647 research outputs found
Advances in immunomodulating therapy of HBV infection
- Publication venue
- Ivyspring International Publisher
- Publication date
- 01/01/2005
- Field of study
Patients with chronic hepatitis B virus (HBV) infection have a higher risk of developing liver cirrhosis and hepatocellular carcinoma. Interferon-α, lamivudine and adefovir dipivoxil are the three approved treatment for chronic HBV infection and offers the only means of preventing the development of these complications. However, the efficacy of these agents, in terms of loss of Hepatitis B e antigen with or without seroconversion to Hepatitis B e antibody, normalization of serum alanine transaminase levels, loss of serum HBV DNA, and improvement in liver histology can only be achieved in 20-30% of those treated. Long-term treatment with either lamivudine or adefovir dipivoxil can result in the development of drug resistant mutants leading to an increased length of treatment with additional nucleoside analogues. These limitations of the current antiviral therapies underline the need for alternative therapies. Specific and nonspecific immunotherapeutic strategies to restore effective virus-specific T cell responses in those with chronic HBV infection offers an interesting alternative approach. These immunotherapeutic therapies include the adoptive transfer of HBV immunity, pegylated interferon and therapeutic vaccine therapies
Forty-eight weeks treatment with clevudine 30 mg qd versus lamivudine 100 mg qd for chronic hepatitis B infection: a double-blind randomized study
- Author
- Publication venue
- The Korean Association for the Study of the Liver
- Publication date
- 01/01/2010
- Field of study
Search for rare quark-annihilation decays, B --> Ds(*) Phi
- Author
- Abe T
- Abrams GS
- Adye T
- Ahmed M
- Ahmed S
- Alam MS
- Albert J
- Aleksan R
- Allen MT
- Allison J
- Allmendinger T
- Altenburg D
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Aston D
- Aubert B
- Azzolini V
- Baak M
- Back JJ
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Barate R
- Bard DJ
- Barlow NR
- Barlow RJ
- Barrett M
- Bartoldus R
- Batignani G
- Battaglia M
- Bauer JM
- Beck TW
- Behera PK
- Bellini F
- Benayoun M
- Benelli G
- Berger N
- Bernard D
- Berryhill JW
- Best D
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhimji W
- Bhuyan B
- Bianchi F
- Biasini M
- Biesiada J
- Blanc F
- Blaylock G
- Blinov AE
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bona M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandenburg G
- Brandt T
- Brau J
- Breon AB
- Brose J
- Brown CL
- Brown CM
- Brown DN
- Brown DN
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- Bugg W
- Bukin AD
- Bula R
- Bulten H
- Buono LD
- Burchat PR
- Burke JP
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- Buzzo A
- Cahn RN
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
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- Cartaro C
- Cavallo N
- Cavoto G
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- Chai X
- Chaisanguanthum KS
- Chao M
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- Chauveau J
- Chavez CA
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- Coleman JP
- Collaboration BABAR
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- Convery MR
- Cossutti F
- Cote D
- Cottingham WN
- Couderc F
- Covarelli R
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Cristinziani M
- Cuhadar-Donszelmann T
- Cunha A
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- de Monchenault GH
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- Dubois-Felsmann GP
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- Kolomensky YG
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- Mayer B
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- McKenna JA
- McMahon TR
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- Mellado B
- Menges W
- Messner R
- Meyer WT
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- Minamora JS
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- Mohanty GB
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- Moore TB
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- Petersen BA
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- Rosenberg EI
- Rotondo M
- Roudeau P
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- Ulmer KA
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- Vasileiadis G
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- Verderi M
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- Wagoner DE
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- Wappler FR
- Watson AT
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams JC
- Willocq SY
- Wilson FF
- Wilson JR
- Wilson MG
- Wilson RJ
- Winklmeier F
- Wisniewski WJ
- Wittgen M
- Wong QK
- Wormser G
- Wright DH
- Wright DM
- Wu J
- Wu SL
- Xie Y
- Yamamoto RK
- Yarritu AK
- Ye S
- Yeche C
- Yi JI
- Yi K
- Young CC
- Yu Z
- Yushkov AN
- Zain SB
- Zallo A
- Zeng Q
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- Zhang J
- Zhang L
- Zhao HW
- Zhu YS
- Ziegler V
- Zito M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 12/12/2005
- Field of study
We report on searches for B- --> Ds- Phi and B- --> Ds*- Phi. In the context
of the Standard Model, these decays are expected to be highly suppressed since
they proceed through annihilation of the b and u-bar quarks in the B- meson.
Our results are based on 234 million Upsilon(4S) --> B Bbar decays collected
with the BABAR detector at SLAC. We find no evidence for these decays, and we
set Bayesian 90% confidence level upper limits on the branching fractions BF(B-
--> Ds- Phi) Ds*- Phi)<1.2x10^(-5). These results
are consistent with Standard Model expectations.Comment: 8 pages, 3 postscript figues, submitted to Phys. Rev. D (Rapid
Communications
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- 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
- Ackers M
- 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
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- 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
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
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- Anderson KJ
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- Andrieux M-L
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- Anh TV
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
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- Ziolkowski M
- Zitoun R
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- Zmouchko VV
- Zobernig G
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- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
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- Acharya BS
- Achkar B
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- Adamek L
- Adelman J
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- Akesson TPA
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- Al Khoury K
- Alberghi GL
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- Aleksa M
- Aleksandrov IN
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- Zhemchugov A
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- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
A Precision Measurement of the Lambda_c Baryon Mass
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- VON WIMMERSPERG TOELLER Jh
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- Wilden L
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- Yi J
- Yi K
- Young Cc
- Yu Z
- Yumiceva Fx
- Yushkov An
- Zain Sb
- Zallo A
- Zeng Q
- Zghiche A
- Zhang J
- Zhang L
- Zhao Hw
- Zhu Ys
- Zito M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2005
- Field of study
The Λc+ baryon mass is measured using Λc+→ΛKS0K+ and Λc+→Σ0KS0K+ decays reconstructed in 232
fb−1 of data collected with the BaBar detector at the PEP-II
asymmetric-energy e+e− storage ring. The Λc+ mass is measured to
be 2286.46±0.14MeV/c2. The dominant systematic uncertainties
arise from the amount of material in the tracking volume and from the magnetic
field strength.Comment: 14 pages, 8 postscript figures, submitted to Phys. Rev.
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
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- Afik Y
- Agheorghiesei C
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- Aleksa M
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- Zanzi D
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- Zeißner SV
- Zemaityte G
- Zeng JC
- Zeng Q
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- Zerwas D
- Zgubič M
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- Zhang Z
- Zhao P
- Zhao X
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- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- 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 NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković 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 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ 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 57.0−5.9 +6.0 (stat.) −3.3 +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
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 
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- Abraham NL
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- Acharya BS
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- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
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- Aguilar-Saavedra JA
- Ahmadov F
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- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
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- Alconada Verzini MJ
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- Allen BW
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- Aloisio A
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- Alshehri AA
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- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
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- Amrouche CS
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- Andari N
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- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
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- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
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- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
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- Cardillo FC
- Carli I
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- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
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- Carrá S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
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- Morales FAJ
- Morange N
- Moreno Llácer M
- Moreno D
- Morettini P
- Morgenstern M
- Morgenstern S
- Mori D
- Mori T
- Morii M
- Morinaga M
- Morisbak V
- Morley AK
- Mornacchi G
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- Morris JD
- Morvaj L
- Moschovakos P
- Mosidze M
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- Motohashi K
- Mount R
- Mountricha E
- Moyse EJW
- Mönig K
- Muanza S
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- Mueller RSP
- Muenstermann D
- Mullen P
- Mullier GA
- Munoz Sanchez FJ
- Murin P
- Murray WJ
- Murrone A
- Muškinja M
- Mwewa C
- Myagkov AG
- Myers J
- Myska M
- Nachman BP
- Nackenhorst O
- Nagai K
- Nagano K
- Nagasaka Y
- Nagata K
- Nagel M
- Nagy E
- Nairz AM
- Nakahama Y
- Nakamura K
- Nakamura T
- Nakano I
- Nanjo H
- Napolitano F
- Naranjo 
- Narayan R
- Nardo R
- Narrias Villar DI
- Naryshkin I
- Naumann T
- Navarro G
- Navarro JLLR
- Nayyar R
- Neal HA
- Nechaeva PY
- Nedden M
- Neep TJ
- Negri A
- Negrini M
- Nektarijevic S
- Nellist C
- Nelson ME
- Nemecek S
- Nemethy P
- Nessi M
- Neubauer MS
- Neumann M
- Newman PR
- Ng TY
- Ng YS
- Nguyen Manh T
- Nguyen DH
- Nguyen HDN
- Nibigira E
- Nickerson RB
- Nicolaidou R
- Nielsen J
- Nikiforou N
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Ninomiya Y
- Nisati A
- Nishu N
- Nisius R
- Nitsche I
- Nitta T
- Nobe T
- Nodulman L
- Noguchi Y
- Nomachi M
- Nomidis I
- Nomura MA
- Nooney T
- Nordberg M
- Nordkvist B
- Norjoharuddeen N
- Novak T
- Novgorodova O
- Novotny R
- Nozaki M
- Nozka L
- Ntekas K
- Nurse E
- Nuti F
- Oakham FG
- Oberlack H
- Obermann T
- Ocariz J
- Ochi A
- Ochoa I
- Ochoa-Ricoux JP
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- Odaka S
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- Oh SH
- Ohm CC
- Oide H
- Okawa H
- Okazaki Y
- Okumura Y
- Okuyama T
- Olariu A
- Oleiro 
- Olivares Pino SA
- Oliveira Damazio D
- Oliver JL
- Olsson MJR
- Olszewski A
- Olszowska J
- Onofre A
- Onogi K
- Onyisi PUE
- Oppen H
- Oreglia MJ
- Oren Y
- Orestano D
- Orgill EC
- Orlando N
- Orr RS
- Osculati B
- Ospanov R
- Otero y Garzon G
- Otono H
- Ouchrif M
- Ould-Saada F
- Ouraou A
- Outschoorn VI
- Ouyang Q
- Owen M
- Owen RE
- Ozcan VE
- Ozturk N
- O’Connor K
- O’Neil DC
- O’Rourke AA
- O’Shea V
- Pacalt J
- Pacey HA
- Pachal K
- Pacheco Pages A
- Pacheco Rodriguez L
- Padilla Aranda C
- Pagan Griso S
- Paganini M
- Palacino G
- Palazzo S
- Palestini S
- Palka M
- Pallin D
- Panagoulias I
- Pandini CE
- Panduro 
- Pani P
- Panizzo G
- Paolozzi L
- Papadopoulou TD
- Papageorgiou K
- Paramonov A
- Paredes 
- Parida B
- Parker AJ
- Parker KA
- Parker MA
- Parodi F
- Parra G
- Parsons JA
- Parzefall U
- Pascuzzi VR
- Pasner JMP
- Pasqualucci E
- Passaggio S
- Pastor O
- Pastore F
- Pasuwan P
- Pataraia S
- Pater JR
- Pathak A
- Pauly T
- Paz I
- Pearson B
- Pedersen M
- Pedraza Lopez S
- Pedro R
- Peixoto APP
- Peleganchuk SV
- Penc O
- Peng C
- Peng H
- Peralva BS
- Perego MM
- Pereira RA
- Pereira RM
- Perepelitsa DV
- Peri F
- Perini L
- Pernegger H
- Perrella S
- Peshekhonov VD
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
- Petit E
- Petridis A
- Petridou C
- Petrillo KF
- Petroff P
- Petrolo E
- Petrov M
- Petrucci F
- Pettee M
- Pettersson NE
- Peyaud A
- Pezoa R
- Pham T
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- Phillips PW
- Piacquadio G
- Pianori E
- Picazio A
- Pickering MA
- Piegaia R
- Pilcher JE
- Pilkington AD
- Pinamonti M
- Pinfold JL
- Pitt M
- Plante IJ
- Pleier M-
- Pleskot V
- Plotnikova E
- Pluth D
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Ponomarenko D
- Pontecorvo L
- Popeneciu GA
- Portillo 
- Pospisil S
- Potamianos K
- Potrap IN
- Potter CJ
- Potti H
- Poulsen T
- Poveda J
- Powell TD
- Pozo 
- Pralavorio P
- Prell S
- Price D
- Price LE
- Primavera M
- Prince S
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Puigdengoles C
- Puri A
- Puzo P
- Qian J
- Qin Y
- Quadt A
- Queitsch-Maitland M
- Quilleuc EP
- Quintero DM
- Qureshi A
- Rados P
- Ragusa F
- Rahal G
- Raine JA
- Rajagopalan S
- Rashid T
- Raspopov S
- Ratti MG
- Rauch DM
- Rauscher F
- Rave S
- Ravina B
- Ravinovich I
- Rawling JH
- Raymond M
- Read AL
- Readioff NP
- Reale M
- Rebuzzi DM
- Redelbach A
- Redlinger G
- Reece R
- Reed RG
- Reeves K
- Regie JB
- Rehnisch L
- Reichert J
- Reiss A
- Rembser C
- Ren H
- Rescigno M
- Resconi S
- Resseguie ED
- Rettie S
- Reynolds E
- Rezanova OL
- Reznicek P
- Richter R
- Richter S
- Richter-Was E
- Ricken O
- Ridel M
- Rieck P
- Riegel CJ
- Rifki O
- Rijssenbeek M
- Rimoldi A
- Rimoldi M
- Rinaldi L
- Ripellino G
- Ristić B
- Ritsch E
- Riu I
- Rivera 
- Rizatdinova F
- Rizvi E
- Rizzi C
- Roberts RT
- Robertson SH
- Robichaud-Veronneau A
- Robinson D
- Robinson JEM
- Robson A
- Rocco E
- Roda C
- Rodina Y
- Rodrigues 
- Rodriguez Bosca S
- Rodriguez Perez A
- Rodriguez Rodriguez D
- Rodríguez 
- Roe S
- Rogan CS
- Roland CPA
- Roloff J
- Romaniouk A
- Romano M
- Rompotis N
- Ronzani M
- Roos L
- Rosati S
- Rosbach K
- Rose P
- Rosien N
- Rossetti V
- Rossi E
- Rossi LP
- Rossini L
- Rosten JHN
- Rosten R
- Rotaru M
- Rothberg J
- Rousseau D
- Roy D
- Rozanov A
- Rozen Y
- Röhrig R
- Ruan X
- Rubbo F
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rutherfoord JP
- Ruthmann N
- Rühr F
- Rüttinger EM
- Ryabov YF
- Rybar M
- Rybkin G
- Ryu S
- Ryzhov A
- Rzehorz GF
- Røhne O
- Sabatini P
- Sabato G
- Sacerdoti S
- Sadrozinski HF
- Sadykov R
- Safai Tehrani F
- Saha P
- Sahinsoy M
- Sahu A
- Sahu S
- Saimpert M
- Saito M
- Saito T
- Sakamoto H
- Sakharov A
- Salamani D
- Salamanna G
- 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
- Sampsonidou D
- Sanchez Pineda A
- Sandaker H
- Sander CO
- Sanders H
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sano Y
- Sansoni A
- Santoni C
- Santos H
- Santos SP
- Santoyo Castillo I
- Sapronov A
- Saraiva JG
- Sargedas 
- Sargsyan L
- Sasaki O
- Sato K
- Sauvan E
- Savard P
- Savic N
- Sawada R
- Sawyer C
- Sawyer L
- Says LP
- Sánchez J
- Sbarra C
- Sbrizzi A
- Scanlon T
- Schaarschmidt J
- Schacht P
- Schachtner BM
- Schaefer D
- Schaefer L
- Schaeffer J
- Schaepe S
- Schaffer AC
- Schaile D
- Schamberger RD
- Scharmberg N
- Schäfer U
- Schegelsky VA
- Scheirich D
- Schenck F
- Schernau M
- Schiavi C
- Schier S
- Schildgen LK
- Schillaci ZM
- Schioppa EJ
- Schioppa M
- Schleicher KE
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schnoor U
- Schoeffel L
- Schoening A
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder T
- Schulte A
- Schultz-Coulon H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schweiger H
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scornajenghi M
- Scuri F
- Scutti F
- Scyboz LM
- Seabra LF
- Searcy J
- Sebastiani CD
- Seema P
- Seidel SC
- Seiden A
- Seiss T
- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Semprini-Cesari N
- Sen S
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian JD
- Shaikh NW
- Shalyugin A
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Sharma A
- Sharma AS
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shen Y
- Sherafati N
- Sherman AD
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shoaleh Saadi D
- Shochet MJ
- Shojaii S
- Shope DR
- Shrestha S
- Shulga E
- Sicho P
- Sickles AM
- Sidebo PE
- Sideras Haddad E
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silva M
- Silverstein SB
- Simic L
- Simion S
- Simioni E
- Simon M
- Simone A
- Sinervo P
- Sinev NB
- Sioli M
- Sipio R
- Siragusa G
- Siral I
- Sivoklokov SY
- Sjölin J
- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Soffa AM
- Soffer A
- Soh DA
- Sokhrannyi G
- Solans Sanchez CA
- Solar M
- Soldatov EY
- Soldevila U
- Solin A
- Solis A
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Song W
- Sopczak A
- Sopkova F
- Sosa D
- Sotiropoulou CL
- Sottocornola S
- Soualah R
- Soukharev AM
- Sousa MJ
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spanò F
- Sperlich D
- Spettel F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spiteri DP
- Spousta M
- Stabile A
- Stamen R
- Stamm S
- Stanecka E
- Stanek RW
- Stanescu C
- Stanitzki MM
- Stapf B
- Stapnes S
- Starchenko EA
- Stark GH
- Stark J
- Stark SH
- Staroba P
- Starovoitov P
- Staszewski R
- Stärz S
- Stegler M
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Sterzo FL
- Stevenson TJ
- Stewart GA
- Stockton MC
- Stoicea G
- Stolte P
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Strom DM
- Stroynowski R
- Ströhmer R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
- Su J
- Suchek S
- Sugaya Y
- Suk M
- Sulin VV
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Sydorenko A
- Sykora I
- Sykora T
- Søgaard A
- Šfiligoj T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Tahirovic E
- Taiblum N
- Takai H
- Takashima R
- Takasugi EH
- Takeda K
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tanaka J
- Tanaka M
- Tanaka R
- Tang F
- Tanioka R
- Tannenwald BB
- Tapia Araya S
- Tapprogge S
- Tarek 
- Tarem S
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares 
- Tayalati Y
- Taylor AC
- Taylor AJ
- Taylor GN
- Taylor PTE
- Taylor W
- Tee AS
- Teixeira-Dias P
- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Thais SJ
- Theveneaux-Pelzer T
- Thiele F
- Thomas JP
- Thompson AS
- Thompson PD
- Thomsen LA
- Thomson E
- Tian Y
- Ticse Torres RE
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Tobon CA
- Todome K
- Todorova-Nova S
- Todt S
- Tojo J
- Tokár S
- Tokushuku K
- Tolley E
- Tomiwa KG
- Tomoto M
- Tompkins L
- Toms K
- Tong B
- Tornambe P
- Torrence E
- Torres H
- Torró Pastor E
- Tosciri C
- Toth J
- Touchard F
- Tovey DR
- Treado CJ
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Trischuk W
- Trocmé B
- Trofymov A
- Troncon C
- Trovatelli M
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tseng JC
- Tsiareshka PV
- Tsirintanis N
- 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
- Turk 
- Turra R
- Tuts PM
- Tylmad M
- Tzovara E
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valdes Santurio E
- Vale MAB
- Vale T
- Valente M
- Valentinetti S
- Valentino D
- Valero A
- Valéry L
- Vallance RA
- Vallier A
- Valls Ferrer JA
- Van Daalen TR
- Van Den Wollenberg W
- Van der Graaf H
- Van Gemmeren P
- Van Nieuwkoop J
- Van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez 
- Vazquez 
- Vazquez JG
- Veatch J
- Vecchio V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Vera AM
- Vercesi V
- Verducci M
- Vergara JC
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vetterli MC
- Viaux Maira N
- 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
- Viret S
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vranjes 
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakamiya K
- Walbrecht VM
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Wang AM
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang P
- Wang Q
- Wang R
- Wang R
- Wang R-
- Wang SM
- Wang W
- Wang WT
- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
- Watkins PM
- Watson AT
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Weatherly P
- Webb AF
- Webb S
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- 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
- Wildauer A
- 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
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Woźniak KW
- Wraight K
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xavier CTC
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- 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
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz H
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yue X
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
- Zgubič M
- Zhang D
- Zhang DF
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- 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 NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur 
- Zwalinski L
- Ženiš T
- Živković 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 calorimeter’s performance during the years 2008–2012 using cosmic-ray muon events and proton–proton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fb−1. 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 proton–proton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
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- Zhemchugov A
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Performance of missing transverse momentum reconstruction with the ATLAS detector using proton–proton collisions at √s = 13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying τ -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fb−1
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