127 research outputs found
Beta cell function following 1 year vildagliptin or placebo treatment and after 12 week washout in drug-naive patients with type 2 diabetes and mild hyperglycaemia: a randomised controlled trial
- Author
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2011
- Field of study
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
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- Villella I
- Vinogradov A
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- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Walker M
- Wallny R
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- Waltenberger W
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- Wang F
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- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
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- Wolfe H
- Wolszczak W
- Womersley WJ
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- Wood JS
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- Wulz C-E
- Wyslouch B
- Xiao H
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- Yang F
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- 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
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
A systematic review, meta-analysis, and meta-regression of the impact of diurnal intermittent fasting during Ramadan on body weight in healthy subjects aged 16 years and above
- Author
- A Adlouni
- A Afrasiabi
- A Agoumi
- A Akanji
- A BaHammam
- A Barkia
- A Celik
- A Chaix
- A Chaix
- A Di Francesco
- A Fahrial Syam
- A Hruby
- A Norouzy
- A Norouzy
- A SaA
- A Shehab
- A Yucel
- AH Jarrar
- AH Sakr
- AR Rahbar
- AS Almeneessier
- AS BaHammam
- AS Roy
- B Bakki
- B Isomaa
- B Nugraha
- B Sadeghirad
- C-J Huang
- CA Rynders
- Cain C. T. Clark
- CS Davis
- D Altman
- DF Stroup
- E Yeoh
- F Azizi
- F Azizi
- F Haouari-Oukerro
- F Mohammadzade
- FB Aksungar
- FM Akrami
- G Farshidfar
- G Prasetya
- GM Finch
- GR Hajer
- H Al-Hourani
- H Alemán-Mateo
- H Chen
- H Fakhrzadeh
- H Fernando
- Haitham A. Jahrami
- HM Al Hourani
- HR Takruri
- I Alam
- I Latiri
- I Suriani
- I Suriani
- J El Ati
- J McNeil
- J Obert
- J Ramadan
- JD Gotthardt
- JF Trepanowski
- JF Trepanowski
- JF Trepanowski
- JJ Deeks
- Joud Alsibai
- JP Higgins
- JP Higgins
- JP Higgins
- JR Alkandari
- JV Gnanou
- K Gabel
- K Sayedda
- K Shirai
- K Trabelsi
- K Varady
- KMS Mansi
- L Dewanti
- L Malekmakan
- M Adawi
- M Alinezhad-Namaghi
- M Assadi
- M Borenstein
- M Cansel
- M Faris
- M Faris
- M Faris
- M Faris
- M Faris
- M Faris
- M Harvie
- M Hatori
- M Headland
- M Lamri-Senhadji
- M López-Bueno
- M Maislos
- M Mazidi
- M Pallayova
- M Pathan
- M Rahman
- M Salahuddin
- M Salehi
- M Tremmel
- M Ünalacak
- MA Alzoghaibi
- MAK Rohin
- MB Hassan
- MC Vardarli
- MI Madkour
- MM Kiyani
- MM Mahmood
- MM Subhan
- MMA Khan Khattak
- MN Harvie
- Mo’ez Al-Islam E. Faris
- MSA Sijavand
- MV Shariatpanahi
- N Al-Numair
- N Ganjali
- N Khan
- N Lessan
- N Lessan
- N Radhakishun
- N Sweileh
- NG AbdulKareem
- NM Harder-Lauridsen
- NS Al-barha
- ON Develioglu
- P Pérez-Martínez
- R Antoni
- R Freire
- R Mushtaq
- RA Talib
- RE Patterson
- RE Patterson
- RV Seimon
- S Abedelmalek
- S Duval
- S Feizollahzadeh
- S Haghighi
- S Ismail
- S Ismail
- S Ismail
- S Kassab
- S Kassab
- S Kul
- S Moosavi
- S Ongsara
- S Racinais
- SA Meo
- SM Abd El-Kader
- SM Nachvak
- SR Stannard
- SRA Hosseini
- SRA Hosseini
- SRA Hosseini
- SS Fedail
- T Moro
- T Sundfør
- TA Begum
- V Ziaee
- WH Ibrahim
- WH Ibrahim
- YY Bilto
- ZV Shariatpanahi
- Ö Kayikçioğlu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2020
- Field of study
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
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
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- Publication venue
- Publication date
- 01/01/2014
- Field of study
Peer reviewe
Study of double parton scattering using W+2-jet events in proton-proton 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
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
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- Albayrak EA
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- Alcaraz Maestre J
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- 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
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- Andreev V
- Andreev Y
- Andrews W
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- Antonelli L
- Antunovic Z
- Apanasevich L
- Apollinari G
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- Arfaei H
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- Auzinger G
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- Azzolini V
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- Baarmand MM
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
Peer reviewe
Measurement of Higgs boson production and properties in the WW decay channel with leptonic final states
- 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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- Publication venue
- Publication date
- 01/12/2013
- 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
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- Publication venue
- Publication date
- 01/01/2014
- Field of study
Peer reviewe
Measurement of the production cross section ratio σ(χb2(1P))/σ(χb1(1P))in pp collisions at √s=8TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram J-L
- Ahmad A
- Ahmad M
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- Albayrak EA
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- Alcaraz Maestre J
- Aldaya Martin M
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- Mossolov V
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- Muniz L
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- Murumaa M
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- Novgorodova O
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- Olaiya E
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- Pitzl D
- Placakyte R
- Plagge M
- Planer M
- Plestina R
- Poehlsen J
- Poehlsen T
- 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
- Prosper H
- Psallidas A
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puigh D
- Puljak I
- Python Q
- Pérez-Calero Yzquierdo A
- Qian SJ
- Quan X
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- Quintario Olmeda A
- Quittnat M
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- Racz A
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- Ramirez Vargas JE
- Rander J
- Ranjan K
- Rappoccio S
- Raspereza A
- Rathjens D
- Ratnikov F
- Ratti SP
- Raupach F
- Raymond DM
- Razis PA
- Rebane L
- Rebassoo F
- Redaelli N
- Redjimi R
- Redondo I
- Regnard S
- Reid ID
- Reis T
- Reithler H
- Rekovic V
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- Rezaei Hosseinabadi F
- Ribeiro Cipriano PM
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- Richman J
- Rinkevicius A
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- Rodozov M
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- Rodríguez-Marrero AY
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- Rosowsky A
- Ross I
- Rossi AM
- Rossini M
- Rougny R
- Rovelli C
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- Ruiz Alvarez JD
- Ruiz-Jimeno A
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- Santoro A
- Saoulidou N
- Sarangi T
- Sarkar S
- Sauvan JB
- Savin A
- Savoy-Navarro A
- Savrin V
- Saxena P
- Scarborough T
- Schael S
- Schettler H
- Schizzi A
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- Schröder M
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- Seidel M
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- Sharma V
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- Shchutska L
- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shipsey I
- Shmatov S
- Shoaib M
- Shrestha S
- Shrinivas A
- Shukla P
- Shumeiko N
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- Sigamani M
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- Sinthuprasith T
- Sirois Y
- Siroli GP
- Sirunyan AM
- Skatchkov N
- Skhirtladze N
- Skinnari L
- Skuja A
- Smirnov I
- Smirnov V
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- Spiridonov A
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- Starodumov A
- Steggemann J
- Steinbrück G
- Stenson K
- Stephans GSF
- Stickland D
- Stieger B
- Stiliaris E
- Stober FM
- Stolin V
- Stolp D
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- Stoye M
- Stoykova S
- Stoynev S
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- Sultanov G
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- Sumowidagdo S
- Sun W
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- Sung K
- Surat UE
- Suwonjandee N
- Svintradze I
- Svyatkovskiy A
- Swain SK
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- Tabarelli de Fatis T
- Tadel M
- Takahashi M
- Takasugi E
- Tali B
- Tambe N
- Tamponi U
- Tan P
- Tao J
- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tavernier S
- Taylor L
- Tcholakov V
- Tenchini R
- Teo WD
- Teodorescu L
- Teyssier D
- Thea A
- Theofilatos K
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- Tiras E
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- Tomalin IR
- Tonelli Manganote EJ
- Tonelli G
- Tonjes MB
- Tonwar SC
- Topakli H
- Topkar A
- Topsis-Giotis I
- Toropin A
- Tosi M
- Tosi N
- Tosi S
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- Traczyk P
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- Trocino D
- Trocsanyi ZL
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- 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
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- Tuuva T
- Tuve C
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- Tzeng YM
- Ujvari B
- Ulmer KA
- Ulrich R
- Umer T
- Uplegger L
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Valls N
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- Vargas Trevino ADR
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- Vazquez Valencia F
- Veelken C
- Veeraraghavan V
- Velasco M
- Velicanu D
- Velkovska J
- Venditti R
- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili M
- Vernieri C
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- Vesztergombi G
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- Vidal Marono M
- Vidal R
- Vila I
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- Vilela Pereira A
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
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- Vitulo P
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- Vlasov E
- Vlimant JR
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner SR
- Wagner-Kuhr J
- Walker M
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- Wang X
- Wang Z
- Wardle N
- Wayand S
- Wayne M
- Weber H
- Weber HA
- Weber M
- Weber M
- Weiler T
- Weinberg M
- Welke C
- Wendland L
- Weng Y
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Wickramage N
- Wilbur S
- Wilken R
- Wilkinson R
- Williams T
- Wimpenny S
- Winer BL
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Wolf M
- Wolf R
- Wolfe H
- Wollny H
- Wolszczak W
- Womersley WJ
- Won S
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- Wood JS
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- Worm SD
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- Wyslouch B
- Wöhri HK
- Würthwein F
- Xiao H
- Xie S
- Xie W
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- Yagil A
- Yalvac M
- Yang F
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- York A
- Yu I
- Yu SS
- Yuldashev BS
- Yumiceva F
- Yücel M
- Zabel J
- Zabi A
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- Zakaria M
- Zalewski P
- Zanetti A
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- Zarubin A
- Zeinali M
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zheng Y
- Zhokin A
- Zhu RY
- Zhukov V
- Zhukova V
- Zito G
- Zotto P
- Zou W
- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- Elsevier
- Publication date
- 01/01/2014
- Field of study
A measurement of the production cross section ratio σ(χb2(1P))/σ(χb1(1P))σ(χb2(1P))/σ(χb1(1P)) is presented. The χb1(1P)χb1(1P) and χb2(1P)χb2(1P) bottomonium states, promptly produced in pp collisions at View the MathML sources=8 TeV, are detected by the CMS experiment at the CERN LHC through their radiative decays χb1,2(1P)→ϒ(1S)+γχb1,2(1P)→ϒ(1S)+γ. The emitted photons are measured through their conversion to e+e−e+e− pairs, whose reconstruction allows the two states to be resolved. The ϒ(1S)ϒ(1S) is measured through its decay to two muons. An event sample corresponding to an integrated luminosity of 20.7 fb−120.7 fb−1 is used to measure the cross section ratio in a phase-space region defined by the photon pseudorapidity, |ηγ|<1.0|ηγ|<1.0; the ϒ(1S)ϒ(1S) rapidity, |yϒ|<1.5|yϒ|<1.5; and the ϒ(1S)ϒ(1S) transverse momentum, View the MathML source7<pTϒ<40 GeV. The cross section ratio shows no significant dependence on the ϒ(1S)ϒ(1S) transverse momentum, with a measured average value of View the MathML source0.85±0.07(stat+syst)±0.08(BF), where the first uncertainty is the combination of the experimental statistical and systematic uncertainties and the second is from the uncertainty in the ratio of the χbχb branching fractions
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
- Abbrescia M
- Abdullin S
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- Zheng Y
- Zhokin A
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- Zhukov V
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- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- 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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- Abbiendi G
- Abbrescia M
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- Abdullin S
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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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