318 research outputs found
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
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- Alverson G
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- Anagnostou G
- Anastassov A
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- Wissing C
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- Wood J
- Wood JS
- Worm SD
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- 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
The 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
- 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
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- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
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- 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
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- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
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- Xiao H
- Xie S
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- Yang M
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- 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
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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
The 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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
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- Ahmad M
- Ahmad WH
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- Ahuja S
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- Akin IV
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- Albayrak EA
- Albergo S
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- Anagnostou G
- Anastassov A
- Anderson J
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- Andrea J
- Andreev V
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- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunes JR
- Antunovic Z
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- Apollinari G
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- Baarmand MM
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- Bauerdick LAT
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- Bedoya CF
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
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- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
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- Akgun B
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- Civinini C
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- CMS Collaboration
- Coarasa Perez JA
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- Cooper SI
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- Cutajar M
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
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- Zhukov V
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The 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
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
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- Acosta JG
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- Cwiok M
- Czellar S
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- Da Costa EM
- Dabrowski A
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
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- Dabrowski A
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- Zhang J
- Zhang L
- Zheng Y
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- Zhukov V
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- Zucchetta A
- Zumerle G
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In 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 jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
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- Yilmaz Y
- Yohay R
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- Yun JC
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- Zakaria M
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- Zatserklyaniy A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
Clinical practice guidelines for post-stroke depression in China
- Author
- Aben I
- Ai-qin Wu
- Almeida OP
- Andersen G
- Andersen G
- Beck AT
- Bennett B
- Brott T
- Bryer JB
- Cai WW
- Campbell Burton CA
- Cao L
- Chemerinski E
- Chemerinski E
- Chen AM
- Chen C
- Clark PC
- Currier MB
- de Man-van Ginkel JM
- De Ryck A
- Desmond DW
- Du F
- Eldred C
- Evans RL
- Fan QY
- Fedoroff JP
- Feigin VL
- Ferro JM
- Flaster M
- Friedland JF
- Fruehwald S
- Fu-ying Zhao
- Fultz NH
- Gainotti G
- Gao J
- Ghika-Schmid F
- Glodzik-Sobanska L
- Gordon WA
- Graven C
- Göthe F
- Hackett ML
- Hackett ML
- Hadidi N
- Hama S
- Hamilton M
- Han Y
- Harris AL
- He LM
- Hebert D
- Horváth S
- Ishizaki J
- Jiang XG
- Jiao JT
- Jorge RE
- Kang JH
- Kim JM
- Kim JM
- Kim JS
- Kishi Y
- Kohen R
- Kouwenhoven SE
- Kuo HK
- Langhammer B
- Lei Li
- Li D
- Liang CP
- Lipsey JR
- Liu KJ
- Mahoney FI
- Maines MD
- Ming-wei Wang
- Montgomery SA
- Morris PL
- Nicholl CR
- Niedermaier N
- Paolucci S
- Paolucci S
- Pompili M
- Radloff LS
- Ramasubbu R
- Rankin J
- Robinson RG
- Robinson RG
- Schottke H
- Schulz R
- Sen-yang Lang
- Shen X
- Shi Y
- Smith D
- Snaith RP
- Spalletta G
- Staub F
- Storor DL
- Suh M
- Sun N
- Sun XY
- Sunami E
- Tan S
- Tang CZ
- Tang WK
- Tang WK
- Townend BS
- Verdelho A
- Wang F
- Wang L
- Wang W
- Wang YQ
- Wei N
- Williams LS
- Withall A
- Wu WJ
- Xiang-dong Du
- Xiong GR
- Xu XM
- Yan D
- Yang G
- Yang L
- Yang Y
- Yang Y
- Yi ZM
- Ying-ying Yue
- Yong-gui Yuan
- You LL
- Yue Y
- Yue Y
- Yun-long Deng
- Zhang N
- Zhang T
- Zhang WN
- Zhang ZJ
- Zhao L
- Zhu J
- Zhu L
- Zung WW
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Performance of CMS muon reconstruction in pp collision events at √s = 7TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
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- Adiguzel A
- Adler V
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- Agram JL
- Aguilar-Benitez M
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- Andreev Y
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- Auzinger G
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- 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
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- Bakken JA
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- Calderon De La Barca Sanchez M
- Calderon A
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- Callner J
- Calvert B
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- Camporesi T
- Capiluppi P
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- Cardaci M
- Carlin R
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- Carrillo Moreno S
- Carroll R
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- Castaldi R
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- Ceballos GG
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- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
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- Cittolin S
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- Cline D
- CMS Collaboration
- Cockerill DJA
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- Cutajar M
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- D'Enterria D
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- Da Costa EM
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- Daskalakis G
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- Lelas D
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- Lemaitre V
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- Leonidov A
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- Letts J
- Levchenko P
- Levchuk L
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- Libeiro T
- Ligabue F
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- Lingemann J
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- Lista L
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- Lobelle Pardo P
- Locci E
- Lohmann W
- Lomidze D
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- Long OR
- Longo E
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- Lopez EL
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- Magana Villalba R
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- McCliment E
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- Melo A
- Melzer-Pellmann I-A
- Menasce D
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- Meneguzzo AT
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- Militaru O
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- Mohanty AK
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- Newbold DM
- Newman HB
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- Newsom CR
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- Nikitenko A
- Nirunpong K
- Nishu N
- Nogima H
- Noonan D
- Norbeck E
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- Novaes SF
- Nowack A
- Nowak F
- Ntomari E
- Nuernberg A
- Nuttens C
- Nuzzo S
- O'Brien C
- O'Dell V
- Oberst O
- Obertino MM
- Obraztsov S
- Ocalan K
- Ochando C
- Ochesanu S
- Odell N
- Odorici F
- Oehler A
- Ofierzynski RA
- Oguri V
- Ojalvo I
- Olaiya E
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- Organtini G
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- Ostapchuk A
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- Ozkorucuklu S
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- Panagiotou A
- Pandolfi F
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- Panwalkar S
- Paoletti S
- Paolucci P
- Papacz P
- Papadopoulos I
- Papageorgiou A
- Pape L
- Paramatti R
- Paramesvaran S
- Parashar N
- Parida B
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- Parracho PGF
- Pashenkov A
- Passaseo M
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- Pastrone N
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- Peltola T
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- Perelygin V
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- Perez JAC
- Perfilov M
- Perieanu A
- Perloff A
- Pernicka M
- Perries S
- Perrotta A
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- Pesaresi M
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- Petrakou E
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- Petrukhin A
- Petrushanko S
- Petyt D
- Pfeiffer A
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- Pieri M
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- Pierro GA
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- Pimiae M
- Pin A
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- Piotrzkowski K
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- Piroue P
- Pitzl D
- Pivarski J
- Plager C
- Plestina R
- Pol ME
- Polatoz A
- Polese G
- Polic D
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popov V
- Pordes R
- Potenza A
- Potenza R
- Pozdnyakov A
- Pozzobon N
- Prado Da Silva WL
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puigh D
- Puljak I
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Rabbertz K
- Racz A
- Radburn-Smith BC
- Radi A
- Ragazzi S
- Rahatlou S
- Rahbaran B
- Rahmat R
- Raics P
- Raidal M
- Rakness G
- Ralph D
- Rander J
- Ranieri R
- Ranjan K
- Rappoccio S
- Raspereza A
- Ratnikov F
- Ratnikova N
- Ratti SP
- Raupach F
- Raval A
- Raymond DM
- Razis PA
- Rebane L
- Rebassoo F
- Redaelli N
- Redjimi R
- Redondo I
- Reece W
- Reid ID
- Reithler H
- Rekovic V
- Remington R
- Renker D
- Rennefeld J
- Renz M
- Reucroft S
- Reyes-Santos MA
- Ribeiro PQ
- Ribnik J
- Riccardi C
- Richards A
- Richman J
- Rikova MI
- Rinkevicius A
- Rios AAO
- Rizzi A
- Ro SR
- Roberts J
- Robles J
- Robmann P
- Rodenburg M
- Rodozov M
- Rodrigo T
- Rodriguez JL
- Rodriguez-Marrero AY
- Roe J
- Roecker S
- Rogan C
- Rogerson S
- Roh Y
- Rohe T
- Rohlf J
- Rohringer C
- Rohringer H
- Roland B
- Roland C
- Roland G
- Rolandi G
- Romano F
- Romanowska-Rybinska K
- Romeo F
- Romero A
- Romero L
- Rommerskirchen T
- Rompotis N
- Ronchese P
- Ronga FJ
- Rose A
- Rose K
- Rosin M
- Rosowsky A
- Ross I
- Rossato K
- Rossi AM
- Rossin R
- Rossini M
- Rougny R
- Rovelli C
- Rovelli T
- Rovere M
- Ruchti R
- Rudolph M
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Rusakov SV
- Ruspa M
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- Sabes D
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- Saha A
- Saini LK
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- Sakharov A
- Sakulin H
- Sakuma T
- Sakumoto W
- Sala L
- Sala S
- Salazar Ibarguen HA
- Salerno R
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- Salvati E
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- Sanchez-Hernandez A
- Sander C
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- Sanders S
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- Santanastasio F
- Santaolalla J
- Santocchia A
- Santoro A
- Saoulidou N
- Saout C
- Sarkar S
- Sarycheva L
- Sasseville M
- Sauerland P
- Savin A
- Savrin V
- Sawley M-C
- Scarborough T
- Schaefer C
- Schael S
- Schettler H
- Scheurer A
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- Schleper P
- Schlieckau E
- Schmanau M
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- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoefbeck R
- Schoerner-Sadenius T
- Schott G
- Schroeder M
- Schul N
- Schum T
- Schwarz T
- Schwick C
- Scodellaro L
- Scurlock B
- Searle M
- Seez C
- Segala M
- Segoni I
- Seitz C
- Seixas J
- Sekmen S
- Sellers P
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- Semenov S
- Sen N
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- Sengupta S
- Senkin S
- Seo E
- Seo H
- Serban AT
- Serin M
- Sever R
- Sexton-Kennedy E
- Sfiligoi I
- Sguazzoni G
- Shah MA
- Sharma A
- Sharma A
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- Sharma V
- Sharma V
- Sharp P
- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shipkowski SP
- Shipsey I
- Shiu JG
- Shivpuri RK
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- Sierra RV
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- Sikler F
- Silkworth C
- Sill A
- Sillou D
- Silva Do Amaral SM
- Silva P
- Silvers D
- Silverwood H
- Silvestre C
- Silvestris L
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- Simon M
- Simon S
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- Simonis HJ
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- Singh G
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- Singovsky A
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- Sirois Y
- Siroli G
- Sirunyan AM
- Skhirtladze N
- Skuja A
- Slaunwhite J
- Smirnov I
- Smith J
- Smith JG
- Smith K
- Smith VJ
- Smith WH
- Smolin D
- Snigirev A
- Snoek H
- Snook B
- Snow GR
- Snowball M
- Soares Jorge L
- Soares MS
- Sobol A
- Sobron Sanudo M
- Soffi L
- Sogut K
- Sola V
- Solano A
- Somalwar S
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- Stephans GSF
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- Stieger B
- Stiliaris E
- Stober FM
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- Stoye M
- Stoykova S
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- Strauss J
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- Strom D
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- Suarez I
- Suarez RG
- Sudano E
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
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- Sumowidagdo S
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- Sung K
- Surat UE
- Svintradze I
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- Tatarinov A
- Taurok A
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- Tcholakov V
- Teischinger F
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- Teo WD
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- Teyssier D
- Thea A
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- Thomsen J
- Thyssen F
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- Tiras E
- Titov M
- Tkaczyk S
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- Tomalin IR
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- Tonelli G
- Tonjes MB
- Tonwar SC
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- Topaksu AK
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- Toropin A
- Torre P
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- Traczyk P
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- Trayanov R
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- Triantis FA
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- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropiano A
- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
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- Tully C
- Tumasyan A
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- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
- Valdata M
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- Valuev V
- Van Doninck W
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- Van Mulders P
- Van Onsem GP
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- Vaughan J
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- Vazquez Valencia F
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- Veeraraghavan V
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- Velicanu D
- Velkovska J
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- Verdini PG
- Veres GI
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- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vichoudis P
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
- Vishnevskiy D
- Vitulo P
- Viviani C
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner P
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Walzel G
- Wan Z
- Wang D
- Wang J
- Wang J
- Wang M
- Wang S
- Wang X
- Wang Z
- Wardle N
- Wardrope D
- Wasserbaech S
- Wayne M
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- Weber HA
- Weber M
- Weber M
- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- 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
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- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
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- 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
arXiv:1206.4071v2.-- Chatrchyan, S. et al.The performance of muon reconstruction, identification, and triggering in CMS has been studied using 40 pb -1 of data collected in pp collisions at 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/c is above 95% over the whole region of pseudorapidity covered by the CMS muon system, < 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 GeVc is higher than 90% over the full η 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 100GeV/c and, using cosmic rays, it is shown to be better than 10% in the central region up to pT = 1 TeV/c. Observed distributions of all quantities are well reproduced by the Monte Carlo simulation.This work was supported by the Austrian Federal Ministry of Science and Research; the Belgium Fonds de la Recherche Scientifique, and Fonds voor Wetenschappelijk Onderzoek; the Brazilian Funding Agencies (CNPq, CAPES, FAPERJ, and FAPESP); the Bulgarian Ministry of Education and Science; CERN; the Chinese Academy of Sciences, Ministry of Science and Technology, and National Natural Science Foundation of China; the Colombian Funding Agency (COLCIENCIAS); the Croatian Ministry of Science, Education and Sport; the Research Promotion Foundation Cyprus; the Estonian Academy of Sciences and NICPB; the Academy of Finland, Finnish Ministry of Education and Culture, and Helsinki Institute of Physics; the Institut National de Physique Nucléaire et de Physique des Particules / CNRS, and Commissariat á l'Energie Atomique et aux Energies Alternatives/CEA, France; the Bundesministerium für Bildung und Forschung, Deutsche Forschungsgemeinschaft, and Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany; the General Secretariat for Research and Technology, Greece; the National Scientific Research Foundation, and National Office for Research and Technology, Hungary; the Department of Atomic Energy and the Department of Science and Technology, India; the Institute for Studies in Theoretical Physics and Mathematics, Iran; the Science Foundation, Ireland; the Istituto Nazionale di Fisica Nucleare, Italy; the Korean Ministry of Education, Science and Technology and the World Class University program of NRF, Korea; the Lithuanian Academy of Sciences; the Mexican Funding Agencies (CINVESTAV, CONACYT, SEP, and UASLP-FAI); the Ministry of Science and Innovation, New Zealand; the Pakistan Atomic Energy Commission; the State Commission for Sci- entific Research, Poland; the Fundaçao para a Ciência e a Tecnologia, Portugal; JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); the Ministry of Science and Technologies of the Russian Federation, the Russian Ministry of Atomic Energy and the Russian Foundation for Basic Research; the Ministry of Science and Technological Development of Serbia; the Ministerio de Ciencia e Innovación, and Programa Consolider-Ingenio 2010, Spain; the Swiss Funding Agencies (ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, and SER); the National Science Council, Taipei; the Scientific and Technical Research Council of Turkey, and Turkish Atomic Energy Authority; the Science and Technology Facilities Council, U.K.; the US Department of Energy, and the US National Science Foundation. Individuals have received support from the Marie-Curie programme and the European Research Council (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l'Industrie et dans l'Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); and the Council of Science and Industrial Research, India.Peer Reviewe
Study of double parton scattering using W+2-jet events in proton-proton collisions at √s=7 TeV
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- Krasnikov N
- Kravchenko I
- Kreczko L
- Kreis B
- Kress M
- Kress T
- Kreuzer P
- Kroeger R
- Krofcheck D
- Krolikowski J
- Kropivnitskaya A
- Kruecker D
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- Kubik A
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- Newman HB
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- Nishu N
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- Novaes SF
- Novgorodova O
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- Planer M
- Plestina R
- Pol ME
- Polatoz A
- Polese G
- Polic D
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popov A
- Popov V
- Potenza A
- Potenza R
- Pozdnyakov A
- Pozzobon N
- Prado Da Silva WL
- Primavera F
- Prokofyev O
- Proskuryakov A
- Prosper H
- Psallidas A
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puigh D
- Puljak I
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- Rappoccio S
- Raspereza A
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- Razis PA
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- Redaelli N
- Redjimi R
- Redondo I
- Reece W
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- Reithler H
- Rekovic V
- Renker D
- Reucroft S
- Riccardi C
- Ricci-Tam F
- Richman J
- Riedl C
- Rinkevicius A
- Rizzi A
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- Robles J
- Robmann P
- Robutti E
- Rodenburg M
- Rodozov M
- Rodrigo T
- Rodrigues Antunes J
- Rodriguez JL
- Rodriguez-Marrero AY
- Roe J
- Roecker S
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- Roland B
- Roland C
- Roland G
- Rolandi G
- Romanowska-Rybinska K
- Romeo F
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- Ronga FJ
- Rose A
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- Rosowsky A
- Ross I
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- Rumerio P
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- Rusakov SV
- Ruspa M
- Russ J
- Rutherford B
- Ryckbosch D
- Ryd A
- Ryu G
- Ryutin R
- Sabes D
- Sacchi R
- Safarzadeh B
- Safonov A
- Safronov G
- Saha A
- Sahin MO
- Saini LK
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- Sakharov A
- Sakulin H
- Sakuma T
- Salazar Ibarguen HA
- Salerno R
- Salfeld-Nebgen J
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- Salvati E
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- Sarangi T
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- Saxena P
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- Schaefer C
- Schael S
- Schettler H
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- Schizzi A
- Schlein P
- Schleper P
- Schlieckau E
- Schmidt A
- Schmidt R
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoefbeck R
- Schoerner-Sadenius T
- Schott G
- Schroeder M
- Schwick C
- Scodellaro L
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- Segala M
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- Sekaric J
- Sekmen S
- Selvaggi G
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- Seo H
- Serban AT
- Serin M
- Seva T
- Sever R
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- Sgandurra L
- Sgaravatto M
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- Shah MA
- Shalhout S
- Sharan M
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- Shipsey I
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- Shoaib M
- Shrestha S
- Shrinivas A
- Shukla P
- Shumeiko N
- Sibille J
- Siegrist P
- Sigamani M
- Sikler F
- Silkworth C
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- Silvers D
- Silverwood H
- Silvestris L
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh AP
- Singh G
- Singh JB
- Singovsky A
- Sinthuprasith T
- Sirois Y
- Siroli GP
- Sirunyan AM
- Skatchkov N
- Skhirtladze N
- Skuja A
- Slaunwhite J
- Smirnov I
- Smirnov V
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- Smith JG
- Smith VJ
- Smith WH
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- Snoek H
- Snook B
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- Spiridonov A
- Spiropulu M
- Sprenger D
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- Staiano A
- Starodumov A
- Steggemann J
- Stein M
- Steinbrueck G
- Stenson K
- Stephans GSF
- Stickland D
- Stieger B
- Stiliaris E
- Stober FM
- Stoeckli F
- Stolin V
- Stone R
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- Strauss J
- Stringer R
- Strobbe N
- Strom D
- Stuart D
- Sturdy J
- Suarez Gonzalez J
- Suarez I
- Suarez RG
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- Sulak L
- Sulimov V
- Sultanov G
- Summers D
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- Suwonjandee N
- Svintradze I
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- Tadel M
- Takahashi M
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- Tapper A
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- Tatarinov A
- Taurok A
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- Teo WD
- Teodorescu L
- Teyssier D
- Thea A
- Theofilatos K
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- Thomassen P
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- Thueer S
- Thyssen F
- Tiko A
- Tikvica L
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- Tiras E
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- Tkaczyk S
- Tlisov D
- To W
- Toback D
- Tomalin IR
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- Topsis-giotis I
- Torassa E
- Toropin A
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- Traczyk P
- Tran NV
- Travaglini R
- Treberer-Treberspurg W
- Treille D
- Trevino ADRV
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Tropiano A
- Troshin S
- Tsamalaidze Z
- Tsirou A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Turkewitz J
- Turner M
- Turner P
- Tuuva T
- Tuve C
- Tytgat M
- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ulrich R
- Umer T
- Uplegger L
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Valls N
- Valuev V
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- Van Mulders P
- Van Onsem GP
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- Veeraraghavan V
- Velasco M
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- Velkovska J
- Venditti R
- Venturi A
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- Verdini PG
- Veres GI
- Vergili M
- Vernieri C
- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal Marono M
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Vilela Pereira A
- Villalba RM
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
- Vishnevskiy D
- Vitulo P
- Vlasov E
- Vlimant JR
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
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- Vuosalo C
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- Wayand S
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- Weber HA
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- Weiler T
- Weinberg M
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- Weng Y
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Wickramage N
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- Wilkinson R
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- Wolszczak W
- Womersley WJ
- Won S
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- Woodard A
- Worm SD
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- Wuerthwein F
- Wulsin HW
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
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- Yu I
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
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- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti A
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- Zeyrek M
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- Zhang L
- Zheng Y
- Zhokin A
- Zhu RY
- Zhukov V
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- Zou W
- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- Publication date
- 01/01/2013
- Field of study
Peer reviewe
- …