953 research outputs found
Flavor conversion of cosmic neutrinos from hidden jets
- Author
- A Atoyan
- A Atoyan
- A MacFadyen
- A. Yu. Smirnov
- AA Abdo
- AA Abdo
- AI MacFadyen
- AP Szabo
- AS Dighe
- B Pontecorvo
- C Lunardini
- CD Matzner
- DC Leonard
- E Bugaev
- E Waxman
- E Waxman
- E Waxman
- EK Akhmedov
- FW Stecker
- J Ahrens
- J Alvarez-Muniz
- J Alvarez-Muniz
- J Granot
- JA Aguilar
- JG Learned
- K Murase
- L Nellen
- L Wang
- L Wolfenstein
- L Wolfenstein
- M Kowalski
- ML Costantini
- N Gupta
- O Mena
- P Lipari
- P Mészáros
- R Enberg
- S Ando
- S Ando
- S Razzaque
- S Razzaque
- S Razzaque
- Soebur Razzaque
- SP Mikheev
- SP Mikheev
- ST Petcov
- T DeYoung
- T Piran
- TK Gaisser
- X-Y Wang
- Y Farzan
- Z Maki
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 22/12/2009
- Field of study
High energy cosmic neutrino fluxes can be produced inside relativistic jets
under the envelopes of collapsing stars. In the energy range E ~ (0.3 - 1e5)
GeV, flavor conversion of these neutrinos is modified by various matter effects
inside the star and the Earth. We present a comprehensive (both analytic and
numerical) description of the flavor conversion of these neutrinos which
includes: (i) oscillations inside jets, (ii) flavor-to-mass state transitions
in an envelope, (iii) loss of coherence on the way to observer, and (iv)
oscillations of the mass states inside the Earth. We show that conversion has
several new features which are not realized in other objects, in particular
interference effects ("L- and H- wiggles") induced by the adiabaticity
violation. The neutrino-neutrino scattering inside jet and inelastic neutrino
interactions in the envelope may produce some additional features at E > 1e4
GeV. We study dependence of the probabilities and flavor ratios in the
matter-affected region on angles theta13 and theta23, on the CP-phase delta, as
well as on the initial flavor content and density profile of the star. We show
that measurements of the energy dependence of the flavor ratios will, in
principle, allow to determine independently the neutrino and astrophysical
parameters.Comment: 56 pages, 19 figures. Minor changes. Accepted by JHEP
Acceptance of Golden Rice in the Philippine Rice Bowl
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2003
- Field of study
Prospective evaluation of chronic pain associated with posterior autologous iliac crest bone graft harvest and its effect on postoperative outcome
- Author
- B Summers
- Carolyn E Schwartz
- DA Dillman
- David A Wang
- David H Kim
- DG Anderson
- E Ahlmann
- ED Arrington
- EE Keller
- EM Younger
- H Eufinger
- H Gundes
- HM Fernandes
- J Canady
- J Cockin
- JC Banwart
- JC Fairbank
- JE Ware Jr
- JK Burkus
- Julia F Martha
- KP Singh
- Ling Li
- N Cowan
- NR Colterjohn
- P Robertson
- Paulette Kowalski
- PD Sawin
- R Puri
- RF Heary
- Rita Bode
- SP Hardy
- Y Mirovsky
- Publication venue
- BioMed Central
- Publication date
- 01/01/2009
- Field of study
<p>Abstract</p> <p>Background</p> <p>Autogenous Iliac Crest Bone Graft (ICBG) has been the "gold standard" for spinal fusion. However, bone graft harvest may lead to complications, such as chronic pain, numbness, and poor cosmesis. The long-term impact of these complications on patient function and well-being has not been established but is critical in determining the value of expensive bone graft substitutes such as recombinant bone morphogenic protein. We thus aimed to investigate the long-term complications of ICBG. Our second aim was to evaluate the psychometric properties of a new measure of ICBG morbidity that would be useful for appropriately gauging spinal surgery outcomes.</p> <p>Methods</p> <p>Prospective study of patients undergoing spinal fusion surgery with autologous ICBG. The SF-36v2, Oswestry Disability Index, and a new 14-item follow-up questionnaire addressing persistent pain, functional limitation, and cosmesis were administered with an 83% response rate. Multiple regression analyses examined the independent effect of ICBG complications on physical and mental health and disability.</p> <p>Results</p> <p>The study population included 170 patients with a mean age of 51.1 years (SD = 12.2) and balanced gender (48% male). Lumbar fusion patients predominated (lumbar = 148; cervical n = 22). At 3.5 years mean follow-up, 5% of patients reported being bothered by harvest site scar appearance, 24% reported harvest site numbness, and 13% reported the numbness as bothersome. Harvest site pain resulted in difficulty with household chores (19%), recreational activity (18%), walking (16%), sexual activity (16%), work activity (10%), and irritation from clothing (9%). Multivariate regression analyses revealed that persistent ICBG complications 3.5 years post-surgery were associated with significantly worse disability and showed a trend association with worse physical health, after adjusting for age, workers' compensation status, surgical site pain, and arm or leg pain. There was no association between ICBG complications and mental health in the multivariate model.</p> <p>Conclusion</p> <p>Chronic ICBG harvest site pain and discomfort is reported by a significant percentage of patients undergoing this procedure more than three years following surgery, and these complications are associated with worse patient-reported disability. Future studies should consider employing a control group that does not include autologous bone graft harvest, e.g., a group utilizing rhBMP, to determine whether eliminating harvest-site morbidity does indeed lead to observable improvement in clinical outcome sufficient to justify the increased cost of bone graft substitutes.</p
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
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- Anulli F
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- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
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- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
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- Badescu E
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- Yilmaz M
- Yoosootiniya R
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- Zarzhitsky P
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- Zhemchugov A
- Zheng S
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- Zitoun R
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- 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 √s = 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 pT≥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 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{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 neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
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- Abreu H
- Acharya BS
- Adam ER
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- Ahsan M
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- Akesson TPA
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- Akimov AV
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- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
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- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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- Zhemchugov A
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- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
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- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
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- Da Costa JGPF
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- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dafinca A
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- Dale O
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- de Renstrom PAB
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
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- Espinal Curull X
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- Esposito B
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- Etienne F
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- Etienvre AI
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- Etzion E
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- Evans H
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- Fabbri L
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- Farrell S
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- Fedorko W
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- Feigl S
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- Feligioni L
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- Feng C
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- Feng EJ
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- Ferrando BMS
- Ferrando J
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- Ferrara V
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- Flowerdew MJ
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- Formica A
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- Forti A
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- Yilmaz M
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- Zaidan R
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- Zaman A
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- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
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- Zeitnitz C
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- Zemla A
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- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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- Zhao Z
- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
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- Abajyan T
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- Abdallah J
- Abdelalim AA
- Abdinov O
- Aben R
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- Meguro T
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- Mehta A
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- Milov A
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- Scherzer MI
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- Schroeder TV
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- Schultens MJ
- Schultes J
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
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- Schwartzman A
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- Schwemling P
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- Schwierz R
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- Searcy J
- Sedov G
- Sedykh E
- Seidel SC
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- Sekhniaidze G
- Sekula SJ
- Selbach KE
- Seliverstov DM
- Sellden B
- Sellers G
- Seman M
- Semprini-Cesari N
- Serfon C
- Serin L
- Serkin L
- Seuster R
- Severini H
- Sfyrla A
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- Shamim M
- Shan LY
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- Shatalov PB
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- Shimojima M
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- Shiyakova M
- Shmeleva A
- Shochet MJ
- Short D
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
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- Simonyan M
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- Sinev NB
- Sipica V
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjoelin J
- Sjursen TB
- Skinnari LA
- Skottowe HP
- Skovpen K
- Skubic P
- Slater NM
- Slavicek T
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smit GVY
- Smith BC
- Smith D
- Smith KM
- Smizanska M
- Smolek K
- Snesarev AA
- Snow J
- Snow SW
- Snyder S
- Sobie R
- Sodomka J
- Soffer A
- Soh DA
- Soiovyallv V
- Solans CA
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- Soldatov EY
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- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Staude A
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- Steinbach P
- Steinberg P
- Stekl I
- Stelzer B
- Stelzer HJ
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- Stoicea G
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- Strachota P
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- Straessner A
- Strandberg J
- Strandberg S
- Strandlie A
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- Stroynowski R
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- Stumer I
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- Styles NA
- Su D
- Subramania HS
- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Suzuki Y
- Svatos M
- Swedish S
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev A
- Tamsett MC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tani K
- Tannoury N
- Tapprogge S
- Tardif D
- Tarem S
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- Tartarelli GF
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- Temming KK
- Ten Kate H
- Teng PK
- Terada S
- Terashi K
- Terron J
- Testa M
- Teuscher RJ
- Therhaag JJ
- Theveneaux-Pelzer T
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tic T
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
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- Trigger IM
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- Tripiana MF
- Triplett N
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- True P
- Trzebinski M
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- Tsarouchas C
- Tseng JC-L
- Tsiakiris M
- Tsiareshka P
- Tsionou D
- Tsipolitis G
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsung J-W
- Tsuno S
- Tsybychev D
- Tua A
- Tudorache A
- Tudorache V
- Tuggle JM
- Tuna AN
- Turala M
- Turecek D
- Turlay E
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Tzanakos G
- Uchida K
- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Unno Y
- Urbaniec D
- Urquijo P
- Usai G
- Uslenghi M
- Vacavant L
- Vacek V
- Vachon B
- Vague FV
- Vahsen S
- Valenta J
- Valentinetti S
- Valero A
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
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- Van der Deijl PC
- van der Geer R
- van der Graaf H
- van der Leeuw R
- van der Poe E
- van der Ster D
- van Eldik N
- van Gemmeren P
- van Huysduynen LH
- van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vannucci F
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vazquez JGP
- Vegni G
- Veillet JI
- Veloso F
- Veness R
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
- Virzi J
- Vitells O
- Viti M
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- Volpini G
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorwerk V
- Vos M
- Voss R
- Voss TT
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wahlen H
- Wahrmund S
- Wakabayashi J
- Walch S
- Walder J
- Walker R
- Walkowiak W
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- Wang C
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- Wang T
- Warburton A
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- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
- Watkins PM
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- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh AT
- Waugh BM
- Weber MS
- Webster JS
- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Wengler T
- Wengu Z
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Wetter J
- Weydert C
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- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicek F
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Willis W
- Willocoq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wynne BM
- Xella S
- Xiao M
- Xie S
- Xu C
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Z′ Models
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
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- Youssef S
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- Yusuff I
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- Zaidan R
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- Zanello L
- Zanzi D
- Zeitnitz C
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- Zemla A
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- Zenin O
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- Zerwas D
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- Zhemchugov A
- Zhong J
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
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