1,146 research outputs found
Non-Markovian quantum jumps
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 05/05/2008
- Field of study
Get PDFOpen quantum systems that interact with structured reservoirs exhibit
non-Markovian dynamics. We present a quantum jump method for treating the
dynamics of such systems. This approach is a generalization of the standard
Monte Carlo Wave Function (MCWF) method for Markovian dynamics. The MCWF method
identifies decay rates with jump probabilities and fails for non-Markovian
systems where the time-dependent rates become temporarily negative. Our
non-Markovian quantum jump (NMQJ) approach circumvents this problem and
provides an efficient unravelling of the ensemble dynamics.Comment: 4 pages, 2 figures.V2: rewritten abstract and introduction, title
modified. V3: published version, new example case with photonic band ga
Novel Data Acquisition System for Silicon Tracking Detectors
- Author
- Publication venue
- Publication date
- 01/01/2003
- Field of study
Full text linkWe have developed a novel data acquisition system for measuring tracking
parameters of a silicon detector in a particle beam. The system is based on a
commercial Analog-to-Digital VME module and a PC Linux based Data Acquisition
System. This DAQ is realized with C++ code using object-oriented techniques.
Track parameters for the beam particles were reconstructed using off-line
analysis code and automatic detector position alignment algorithm.
The new DAQ was used to test novel Czochralski type silicon detectors. The
important silicon detector parameters, including signal size distributions and
signal to noise distributions, were successfully extracted from the detector
under study. The efficiency of the detector was measured to be 95 %, the
resolution about 10 micrometers, and the signal to noise ratio about 10.Comment: Talk from the 2003 Computing in High Energy and Nuclear Physics
(CHEP03), La Jolla, Ca, USA, March 2003, 6 pages, LaTeX, 5 eps figures. PSN
TUGP00
Processing and Interconnections of Finely Segmented Semiconductor Pixel Detectors for Applications in Particle Physics and Photon Detection
- Publication venue
- Publication date
- 19/02/2021
- Field of study
Get PDFRadiation hardness is in the focus of the development of particle tracking and photon imaging detector installations. Semiconductor detectors, widely used in particle physics experiments, have turned into capacitive-coupled (AC-coupled) detectors from the originally developed conductively coupled (DC-coupled) detectors. This is due to the superior isolation of radiation-induced leakage current in AC-coupled detectors. However, some modern detector systems, such as the tracking detectors in the CERN LHC CMS or ATLAS experiments, are still DC-coupled. This originates from the difficulty of implementing AC coupling on very small pixel detector areas. In this report, we describe our advances in the detector processing technology. The first topic is the applications of the atomic layer deposition processing technology, which enables the very high densities of capacitance and resistance that are needed when the dimensions of the physical segmentation of pixel detectors need to be scaled down. The second topic is the flip-chip/bump-bonding interconnection technology, which is necessary in order to manufacture pixel detector modules on a large scale with a more than 99% yield of noise-free and faultless pixels and detector channels.Peer reviewe
Sandeels in the diets of seals: application of novel and conventional methods of analysis to faeces from seals in the Moray Firth area of Scotland
- Author
- Publication venue
- 'Cambridge University Press (CUP)'
- Publication date
- Field of study
Full text linkMeasurement of the Z/gamma* + b-jet cross section in pp collisions at 7 TeV
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe production of b jets in association with a Z/gamma* boson is studied
using proton-proton collisions delivered by the LHC at a centre-of-mass energy
of 7 TeV and recorded by the CMS detector. The inclusive cross section for
Z/gamma* + b-jet production is measured in a sample corresponding to an
integrated luminosity of 2.2 inverse femtobarns. The Z/gamma* + b-jet cross
section with Z/gamma* to ll (where ll = ee or mu mu) for events with the
invariant mass 60 < M(ll) < 120 GeV, at least one b jet at the hadron level
with pT > 25 GeV and abs(eta) < 2.1, and a separation between the leptons and
the jets of Delta R > 0.5 is found to be 5.84 +/- 0.08 (stat.) +/- 0.72 (syst.)
+(0.25)/-(0.55) (theory) pb. The kinematic properties of the events are also
studied and found to be in agreement with the predictions made by the MadGraph
event generator with the parton shower and the hadronisation performed by
PYTHIA.Comment: Submitted to the Journal of High Energy Physic
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
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- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
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- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
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- Zarubin A
- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
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- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Wolszczak W
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu L
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yucel M
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zeinali M
- Zeise M
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zheng Y
- Zhokin A
- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- Publication date
- 01/01/2013
- Field of study
Get PDFIn OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Measurement of the t(t)over-bar production cross section in the dilepton channel in pp collisions at âs=8 TeV
- Author
- Abdelalim AA
- Adam W
- Adler Volker
- Alda WL
- Alderweireldt S
- Alves GA
- Antunovic Z
- Asawatangtrakuldee C
- Assran Y
- Attikis A
- Avila C
- Ban Y
- Bansal M
- Bansal S
- Basegmez S
- Beernaert Kelly
- Beliy N
- Beluffi C
- Benucci Leonardo
- Bergauer T
- Bernardes CA
- Besancon M
- Bian JG
- Blekman F
- Blyweert S
- Brigljevic V
- Bruno G
- Caebergs T
- Caillol C
- Carvalho W
- Castello R
- Caudron A
- Ceard L
- Chatrchyan S
- Chen GM
- Chen HS
- Chen M
- Chinellato J
- Cimmino Anna
- Clerbaux B
- Cornelis T
- Costantini Silvia
- Couderc F
- Custodio A
- D'Hondt J
- Da Costa EM
- Da Silva WLP
- Da Silveira GG
- Damiao DD
- Daubie E
- De Lentdecker G
- De Souza SF
- De Wolf EA
- Delaere C
- Dias FA
- Diblen SS
- Dildick Sven
- Dimitrov A
- Dragicevic M
- du Pree T
- Du R
- Eerola P
- Elgammal S
- Ero J
- Fabjan C
- Favart D
- Favart L
- Fedi G
- Figueiredo DM
- Finger M
- Finger M
- Florez C
- Forthomme L
- Friedl M
- Fruhwirth R
- Garcia Guillaume
- Garcia JMV
- Gay APR
- Genchev V
- Ghete VM
- Giammanco A
- Glushkov I
- Godinovic N
- Gomez JP
- Gonzalez JS
- Gregores EM
- Guo Y
- Hadjiiska R
- Hammad GH
- Harkonen J
- Hartl C
- Heracleous N
- Hollar J
- Hormann N
- Hrubec J
- Iaydjiev P
- Janssen X
- Jeitler M
- Jez P
- Jiang CH
- Kadastik M
- Kadija K
- Kalogeropoulos A
- Kamel AE
- Karimaki V
- Keaveney J
- Khachatryan V
- Kiesenhofer W
- Kim TJ
- Kinnunen R
- Klein Benjamin
- Knunz V
- Knutsson A
- Komm M
- Kortelainen MJ
- Kovac M
- Kozhuharov V
- Krammer M
- Kratschmer I
- Lampen T
- Lassila-Perini K
- Lehti S
- Lelas D
- Lellouch Jeremie
- Lemaitre V
- Leonard A
- Li Q
- Li W
- Liang D
- Liang S
- Liao J
- Liko D
- Linden T
- Litov L
- Liu S
- Lowette S
- Luetic J
- Luukka P
- Luyckx S
- Maenpaa T
- Maes M
- Mahmoud MA
- Malbouisson H
- Malek M
- Manganote EJT
- Mao Y
- Marage PE
- Marinov A
- Marono MV
- Martins CD
- Martins MC
- Martins T
- Mavromanolakis G
- McCartin Joseph
- Mekterovic D
- Meng X
- Mercadante PG
- Mikulec I
- Militaru O
- Mohammadi A
- Montoya CAC
- Moreno BG
- Morovic S
- Mossolov V
- Mousa J
- Mucibello L
- Mundim L
- Muntel M
- Murumaa M
- Nicolaou C
- Nogima H
- Novaes SF
- Nuttens C
- Ocampo Rios Alberto Andres
- Ochesanu S
- Olbrechts A
- Padula SS
- Pagano D
- Pavlov B
- Peltola T
- Pereira AV
- Pernie L
- Petkov P
- Pin A
- Piotrzkowski K
- Piperov S
- Plestina R
- Pol ME
- Polic D
- Popov A
- Ptochos F
- Puljak I
- Qian SJ
- Quertenmont L
- Rabady D
- Radi A
- Rahbaran B
- Raidal M
- Razis PA
- Rebane L
- Reis T
- Rodozov M
- Rohringer H
- Roland B
- Rougny R
- Ryckbosch Dirk
- Sanabria JC
- Santaolalla J
- Santoro A
- Schofbeck R
- Selvaggi M
- Seva T
- Shumeiko N
- Sierra LFC
- Sigamani Michael
- Sirunyan AM
- Souza MHG
- Strauss J
- Strobbe Nadja
- Strom D
- Sultanov G
- Sznajder A
- Tao J
- Taurok A
- Tavernier S
- Thomas L
- Thyssen Filip
- Tiko A
- Tikvica L
- Tomei TRFP
- Treberer-Treberspurg W
- Tumasyan A
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tuuva T
- Tytgat Michael
- Van Doninck W
- Van Haevermaet H
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
- Van Remortel N
- Van Spilbeeck A
- Vander Velde C
- Vanlaer P
- Villella I
- Voutilainen M
- Vutova M
- Walsh SinĂŠad Mary
- Waltenberger W
- Wang D
- Wang J
- Wang X
- Wang Z
- Wendland L
- Wulz CE
- Yazgan Efe
- Zaganidis Nikolaos
- Zhang L
- Zou W
- Publication venue
- Publication date
- 01/01/2014
- Field of study
Get PDFThe top-antitop quark (t (t) over bar) production cross section is measured in proton-proton collisions at root s = 8 TeV with the CMS experiment at the LHC, using a data sample corresponding to an integrated luminosity of 5.3 fb(-1). The measurement is performed by analysing events with a pair of electrons or muons, or one electron and one muon, and at least two jets, one of which is identified as originating from hadronisation of a bottom quark. The measured cross section is 239 +/- 2 (stat.) +/- 11 (syst.) +/- 6 (lum.) pb, for an assumed top-quark mass of 172.5 GeV, in agreement with the prediction of the standard model
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
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- Blumenfeld B
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- Bonacorsi D
- Bonato A
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- Bornheim A
- Borras K
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- Bortignon P
- Bortoletto D
- Bose S
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- Bostock F
- Botta C
- Boudoul G
- Boulahouache C
- Boumediene D
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- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
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- Brinkerhoff A
- Broccolo G
- Brochero Cifuentes JA
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
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- Bryer AG
- Buchmann MA
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- Busson P
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- Butler PH
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- Bylsma B
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
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- Cappello G
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- Casal B
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- Castaldi R
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- Castro A
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- Cavallari F
- Cavallo FR
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- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
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- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
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- Chen GM
- Chen HS
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- Chen KH
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- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Cho Y
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
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- Chwalek T
- Ciesielski R
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- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
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- Collard C
- Colling D
- Conetti S
- Contardo D
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- Conway J
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- Cooper SI
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- Cornelis T
- Correa Martins Junior M
- Cortezon EP
- Cossutti F
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- Costa S
- Costantini S
- Coughlan JA
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- Covarelli R
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- Cuplov V
- Cure B
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- Cutajar M
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- Czellar S
- D'Agnolo RT
- D'Alessandro R
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- D'Enterria D
- D'Hondt J
- Da Costa EM
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Das S
- Daskalakis G
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- Daubie E
- Dauncey P
- David A
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- de Barbaro P
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- de Cassagnac RG
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- de Fatis TT
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- De La Cruz B
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- de Monchenault GH
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- De Roeck A
- de Troconiz JF
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- del Arbol PMR
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- Dirkes G
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- Djordjevic M
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- Dobson M
- Dobur D
- Doesburg R
- Dogangun O
- Dolen J
- Dominguez Vazquez D
- Dominguez A
- Dominik W
- Don CKK
- Dorigo T
- Dorney B
- Doroba K
- Dozen C
- Draeger J
- Dragicevic M
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- Dremin I
- Drouhin F
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- du Pree T
- Duarte Campderros J
- Duarte J
- Dubinin M
- Dudero PR
- Dudko L
- Duenser M
- Dugad S
- Duggan D
- Dumanoglu I
- Dupont-Sagorin N
- Duric S
- Duris J
- Durkin LS
- Duru F
- Dutta D
- Dutta S
- Dutta V
- Dzelalija M
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- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
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- Elgammal S
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- Ellison J
- Elmer P
- Elvira VD
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- Engh D
- Eno SC
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- Erbacher R
- Erdmann M
- Erdmann W
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- Yilmaz Y
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
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- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
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