145 research outputs found
Measurement of b hadron lifetimes in exclusive decays containing a J/psi in p-pbar collisions at sqrt(s)=1.96TeV
- Author
- Aaltonen T
- Gonzalez BA
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Badgett W
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Bland KR
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Cabrera S
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung WH
- Chung YS
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Crescioli F
- Almenar CC
- Cuevas J
- Culbertson R
- Dagenhart D
- d'Ascenzo N
- Datta M
- de Barbaro P
- De Cecco S
- De Lorenzo G
- Dell'Orso M
- Deluca C
- Demortier L
- Deng J
- Deninno M
- Devoto F
- d'Errico M
- Di Canto A
- Di Ruzza B
- Dittmann JR
- D'Onofrio M
- Donati S
- Dong P
- Dorigo T
- Ebina K
- Elagin A
- Eppig A
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eusebi R
- Fang HC
- Farrington S
- Feindt M
- Fernandez JP
- Ferrazza C
- Field R
- Flanagan G
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Furic I
- Gallinaro M
- Galyardt J
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerchtein E
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Ginsburg CM
- Giokaris N
- Giromini P
- Giunta M
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldin D
- Goldschmidt N
- Golossanov A
- Gomez G
- Gomez-Ceballos G
- Goncharov M
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Gresele A
- Grinstein S
- Grosso-Pilcher C
- Group RC
- da Costa JG
- Gunay-Unalan Z
- Haber C
- Hahn SR
- Halkiadakis E
- Hamaguchi A
- Han JY
- Happacher F
- Hara K
- Hare D
- Hare M
- Harr RF
- Hatakeyama K
- Hays C
- Heck M
- Heinrich J
- Herndon M
- Hewamanage S
- Hidas D
- Hocker A
- Hopkins W
- Horn D
- Hou S
- Hughes RE
- Hurwitz M
- Husemann U
- Hussain N
- Hussein M
- Huston J
- Introzzi G
- Iori M
- Ivanov A
- James E
- Jang D
- Jayatilaka B
- Jeon EJ
- Jha MK
- Jindariani S
- Johnson W
- Jones M
- Joo KK
- Jun SY
- Junk TR
- Kamon T
- Karchin PE
- Kato Y
- Ketchum W
- Keung J
- Khotilovich V
- Kilminster B
- Kim DH
- Kim HS
- Kim HW
- Kim JE
- Kim MJ
- Kim SB
- Kim SH
- Kim YK
- Kimura N
- Klimenko S
- Kondo K
- Kong DJ
- Konigsberg J
- Korytov A
- Kotwal AV
- Kreps M
- Kroll J
- Krop D
- Krumnack N
- Kruse M
- Krutelyov V
- Kuhr T
- Kurata M
- Kwang S
- Laasanen AT
- Labarga L
- Lami S
- Lammel S
- Lancaster M
- Lander RL
- Lannon K
- Lath A
- Latino G
- Lazzizzera I
- LeCompte T
- Lee E
- Lee HS
- Lee JS
- Lee SW
- Leo S
- Leone S
- Lewis JD
- Lin CJ
- Linacre J
- Lindgren M
- Lipeles E
- Lister A
- Litvintsev DO
- Liu C
- Liu Q
- Liu T
- Lockwitz S
- Lockyer NS
- Loginov A
- Lucchesi D
- Lueck J
- Lujan P
- Lukens P
- Lungu G
- Lys J
- Lysak R
- Madrak R
- Maeshima K
- Makhoul K
- Maksimovic P
- Malde S
- Malik S
- Manca G
- Manousakis-Katsikakis A
- Margaroli F
- Marino C
- Martinez M
- Martinez-Ballarin R
- Mastrandrea P
- Mathis M
- Mattson ME
- Mazzanti P
- McFarland KS
- McIntyre P
- McNulty R
- Mehta A
- Mehtala P
- Menzione A
- Mesropian C
- Miao T
- Mietlicki D
- Mitra A
- Miyake H
- Moed S
- Moggi N
- Mondragon MN
- Moon CS
- Moore R
- Morello MJ
- Morlock J
- Fernandez PM
- Mukherjee A
- Muller T
- Murat P
- Mussini M
- Nachtman J
- Nagai Y
- Naganoma J
- Nakano I
- Napier A
- Nett J
- Neu C
- Neubauer MS
- Nielsen J
- Nodulman L
- Norniella O
- Nurse E
- Oakes L
- Oh SH
- Oh YD
- Oksuzian I
- Okusawa T
- Orava R
- Ortolan L
- Griso SP
- Pagliarone C
- Palencia E
- Papadimitriou V
- Paramonov AA
- Patrick J
- Pauletta G
- Paulini M
- Paus C
- Pellett DE
- Penzo A
- Phillips TJ
- Piacentino G
- Pianori E
- Pilot J
- Pitts K
- Plager C
- Pondrom L
- Potamianos K
- Poukhov O
- Prokoshin F
- Pronko A
- Ptohos F
- Pueschel E
- Punzi G
- Pursley J
- Rahaman A
- Ramakrishnan V
- Ranjan N
- Redondo I
- Renton P
- Rescigno M
- Rimondi F
- Ristori L
- Robson A
- Rodrigo T
- Rodriguez T
- Rogers E
- Rolli S
- Roser R
- Rossi M
- Ruffini F
- Ruiz A
- Russ J
- Rusu V
- Safonov A
- Sakumoto WK
- Santi L
- Sartori L
- Sato K
- Saveliev V
- Savoy-Navarro A
- Schlabach P
- Schmidt A
- Schmidt EE
- Schmidt MP
- Schmitt M
- Schwarz T
- Scodellaro L
- Scribano A
- Scuri F
- Sedov A
- Seidel S
- Seiya Y
- Semenov A
- Sforza F
- Sfyrla A
- Shalhout SZ
- Shears T
- Shepard PF
- Shimojima M
- Shiraishi S
- Shochet M
- Shreyber I
- Simonenko A
- Sinervo P
- Sissakian A
- Sliwa K
- Smith JR
- Snider FD
- Soha A
- Somalwar S
- Sorin V
- Squillacioti P
- Stanitzki M
- St Denis R
- Stelzer B
- Stelzer-Chilton O
- Stentz D
- Strologas J
- Strycker GL
- Sudo Y
- Sukhanov A
- Suslov I
- Takemasa K
- Takeuchi Y
- Tang J
- Tecchio M
- Teng PK
- Thom J
- Thome J
- Thompson GA
- Thomson E
- Ttito-Guzman P
- Tkaczyk S
- Toback D
- Tokar S
- Tollefson K
- Tomura T
- Tonelli D
- Torre S
- Torretta D
- Totaro P
- Trovato M
- Tu Y
- Turini N
- Ukegawa F
- Uozumi S
- Varganov A
- Vataga E
- Vazquez F
- Velev G
- Vellidis C
- Vidal M
- Vila I
- Vilar R
- Vogel M
- Volpi G
- Wagner P
- Wagner RL
- Wakisaka T
- Wallny R
- Wang SM
- Warburton A
- Waters D
- Weinberger M
- Wenzel H
- Wester WC
- Whitehouse B
- Whiteson D
- Wicklund AB
- Wicklund E
- Wilbur S
- Wick F
- Williams HH
- Wilson JS
- Wilson P
- Winer BL
- Wittich P
- Wolbers S
- Wolfe H
- Wright T
- Wu X
- Wu Z
- Yamamoto K
- Yamaoka J
- Yang T
- Yang UK
- Yang YC
- Yao WM
- Yeh GP
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Zanetti A
- Zeng Y
- Zucchelli SM
- Predoi V
- Price LR
- Prijatelj M
- Principe M
- Prix R
- Prodi GA
- Prokhorov L
- Puncken O
- Punturo M
- Puppo P
- Quetschke V
- Raab FJ
- Rabeling DS
- Racz I
- Radke T
- Radkins H
- Raffai P
- Rakhmanov M
- Rankins B
- Rapagnani P
- Raymond V
- Re V
- Reed CM
- Reed T
- Regimbau T
- Reid S
- Reitze DH
- Ricci F
- Riesen R
- Riles K
- Roberts P
- Robertson NA
- Robinet F
- Robinson C
- Robinson EL
- Rocchi A
- Roddy S
- Rolland L
- Rollins J
- Romano JD
- Romano R
- Romie JH
- Rosinska D
- Rover C
- Rowan S
- Rudiger A
- Ruggi P
- Ryan K
- Sakata S
- Sakosky M
- Salemi F
- Sammut L
- de la Jordana LS
- Sandberg V
- Sannibale V
- Santamaria L
- Santostasi G
- Saraf S
- Sassolas B
- Sathyaprakash BS
- Sato S
- Satterthwaite M
- Saulson PR
- Savage R
- Schilling R
- Schnabel R
- Schofield RMS
- Schulz B
- Schutz BF
- Schwinberg P
- Scott J
- Scott SM
- Searle AC
- Seifert F
- Sellers D
- Sengupta AS
- Sentenac D
- Sergeev A
- Shaddock DA
- Shapiro B
- Shawhan P
- Shoemaker DH
- Sibley A
- Siemens X
- Sigg D
- Singer A
- Sintes AM
- Skelton G
- Slagmolen BJJ
- Slutsky J
- Smith JR
- Smith MR
- Smith ND
- Somiya K
- Sorazu B
- Speirits FC
- Sperandio L
- Stein AJ
- Stein LC
- Steinlechner S
- Steplewski S
- Stochino A
- Stone R
- Strain KA
- Strigin S
- Stroeer AS
- Sturani R
- Stuver AL
- Summerscales TZ
- Sung M
- Susmithan S
- Sutton PJ
- Swinkels B
- Szokoly GP
- Tacca M
- Talukder D
- Tanner DB
- Tarabrin SP
- Taylor JR
- Taylor R
- Thomas P
- Thorne KA
- Thorne KS
- Thrane E
- Thuring A
- Titsler C
- Tokmakov KV
- Toncelli A
- Tonelli M
- Torre O
- Torres C
- Torrie CI
- Tournefier E
- Travasso F
- Traylor G
- Trias M
- Tseng K
- Turner L
- Ugolini D
- Urbanek K
- Vahlbruch H
- Vaishnav B
- Vajente G
- Vallisneri M
- van den Brand JFJ
- Van den Broeck C
- van der Putten S
- van der Sluys MV
- van Veggel AA
- Vass S
- Vasuth M
- Vaulin R
- Vavoulidis M
- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Veltkamp C
- Verkindt D
- Vetrano F
- Vicere A
- Villar AE
- Vinet JY
- Vocca H
- Vorvick C
- Vyachanin SP
- Waldman SJ
- Wallace L
- Wanner A
- Ward RL
- Was M
- Wei P
- Weinert M
- Weinstein AJ
- Weiss R
- Wen L
- Wen S
- Wessels P
- West M
- Westphal T
- Wette K
- Whelan JT
- Whitcomb SE
- White D
- Whiting BF
- Wilkinson C
- Willems PA
- Williams L
- Willke B
- Winkelmann L
- Winkler W
- Wipf CC
- Wiseman AG
- Woan G
- Wooley R
- Worden J
- Yakushin I
- Yamamoto H
- Yamamoto K
- Yeaton-Massey D
- Yoshida S
- Yu P
- Yvert M
- Zanolin M
- Zhang L
- Zhang Z
- Zhao C
- Zotov N
- Zucker ME
- Zweizig J
- Publication venue
- Publication date
- 01/12/2010
- Field of study
We report on a measurement of b-hadron lifetimes in the fully reconstructed
decay modes B^+ -->J/Psi K+, B^0 --> J/Psi K*, B^0 --> J/Psi Ks, and Lambda_b
--> J/Psi Lambda using data corresponding to an integrated luminosity of 4.3
fbâ1, collected by the CDF II detector at the Fermilab Tevatron. The
measured lifetimes are ÏB^+ = 1.639±0.009(stat)±0.009(syst) ps, ÏB^0 = 1.507±0.010(stat)±0.008(syst) ps and ÏLambda_b = 1.537±0.045(stat)±0.014(syst) ps. The lifetime ratios are ÏB^+/ÏB^0 = 1.088±0.009(stat)±0.004(syst) and ÏLambda_b/ÏB^0 = 1.020±0.030(stat)±0.008(syst). These are the most precise determinations
of these quantities from a single experiment.Comment: revised version. accepted for PRL publicatio
Measurement of ZZ production in leptonic final states at {\surd}s of 1.96 TeV at CDF
- Author
- Aaltonen T.
- Alvarez Gonzalez B.
- Amerio S.
- Amidei D.
- Anastassov A.
- Annovi A.
- Antos J.
- Apollinari G.
- Appel J. A.
- Aptekar RL
- Arisawa T.
- Artikov A.
- Asaadi J.
- Ashmanskas W.
- Auerbach B.
- Aurisano A.
- Azfar F.
- Badgett W.
- Bae T.
- Barbaro-Galtieri A.
- Barnes V. E.
- Barnett B. A.
- Barria P.
- Bartos P.
- Bauce M.
- Bedeschi F.
- Behari S.
- Bellettini G.
- Bellinger J.
- Benjamin D.
- Beretvas A.
- Bhatti A.
- Bisello D.
- Bizjak I.
- Bland K. R.
- Blumenfeld B.
- Bocci A.
- Bodek A.
- Bortoletto D.
- Boudreau J.
- Boveia A.
- Boynton WV
- Briggs MS
- Brigliadori L.
- Bromberg C.
- Brucken E.
- Budagov J.
- Budd H. S.
- Burkett K.
- Busetto G.
- Bussey P.
- Buzatu A.
- Calamba A.
- Calancha C.
- Camarda S.
- Campanelli M.
- Campbell M.
- Canelli F.
- Carls B.
- Carlsmith D.
- Carosi R.
- Carrillo S.
- Carron S.
- Casal B.
- Casarsa M.
- Castro A.
- Catastini P.
- Cauz D.
- Cavaliere V.
- Cavalli-Sforza M.
- Cerri A.
- Cerrito L.
- Chen Y. C.
- Chertok M.
- Chiarelli G.
- Chlachidze G.
- Chlebana F.
- Cho K.
- Chokheli D.
- Chung W. H.
- Chung Y. S.
- Ciocci M. A.
- Clark A.
- Clarke C.
- Cline TL
- Compostella G.
- Connaughton V
- Convery M. E.
- Conway J.
- Corbo M.
- Cordelli M.
- Cox C. A.
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- Crescioli F.
- Cuevas J.
- Culbertson R.
- d'Ascenzo N.
- d'Errico M.
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- da Costa J. Guimaraes
- Dagenhart D.
- Datta M.
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- Dell'Orso M.
- Demortier L.
- Deninno M.
- Devoto F.
- Di Canto A.
- Di Ruzza B.
- Dittmann J. R.
- Donati S
- Dong P.
- Dorigo M.
- Dorigo T.
- Ebina K.
- Elagin A.
- Eppig A.
- Erbacher R.
- Errede S.
- Ershaidat N.
- Eusebi R.
- Farrington S.
- Feindt M.
- Fernandez J. P.
- Fernandez P. Movilla
- Field R.
- Flanagan G.
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- Frank M. J.
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- Gerberich H.
- Gerchtein E.
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- Giannetti P.
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- Glenzinski D.
- Gold M.
- Goldin D.
- Goldschmidt N.
- Goldsten JO
- Golossanov A.
- Golovin D
- Gomez G.
- Gomez-Ceballos G.
- Goncharov M.
- Gonzalez O.
- Gorelov I.
- Goshaw A. T.
- Goulianos K.
- Grinstein S.
- Griso S. Pagan
- Grosso-Pilcher C.
- Group R. C.
- Hahn S. R.
- Halkiadakis E.
- Hamaguchi A.
- Han J. Y.
- Happacher F.
- Hara K.
- Hare D.
- Hare M.
- Harr R. F.
- Hatakeyama K.
- Hays C.
- Heck M.
- Heinrich J.
- Herndon M.
- Hewamanage S.
- Hocker A.
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- Horn D.
- Hou S.
- Hughes R. E.
- Hurley KC
- Hurwitz M.
- Husemann U.
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- Jayatilaka B.
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- Junk T. R.
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- Karchin P. E.
- Kasmi A.
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- Keung J.
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- Knoepfel K.
- Kondo K.
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- Konigsberg J.
- Kotwal A. V.
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- Krimm HA
- Kroll J.
- Krop D.
- Kruse M.
- Krutelyov V.
- Kuhr T.
- Kurata M.
- Kwang S.
- Laasanen A. T.
- Lami S.
- Lammel S.
- Lancaster M.
- Lander R. L.
- Lannon K.
- Lath A.
- Latino G.
- LeCompte T.
- Lee E.
- Lee H. S.
- Lee J. S.
- Lee S. W.
- Leo S.
- Leone S.
- Lewis J. D.
- Limosani A.
- Lin C. -J.
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- Lindgren M.
- Lipeles E.
- Lister A.
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- Lockwitz S.
- Loginov A.
- Lucchesi D.
- Lueck J.
- Lujan P.
- Lukens P.
- Lungu G.
- Lys J.
- Lysak R.
- Madrak R.
- Maeshima K.
- Maestro P.
- Malik S.
- Manca G.
- Manousakis-Katsikakis A.
- Margaroli F.
- Marino C.
- Martinez M.
- Mastrandrea P.
- Mastroberardino A
- Masubuchi T
- Matera K.
- Mathes M
- Matsumoto H
- Matsunaga H
- Matsushita T
- Mattravers C
- Mattson M. E.
- Mazzacane A.
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- McFarland K. S.
- McIntyre P.
- McNulty R.
- Mehta A.
- Mehtala P.
- Mesropian C.
- Miao T.
- Mietlicki D.
- Mitra A.
- Mitrofanov I
- Miyake H.
- Moed S.
- Moggi N.
- Mondragon M. N.
- Moon C. S.
- Moore R.
- Morello M. J.
- Morlock J.
- Mukherjee A.
- Muller Th
- Murat P.
- Mussini M.
- Nachtman J.
- Nagai Y.
- Naganoma J.
- Nakano I.
- Napier A.
- Nett J.
- Neu C.
- Neubauer M. S.
- Nielsen J.
- Nodulman L.
- Noh S. Y.
- Norniella O.
- Oakes L.
- Oh S. H.
- Oh Y. D.
- Ohno M
- Oksuzian I.
- Okusawa T.
- Orava R.
- Ortolan L.
- Pagliarone C.
- Pal'shin VD
- Palencia E.
- Papadimitriou V.
- Paramonov A. A.
- Patrick J.
- Pauletta G.
- Paulini M.
- Paus C.
- Pellett D. E.
- Penzo A.
- Phillips T. J.
- Piacentino G.
- Pianori E.
- Pilot J.
- Pitts K.
- Plager C.
- Pondrom L.
- Poprocki S.
- Potamianos K.
- Pranko A.
- Prokoshin F.
- Ptohos F.
- Punzi G.
- Rahaman A.
- Ramakrishnan V.
- Ranjan N.
- Rau A
- Redondo I.
- Renton P.
- Rescigno M.
- Riddick T.
- Rimondi F.
- Ristori L.
- Robson A.
- Rodrigo T.
- Rodriguez T.
- Rogers E.
- Rolli S.
- Roser R.
- Ruffini F.
- Ruiz A.
- Russ J.
- Rusu V.
- Safonov A.
- Sakumoto W. K.
- Sakurai Y.
- Sanin A
- Sannibale V
- Santamaria L
- Santi L.
- Santiago-Prieto I
- Santostasi G
- Saraf S
- Sassolas B
- Sathyaprakash BS
- Sato K.
- Sato S
- Satterthwaite M
- Saulson PR
- Savage R
- Saveliev V.
- Savoy-Navarro A.
- Schilling R
- Schlabach P.
- Schlamminger S
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- Zotov N
- Zucchelli S.chelli S.
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2011
- Field of study
In this paper we present a precise measurement of the total ZZ production
cross section in pp collisions at {\surd}s= 1.96 TeV, using data collected with
the CDF II detector corresponding to an integrated luminosity of approximately
6 fb-1. The result is obtained by combining separate measurements in the
four-charged (lll'l'), and two-charged-lepton and two-neutral-lepton (llvv)
decay modes of the Z. The combined measured cross section for pp {\to} ZZ is
1.64^(+0.44)_(-0.38) pb. This is the most precise measurement of the ZZ
production cross section in 1.96 TeV pp collisions to date.Comment: submitted to Phys. Rev. Let
Combined measurement of differential and total cross sections in the HâŻââŻÎłÎł and the HâŻââŻZZ*âŻââŻ4â decay channels at s=13 TeV with the ATLAS detector
- Author
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- Zhemchugov A
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- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fbâ1 of 13 TeV protonâproton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured Hâγγ and HâZZ*(â4â event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0â5.9 +6.0 (stat.) â3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for High-Mass Resonances Decaying to ÏÎœ in pp Collisions at âs=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
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- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
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- Aliev M
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- Amadio BT
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- Amor Dos Santos SP
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- Amrouche CS
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- Angelidakis S
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- Angerami A
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- Antrim DJ
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- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to ÏÎœ using proton-proton collisions at âs=13 TeV produced by the Large Hadron Collider is presented. Only Ï-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fbâ1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible ÏÎœ production cross section. Heavy WâČ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2â3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Search for the direct production of charginos and neutralinos in final states with tau leptons in âs=13 TeV collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Zhemchugov A
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- Zibell A
- Zieminska D
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- Zimmermann C
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- Zobernig G
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fbâ1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ËÏ+1 ËÏâ1 pair production and of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the Ë ÏL state is set to be halfway between the masses of the Ëϱ1 and the ËÏ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ËÏ+1 ËÏâ1 for a massless ËÏ01. Common Ëϱ1 and ËÏ02 masses up to 760 GeV are excluded in the case of production of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 assuming a massless ËÏ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the Ëϱ1 and the ËÏ01 are also studied by varying the Ë ÏL mass between the masses of the Ëϱ1 and the ËÏ01
Measurement of differential cross sections and W + /W â cross-section ratios for W boson production in association with jets at âs =8 TeV with the ATLAS detector
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- Mizukami A
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- Sforza F
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- Siral I
- Sivoklokov S Yu
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- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
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- Smart BH
- Smieskoa J
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- Sulin VV
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- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
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- Ucchielli G
- Ueda I
- Ughetto M
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- Ungaro FC
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- Vacavant L
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- Valderanis C
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- Valero A
- Valery L
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- van Woerden MC
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- Varvell KE
- Vasquez GA
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- Vazquez JG Panduro
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- Veeraraghavan V
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- Viazlo O
- Vichou I
- Vickey T
- Vie S
- Viehhauser GHA
- Vigani L
- Villa M
- Villar DI Narrias
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- Vivarelli I
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- von der Schmitt H
- von Toerne E
- Vorobe V
- Vorobev K
- Vos M
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- Vossebeld JH
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- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
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- Wallangen V
- Walls FM Garay
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- Weingarten J
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- Wermes N
- Werner MD
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- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
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- Whitmore BW
- Wickens FJ
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- Wiik-Fuchs LAM
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- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobischu M
- Wolf A
- Wolf TMH
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- Wolter MW
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- Wong KH Yau
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wotschack J
- Wozniak KW
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
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- Xu L
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- Xu W
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
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- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
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- 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
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
This paper presents a measurement of the W boson production cross section and the W + /W â cross-section ratio, both in association with jets, in proton--proton collisions at s â =8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb â1 . Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W + /W â the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proto
Operation and performance of the ATLAS Tile Calorimeter in Run 1
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouelfadl 
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
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- Alshehri AA
- Alstaty MI
- Alvarez 
- Alviggi MG
- Amadio BT
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- Amor 
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- Zwalinski L
- ZÌenisÌ T
- ZÌivkovicÌ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeterâs performance during the years 2008â2012 using cosmic-ray muon events and protonâproton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fbâ1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from protonâproton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at âs=8 TeV with the ATLAS detector
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- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
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- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
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- Zerwas D
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- 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
- Zou R
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of âs=8 TeV is presented. The results are based on an integrated luminosity of 20.2 fbâ1 recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying |ηγ|40GeV and EÎłT,2>30 GeV for the two leading photons ordered in transverse energy produced in the interaction. The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is 16.8 ± 0.8â pb . The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%
Search for supersymmetry in events with four or more leptons in âs =13 TeV pp collisions with ATLAS
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- 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
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J
- Argyropoulos S
- Arik M
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
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- Kotwal A
- Koulouris A
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- Zinser M
- Ziolkowski M
- Zobernig G
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- zur Nedden M
- Zwalinski L
- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
Results from a search for supersymmetry in events with four or more charged leptons (electrons, muons and taus) are presented. The analysis uses a data sample corresponding to 36.1 fb â1 of proton-proton collisions delivered by the Large Hadron Collider at s â =13 TeV and recorded by the ATLAS detector. Four-lepton signal regions with up to two hadronically decaying taus are designed to target a range of supersymmetric scenarios that can be either enriched in or depleted of events involving the production and decay of a Z boson. Data yields are consistent with Standard Model expectations and results are used to set upper limits on the event yields from processes beyond the Standard Model. Exclusion limits are set at the 95% confidence level in simplified models of General Gauge Mediated supersymmetry, where higgsino masses are excluded up to 295 GeV. In R -parity-violating simplified models with decays of the lightest supersymmetric particle to charged leptons, lower limits of 1.46 TeV, 1.06 TeV, and 2.25 TeV are placed on wino, slepton and gluino masses, respectively
Study of ordered hadron chains with the ATLAS detector
- Author
- Aaboud M
- Aad G
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- Abdinov O
- Abeloos B
- Abidi SH
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
The analysis of the momentum difference between charged hadrons in high-energy proton-proton collisions is performed in order to study coherent particle production. The observed correlation pattern agrees with a model of a helical QCD string fragmenting into a chain of ground-state hadrons. A threshold momentum difference in the production of adjacent pairs of charged hadrons is observed, in agreement with model predictions. The presence of low-mass hadron chains also explains the emergence of charge-combination-dependent two-particle correlations commonly attributed to Bose-Einstein interference. The data sample consists of 190 ÎŒbâ1 of minimum-bias events collected with proton-proton collisions at a center-of-mass energy âs=7 TeV in the early low-luminosity data taking with the ATLAS detector at the LHC
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