1,124 research outputs found
Measurement of the Z/gamma* + b-jet cross section in pp collisions at 7 TeV
- Author
- Abbaneo D.
- Abbiendi G.
- Abbrescia M.
- Abdullin S.
- Acosta D.
- Acosta J. G.
- Acosta M. Vazquez
- Adair A.
- Adam N.
- Adam W.
- Adams M. R.
- Adams T.
- Adiguzel A.
- Adler V.
- Adzic P.
- Afanasiev S.
- Agostino L.
- Agram J-L
- Aguilar-Benitez M.
- Aguilo E.
- Ahmad M.
- Ahmad W. Haj
- Ahuja S.
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe production of b jets in association with a Z/gamma* boson is studied
using proton-proton collisions delivered by the LHC at a centre-of-mass energy
of 7 TeV and recorded by the CMS detector. The inclusive cross section for
Z/gamma* + b-jet production is measured in a sample corresponding to an
integrated luminosity of 2.2 inverse femtobarns. The Z/gamma* + b-jet cross
section with Z/gamma* to ll (where ll = ee or mu mu) for events with the
invariant mass 60 < M(ll) < 120 GeV, at least one b jet at the hadron level
with pT > 25 GeV and abs(eta) < 2.1, and a separation between the leptons and
the jets of Delta R > 0.5 is found to be 5.84 +/- 0.08 (stat.) +/- 0.72 (syst.)
+(0.25)/-(0.55) (theory) pb. The kinematic properties of the events are also
studied and found to be in agreement with the predictions made by the MadGraph
event generator with the parton shower and the hadronisation performed by
PYTHIA.Comment: Submitted to the Journal of High Energy Physic
Compressed representation of a partially defined integer function over multiple arguments
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
Get PDFIn OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- 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
- 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
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
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
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yu I
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- 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
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
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- Zito G
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- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Get PDFA 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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
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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- Ujvari B
- Ulmer KA
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- Uzunian A
- Vaandering EW
- Valls N
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- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
- Vishnevskiy D
- Vitulo P
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
- 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 X
- Wang J
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- Wang M
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- Wang X
- Wang Z
- Wardle N
- Wasserbaech S
- Wayand S
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- Weber HA
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- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
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- Xiao H
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- Yilmaz Y
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- Yumiceva F
- Yun JC
- Zabel J
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- Zaganidis N
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- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
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- Zielinski M
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- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Get PDFJet 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
Search for heavy Majorana neutrinos in e+-e+-+ jets and e+-Îź+-+ jets events in proton-proton collisions at s = 8 sâ=8 TeV
- Author
- Abdelalim A. A.
- Abdulsalam A.
- Abu Zeid S.
- Adam W.
- Ahmad M.
- Ahuja S.
- Alda Junior W. L.
- Alderweireldt S.
- Aleksandrov A.
- Alves F. L.
- Alves G. A.
- Antropov I.
- Antunovic Z.
- Asawatangtrakuldee C.
- Asilar E.
- Attikis A.
- Avila C.
- Baffioni S.
- Ban Y.
- Basegmez S.
- Beaudette F.
- Belchior Batista Das Chagas E.
- Beliy N.
- Beluffi C.
- Benucci L.
- Bergauer T.
- Bernardes C. A.
- Besancon M.
- Bian J. G.
- Blekman F.
- Bondu O.
- Brandstetter J.
- Brigljevic V.
- Brito L.
- Brochet S.
- Brondolin E.
- Brun H.
- Bruno G.
- Busson P.
- Cabrera A.
- Cadamuro L.
- Caillol C.
- Calpas B.
- Carvalho W.
- Cassagnac R. Granier de
- Caudron A.
- Ceard L.
- Chaparro Sierra L. F.
- Chapon E.
- Charlot C.
- Chen G. M.
- Chen H. S.
- Chen M.
- Cheng T.
- Chinellato J.
- Cimmino A.
- Clerbaux B.
- Cornelis T.
- Correa Martins Junior M.
- Couderc F.
- Crucy S.
- Custodio A.
- D\u27Hondt J.
- Da Costa E. M.
- Daci N.
- Davignon O.
- De Bruyn I.
- De Jesus Damiao D.
- De Lentdecker G.
- De Oliveira Martins C.
- De Souza Santos A.
- De Visscher S.
- De Wolf E. A.
- Dejardin M.
- Delaere C.
- Delcourt M.
- Denegri D.
- Deroover K.
- Dimitrov A.
- Dobur D.
- Dogra S.
- Dragicevic M.
- Du R.
- Eerola P.
- Elkafrawy T.
- ErĂś J.
- Fabbro B.
- Fagot A.
- Fang W.
- Fasanella G.
- Faure J. L.
- Favaro C.
- Favart D.
- Favart L.
- Fernandez Perez Tomei T. R.
- Ferri F.
- Filipovic N.
- Finger M.
- Flechl M.
- Florez C.
- Fonseca De Souza S.
- Forthomme L.
- Friedl M.
- FrĂźhwirth R.
- Ganjour S.
- Garcia G.
- Ghete V. M.
- Giammanco A.
- Givernaud A.
- Glushkov I.
- Godinovic N.
- Goldouzian R.
- Gomez Moreno B.
- Gomez J. P.
- Gras P.
- Grebenyuk A.
- Gregores E. M.
- Gul M.
- Hadjiiska R.
- Hamer M.
- Hammad G. H.
- Hartl C.
- Hensel C.
- Heracleous N.
- Hrubec J.
- Huertas Guativa L. M.
- HärkÜnen J.
- HĂśrmann N.
- Iaydjiev P.
- Jafari A.
- Janssen X.
- Jarry P.
- Jeitler M.
- Jez P.
- Jiang C. H.
- Jo M.
- Kadastik M.
- Kadija K.
- Karapostoli G.
- Karimäki V.
- Keaveney J.
- Khachatryan V.
- Kinnunen R.
- Knutsson A.
- Komm M.
- Kovac M.
- Krammer M.
- Krätschmer I.
- KĂśnig A.
- Lampen T.
- Lassila-Perini K.
- Lauwers J.
- Leggat D.
- Lehti S.
- Lelas D.
- Lemaitre V.
- Lenzi T.
- Leonard A.
- Li Q.
- Liko D.
- Linden T.
- Lisniak S.
- Litov L.
- Liu S.
- Locci E.
- Lowette S.
- Luetic J.
- Luukka P.
- Luyckx S.
- Machet M.
- Maerschalk T.
- Mahmoud M. A.
- Malbouisson H.
- Malcles J.
- Mao Y.
- Marinov A.
- Matos Figueiredo D.
- Matsushita T.
- Mavromanolakis G.
- Mccartin J.
- Mercadante P. G.
- Mertens A.
- Micanovic S.
- Mikulec I.
- Mine P.
- Monchenault G. Hamel de
- Moon C. S.
- Moortgat S.
- Mora Herrera C.
- Moraes A.
- Moreels L.
- Mossolov V.
- Mousa J.
- Mundim L.
- Murumaa M.
- Musich M.
- Nicolaou C.
- Nogima H.
- Novaes S. F.
- Nuttens C.
- Ocampo Rios A. A.
- Olbrechts A.
- Padula Sandra S.
- Pavlov B.
- Pekkanen J.
- Peltola T.
- Pernie L.
- Perrini L.
- Petkov P.
- Piotrzkowski K.
- Plestina R.
- Pol M. E.
- Poyraz D.
- Prado Da Silva W. L.
- Ptochos F.
- Puljak I.
- Python Q.
- Qian S. J.
- Quertenmont L.
- Rabady D.
- Rad N.
- Rahbaran B.
- Raidal M.
- Rander J.
- Randle-conde A.
- Razis P. A.
- Rebello Teles P.
- Ribeiro Cipriano P. M.
- Rodozov M.
- Rohringer H.
- Romeo F.
- Romero Abad D.
- Rosowsky A.
- Ruiz Vargas J. C.
- Ryckbosch D.
- Rykaczewski H.
- Salama E.
- Salva S.
- Sanabria J. C.
- Santoro A.
- Schieck J.
- SchĂśfbeck R.
- Selvaggi M.
- Seva T.
- Shaheen S. M.
- Shumeiko N.
- Sigamani M.
- Sirunyan A. M.
- Spiezia A.
- Stoykova S.
- Strauss J.
- Strom D.
- Suarez Gonzalez J.
- Sudic L.
- Sultanov G.
- Sznajder A.
- Talvitie J.
- Tao J.
- Tavernier S.
- Tiko A.
- Titov M.
- Tonelli Manganote E. J.
- Treberer-Treberspurg W.
- Tumasyan A.
- Tuominiemi J.
- Tuovinen E.
- Tuuva T.
- Tytgat M.
- Van De Klundert M.
- Van Doninck W.
- Van Driessche W.
- Van Haevermaet H.
- Van Mechelen P.
- Van Mulders P.
- Van Onsem G. P.
- Van Parijs I.
- Van Remortel N.
- Van Spilbeeck A.
- Vander Velde C.
- Vanlaer P.
- Veelken C.
- Vidal Marono M.
- Vilela Pereira A.
- Voutilainen M.
- Vutova M.
- Waltenberger W.
- Wang C.
- Wang D.
- Wang Z.
- Wendland L.
- Wulz C.-E.
- Xu Z.
- Yazgan E.
- Yonamine R.
- Zaganidis N.
- Zenoni F.
- Zghiche A.
- Zhang F.
- Zhang H.
- {etal} P.
- Publication venue
- Scuola Internazionale Superiore di Studi Avanzati
- Publication date
- 26/09/2016
- Field of study
Get PDFA search is performed for heavy Majorana neutrinos (N) decaying into a W boson and a lepton using the CMS detector at the Large Hadron Collider. A signature of two jets and either two same sign electrons or a same sign electron-muon pair is searched for using 19.7 fbâ1 of data collected during 2012 in proton-proton collisions at a centre-of-mass energy of 8 TeV. The data are found to be consistent with the expected standard model (SM) background and, in the context of a Type-1 seesaw mechanism, upper limits are set on the cross section times branching fraction for production of heavy Majorana neutrinos in the mass range between 40 and 500 GeV. The results are additionally interpreted as limits on the mixing between the heavy Majorana neutrinos and the SM neutrinos. In the mass range considered, the upper limits range between 0.00015â0.72 for |VeN|2 and 6.6 Ă 10â5â0.47 for |VeNVÎźNâ|2/(|VeN|2â+â|VÎźN|2), where VâN is the mixing element describing the mixing of the heavy neutrino with the SM neutrino of flavour â. These limits are the most restrictive direct limits for heavy Majorana neutrino masses above 200 GeV
Search for pair-produced resonances decaying to jet pairs in proton-proton collisions at âs=8 TeV
- Author
- Adam W.
- Adler Volker
- Agram J. -L.
- Ahmad W. Haj
- Alda Junior W. L.
- Alderweireldt S.
- Aleksandrov A.
- Alvarez J. D. Ruiz
- Alves G. A.
- Andrea J.
- Antunovic Z.
- Asawatangtrakuldee C.
- Asin I.
- Assran Y.
- Ata M.
- Attikis A.
- Aubin A.
- Autermann C.
- Avila C.
- Baffioni S.
- Ban Y.
- Bansal S.
- Bartosik N.
- Basegmez S.
- Beauceron S.
- Beaudette F.
- Beaupere N.
- Beernaert Kelly
- Behr J.
- Behrens U.
- Beliy N.
- Bell A. J.
- Beluffi C.
- Benucci Leonardo
- Beranek S.
- Bergauer T.
- Bernardes C. A.
- Bernet C.
- Besancon M.
- Bethani A.
- Bian J. G.
- Blekman F.
- Bloch D.
- Blyweert S.
- Bodlak M.
- Bontenackels M.
- Borras K.
- Boudoul G.
- Bouvier E.
- Brigljevic V.
- Brito L.
- Brochet S.
- Brodski M.
- Brom J. -M.
- Bruno G.
- Burgmeier A.
- Busson P.
- Cabrera A.
- Caebergs T.
- Caillol C.
- Cakir A.
- Calligaris L.
- Campbell A.
- Carvalho W.
- Castello R.
- Caudron A.
- Ceard L.
- Chabert E. C.
- Chapon E.
- Chariot C.
- Chasserat J.
- Chen G. M.
- Chen H. S.
- Chen M.
- Cheng T.
- Cherepanov V.
- Chierici R.
- Chinellato J.
- Choudhury S.
- Cimmino Anna
- Clerbaux B.
- Collard C.
- Contardo D.
- Conte E.
- Cornelis T.
- Correa Martins Junior M.
- Costantini Silvia
- Costanza F.
- Couderc F.
- Crucy Shannon Rebecca
- Custodio A.
- D'Hondt J.
- Da Costa E. M.
- Da Silveira G. G.
- Daci N.
- Dahms T.
- Dalchenko M.
- Daubie E.
- de Cassagnac R. Granier
- De Jesus Damiao D.
- De Lentdecker G.
- De Monchenault G. Hamel
- De Oliveira Martins C.
- De Wolf E. A.
- Dejardin M.
- Delaere C.
- Denegri D.
- Depasse P.
- Dietz-Laursonn E.
- Dildick Sven
- Dimitrov A.
- Dobrzynski L.
- Dobur D.
- Dogra S.
- Dolinska G.
- Donckt M. Vander
- Dooling S.
- Dorland T.
- Dos Reis Martins T.
- Dragicevic M.
- du Pree T.
- Du R.
- Duchardt D.
- Eckerlin G.
- Eckstein D.
- Edelhoff M.
- Eerola P.
- Eichhorn T.
- El Mamouni H.
- Elgammall S.
- Erdmann M.
- Erdogan Y.
- Eroe J.
- Fabbro B.
- Fagot Alexis
- Fan J.
- Faure J. L.
- Favaro C.
- Favart D.
- Favart L.
- Fay J.
- Feld L.
- Fernandez Perez Tomei T. R.
- Ferri F.
- Filipovic N.
- Finger M.
- Finger M.
- Fischer R.
- Florent A.
- Florez C.
- Flucke G.
- Fluegge G.
- Fonseca De Souza S.
- Fontaine J. -C.
- Forthomme L.
- Friedl M.
- Fruehwirth R.
- Gadrat S.
- Ganjour S.
- Garcia Guillaume
- Garcia J. Garay
- Garcia J. M. Vizan
- Gascon S.
- Gay A. P. R.
- Geenen H.
- Geiser A.
- Geisler M.
- Gele D.
- Genchev V.
- Ghete V. M.
- Giammanco A.
- Givernaud A.
- Gizhko A.
- Glushkov I.
- Godinovic N.
- Goerlach U.
- Goetzmann C.
- Gomez J. P.
- Gonzalez J. Suarez
- Gouzevitch M.
- Gras P.
- Grebenyuk A.
- Gregores E. M.
- Gueth A.
- Gunnellini P.
- Hadjiiska R.
- Hammad G. H.
- Harkonen J.
- Hartl C.
- Hauk J.
- Hebbeker T.
- Heidemann C.
- Heister A.
- Hempel M.
- Heracleous N.
- Hoehle F.
- Hoemann N.
- Hoepfner K.
- Hollar J.
- Hrubec J.
- Iaydjiev P.
- Ille B.
- Jafari A.
- Janssen X.
- Jarry P.
- Jeitler M.
- Jez P.
- Jiang C. H.
- Jung H.
- Kadastik M.
- Kadija K.
- Kalogeropoulos A.
- Kame A. Ellithi
- Kargoll B.
- Karimaki V.
- Kasemann M.
- Katsas P.
- Keaveney J.
- Khachatryan V.
- Kieseler J.
- Kiesenhofer W.
- Kinnunen R.
- Klein K.
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- Treberer-Treberspurg W.
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- Tumasyan A.
- Tuominen E.
- Tuominiemi J.
- Tuovinen E.
- Tuuva T.
- Tytgat Michael
- Van De Klundert M.
- Van Doninck W.
- Van Haevermaet H.
- Van Hove P.
- Van Mechelen P.
- Van Mulders P.
- Van Onsem G. P.
- Van Remortel N.
- Van Spilbeeck A.
- Vanlaer P.
- Veelken C.
- Velde C. Vander
- Verdier P.
- Vilela Pereira A.
- Villella I.
- Viret S.
- Voutilainen M.
- Vutova M.
- Waltenberger W.
- Wang D.
- Wang J.
- Wang Z.
- Weber H.
- Weber M.
- Wendland L.
- Wittmer B.
- Wulz C. -E.
- Xiao H.
- Xu Z.
- Yazgan Efe
- Yilmaz Y.
- Zabi A.
- Zaganidis Nikolaos
- Zenoni F.
- Zhukov V.
- Zou W.
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2015
- Field of study
Get PDFResults are reported of a general search for pair production of heavy resonances decaying to pairs of hadronic jets in events with at least four jets. The study is based on up to 19.4 fb(-1) of integrated luminosity from proton-proton collisions at a center-of-mass energy of 8 TeV, recorded with the CMS detector at the LHC. Limits are determined on the production of scalar top quarks (top squarks) in the framework of R-parity violating supersymmetry and on the production of color-octet vector bosons (colorons). First limits at the LHC are placed on top squark production for two scenarios. The first assumes decay to a bottom quark and a light-flavor quark and is excluded for masses between 200 and 385 GeV, and the second assumes decay to a pair of light-flavor quarks and is excluded for masses between 200 and 350 GeV at 95% confidence level. Previous limits on colorons decaying to light-flavor quarks are extended to exclude masses from 200 to 835 GeV
Measurement of the t-channel single top quark production cross section in pp collisions at âs =7 TeV
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- Publication venue
- Publication date
- 01/01/2011
- Field of study
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