181 research outputs found
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
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- 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
- Alcaraz Maestre J
- Alda Junior WL
- Aldaya Martin M
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
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- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunovic Z
- Apanasevich L
- Appelt E
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- Arcidiacono R
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- Asghar MI
- Askew A
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- Attikis A
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- Avetisyan A
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- Azhgirey I
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- Bagliesi G
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- Barbagli G
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- Yildirim E
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
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- Zanetti M
- Zang J
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- Zeinali M
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- Zeyrek M
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- Zhang Z
- Zheng Y
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- Zhu B
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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
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
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- 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
- Alcaraz Maestre J
- Alda Junior WL
- Alexander J
- Aliev T
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- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
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- Andrea J
- Andreev V
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- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunovic Z
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- Appelt E
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
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- Asawatangtrakuldee C
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- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
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- Bacchetta N
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- Baden A
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- Baffioni S
- Bagliesi G
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- Bainbridge R
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- Bakirci MN
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- Bhatti A
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
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- Zabi A
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- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- 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
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
- Abbrescia M
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- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
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- Cortezon EP
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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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
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- 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
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- Cockerill DJA
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- Stober FM
- Stoeckli F
- Stolin V
- Stone R
- Stoye M
- Stoykova S
- Stoynev S
- Strauss J
- Stringer R
- Strobbe N
- Strom D
- Stuart D
- Sturdy J
- Suarez I
- Suarez RG
- Sudano E
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
- Sumorok K
- Sumowidagdo S
- Sun W
- Sung K
- Surat UE
- Svintradze I
- Svyatkovskiy A
- Swanson J
- Swartz M
- Symonds P
- Szillasi Z
- Szleper M
- Sznajder A
- Tadel M
- Takahashi M
- Tali B
- Tambe N
- Tan P
- Tao J
- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tauscher L
- Taylor L
- Tcholakov V
- Teischinger F
- Temple J
- Tenchini R
- Teng H
- Teo WD
- Teodorescu L
- Teyssier D
- Thea A
- Theofilatos K
- Thiebaux C
- Thom J
- Thomas L
- Thomas S
- Thompson J
- Thomsen J
- Thyssen F
- Tiko A
- Timciuc V
- Tinti G
- Tiras E
- Titov M
- Tkaczyk S
- To W
- Toback D
- Tomalin IR
- Tomaszewska J
- Tonelli G
- Tonjes MB
- Tonwar SC
- Topakli H
- Topaksu AK
- Torassa E
- Toropin A
- Torre P
- Tosi M
- Tosi S
- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Triantis FA
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropiano A
- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tupputi S
- Turkewitz J
- Turner M
- Tuuva T
- Tuve C
- Twedt E
- Tytgat M
- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
- Valdata M
- Valls N
- Valuev V
- Van Doninck W
- Van Haevermaet H
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
- Van Remortel N
- Van Spilbeeck A
- Vander Velde C
- Vanelderen L
- Vanini S
- Vanlaer P
- Varela J
- Varelas N
- Vargas JER
- Vartak A
- Vasil'ev S
- Vaughan J
- Vavilov S
- Vazquez Valencia F
- Veelken C
- Veeraraghavan V
- Velasco M
- Velicanu D
- Velkovska J
- Ventura S
- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili LN
- Vergili M
- 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
- Weber H
- 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
- 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
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
Constraints on models of the Higgs boson with exotic spin and parity using decays to bottom-antibottom quarks in the full CDF data set
- Author
- A. aa
- A. aa
- A. aa
- A. ab
- A. aqar
- A. ay
- A. az
- A. bc
- A. bc
- A. bdbebf
- A. bi
- A. bn
- A. c
- A. F. ax
- A. fg
- A. M. bd
- A. p
- A. T. ax
- Aaltonen
- Amerio
- Amidei
- Anastassov A. p
- Annovi A. r
- Antos
- Apollinari G. p
- Appel J. A. p
- Arisawa
- Artikov A. n
- Asaadi
- Ashmanskas W. p
- Auerbach B. b
- Aurisano
- Azfar
- B. L. aj
- B. p
- Badgett W. p
- Bae
- Barbaro Galtieri
- Barnes
- Barnett B. A. x
- Barria
- Bartos
- Bauce
- Bedeschi
- Behari S. p
- Bellettini
- Bellinger
- Benjamin D. o
- Beretvas A. p
- Bhatti
- Bland K. R. e
- Blumenfeld B. x
- Bocci A. o
- Bodek
- Bortoletto
- Boudreau
- Boveia A. l
- Brigliadori
- Bromberg
- Brucken
- Budagov J. n
- Budd
- Burkett K. p
- Busetto
- Bussey P. t
- Butti
- Buzatu A. t
- C. ae
- C. ag
- C. am
- C. aqar
- C. aqat
- C. az
- C. bd
- C. bj
- C. bl
- C. l
- Calamba A. k
- Camarda S. d
- Campanelli
- Canelli F. l
- Carls B. w
- Carlsmith
- Carosi
- Carrillo S. q
- Casal B. j
- Casarsa
- Castro
- Catastini P. u
- CAUZ Diego
- Cavaliere V. w
- Cerri
- Cerrito
- Chen Y. C. a
- Chertok M. h
- Chiarelli
- Chlachidze G. p
- Cho
- Chokheli D. n
- Clark A. s
- Clarke
- Convery M. E. p
- Conway J. h
- Corbo M. p
- Cordelli M. r
- Cox C. A. h
- Cox D. J. h
- Cremonesi
- Cruz
- Cuevas J. j
- Culbertson R. p
- D'Ascenzo N. p
- D'Errico
- D'Onofrio
- D. ac
- D. af
- D. af
- D. al
- D. anao
- D. ap
- D. ax
- D. bc
- D. bc
- D. bc
- D. bm
- D. H. zbqbrbsbtbubv
- D. J. zbqbrbsbtbubv
- Datta M. p
- De Barbaro
- Demortier
- Deninno M. f
- Devoto
- Di Canto
- Di Ruzza
- Dittmann J. R. e
- Donati
- Dorigo
- Driutti
- E. ap
- E. ap
- E. ap
- E. J. zbqbrbsbtbubv
- E. vbp
- Ebina
- Edgar
- Elagin
- Erbacher R. h
- Errede S. w
- Esham B. w
- F. am
- F. aq
- F. aq
- F. aqar
- F. aqas
- F. ba
- F. bh
- F. vbp
- Farrington
- Fernández Ramos
- Field R. q
- Flanagan G. p
- Forrest R. h
- Franklin M. u
- Freeman J. C. p
- Frisch H. l
- Funakoshi
- G. ab
- G. ae
- G. anao
- G. aq
- G. aqar
- G. aqar
- G. aqas
- G. aqauav
- G. az
- Galloni
- Garfinkel
- Garosi
- Gerberich H. w
- Gerchtein E. p
- Giagu
- Giakoumopoulou V. c
- Gibson
- Ginsburg C. M. p
- Giokaris N. c
- Giromini P. r
- Glagolev V. n
- Glenzinski D. p
- Gold
- Goldin
- Golossanov A. p
- Gomez Ceballos
- Gomez G. j
- Goncharov
- González López
- Gorelov
- Goshaw A. T. o
- Goulianos
- Gramellini E. f
- Grosso Pilcher
- Group
- Guimaraes Da Costa
- H. aj
- H. aw
- H. bh
- H. bj
- H. H. ap
- H. S. ay
- H. S. zbqbrbsbtbubv
- H. S. zbqbrbsbtbubv
- Hahn S. R. p
- Han
- Happacher F. r
- Hara
- Hare
- Harr
- Harrington Taber
- Hatakeyama K. e
- Hays
- Heinrich
- Herndon
- Hocker A. p
- Hong
- Hopkins W. p
- Hou S. a
- Hughes
- Husemann
- Hussein
- Huston
- I. ad
- I. ah
- I. ai
- I. ak
- I. bj
- I. zbqbrbsbtbubv
- Introzzi
- Iori
- Ivanov A. h
- J. aa
- J. ag
- J. ai
- J. ap
- J. ap
- J. ap
- J. aw
- J. bc
- J. bc
- J. bk
- J. bm
- J. E. zbqbrbsbtbubv
- J. mbo
- J. P. ad
- J. S. af
- J. S. zbqbrbsbtbubv
- J. u
- J. Y. ay
- James E. p
- Jang D. k
- Jayatilaka B. p
- Jeon
- Jindariani S. p
- Jones
- Joo
- Jun S. Y. k
- Junk T. R. p
- K. aa
- K. ag
- K. aj
- K. al
- K. aw
- K. az
- K. bh
- K. bh
- K. bh
- K. bi
- K. bk
- K. bk
- K. bk
- K. K. zbqbrbsbtbubv
- K. zbqbrbsbtbubv
- Kambeitz M. y
- Kamon
- Karchin
- Kasmi A. e
- Kato
- Ketchum W. l
- Keung
- Kilminster B. p
- Kim
- Kim
- Kim
- Kim
- Kim
- Kim
- Kim M. J. r
- Kim Y. K. l
- Kimura
- Kirby M. p
- Knoepfel K. p
- Kondo
- Kong
- Konigsberg J. q
- Kotwal A. V. o
- Kreps M. y
- Kroll
- Kruse M. o
- Kuhr T. y
- Kurata
- L. ac
- L. am
- L. az
- L. bm
- L. fg
- L. paq
- Laasanen
- Lammel S. p
- Lancaster
- Lannon
- Latino
- Lee
- Lee
- Leo S. w
- Leone
- Lewis J. D. p
- Limosani A. o
- Lipeles
- Lister A. s
- Liu
- Liu
- Liu T. p
- Lockwitz
- Loginov
- Lucà A. r
- Lucchesi
- Lueck J. y
- Lujan
- Lukens P. p
- Lungu
- Lys
- Lysak
- M. ab
- M. ac
- M. ac
- M. ae
- M. af
- M. ag
- M. ai
- M. ai
- M. anao
- M. anao
- M. aq
- M. aqar
- M. aqat
- M. ax
- M. ax
- M. ba
- M. babb
- M. bd
- M. bdbg
- M. bh
- M. bh
- M. bi
- M. bm
- M. E. bl
- M. fg
- M. J. aqat
- Madrak R. p
- Maestro
- Malik
- Manca
- Manousakis Katsikakis
- Marchese L. f
- Margaroli
- Marino
- Matera K. w
- Mattson
- Mazzacane A. p
- Mazzanti P. f
- McNulty
- Mehta
- Mehtala
- Mesropian
- Miao T. p
- Mietlicki
- Mitra A. a
- Miyake
- Moed S. p
- Moggi N. f
- Moon C. S. p
- Moore R. p
- Morello
- Mukherjee A. p
- Muller T. y
- Murat P. p
- Mussini
- N. bk
- Nachtman J. p
- Nagai
- Naganoma
- Nakano
- Napier
- Nett
- Neu
- Nigmanov
- Nodulman L. b
- Noh
- Norniella O. w
- O. ad
- Oakes
- Oh
- Oh S. H. o
- Oksuzian
- Okusawa
- Orava
- Ortolan L. d
- P. aa
- P. ai
- P. am
- P. an
- P. ap
- P. aqar
- P. aqas
- P. aqas
- P. aqas
- P. aqat
- P. ay
- P. E. bl
- P. F. aw
- P. mbo
- P. vbp
- Pagliarone
- Palencia E. j
- Palni
- Papadimitriou V. p
- Parker
- PAULETTA Giovanni
- Paulini M. k
- Paus
- Phillips T. J. o
- Piacentino G. p
- Pianori
- Pilot J. h
- Pitts K. w
- Plager C. i
- Pondrom
- Poprocki S. p
- Potamianos
- Pranko
- Prokoshin F. n
- Ptohos F. r
- Punzi
- Q. ax
- R. ab
- R. af
- R. aq
- R. C. pbj
- R. E. aj
- R. F. bl
- R. mbo
- R. t
- R. vbp
- Redondo Fernández
- Renton
- Rescigno
- Rimondi F. f
- Ristori
- Robson A. t
- Rodriguez
- Rolli
- Ronzani
- Roser R. p
- Rosner J. L. l
- Ruffini
- Ruiz A. j
- Russ J. k
- Rusu V. p
- S. ai
- S. am
- S. anao
- S. aq
- S. aqar
- S. az
- S. B. zbqbrbsbtbubv
- S. ba
- S. bi
- S. bn
- S. H. bh
- S. mbo
- S. Y. zbqbrbsbtbubv
- S. zbqbrbsbtbubv
- S.t. Denis
- Sakumoto
- Sakurai
- SANTI Lorenzo Gianni
- Sato
- Saveliev V. p
- Savoy Navarro
- Schlabach P. p
- Schmidt E. E. p
- Schwarz
- Scodellaro L. j
- Scuri
- Seidel
- Seiya
- Semenov A. n
- Sforza
- Shalhout S. Z. h
- Shears
- Shepard
- Shimojima
- Shochet M. l
- Shreyber Tecker
- Simonenko A. n
- Sliwa
- Smith J. R. h
- Snider F. D. p
- Song
- Sorin V. d
- Stancari M. p
- Stentz D. p
- Strologas
- Sudo
- Sukhanov A. p
- Suslov I. n
- T. ab
- T. af
- T. af
- T. al
- T. al
- T. ap
- T. aw
- T. bh
- T. bk
- T. p
- T. vbp
- T. zbcbqbrbsbtbubv
- T. zbqbrbsbtbubv
- Takemasa
- Takeuchi
- Tang J. l
- Tecchio
- Teng P. K. a
- Thom J. p
- Thomson
- Thukral
- Toback
- Tokar
- Tollefson
- Tomura
- Tonelli D. p
- Torre S. r
- Torretta D. p
- Totaro
- Trovato
- U. bn
- U. K. zbqbrbsbtbubv
- Ukegawa
- Uozumi
- V. bc
- V. E. ax
- Vázquez F. q
- Velev G. p
- Vellidis C. p
- Vernieri
- Vidal
- Vilar R. j
- Vizán J. j
- Vogel
- Volpi G. r
- W. bm
- W. K. ay
- W. M. aa
- Wagner
- Wallny R. p
- Wang S. M. a
- Waters
- Wester W. C. p
- Whiteson
- Wicklund A. B. b
- Wilbur S. h
- Williams
- Wilson
- Wilson P. p
- Winer
- Wittich P. p
- Wolbers S. p
- Wolfe
- Wright
- Wu X. s
- Wu Z. e
- Y. al
- Y. al
- Y. bh
- Y. bh
- Y. bh
- Y. bk
- Y. bk
- Y. C. zbqbrbsbtbubv
- Y. D. zbqbrbsbtbubv
- Y. J. zbqbrbsbtbubv
- Yamamoto
- Yamato
- Yang
- Yang
- Yang T. p
- Yao
- Yeh G. P. p
- Yi K. p
- Yoh J. p
- Yorita
- Yoshida
- Yu
- Yu G. B. o
- Z. bc
- Zanetti
- Zeng Y. o
- Zhou C. o
- Zucchelli S. fg
- Publication venue
- Publication date
- 01/01/2015
- Field of study
A search for particles with the same mass and couplings as those of the standard model Higgs boson but different spin and parity quantum numbers is presented. We test two specific alternative Higgs boson hypotheses: a pseudoscalar Higgs boson with spin-parity JP=0- and a gravitonlike Higgs boson with JP=2+, assuming for both a mass of 125GeV/c2. We search for these exotic states produced in association with a vector boson and decaying into a bottom-antibottom quark pair. The vector boson is reconstructed through its decay into an electron or muon pair, or an electron or muon and a neutrino, or it is inferred from an imbalance in total transverse momentum. We use expected kinematic differences between events containing exotic Higgs bosons and those containing standard model Higgs bosons. The data were collected by the CDF experiment at the Tevatron proton-antiproton collider, operating at a center-of-mass energy of s=1.96TeV, and correspond to an integrated luminosity of 9.45fb-1. We exclude deviations from the predictions of the standard model with a Higgs boson of mass 125GeV/c2 at the level of 5 standard deviations, assuming signal strengths for exotic boson production equal to the prediction for the standard model Higgs boson, and set upper limits of approximately 30% relative to the standard model rate on the possible rate of production of each exotic state
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
- 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
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- 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
Search for quark compositeness in dijet angular distributions from pp collisions at √s̅ = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
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- Publication venue
- Publication date
- 01/01/2012
- Field of study
Peer reviewe
Measurement of the Pseudorapidity and Centrality Dependence of the Transverse Energy Density in Pb-Pb Collisions at √sNN=2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
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- Alda Junior WL
- Aldaya Martin M
- Alexander J
- Aliev T
- Alimena J
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- Alverson G
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- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
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- Andreev Y
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- Antunovic Z
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- Arcidiacono R
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- Asawatangtrakuldee C
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- Yilmaz Y
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- Yumiceva F
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- Zanetti M
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- Zatserklyaniy A
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The transverse energy (E-T) in Pb-Pb collisions at 2.76 TeV nucleon-nucleon center-of-mass energy (root s(NN)) has been measured over a broad range of pseudorapidity (eta) and collision centrality by using the CMS detector at the LHC. The transverse energy density per unit pseudorapidity (dE(T)/d eta) increases faster with collision energy than the charged particle multiplicity. This implies that the mean energy per particle is increasing with collision energy. At all pseudorapidities, the transverse energy per participating nucleon increases with the centrality of the collision. The ratio of transverse energy per unit pseudorapidity in peripheral to central collisions varies significantly as the pseudorapidity increases from eta = 0 to vertical bar eta vertical bar = 5.0. For the 5% most central collisions, the energy density per unit volume is estimated to be about 14 GeV/fm(3) at a time of 1 fm/c after the collision. This is about 100 times larger than normal nuclear matter density and a factor of 2.6 times higher than the energy density reported at root s(NN) = 200 GeV at the Relativistic Heavy Ion Collider
Search for supersymmetry in hadronic final states using MT2 in pp collisions at √s = 7 TeV
- Author
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- Abbiendi G
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- Abdullin S
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Open Access: This article is distributed under the terms of the Creative Commons Attribution License.-- et al.A search for supersymmetry or other new physics resulting in similar final states is presented using a data sample of 4.73 fb−1 of pp collisions collected at √s = 7 TeV with the CMS detector at the LHC. Fully hadronic final states are selected based on the variable M T2, an extension of the transverse mass in events with two invisible particles. Two complementary studies are performed. The first targets the region of parameter space with medium to high squark and gluino masses, in which the signal can be separated from the standard model backgrounds by a tight requirement on M T2. The second is optimized to be sensitive to events with a light gluino and heavy squarks. In this case, the M T2 requirement is relaxed, but a higher jet multiplicity and at least one b-tagged jet are required. No significant excess of events over the standard model expectations is observed. Exclusion limits are derived for the parameter space of the constrained minimal supersymmetric extension of the standard model, as well as on a variety of simplified model spectra.European Commission; Federal Ministry of Science, Research and Economy (Austria); Agency for Innovation by Science and Technology (Belgium); Conselho Nacional de Desenvolvimento Científico e Tecnológico (Brasil); Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (Brasil); Fundação Carlos Chagas Filho de Amparo à Pesquisa do Estado do Rio de Janeiro; Fundação de Amparo à Pesquisa do Estado de São Paulo; Colciencias (Colombia); Ministry of Science, Education and Sports of the Republic of Croatia; Research Promotion Foundation (Cyprus); Centre National de la Recherche Scientifique (France); Bundesministerium für Bildung und Forschung (Deutschland); Deutsche Forschungsgemeinschaft; General Secretariat of Research and Technology (Greece); National Office for Research and Technology (Hungary); Institute for Research in Fundamental Sciences (Iran); Science Foundation Ireland; Istituto Nazionale di Fisica Nucleare (Italia); National Research Foundation of Korea; Centro de Investigación y de Estudios Avanzados del Instituto Politécnico Nacional (México); Consejo Nacional de Ciencia y Tecnología (México); Secretaría de Educación Pública (México); Universidad Autónoma de San Luis Potosí; Pakistan Atomic Energy Commission; Fundação para a Ciência e a Tecnologia (Portugal); Joint Institute for Nuclear Research (Russia); Russian Foundation for Basic Research; Ministry of Education, Science and Technological Development (Serbia); Ministerio de Ciencia e Innovación (España); Centro Nacional de Física de Partículas, Astropartículas y Nuclear (España); Swiss National Science Foundation; The Scientific and Technological Research Council of Turkey; Turkish Atomic Energy Authority; Alfred P. Sloan Foundation; Alexander von Humboldt Foundation; Science and Technology Facilities Council (UK); Department of Energy (US); National Science Foundation (US).Peer Reviewe
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