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich Na
- Ruschke A
- Russell Hl
- Rutherfoord Jp
- Ruthmann N
- Ryabov Yf
- Rybar M
- Rybkin G
- Ryu S
- Ryzhov A
- Rzehorz Gf
- Saavedra Af
- Sabato G
- Sacerdoti S
- Sadrozinski HF-
- Sadykov R
- Safai Tehrani F
- Saha P
- Sahinsoy M
- Saimpert M
- Saito T
- Sakamoto H
- Sakurai Y
- Salamanna G
- Salamon A
- Salazar Loyola Je
- Salek D
- Sales De Bruin Ph
- Salihagic D
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Sammel D
- Sampsonidis D
- Sanchez Martinez V
- Sanchez A
- Sanchez J
- Sandaker H
- Sandbach Rl
- Sander Hg
- Sandhoff M
- Sandoval C
- Sandstroem R
- Sankey Dpc
- Sannino M
- Sansoni A
- Santoni C
- Santonico R
- Santos H
- Santoyo Castillo I
- Sapp K
- Sapronov A
- Saraiva Jg
- Sarrazin B
- Sasaki O
- Sasaki Y
- Sato K
- Sauvage G
- Sauvan E
- Savage G
- Savard P
- Savic N
- Sawyer C
- Sawyer L
- Saxon J
- Sbarra C
- Sbrizzi A
- Scanlon T
- Scannicchio Da
- Scarcella M
- Scarfone V
- Schaarschmidt J
- Schacht P
- Schachtner Bm
- Schaefer D
- Schaefer R
- Schaeffer J
- Schaepe S
- Schaetzel S
- Schafer U
- Schaffer Ac
- Schaile D
- Schamberger Rd
- Scharf V
- Schegelsky Va
- Scheirich D
- Schernau M
- Schiavi C
- Schier S
- Schillo C
- Schioppa M
- Schlenker S
- Schmidt-Sommerfeld Kr
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schneider B
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock Bd
- Schopf E
- Schott M
- Schovancova J
- Schramm S
- Schreyer M
- Schuh N
- Schulte A
- Schultens Mj
- Schultz-Coulon H-
- Schulz H
- Schumacher M
- Schumm Ba
- Schune P
- Schwartzman A
- Schwarz Ta
- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
- Schwindt T
- Sciolla G
- Scuri F
- Scutti F
- Searcy J
- Seema P
- Seidel Sc
- Seiden A
- Seifert F
- Seixas Jm
- Sekhniaidze G
- Sekhon K
- Sekula Sj
- Seliverstov Dm
- Semprini-Cesari N
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Seuster R
- Severini H
- Sfiligoj T
- 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
- Sherwood P
- Shi L
- Shimizu S
- Shimmin Co
- Shimojima M
- Shiyakova M
- Shmeleva A
- Shoaleh Saadi D
- Shochet Mj
- Shojaii S
- Shrestha S
- Shulga E
- Shupe Ma
- Sicho P
- Sickles Am
- Sidebo Pe
- Sidiropoulou O
- Sidorov D
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silverstein Sb
- Simak V
- Simic L
- Simion S
- Simioni E
- Simmons B
- Simon D
- Simon M
- Sinervo P
- Sinev Nb
- Sioli M
- Siragusa G
- Sivoklokov Sy
- Sjolin J
- Skinner Mb
- Skottowe Hp
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart Bh
- Smestad L
- Smiesko J
- Smirnov Sy
- Smirnov Y
- Smirnova Ln
- Smirnova O
- Smith Mnk
- Smith Rw
- Smizanska M
- Smolek K
- Snesarev Aa
- 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
- Song Hy
- Sood A
- Sopczak A
- Sopko V
- Sorin V
- Sosa D
- Sotiropoulou Cl
- Soualah R
- Soukharev Am
- South D
- Sowden Bc
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spettel F
- Spighi R
- Spigo G
- Spiller La
- Spousta M
- St Denis Sdrd
- St Panagiotopoulou Spe
- Stabile A
- Stamen R
- Stamm S
- Stanecka E
- Stanek Rw
- Stanescu C
- Stanescu-Bellu M
- Stanitzki Mm
- Stapnes S
- Starchenko Ea
- Stark Gh
- Stark J
- Staroba P
- Starovoitov P
- Starz S
- Staszewski R
- Steinberg P
- Stelzer B
- Stelzer Hj
- Stelzer-Chilton O
- Stenzel H
- 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 M
- Strizenec P
- Strohmer R
- Strom Dm
- Stroynowski R
- Strubig A
- Stucci Sa
- Stugu B
- Styles Na
- Su D
- Su J
- Suchek S
- Sugaya Y
- Suk M
- Sulin Vv
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Sundermann Je
- Suruliz K
- Susinno G
- Sutton Mr
- Suzuki S
- Svatos M
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
- Taccini C
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
- Takai H
- Takashima R
- Takeshita T
- Takubo Y
- Talby M
- Talyshev Aa
- Tan Kg
- Tanaka J
- Tanaka M
- Tanaka R
- Tanaka S
- Tannenwald Bb
- Tapia Araya S
- Tapprogge S
- Tarem S
- Tartarelli Gf
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor Ac
- Taylor Gn
- Taylor Pte
- Taylor W
- Teischinger Fa
- Teixeira-Dias P
- Temming Kk
- Temple D
- Ten Kate H
- Teng Pk
- Teoh Jj
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher Rj
- The Ac
- Theveneaux-Pelzer T
- Thomas Jp
- Thomas-Wilsker J
- Thompson As
- Thompson En
- Thompson Pd
- Thomsen La
- Thomson E
- Thomson M
- Tibbetts Mj
- Ticse Torres Re
- Tikhomirov Vo
- Tikhonov Ya
- Timoshenko S
- Tipton P
- Tisserant S
- Todome K
- Todorov T
- Todorova-Nova S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
- Tomlinson L
- Tomoto M
- Tompkins L
- Toms K
- Tong B
- Torrence E
- Torres H
- Torro Pastor E
- Toth J
- Touchard F
- Tovey Dr
- Trefzger T
- Tricoli A
- Trigger Im
- Trincaz-Duvoid S
- Tripiana Mf
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- Truong L
- Trzebinski M
- Trzupek A
- Tseng JC-
- Tsiareshka Pv
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze Eg
- Tsui Km
- Tsukerman Ii
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna An
- Tupputi Sa
- Turchikhin S
- Turecek D
- Turgeman D
- Turra R
- Turvey Aj
- Tuts Pm
- Tyndel M
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro Fc
- Unno Y
- Unverdorben C
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Usanova A
- Vacavant L
- Vacek V
- Vachon B
- Valderanis C
- Valdes Santurio E
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallier A
- Valls Ferrer Ja
- Van Den Wollenberg W
- Van Der Deijl Pc
- van der Graaf H
- van Eldik N
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- van Woerden Mc
- Vanadia M
- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes Ew
- Varol T
- Varouchas D
- Vartapetian A
- Varvell Ke
- Vasquez Jg
- Vazeille F
- Vazquez Schroeder T
- Veatch J
- Veeraraghavan V
- Veloce Lm
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen Jc
- Vest A
- Vetterli Mc
- 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
- Vittori C
- Vivarelli I
- Vlachos S
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- 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
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Wang C
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang K
- Wang R
- Wang Sm
- Wang T
- Wang T
- Wang W
- Wang X
- Wanotayaroj C
- Warburton A
- Ward Cp
- Wardrope Dr
- Washbrook A
- Watkins Pm
- Watson At
- 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
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner Md
- Werner P
- Wessels M
- Wetter J
- Whalen K
- Whallon Nl
- Wharton Am
- White A
- White Mj
- White R
- Whiteson D
- Wickens Fj
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs Lam
- Wildauer A
- Wilk F
- Wilkens Hg
- Williams Hh
- Williams S
- Willis C
- Willocq S
- Wilson Ja
- Wingerter-Seez I
- Winklmeier F
- Winston Oj
- Winter Bt
- Wittgen M
- Wittkowski J
- Wolf Tmh
- Wolter Mw
- Wolters H
- Worm Sd
- Wosiek Bk
- Wotschack J
- Woudstra Mj
- Wozniak Kw
- Wu M
- Wu M
- Wu Sl
- Wu X
- Wu Y
- Wyatt Tr
- Wynne Bm
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-
- Yap Yc
- Yasu Y
- Yatsenko E
- Yau Wong Kh
- Ye J
- Ye S
- Yeletskikh I
- Yen Al
- Yildirim E
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young Cjs
- Youssef S
- Yu Dr
- Yu J
- Yu J
- Yu Jm
- Yuan L
- Yuen Spy
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev Am
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng Jc
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- 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 M
- Zhou N
- 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
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Searches for new resonances decaying into two photons in the ATLAS experiment at the CERN Large Hadron Collider are described. The analysis is based on proton-proton collision data corresponding to an integrated luminosity of 3.2 fb−1 at s√=13 TeV recorded in 2015. Two searches are performed, one targeted at a spin-2 particle of mass larger than 500 GeV, using Randall-Sundrum graviton states as a benchmark model, and one optimized for a spin-0 particle of mass larger than 200 GeV. Varying both the mass and the decay width, the most significant deviation from the background-only hypothesis is observed at a diphoton invariant mass around 750 GeV with local significances of 3.8 and 3.9 standard deviations in the searches optimized for a spin-2 and spin-0 particle, respectively. The global significances are estimated to be 2.1 standard deviations for both analyses. The consistency between the data collected at 13 TeV and 8 TeV is also evaluated. Limits on the production cross section times branching ratio to two photons for the two resonance types are reported
Measurements of top-quark pair differential cross-sections in the lepton plus jets channel in pp collisions at root s=8 TeV using the ATLAS detector
- Author
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- Zibell A
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Measurements of normalized differential cross-sections of top-quark pair production are presented as a function of the top-quark, tt¯tt¯ system and event-level kinematic observables in proton–proton collisions at a centre-of-mass energy of s√=8TeVs=8TeV . The observables have been chosen to emphasize the tt¯tt¯ production process and to be sensitive to effects of initial- and final-state radiation, to the different parton distribution functions, and to non-resonant processes and higher-order corrections. The dataset corresponds to an integrated luminosity of 20.3 fb −1−1 , recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of the jets tagged as originating from a b-quark. The measured spectra are corrected for detector effects and are compared to several Monte Carlo simulations. The results are in fair agreement with the predictions over a wide kinematic range. Nevertheless, most generators predict a harder top-quark transverse momentum distribution at high values than what is observed in the data. Predictions beyond NLO accuracy improve the agreement with data at high top-quark transverse momenta. Using the current settings and parton distribution functions, the rapidity distributions are not well modelled by any generator under consideration. However, the level of agreement is improved when more recent sets of parton distribution functions are used
Erratum to: Measurement of the W boson polarisation in tt^{¯} events from pp collisions at √s = 8 TeV in the lepton + jets channel with Atlas
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- Zieminska D
- Zimine NI
- Zimmermann C
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- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
1 Erratum to: Eur. Phys. J. C (2017) 77:264 [https://doi.org/10.1140/epjc/s10052-017-4819-4]. The original article can be found online at [https://doi.org/10.1140/epjc/s10052-017-4819-4]
Measurement of the W-boson mass in pp collisions at s√=7TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam E Romero
- Adamczyk L
- Adams DL
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich L Cerda
- Albert J
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
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- Alviggi MG
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- Anderson KJ
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- Aoki M
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- Araya S Tapia
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 18/12/2017
- Field of study
A measurement of the mass of the W boson is presented based on proton–proton collision data recorded in 2011 at a centre-of-mass energy of 7 TeV with the ATLAS detector at the LHC, and corresponding to 4.6 fb−1 of integrated luminosity. The selected data sample consists of 7.8×106 candidates in the W→μν channel and 5.9×106 candidates in the W→eν channel. The W-boson mass is obtained from template fits to the reconstructed distributions of the charged lepton transverse momentum and of the W boson transverse mass in the electron and muon decay channels, yielding mW=80370=80370±7 (stat.)±11(exp. syst.)±14 (mod. syst.) MeV±19MeV, where the first uncertainty is statistical, the second corresponds to the experimental systematic uncertainty, and the third to the physics-modelling systematic uncertainty. A measurement of the mass difference between the W+ and W− bosons yields mW+−mW−=−29±28 MeV
Performance of algorithms that reconstruct missing transverse momentum in √s= 8 TeV proton-proton collisions in the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
The reconstruction and calibration algorithms used to calculate missing transverse momentum (EmissT ) with the ATLAS detector exploit energy deposits in the calorimeter and tracks reconstructed in the inner detector as well as the muon spectrometer. Various strategies are used to suppress effects arising from additional proton–proton interactions, called pileup, concurrent with the hard-scatter processes. Tracking information is used to distinguish contributions from the pileup interactions using their vertex separation along the beam axis. The performance of the EmissT reconstruction algorithms, especially with respect to the amount of pileup, is evaluated using data collected in proton–proton collisions at a centre-of-mass energy of 8 TeV during 2012, and results are shown for a data sample corresponding to an integrated luminosity of 20.3fb−1. The simulation and modelling of EmissT in events containing a Z boson decaying to two charged leptons (electrons or muons) or a W boson decaying to a charged lepton and a neutrino are compared to data. The acceptance for different event topologies, with and without high transverse momentum neutrinos, is shown for a range of threshold criteria for EmissT , and estimates of the systematic uncertainties in the EmissT measurements are presented.ATLAS Collaboration, for complete list of authors see dx.doi.org/10.1140/epjc/s10052-017-4780-2Funding: We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently.We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, HGF, and MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; RCN, Norway; MNiSW and NCN, Poland; FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, UK; DOE and NSF, United States of America. In addition, individual groups and members have received support from BCKDF, the Canada Council, CANARIE, CRC, Compute Canada, FQRNT, and the Ontario Innovation Trust, Canada; EPLANET, ERC, FP7, Horizon 2020 and Marie Skłodowska-Curie Actions, European Union; Investissements d’Avenir Labex and Idex, ANR, Région Auvergne and Fondation Partager le Savoir, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF; BSF, GIF and Minerva, Israel; BRF, Norway; Generalitat de Catalunya, Generalitat Valenciana, Spain; the Royal Society and Leverhulme Trust, United Kingdom. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN, the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA), the Tier-2 facilities worldwide and large non-WLCG resource providers. Major contributors of computing resources are listed in Ref. [58].</p
China's Strategy of Sending Students Abroad under the Modernization Policy
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- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- Sykora I
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- Tsiareshka PV
- Tsipolitis G
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- Tsiskaridze S
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- Tskhadadze EG
- Tsui KM
- Tsukerman II
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- Vilucchi E
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- Vinogradov VB
- Vittori C
- Vivarelli I
- Vlachos S
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- Volpi G
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- von der Schmitt H
- von Toerne E
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- Vukotic I
- Vykydal Z
- Wagner P
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- Wanotayaroj C
- Warburton A
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- Weingarten J
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- Wickens FJ
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- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
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- Wilkens HG
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- Williams S
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- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wittkowski J
- Wolf TMH
- Wolter MW
- Wolters H
- Wong KH Yau
- Worm SD
- Wosiek BK
- Wotschack J
- Woudstra MJ
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- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yuen SPY
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- 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 M
- Zhou N
- 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
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Wiley'
- Publication date
- 01/09/1994
- Field of study
See paper for full list of authors, 24 pages plus author list + cover pages (43 pages total), 6 figures, 5 tables, submitted to JHEP.International audienceA measurement of the t-channel single-top-quark and single-top-antiquark production cross-sections in the lepton+je ts channel is presented, using 3.2 fb−1 of proton--proton collision data at a centre-of-mass energy of 13 TeV, recorded with the ATLAS detector at the LHC in 2015. Events are selected by requiring one charged lepton (electron or muon), missing transverse momentum, and two jets with high transverse momentum, exactly one of which is required to be b-tagged. Using a binned maximum-likelihood fit to the discriminant distribution of a neural network, the cross-sections are determined to be σ(tq)=156±5(stat.)±27(syst.)±3(lumi.) pb for single top-quark production and σ(t¯q)=91±4(stat.)±18(syst.)±2(lumi.) pb for single top-antiquark production, assuming a top-quark mass of 172.5 GeV. The cross-section ratio is measured to be Rt=σ(tq)/σ(t¯q)=1.72±0.09(stat.)±0.18(syst.)
Measurements of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Z</mml:mi><mml:mi>γ</mml:mi></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Z</mml:mi><mml:mi>γ</mml:mi><mml:mi>γ</mml:mi></mml:math>production in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:math>collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mn>8</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>TeV</mml:mi></mml:math>with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- Abolins M
- AbouZeid OS
- Abraham NL
- 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
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- Akimov AV
- Alberghi GL
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- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
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- Alhroob M
- Aliev M
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- Alison J
- Alkire SP
- Allbrooke BMM
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- Allport PP
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- Alviggi MG
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
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- Åkesson TPA
- Åsman B
- Ženiš T
- Živković L
- Publication venue
- American Physical Society (APS)
- Publication date
- 01/01/2016
- Field of study
The production of Z bosons with one or two isolated high-energy photons is studied using pp collisions at s=8 TeV. The analyses use a data sample with an integrated luminosity of 20.3 fb-1 collected by the ATLAS detector during the 2012 LHC data taking. The Zγ and Zγγ production cross sections are measured with leptonic (e+e-, μ+μ-, νν) decays of the Z boson, in extended fiducial regions defined in terms of the lepton and photon acceptance. They are then compared to cross-section predictions from the Standard Model, where the sources of the photons are radiation off initial-state quarks and radiative Z-boson decay to charged leptons, and from fragmentation of final-state quarks and gluons into photons. The yields of events with photon transverse energy ET>250 GeV from +-γ events and with ET>400 GeV from ννγ events are used to search for anomalous triple gauge-boson couplings ZZγ and Zγγ. The yields of events with diphoton invariant mass mγγ>200 GeV from +-γγ events and with mγγ>300 GeV from ννγγ events are used to search for anomalous quartic gauge-boson couplings ZZγγ and Zγγγ. No deviations from Standard Model predictions are observed and limits are placed on parameters used to describe anomalous triple and quartic gauge-boson couplings
Search for triboson W±W±W∓ production in pp collisions at √s = 8 TeV with the ATLAS detector
- Author
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- Aad G
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- Publication venue
- Publication date
- 01/03/2017
- Field of study
This paper reports a search for triboson
W±W±W∓ production in two decay channels
(W±W±W∓ → ±ν±ν∓ν and W±W±W∓ → ±ν±ν j j
with = e, μ) in proton-proton collision data corresponding
to an integrated luminosity of 20.3 fb−1 at a centreof-mass
energy of 8 TeV with the ATLAS detector at the
Large Hadron Collider. Events with exactly three charged
leptons, or two leptons with the same electric charge in association
with two jets, are selected. The total number of events
observed in data is consistent with the Standard Model (SM)
predictions. The observed 95% confidence level upper limit
on the SM W±W±W∓ production cross section is found to
be 730 fb with an expected limit of 560 fb in the absence of
SM W±W±W∓ production. Limits are also set on WWWW
anomalous quartic gauge couplings
- …