166 research outputs found
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Alderweireldt S
- Alexander J
- Aliev T
- Alimena J
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- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
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- Askew A
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- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baeni L
- Baffioni S
- Bagliesi G
- Bahtiyar H
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
- Ban Y
- Banerjee S
- Banerjee S
- Bansal M
- Bansal S
- Barbagli G
- Barberis E
- Barbone L
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
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- Barney D
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- Basegmez S
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- Battilana C
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- Bazterra VE
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- Beaudette F
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- Beernaert K
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- Behrenhoff W
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- Bialkowska H
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- Bianchi G
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- Bitioukov S
- Blekman F
- Blobel V
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- Carlsmith D
- Carrillo Montoya CA
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- Cepeda M
- Cerati GB
- Cerci DS
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- Cerminara G
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- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan KM
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- Chang P
- Chang S
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Chaparro Sierra LF
- Charaf O
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- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
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- Checchia P
- Chen GM
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- Chertok M
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- Cheung HWK
- Chhibra SS
- Chierici R
- Chinellato J
- Chiochia V
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- Chlebana F
- Choi M
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- Choi Y
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- Chou JP
- Choudhary BC
- Choudhury S
- Christiansen T
- Christopher G
- Chuang SH
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
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- Cline D
- CMS Collaboration
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- Cutajar M
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- d'Enterria D
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- de Monchenault GH
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- Fasanella D
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- Favaro C
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- Fedi G
- Fehling D
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- Zheng Y
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- 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
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 the Positive Muon Anomalous Magnetic Moment to 0.20 ppm
- Author
- Aguillard DP
- Albahri T
- Allspach D
- Anisenkov A
- Badgley K
- Baeßler S
- Bailey I
- Bailey L
- Baranov VA
- Barlas-Yucel E
- Barrett T
- Barzi E
- Bedeschi F
- Berz M
- Bhattacharya M
- Binney HP
- Bloom P
- Bono J
- Bottalico E
- Bowcock T
- Braun S
- Bressler M
- Cantatore G
- Carey RM
- Casey BCK
- Cauz D
- Chakraborty R
- Chapelain A
- Chappa S
- Charity S
- Chen C
- Cheng M
- Chislett R
- Chu Z
- Chupp TE
- Claessens C
- Convery ME
- Corrodi S
- Cotrozzi L
- Crnkovic JD
- Dabagov S
- Debevec PT
- Di Falco S
- Di Sciascio G
- Drendel B
- Driutti A
- Duginov VN
- Eads M
- Edmonds A
- Esquivel J
- Farooq M
- Fatemi R
- Ferrari C
- Fertl M
- Fienberg AT
- Fioretti A
- Flay D
- Foster SB
- Friedsam H
- Froemming NS
- Gabbanini C
- Gaines I
- Galati MD
- Ganguly S
- Garcia A
- George J
- Gibbons LK
- Gioiosa A
- Giovanetti KL
- Girotti P
- Gohn W
- Goodenough L
- Gorringe T
- Grange J
- Grant S
- Gray F
- Haciomeroglu S
- Halewood-Leagas T
- Hampai D
- Han F
- Hempstead J
- Hertzog DW
- Hesketh G
- Hess E
- Hibbert A
- Hodge Z
- Hong KW
- Hong R
- Hu T
- Hu Y
- Iacovacci M
- Incagli M
- Kammel P
- Kargiantoulakis M
- Karuza M
- Kaspar J
- Kawall D
- Kelton L
- Keshavarzi A
- Kessler DS
- Khaw KS
- Khechadoorian Z
- Khomutov NV
- Kiburg B
- Kiburg M
- Kim O
- Kinnaird N
- Kraegeloh E
- Krylov VA
- Kuchinskiy NA
- Labe KR
- LaBounty J
- Lancaster M
- Lee S
- Li B
- Li D
- Li L
- Logashenko I
- Lorente Campos A
- Lu Z
- Lucà A
- Lukicov G
- Lusiani A
- Lyon AL
- MacCoy B
- Madrak R
- Makino K
- Mastroianni S
- Miller JP
- Miozzi S
- Mitra B
- Morgan JP
- Morse WM
- Mott J
- Nath A
- Ng JK
- Nguyen H
- Oksuzian Y
- Omarov Z
- Osofsky R
- Park S
- Pauletta G
- Piacentino GM
- Pilato RN
- Pitts KT
- Plaster B
- Pohlman N
- Polly CC
- Počanić D
- Price J
- Quinn B
- Qureshi MUH
- Ramachandran S
- Ramberg E
- Reimann R
- Roberts BL
- Rubin DL
- Santi L
- Schlesier C
- Schreckenberger A
- Semertzidis YK
- Shemyakin D
- Sorbara M
- Stapleton J
- Still D
- Stoughton C
- Stratakis D
- Stöckinger D
- Swanson HE
- Sweetmore G
- Sweigart DA
- Syphers MJ
- Tarazona DA
- Teubner T
- Tewsley-Booth AE
- Tishchenko V
- Tran NH
- Turner W
- Valetov E
- Vasilkova D
- Venanzoni G
- Volnykh VP
- Walton T
- Weisskopf A
- Welty-Rieger L
- Winter P
- Wu Y
- Yu B
- Yucel M
- Zeng Y
- Zhang C
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2023
- Field of study
We present a new measurement of the positive muon magnetic anomaly, a_{μ}≡(g_{μ}-2)/2, from the Fermilab Muon g-2 Experiment using data collected in 2019 and 2020. We have analyzed more than 4 times the number of positrons from muon decay than in our previous result from 2018 data. The systematic error is reduced by more than a factor of 2 due to better running conditions, a more stable beam, and improved knowledge of the magnetic field weighted by the muon distribution, ω[over ˜]_{p}^{'}, and of the anomalous precession frequency corrected for beam dynamics effects, ω_{a}. From the ratio ω_{a}/ω[over ˜]_{p}^{'}, together with precisely determined external parameters, we determine a_{μ}=116 592 057(25)×10^{-11} (0.21 ppm). Combining this result with our previous result from the 2018 data, we obtain a_{μ}(FNAL)=116 592 055(24)×10^{-11} (0.20 ppm). The new experimental world average is a_{μ}(exp)=116 592 059(22)×10^{-11} (0.19 ppm), which represents a factor of 2 improvement in precision
The neurobiological link between OCD and ADHD
- Author
- A Abramovitch
- A Abramovitch
- A Aycicegi
- A Bari
- A Bruno
- A Buot
- A Costa
- A Dimoska
- A Ghaleiha
- A Heils
- A Olley
- A Reiner
- AC Wood
- AH Zohar
- AJ Fallgatter
- AJ Fallgatter
- AJ Fallgatter
- AJ Geburek
- AM Boonstra
- American Psychiatric Association
- AR Crossman
- B Albrecht
- B Albrecht
- B Albrecht
- B Aouizerate
- B Camarena
- B Franke
- B Franke
- B Harkin
- B Hoza
- B Kopp
- B Porton
- B Sheppard
- BE Yerys
- BL Goldman
- BM Gu
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- C Benkelfat
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- D Behar
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Study of double parton scattering using W+2-jet events in proton-proton collisions at √s=7 TeV
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- Zsigmond AJ
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
Peer reviewe
Search for new physics in the multijet and missing transverse momentum final state in proton-proton collisions at √s=8 Tev
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam W
- Adams MR
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- Adzic P
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- Publication venue
- Publication date
- 01/01/2014
- Field of study
Peer reviewe
Measurements of the tt¯ charge asymmetry using the dilepton decay channel in pp collisions at √s=7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Alderweireldt S
- Alexander J
- Aliev T
- Alimena J
- Alvarez JDR
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Androsov K
- Antonelli L
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arneodo M
- Arora S
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asin I
- Askew A
- Aslanoglou X
- Assran Y
- Ata M
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
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- Publication venue
- Publication date
- 01/01/2014
- Field of study
Peer reviewe
Searches for new physics using the t(t)over-bar invariant mass distribution in pp collisions at √s=8 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
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- Alderweireldt S
- Alexander J
- Aliev T
- Alimena J
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- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Androsov K
- Antonelli L
- Antunovic Z
- Apanasevich L
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- Arenton MW
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- Asawatangtrakuldee C
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- Autermann C
- Auzinger G
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- Azzolini V
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- Baarmand MM
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- Bagliesi G
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- Bauer G
- Bauerdick LAT
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- Carlsmith D
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- Casasso S
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- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
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- 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
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- 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
- 'American Physical Society (APS)'
- Publication date
- 01/01/2013
- Field of study
This is the pre-print version of the final published paper that is available from the link belowSearches for anomalous top quark-antiquark production are presented, based on pp collisions at √s=8 TeV . The data, corresponding to an integrated luminosity of 19:7 fb^-1, were collected with the CMS detector at the LHC. The observed tt invariant mass spectrum is found to be compatible with the standard model prediction. Limits on the production cross section times branching fraction probe, for the first time, a region of parameter space for certain models of new physics not yet constrained by precision measurements
Measurement of associated production of vector bosons and top quark-antiquark pairs in pp collisions at √s=7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Civinini C
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- Coarasa Perez JA
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- Cussans D
- Custodio A
- Cutajar M
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- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Dabrowski A
- Daci N
- Dahmes B
- Dahms T
- Dalchenko M
- Dallavalle GM
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- Daubie E
- Dauncey P
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- de Cassagnac RG
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- Yilmaz Y
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- Zhang Z
- Zheng Y
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- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
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- Zou W
- Zsigmond AJ
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2013
- Field of study
PubMed ID: 23679709The first measurement of vector-boson production associated with a top quark-antiquark pair in proton-proton collisions at s √ =7 TeV is presented. The results are based on a data set corresponding to an integrated luminosity of 5.0 fb^−1 , recorded by the CMS detector at the LHC in 2011. The measurement is performed in two independent channels through a trilepton analysis of tt ¯ Z events and a same-sign dilepton analysis of tt ¯ V (V=W or Z ) events. In the trilepton channel a direct measurement of the tt ¯ Z cross section σ tt ¯ Z =0.28 [+0.14 −0.11] (stat) [+0.06 −0.03] (syst) pb is obtained. In the dilepton channel a measurement of the tt ¯ V cross section yields σtt¯V=0.43 [+0.17 −0.15] (stat) [+0.09 −0.07] (syst) pb . These measurements have a significance, respectively, of 3.3 and 3.0 standard deviations from the background hypotheses and are compatible, within uncertainties, with the corresponding next-to-leading order predictions of 0.137[+0.012 −0.016] and 0.306 [+0.031 −0.053] pb
Measurement of the production cross section for Z gamma -> nu(nu)over-bar gamma in pp collisions at √s=7 TeV and limits on ZZ gamma and Z gamma gamma triple gauge boson couplings
- Author
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- Abbiendi G
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
This article is the pre-print version of the final published paper that is available from the link below.A measurement of the Z → vvγ cross section in pp collisions at root s = 7TeV is presented, using data corresponding to an integrated luminosity of 5.0 fb-1 collected with the CMS detector. This measurement is based on the observation of events with an imbalance of transverse energy in excess of 130 GeV and a single photon in the absolute pseudorapidity range |n| < 1:4 with transverse energy above 145 GeV. The Z →vvγ production cross section is measured to be 21.1±4.2 (stat:)±4.3 (syst:)±0.5 (lum:) fb, which agrees with the standard model prediction of 21.9±1.1 fb. The results are combined with the CMS measurement of Z production in the l+l- γ final state (where l is an electron or a muon) to yield the most stringent limits to date on triple gauge boson couplings: |hZ3|< 2.7 x 10-3, |hZ4| < 1,3 x 10-5 for ZZγ and |hγ3| < 2.9 x10-3, |hγ4| < 1.5 x 10-5 for Zγγ couplings
Measurement of the differential and double-differential Drell-Yan cross sections in proton-proton collisions at root s=7 TeV
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
Copyright @ 2013 CERN,
for the bene t of the CMS collaboration. This article is distributed under the terms of the Creative Commons
Attribution License which permits any use, distribution and reproduction in any medium,
provided the original author(s) and source are credited.Measurements of the differential and double-differential Drell-Yan cross sections are presented using an integrated luminosity of 4.5 (4.8) fb−1 in the dimuon (dielectron) channel of proton-proton collision data recorded with the CMS detector at the LHC at s√ = 7 TeV. The measured inclusive cross section in the Z-peak region (60–120 GeV) is σ(ℓℓ) = 986.4 ± 0.6 (stat.) ± 5.9 (exp. syst.) ± 21.7 (th. syst.) ± 21.7 (lum.) pb for the combination of the dimuon and dielectron channels. Differential cross sections dσ/dm for the dimuon, dielectron, and combined channels are measured in the mass range 15 to 1500 GeV and corrected to the full phase space. Results are also presented for the measurement of the double-differential cross section d2σ/dm d|y| in the dimuon channel over the mass range 20 to 1500 GeV and absolute dimuon rapidity from 0 to 2.4. These measurements are compared to the predictions of perturbative QCD calculations at next-to-leading and next-to-next-to-leading orders using various sets of parton distribution functions.The Austrian
Federal Ministry of Science and Research and the Austrian Science Fund; the Belgian Fonds
de la Recherche Scienti que, 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 Ministry of Education and Research, Recurrent
nancing contract SF0690030s09 and European Regional Development Fund, Estonia; the
Academy of Finland, Finnish Ministry of Education and Culture, and Helsinki Institute of
Physics; the Institut National de Physique Nucl eaire et de Physique des Particules / CNRS,
and Commissariat a l' Energie Atomique et aux Energies Alternatives / CEA, France; the
Bundesministerium f ur Bildung und Forschung, Deutsche Forschungsgemeinschaft, and
Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany; the General Secretariat
for Research and Technology, Greece; the National Scienti c Research Foundation, and National Innovation O ce, 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, Republic of Korea; the Lithuanian Academy of Sciences;
the Mexican Funding Agencies (CINVESTAV, CONACYT, SEP, and UASLP-FAI);
the Ministry of Business, Innovation and Employment, New Zealand; the Pakistan Atomic
Energy Commission; the Ministry of Science and Higher Education and the National Science
Centre, Poland; the Funda c~ao para a Ci^encia e a Tecnologia, Portugal; JINR, Dubna;
the Ministry of Education and Science of the Russian Federation, the Federal Agency of
Atomic Energy of the Russian Federation, Russian Academy of Sciences, and the Russian
Foundation for Basic Research; the Ministry of Education, Science and Technological Development
of Serbia; the Secretar a de Estado de Investigaci on, Desarrollo e Innovaci on
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 Thailand Center of Excellence in Physics, the Institute for the Promotion of
Teaching Science and Technology of Thailand, Special Task Force for Activating Research
and the National Science and Technology Development Agency of Thailand; the Scienti c
and Technical Research Council of Turkey, and Turkish Atomic Energy Authority; the
Science and Technology Facilities Council, UK; the US Department of Energy, and the US
National Science Foundation
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