23 research outputs found
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
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- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
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- Bachacou H
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- Backhaus M
- Badescu E
- Bagnaia P
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- Bai Y
- Bailey DC
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- Baker MD
- Baker OK
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- BScher V
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- Buckingham RM
- Buckley AG
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- Budagov IA
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- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
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- Castanheira MTD
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- Chapman JD
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- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
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- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
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- Chromek-Burckhart D
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- Whitaker SP
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- White MJ
- White S
- Whitehead SR
- Whiteson D
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- Wickens FJ
- Wiedenmann W
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- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
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- Wilkens HG
- Will JZ
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- Williams HH
- Willis W
- Willocq S
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- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
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- Wraight K
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- Xella S
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- Xu G
- Yabsley B
- Yacoobb S
- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Search for the bcâ meson in hadronic Z decays
- Author
- Abbaneo D.
- Ajaltouni Ziad,
- Alemany R.
- Aleppo M.
- Antonelli A.
- Apollonio M.
- Armstrong S R.
- Aubert J.J.
- Azzurri P.
- Bagliesi G.
- Barate R.
- Barres A.
- Batignani G.
- Bazarko A O.
- Becker U.
- Benchouk C.
- Bencivenni G.
- Bettarini S.
- Betteridge A P.
- Beuselinck R.
- Bhrer A.
- Binnie D M.
- Black S N.
- Blair G A.
- Bloch-Devaux B.
- Blondel A.
- Blum W.
- Bologna G.
- Bonissent A.
- Bonneaud G.
- Booth C N.
- Bosisio L.
- Bossi F.
- Boswell R.
- Botterill D R.
- Boucrot J.
- Bourdon P.
- Bowdery C K.
- Boyer Claudine
- Bozzi C.
- Brandt S.
- Brew C A J.
- Brient J C.
- Bright-Thomas P.
- Bryant L M.
- Bscher V.
- Bujosa G.
- Buskulic D.
- Calderini G.
- Callot O.
- Calvet D.
- Candlin D J.
- Capon G.
- Carpinelli M.
- Carr J.
- Cartwright S L.
- Casado M P.
- Casper D.
- Cattaneo M.
- Cerutti F.
- Chambers J T.
- Charles E.
- Chen S.
- Chiarella V.
- Chmeissani M.
- Choi Y.
- CiocciM A.
- Ciulli V.
- Clifft R W.
- Colaleo A.
- Colas P.
- Colrain P.
- Comas P.
- Combley F.
- Corden M.
- Cordier A.
- Cowan G.
- Coyle P.
- Crawford G.
- Creanza D.
- Crespo J M.
- Curtis L.
- Dann JH.
- Daskalakis G.
- Davier M.
- De Palma M.
- Decamp D.
- Delfino M.
- Dell'Orso R.
- Della Marina R.
- Diaconu C.
- Dietl H.
- Dissertori G.
- Dornan P J.
- Dorris S J.
- Duflot L.
- Dydak F.
- Edgecock T R.
- Elmer P.
- Emery S.
- Etienne F.
- Falvard Alain
- Fantechi R.
- Fearnley T.
- Felici G.
- Ferdi C.
- Ferguson D P S.
- Fernandez-Bosman M.
- Fernndez E.
- Ferrante I.
- Finch A J.
- Fo L.
- Focardi E.
- Forti F.
- Forty R W.
- Foster F.
- Frank M.
- Galla A.
- Ganis G.
- Gao Y S.
- Gao Y.
- Garrido L.
- Gay Pascal
- Gelao G.
- Georgiopoulos C.
- Geweniger C.
- Ghez P.
- Giannini G.
- Giassi A.
- Giehl I.
- Giorgi M A.
- Girone M.
- Girtler P.
- Gobbo B.
- Gonzlez S.
- Goodsir S.
- Gotzhein C.
- Goy C.
- Graefe G.
- Green M G.
- Greene A M.
- GreeningT C.
- Gregorio A.
- Grivaz J F.
- Grupen C.
- Guicheney C.
- Hagelberg R.
- Halley A W.
- Hanke P.
- Hansen J B.
- Hansen J R.
- Hansen JD.
- Hansen P H.
- Hansper G.
- Harvey J.
- Hayes O J.
- Haywood S.
- Hcker A.
- Henrard Pierre
- Hepp V.
- Heusse P.
- Hoffmann C.
- Hu H.
- Huang X.
- Hughes G.
- Iaselli G.
- Jacholkowska A.
- Jacquet M.
- Jaffe D E.
- Jakobs K.
- Janot P.
- Jin S.
- Johnson R P.
- Jost B.
- Jousset J.
- Juste A.
- Kelly M S.
- Kim D W.
- Kim H Y.
- Kleinknecht K.
- Kluge E E.
- Kneringer E.
- Knobloch J.
- Knowles I G.
- Konstantinidis N.
- Kozanecki W.
- Kroha H.
- Kuhn D.
- Kyriakis A.
- Lanon E.
- Laurelli P.
- Le Diberder F.
- Lees J P.
- Lefranois J.
- Lehraus I.
- Lehto M H.
- Lemaire M C.
- Leroy O.
- Ligabue F.
- Lin Jiali
- Litke A M.
- Locci E.
- Ltjens G.
- Lucotte A.
- Lusiani A.
- Lutters G.
- Lutz A M.
- Lutz G.
- Lynch J G.
- Maggi G.
- Maggi M.
- Maley P.
- Marinelli N.
- Markou C.
- Marrocchesi P S.
- Martin E B.
- Martinez M.
- Mato P.
- McNamara P A.
- McNeil M A.
- Medcalf T.
- Messineo A.
- Michel B.
- Minard M N.
- Minten A.
- Miquel R.
- Mir L M.
- Mnner W.
- Moneta L.
- Monteil S.
- Montret Jean-Claude
- Moser H G.
- Motsch F.
- Moutoussi A.
- Murtas F.
- Murtas G P.
- Musolino G.
- Nachtman J M.
- Nash J.
- Newton W M.
- Nief J Y.
- Nielsen J.
- Nikolic I.
- Nilsson B S.
- Norton P R.
- Nuzzo S.
- O'Shea V.
- Orejudos W.
- Orteu S.
- Ouyang Q.
- Pacheco A.
- Padilla C.
- Palla F.
- Pallin D.
- Pan Y B.
- Park I C.
- Parrini G.
- Parsons M I.
- Pascual A.
- Passalacqua L.
- Payre P.
- Pep-Altarelli M.
- Perlas J A.
- Perret Pascal
- Perrodo P.
- Pietrzyk B.
- Podlyski F.
- Prez P.
- Proriol Joseph
- Pusztaszeri J F.
- Putzer A.
- Quast G.
- Ragusa F.
- Raine C.
- Rander J.
- Ranieri A.
- Ranjard F.
- Raso G.
- Reeve J.
- Renardy J F.
- Renk B.
- Rensch B.
- Rensing P.
- Richter R H.
- Riu I.
- Rizzo G.
- Rohne E.
- Rolandi L.
- Rosado-Schlosser A.
- Rosnet P.
- Rossignol J.M.
- Rothberg J E.
- Rouge A.
- Roussarie A.
- Rousseau D.
- Rudolph G.
- Ruggieri F.
- Saadi Y.
- Sadouki A.
- Sanchez F.
- Sander H G.
- Sanguinetti G.
- Saraiva P.
- Scarr J M.
- Schael S.
- Schlatter D.
- Schmidt M.
- Schmitt M.
- Schneider O.
- Schuller J P.
- Schune M H.
- Schwindling J.
- Sciab A.
- Scott I J.
- Sedgbeer J K.
- Selvaggi G.
- Settles R.
- Seywerd H C J.
- Silvestris L.
- Simion S.
- Simopoulou E.
- Siotis I.
- Sloan T.
- Smith K.
- Smolik L.
- Sommer J.
- Spagnolo P.
- Stacey A M.
- Steinberger J.
- Stenzel H.
- Stephan F.
- Strong J A.
- Talby M.
- Taylor G.
- Teixeira-Dias P.
- Tejessy W.
- Tempesta P.
- Tenchini R.
- Teubert F.
- Thompson A S.
- Thompson J C.
- Thompson L F.
- Thomson E.
- Thomson F.
- Thulasidas M.
- Tittel K.
- Tomalin I R.
- Tonelli G.
- Tournefier E.
- Trabelsi A.
- Trabelsi Karim
- Tricomi A.
- Turnbull R M.
- Valassi A.
- Vallage B.
- VanGemmeren P.
- Vannini C.
- Veillet J J.
- Verderi M.
- Verdini P G.
- Videau H.
- Videau I.
- VonWimmersperg-Toeller J H.
- Wachsmuth H.
- Wagner A.
- Walsh J.
- Wang T.
- Wasserbaech S.
- Werner S.
- Wiedenmann W.
- Williams M D.
- Williams M I.
- Wnnen A.
- Wolf G.
- Wright A E.
- Wu SL.
- Wu X.
- Wunsch M.
- Xie Y.
- Xu R.
- Xue S.
- Yamartino J M.
- Zachariadou K.
- Zeitnitz C.
- Zerwas D.
- Zhang J.
- Zhang L.
- Zhao W.
- Zito G.
- Zobernig G.
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1997
- Field of study
A search for the Bc meson decaying into the channels J/psi pi+ and J/psi l nu (l = e or mu) is performed in a sample of 3.9 million hadronic Z decays collected by the ALEPH detector. This search results in the observation of 0 and 2 candidates in each of these channels, respectively, while 0.44 and 0.81 background events are expected. The following 90\% confidence level upper limits are derived: Br(Z->Bc X)/Br(Z->q q )*Br(Bc->J/psi pi+) 3.6 10^-5 Br(Z->Bc X)/Br(Z->q q )*Br(Bc->J/psi l nu) 5.2 10^-5 An additional Bc->J/psi(e+e-) mu nu candidate with very low background probability, found in an independent analysis, is also described in detail
Study of muon-pair production at centre-of-mass energies from 20 to 136 GeV with the Aleph detector
- Author
- Abbaneo D.
- Affholderbach K.
- Ajaltouni Ziad,
- Alemany R.
- Aleppo M.
- Antonelli A.
- Apollonio M.
- Armstrong S R.
- Aubert J.J.
- Azzurri P.
- Bagliesi G.
- Barres A.
- Batignani G.
- Bazarko a O.
- Becker U.
- Benchouk C.
- Bencivenni G.
- Berlich R.
- Bettarini S.
- Betteridge a P.
- Beuselinck R.
- Bhrer A.
- Binnie D M.
- Black S N.
- Blair G A.
- Bloch-Devaux B.
- Blondel A.
- Blum W.
- Bologna G.
- Bonissent A.
- Booth C N.
- Bosisio L.
- Bossi F.
- Boswell R.
- Botterill D R.
- Boucrot J.
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- Trabelsi A.
- Trabelsi Karim
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- Videau H.
- Videau I.
- von Wimmersperg-Toeller J H.
- Wachsmuth H.
- Wagner A.
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- Wang T.
- Wasserbaech S.
- Werner S.
- Whelan E P.
- Wiedenmann W.
- Williams M D.
- Williams Mi.
- Williams R W.
- Wnnen A.
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- Zachariadou K.
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- Zerwas D.
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- Zhang L.
- Zhao W.
- Zheng M.
- Zito G.
- Zobernig G.
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1997
- Field of study
The total cross section and the forward-backward asymmetry for the process e+eââÎŒ+ÎŒâ(nÎł) are measured in the energy range 20-136 GeV by reconstructing the effective centre-of-mass energy after initial state radiation. The analysis is based on the data recorded with the ALEPH detector at LEP between 1990 and 1995, corresponding to a total integrated luminosity of 143.5 pbâ1. Two different approaches are used: in the first one an exclusive selection of events with hard initial state radiation in the energy range 20-88 GeV is directly compared with the Standard Model predictions showing good agreement. In the second one, all events are used to obtain a precise measurement of the energy dependence of Ï0 and AFB0â from a model independent fit, enabling constraints to be placed on models with extra Z bosons
Identification of boosted Higgs bosons decaying into b-quark pairs with the ATLAS detector at 13 TeV
- Author
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu CG
- Zhu H
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- Zhu Y
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
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- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2019
- Field of study
This paper describes a study of techniques for identifying Higgs bosons at high transverse momenta decaying into bottom-quark pairs, HâbbÂŻ , for protonâproton collision data collected by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy sâ=13 TeV . These decays are reconstructed from calorimeter jets found with the anti- kt R=1.0 jet algorithm. To tag Higgs bosons, a combination of requirements is used: b-tagging of R=0.2 track-jets matched to the large-R calorimeter jet, and requirements on the jet mass and other jet substructure variables. The Higgs boson tagging efficiency and corresponding multijet and hadronic top-quark background rejections are evaluated using Monte Carlo simulation. Several benchmark tagging selections are defined for different signal efficiency targets. The modelling of the relevant input distributions used to tag Higgs bosons is studied in 36 fb â1 of data collected in 2015 and 2016 using gâbbÂŻ and Z(âbbÂŻ)Îł event selections in data. Both processes are found to be well modelled within the statistical and systematic uncertainties
Observation of Electroweak Production of a Same-Sign W Boson Pair in Association with Two Jets in pp Collisions root s=13 TeV with the ATLAS Detector
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- Aad G
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- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
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- Biglietti M
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- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Bittrich C
- Bjergaard DM
- Black JE
- Black KM
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
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- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
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- Boonekamp M
- Borisov A
- Borissov G
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- Brau B
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- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Bscher V
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Bugge MK
- Bulekov O
- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
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- Burke S
- Burmeister I
- Burr JTP
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
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- Camincher C
- Campana S
- Campanelli M
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- Campoverde A
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- Cantero J
- Cao T
- Cao Y
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castillo IS
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
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- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chapman JD
- Chargeishvili B
- Charlton DG
- Chau CC
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- Chekanov S
- Chekulaev S
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen CH
- Chen H
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- Chen S
- Chen SJ
- Chen X
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- Chen Y-H
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- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
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- Chitan A
- Chiu I
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- Christodoulou V
- Chu MC
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- Ciocio A
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- Corga KDV
- Cormier F
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- Cornell SD
- Corpe LD
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- Czodrowski P
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- D'Auria S
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- D'onofrio A
- D'Onofrio M
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- Da Via C
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- Dai T
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- Daubney T
- Davey W
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- De Benedetti A
- De Beurs M
- De Bruin PHS
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DEF
- De Lorenzi F
- De Maria A
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santis M
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- De Sousa MJDCS
- De K
- Debenedetti C
- Dedovich D
- Dehghanian N
- Deiana AM
- Del Gaudio M
- Del Peso J
- Delgove D
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- Dell'Acqua A
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- Denysiuk D
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- Deviveiros PO
- Dewhurst A
- Dhaliwal S
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- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Micco B
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- Di Petrillo KF
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- Eckardt C
- Ecker KM
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- Eigen G
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- Favareto A
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- Fiolhais MCN
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- Fleck I
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- Fletcher RRM
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- Flierl BM
- Flores LF
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- Freund B
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- Froidevaux D
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- Fusayasu T
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- Gkougkousis EL
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- Knue A
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- Kodys P
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- Kourkoumelis C
- Kourlitis E
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- Zhemchugov A
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 18/10/2019
- Field of study
This Letter presents the observation and measurement of electroweak production of a same-sign
W
boson pair in association with two jets using
36.1
â
â
fb
â
1
of proton-proton collision data recorded at a center-of-mass energy of
â
s
=
13
â
â
TeV
by the ATLAS detector at the Large Hadron Collider. The analysis is performed in the detector fiducial phase-space region, defined by the presence of two same-sign leptons, electron or muon, and at least two jets with a large invariant mass and rapidity difference. A total of 122 candidate events are observed for a background expectation of
69
±
7
events, corresponding to an observed signal significance of 6.5 standard deviations. The measured fiducial signal cross section is
Ï
fid
=
2.89
+
0.51
â
0.48
(
stat
)
+
0.29
â
0.28
(
syst
)
â
â
fb
Dijet azimuthal correlations and conditional yields in pp and p plus Pb collisions at â{S}^NN=5.02 TeV with the ATLAS detector
- Author
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- Aad G
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- Soldatov EY
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- Strandberg J
- Strandberg S
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- Torres RET
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- Tsukerman II
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- Ueda I
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- Urban J
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- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
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- Valentinetti S
- Valero A
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- Valls Ferrer JA
- Van Daalen TR
- Van Gemmeren P
- Van Vulpen I
- Vanadia M
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- Varnes EW
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- Vichou I
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- Viehhauser GHA
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- von Buddenbrock SE
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- Vukotic I
- Wagner P
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- Wahlberg H
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- Wallangen V
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- Warburton A
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- Wardrope DR
- Washbrook A
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- Watson MF
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- Waugh BM
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- Weber SA
- Weber SM
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
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- Wengler T
- Wenig S
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- Werner MD
- Werner P
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilk F
- Wilkens HG
- Wilkins LJ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yue X
- Yuen SPY
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeiner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang DF
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/09/2019
- Field of study
This paper presents a measurement of forward-forward and forward-central dijet azimuthal angular correlations and conditional yields in proton-proton (pp) and proton-lead (p + Pb) collisions as a probe of the nuclear gluon density in regions where the fraction of the average momentum per nucleon carried by the parton entering the hard scattering is low. In these regions, gluon saturation can modify the rapidly increasing parton distribution function of the gluon. The analysis utilizes 25 pb^{-1} of pp data and 360 mp^{-1} of p + Pb data, both at {S}^NN=5.02 TeV, collected in 2015 and 2016, respectively, with the ATLAS detector at the Large Hadron Collider. The measurement is performed in the center-of-mass frame of the nucleon-nucleon system in the rapidity range between -4.0 and 4.0 using the two highest transverse-momentum jets in each event, with the highest transverse-momentum jet restricted to the forward rapidity range. No significant broadening of azimuthal angular correlations is observed for forward-forward or forward-central dijets in p + Pb compared to pp collisions. For forward-forward jet pairs in the proton-going direction, the ratio of conditional yields in p + Pb collisions to those in pp collisions is suppressed by approximately 20%, with no significant dependence on the transverse momentum of the dijet system. No modification of conditional yields is observed for forward-central dijets
Fast simulation of muons produced at the SHiP experiment using generative adversarial networks
- Author
- Ahdida C
- Albanese R
- Alexandrov A
- Anokhina A
- Aoki S
- Arduini G
- Atkin E
- Azorskiy N
- Back JJ
- Bagulya A
- Baranov A
- Bardou F
- Barker GJ
- Battistin M
- Bauche J
- Bay A
- Bayliss V
- Bencivenni G
- Berdnikov AY
- Berdnikov YA
- Berezkina I
- Bertani M
- Betancourt C
- Bezshyiko I
- Bezshyyko O
- Bick D
- Bieschke S
- Blanco A
- Boehm J
- Bogomilov M
- Bondarenko K
- Bonivento WM
- Borburgh J
- Boyarsky A
- Brenner R
- Breton D
- Brundler R
- Bruschi M
- Bscher V
- Buonaura A
- Buontempo S
- Cadeddu S
- Calcaterra A
- Calviani M
- Campanelli M
- Casolino M
- Cavalcante ABR
- Charitonidis N
- Chau P
- Chauveau J
- Chepurnov A
- Chernyavskiy M
- Choi K-Y
- Chumakov A
- Ciambrone P
- Congedo L
- Cornelis K
- Cristinziani M
- Crupano A
- D'Ambrosio N
- D'Appollonio G
- Dallavalle GM
- Datwyler A
- De Carvalho Saraiva J
- De Lellis G
- De Magistris M
- De Roeck A
- De Serio M
- De Simone D
- Dedenko L
- Dergachev P
- Di Crescenzo A
- Di Marco N
- Diaz PS
- Dib C
- Dijkstra H
- Dipinto P
- Dmitrenko V
- Dmitrievskiy S
- Dolmatov A
- Domenici D
- Donskov S
- Dos Santos FB
- Dougherty LA
- Drohan V
- Dubreuil A
- Ehlert M
- Enik T
- Etenko A
- Fabbri F
- Fabbri L
- Fabich A
- Fedin O
- Fedotovs F
- Felici G
- Ferro-Luzzi M
- Filippov K
- Fini RA
- Fonte P
- Franco C
- Fraser M
- Fresa R
- Froeschl R
- Fukuda T
- Galan FS
- Galati G
- Gall J
- Gatignon L
- Gavrilov G
- Gentile V
- Gerlach S
- Goddard B
- Golinka-Bezshyyko L
- Golovatiuk A
- Golubkov D
- Golutvin A
- Gorbounov P
- Gorbunov D
- Gorbunov S
- Gorkavenko V
- Gornushkin Y
- Gorshenkov M
- Grachev V
- Grandchamp AL
- Granich G
- Graverini E
- Grenard J-L
- Grenier D
- Grichine V
- Gruzinskii N
- Guler AM
- Guz Y
- Haefeli GJ
- Hagner C
- Hakobyan H
- Harris IW
- Hessler C
- Hollnagel A
- Hosseini B
- Hushchyn M
- Iaselli G
- Iuliano A
- Ivantchenko V
- Jacobsson R
- Jokovic D
- Jonker M
- Kadenko I
- Kain V
- Kaiser B
- Kamiscioglu C
- Kershaw K
- Khabibullin M
- Khalikov E
- Khaustov G
- Khoriauli G
- Khotyantsev A
- Kim SH
- Kim V
- Kim YG
- Kitagawa N
- Ko J-W
- Kodama K
- Kolesnikov A
- Kolev D
- Kolosov V
- Komatsu M
- Kondrateva N
- Kono A
- Konovalova N
- Kormannshaus S
- Korol'ko I
- Korol I
- Korzenev A
- Kostyukhin V
- Kovalenko S
- Krasilnikova I
- Kudenko Y
- Kurbatov E
- Kurbatov P
- Kurochka V
- Kuznetsova E
- Lacker HM
- Lamont M
- Lanfranchi G
- Lantwin O
- Lauria A
- Lee KS
- Lee KY
- Levy J-M
- Lopes L
- Loschiavo VP
- Lyubovitskij V
- Maalmi J
- Magnan A
- Maleev V
- Malinin A
- Manabe Y
- Managadze AK
- Manfredi M
- Marsh S
- Marshall AM
- Mefodev A
- Mermod P
- Miano A
- Mikado S
- Mikhaylov Y
- Milstead DA
- Mineev O
- Montanari A
- Montesi MC
- Morishima K
- Movchan S
- Muttoni Y
- Naganawa N
- Naing ST
- Nakamura M
- Nakano T
- Nasybulin S
- Ninin P
- Nishio A
- Novikov A
- Obinyakov B
- Ogawa S
- Okateva N
- Opitz B
- Osborne J
- Ovchynnikov M
- Owen PH
- Owtscharenko N
- Pacholek P
- Paoloni A
- Park BD
- Park SK
- Pastore A
- Patel M
- Pereyma D
- Perillo-Marcone A
- Petkov GL
- Petridis K
- Petrov A
- Platia EK
- Podgrudkov D
- Poliakov V
- Polukhina N
- Prieto JP
- Prokudin M
- Prota A
- Quercia A
- Rademakers A
- Rakai A
- Ratnikov F
- Rawlings T
- Redi F
- Ricciardi S
- Rinaldesi M
- Robbe P
- Rodin V
- Rodin V
- Roganova T
- Rokujo H
- Rosa G
- Rovelli T
- Ruchayskiy O
- Ruf T
- Samoylenko V
- Samsonov V
- Saputi A
- Sato O
- Savchenko ES
- Schliwinski JS
- Schmidt-Parzefall W
- Serra N
- Sgobba S
- Shadura O
- Shakin A
- Shaposhnikov M
- Shatalov P
- Shchedrina T
- Shchutska L
- Shevchenko V
- Shibuya H
- Shihora L
- Shirobokov S
- Shustov A
- Silverstein SB
- Simone S
- Simoniello R
- Skorokhvatov M
- Smirnov S
- Sohn JY
- Sokolenko A
- Sola EL
- Solodko E
- Starkov N
- Stoel L
- Storaci B
- Stramaglia ME
- Sukhonos D
- Suzuki Y
- Takahashi S
- Tastet JL
- Teterin P
- Timiryasov I
- Tioukov V
- Tommasini D
- Torii M
- Tosi N
- Treille D
- Tsenov R
- Ulin S
- Ull AS
- Ustyuzhanin A
- Uteshev Z
- Van Herwijnen E
- Van Waasen S
- Vankova-Kirilova G
- Vannucci F
- Venkova P
- Venturi V
- Vilchinski S
- Villa M
- Vincke H
- Vincke H
- Visone C
- Vlasik K
- Volkov A
- Voronkov R
- Wanke R
- Wertelaers P
- Woo J-K
- Wurm M
- Xella S
- Yilmaz D
- Yilmazer AU
- Yoon CS
- Zarubin P
- Zarubina I
- Zaytsev Y
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
This paper presents a fast approach to simulating muons produced in interactions of the SPS proton beams with the target of the SHiP experiment. The SHiP experiment will be able to search for new long-lived particles produced in a 400 GeV/c SPS proton beam dump and which travel distances between fifty metres and tens of kilometers. The SHiP detector needs to operate under ultra-low background conditions and requires large simulated samples of muon induced background processes. Through the use of Generative Adversarial Networks it is possible to emulate the simulation of the interaction of 400 GeV/c proton beams with the SHiP target, an otherwise computationally intensive process. For the simulation requirements of the SHiP experiment, generative networks are capable of approximating the full simulation of the dense fixed target, offering a speed increase by a factor of Script O(106). To evaluate the performance of such an approach, comparisons of the distributions of reconstructed muon momenta in SHiP's spectrometer between samples using the full simulation and samples produced through generative models are presented. The methods discussed in this paper can be generalised and applied to modelling any non-discrete multi-dimensional distribution
The Definition of Art in the Customs Law
- Author
- A K Leah
- Arthur V Jacoby
- Bleistein V. Donaldson Lithographing Co
- Brancusi
- C H Farley
- C Ruiz
- Council Directive
- Cristina Sala
- G Fotherby
- G Pooke
- H Singerman
- I Tarsis
- Ingrid Raab
- J Hagen
- J L Darraby
- J Levine
- J T Dean
- K Orcutt
- Krystyna Gmurzynska-Bscher
- L D Boff
- L Hunt
- Lazarus
- M Costanza
- M Gayford
- M Govan
- M Kennedy
- M Lang
- M N Berry
- P Crowther
- Peters V Us
- Petry V Co
- Reinhard Onnasch
- Robertson V Glendinning
- S Giry
- S J C Hemels
- Stern V Us
- T Mann
- Tiffany V Us
- Treas
- Treas
- Tutton V Viti
- U S V Ehrich
- U S V Perry
- Us V
- Volker Huber V
- Westfïżœlischer Kunstverein V. Hauptzollamt
- Young V Bohn
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2013
- Field of study
Fast simulation of muons produced at the SHiP experiment using Generative Adversarial Networks
- Author
- Ahdida C.
- Albanese R.
- Alexandrov A.
- Anokhina A.
- Aoki S.
- Arduini G.
- Atkin E.
- Azorskiy N.
- Back J. J.
- Bagulya A.
- Baranov A.
- Bardou F.
- Barker G. J.
- Battistin M.
- Bauche J.
- Bay A.
- Bayliss V
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- Prokudin M.
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- Rodin Viktor
- Rodin Volodymyr
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- Simoniello R.
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- Stramaglia M. E.
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- Suzuki Y.
- Takahashi S.
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- Teterin P.
- Timiryasov I
- Tioukov V
- Tommasini D.
- Torii M.
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- Treille D.
- Tsenov R.
- Ulin S.
- Ull A. Sanz
- Ustyuzhanin A.
- Uteshev Z.
- van Herwijnen E.
- van Waasen S.
- Vankova-Kirilova G.
- Vannucci F.
- Venkova P.
- Venturi V.
- Vilchinski S.
- Villa M.
- Vincke Heinz
- Vincke Helmut
- Visone C.
- Vlasik K.
- Volkov A.
- Voronkov R.
- Wanke R.
- Wertelaers P.
- Woo J-K
- Wurm M.
- Xella S.
- Yilmaz D.
- Yilmazer A. U.
- Yoon C. S.
- Zarubin P.
- Zarubina I
- Zaytsev Yu
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
This paper presents a fast approach to simulating muons produced in interactions of the SPS proton beams with the target of the SHiP experiment. The SHIP experiment will be able to search for new long-lived particles produced in a 400 GeV/c SPS proton beam dump and which travel distances between fifty metres and tens of kilometers. The SHiP detector needs to operate under ultra-low background conditions and requires large simulated samples of muon induced background processes. Through the use of Generative Adversarial Networks it is possible to emulate the simulation of the interaction of 400 GeV/c proton beams with the SHiP target, an otherwise computationally intensive process. For the simulation requirements of the SHiP experiment, generative networks are capable of approximating the full simulation of the dense fixed target, offering a speed increase by a factor of O(10(6)). To evaluate the performance of such an approach, comparisons of the distributions of reconstructed muon momenta in SHiP's spectrometer between samples using the full simulation and samples produced through generative models are presented. The methods discussed in this paper can be generalised and applied to modelling any non-discrete multi-dimensional distribution
Cross Section for b Jet Production in ppâ Collisions at sâ = 1.8 TeV
- Author
- Abbott B.
- Abolins M.
- Abramov V.
- Acharya B S.
- Adams D L.
- Adams M.
- Alves G A.
- Amos N.
- Anderson E W.
- Baarmand M M.
- Babintsev V V.
- Babukhadia L.
- Baden A.
- Baldin B.
- Balm P W.
- Banerjee S.
- Bantly J.
- Barberis E.
- Baringer P.
- Bartlett J F.
- Bassler U.
- Bean A.
- Begel M.
- Belyaev A.
- Beri S B.
- Bernardi G.
- Bertram I.
- Besson A.
- Bezzubov V A.
- Bhat P C.
- Bhatnagar V.
- Bhattacharjee M.
- Bhler M.
- Bhnlein A.
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- Borcherding F.
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- Brooijmans G.
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- Castilla-Valdez H.
- Chakraborty D.
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- Choi S.,
- Chopra S.
- Christenson J H.
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- Gartung P.
- Gavrilov V.
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- Genser K.
- Gerber C E.
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- Hansen Scott
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- Hebert Christian
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- Heuring T.
- Hirosky R.
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- Parua N.
- Paterno M.
- Patwa A.
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- Piegaia R.
- Piekarz H.
- Pope B G.
- Popkov E.
- Prosper H B.
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- Simak V.
- Singh H.
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- Sirotenko V.
- Slattery P.
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- Smith R P.
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- Snow J.
- Snyder S.
- Solomon J.
- Sorin V.
- Sosebee M.
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- Souza M.
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- Steinbruck G.
- Stephens R W.
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- Stichelbaut F.
- Stoker D.
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- Streets K.
- Strovink M.
- Stutte L.
- Sznajder A.
- Taylor W.
- Tentindo-Repond S.
- Thompson J.
- Toback D.
- Tripathi S M.
- Trippe T G.
- Turcot a S.
- Tuts P M.
- van Gemmeren P.
- van Kooten R.
- Vaniev V.
- Varelas N.
- Volkov a A.
- Vorobev a P.
- Wahl H D.
- Wang H.
- Wang Z M.
- Warchol J.
- Watts G.
- Wayne M.
- Weerts H.
- White A.
- White J T.
- Whiteson D.
- Wightman J A.
- Wijngaarden D A.
- Willis S.
- Wimpenny S J.
- Wirjawan J V D.
- Womersley J.
- Wood D R.
- Yamada R.
- Yamin P.
- Yasuda T.
- Yip K.
- Youssef S.
- Yu J.
- Yu Z.
- Zanabria M.
- Zheng H.
- Zhou Z.
- Zhu Z H.
- Zielinski M.
- Zieminska D.
- Zieminski A.
- Zutshi V.
- Zverev E G.
- Zylberstejn A.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2000
- Field of study
Bottom quark production in pbar-p collisions at sqrt(s)=1.8 TeV is studied with 5 inverse picobarns of data collected in 1995 by the DO detector at the Fermilab Tevatron Collider. The differential production cross section for b jets in the central rapidity region (|y(b)| < 1) as a function of jet transverse energy is extracted from a muon-tagged jet sample. Within experimental and theoretical uncertainties, DO results are found to be higher than, but compatible with, next-to-leading-order QCD predictions. (arXiv