590 research outputs found
Study of the B +â J / Ï Î ÂŻ p decay in proton-proton collisions at âs = 8 TeV
- Author
- Adam W
- Alves FL
- Ambrogi F
- Beghin D
- Bergauer T
- Bilin B
- Blekman F
- Bols ES
- Bondu O
- Brandstetter J
- Brun H
- Bruno G
- Caputo C
- Chhibra SS
- Clerbaux B
- Cornelis T
- Darwish MR
- David P
- De Clercq J
- De Lentdecker G
- De Wolf EA
- Delaere C
- Delannoy H
- Delcourt M
- Di Croce D
- Dobur D
- Dorney B
- Dragicevic M
- Drugakov V
- DâHondt J
- Erö J
- Escalante Del Valle A
- Favart L
- Flechl M
- FrĂŒhwirth R
- Giammanco A
- Grebenyuk A
- Janssen X
- Jeitler M
- Kalsi AK
- Khvastunov I
- Krammer N
- KrÀtschmer I
- Lauwers J
- Lelek A
- Lemaitre V
- Liko D
- Lontkovskyi D
- Lowette S
- Luetic J
- Madlener T
- Magitteri A
- Marchesini I
- Mikulec I
- Moortgat S
- Moreels L
- Mossolov V
- Niedziela M
- Pieters M
- Popov A
- Postiau N
- Prisciandaro J
- Python Q
- Rad N
- Rejeb Sfar H
- Roskas C
- Saggio A
- Schieck J
- Schöfbeck R
- Sirunyan AM
- Skovpen K
- Spanring M
- Spitzbart D
- Starling E
- Suarez Gonzalez J
- Tavernier S
- Thomas L
- Trocino D
- Tumasyan A
- Tytgat M
- Van Doninck W
- Van Haevermaet H
- Van Mechelen P
- Van Mulders P
- Van Parijs I
- Van Putte S
- Van Remortel N
- Vander Velde C
- Vanlaer P
- Vannerom D
- Verbeke W
- Vermassen B
- Vidal Marono M
- Vischia P
- Vit M
- Waltenberger W
- Wulz CE
- Zaganidis N
- Zarucki M
- Zobec J
- Publication venue
- eScholarship, University of California
- Publication date
- 01/12/2019
- Field of study
A study of the B +â J / Ï Î ÂŻ p decay using proton-proton collision data collected at s = 8 TeV by the CMS experiment at the LHC, corresponding to an integrated luminosity of 19.6 fbâ1, is presented. The ratio of branching fractions B(B+âJ/ÏÎÂŻp)/B(B+âJ/ÏKâ(892)+) is measured to be (1.054 ± 0.057(stat) ± 0.035(syst) ± 0.011(B))%, where the last uncertainty reflects the uncertainties in the world-average branching fractions of Î ÂŻ and K*(892) + decays to reconstructed final states. The invariant mass distributions of the J / Ï Î ÂŻ , J/Ïp, and Î ÂŻ p systems produced in the B +â J / Ï ÎÂŻ p decay are investigated and found to be inconsistent with the pure phase space hypothesis. The analysis is extended by using a model-independent angular amplitude analysis, which shows that the observed invariant mass distributions are consistent with the contributions from excited kaons decaying to the Î ÂŻ p system. [Figure not available: see fulltext.
Search for new neutral Higgs bosons through the H â ZAâ â+ââb b ÂŻ process in pp collisions at âs = 13 TeV
- Author
- Adam W
- Alves FL
- Alves GA
- Ambrogi F
- Beghin D
- Bergauer T
- Bilin B
- Blekman F
- Bols ES
- Bondu O
- Brandstetter J
- Brun H
- Bruno G
- Caputo C
- Chhibra SS
- Clerbaux B
- Cornelis T
- Correia Silva G
- Darwish MR
- David P
- De Clercq J
- De Lentdecker G
- De Wolf EA
- Delaere C
- Delannoy H
- Delcourt M
- Di Croce D
- Dobur D
- Dorney B
- Dragicevic M
- Drugakov V
- DâHondt J
- Erö J
- Escalante Del Valle A
- Favart L
- Flechl M
- FrĂŒhwirth R
- Giammanco A
- Grebenyuk A
- Hensel C
- Janssen X
- Jeitler M
- Kalsi AK
- Khvastunov I
- Krammer N
- KrÀtschmer I
- Lelek A
- Lemaitre V
- Liko D
- Lontkovskyi D
- Lowette S
- Madlener T
- Magitteri A
- Marchesini I
- Mikulec I
- Moortgat S
- Moraes A
- Mossolov V
- Niedziela M
- Pieters M
- Popov A
- Postiau N
- Prisciandaro J
- Python Q
- Rad N
- Rejeb Sfar H
- Roskas C
- Saggio A
- Schieck J
- Schöfbeck R
- Sirunyan AM
- Skovpen K
- Spanring M
- Spitzbart D
- Starling E
- Suarez Gonzalez J
- Tavernier S
- Thomas L
- Trocino D
- Tumasyan A
- Tytgat M
- Van Doninck W
- Van Haevermaet H
- Van Mechelen P
- Van Mulders P
- Van Putte S
- Van Remortel N
- Vander Velde C
- Vanlaer P
- Vannerom D
- Verbeke W
- Vermassen B
- Vidal Marono M
- Vischia P
- Vit M
- Waltenberger W
- Wulz CE
- Zaganidis N
- Zarucki M
- Zobec J
- Publication venue
- eScholarship, University of California
- Publication date
- 01/03/2020
- Field of study
This paper reports on a search for an extension to the scalar sector of the standard model, where a new CP-even (odd) boson decays to a Z boson and a lighter CP-odd (even) boson, and the latter further decays to a b quark pair. The Z boson is reconstructed via its decays to electron or muon pairs. The analysed data were recorded in proton-proton collisions at a center-of-mass energy s = 13 TeV, collected by the CMS experiment at the LHC during 2016, corresponding to an integrated luminosity of 35.9 fbâ1. Data and predictions from the standard model are in agreement within the uncertainties. Upper limits at 95% confidence level are set on the production cross section times branching fraction, with masses of the new bosons up to 1000 GeV. The results are interpreted in the context of the two-Higgs-doublet model. [Figure not available: see fulltext.]
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Measurement of the top quark Yukawa coupling from t t kinematic distributions in the lepton+jets final state in proton-proton collisions at s =13 TeV MEASUREMENT of the TOP QUARK YUKAWA COUPLING from ... SIRUNYAN et al.
- Author
- Adam W
- Ambrogi F
- Beghin D
- Bergauer T
- Bilin B
- Blekman F
- Bols ES
- Bondu O
- Brandstetter J
- Brun H
- Bruno G
- Caputo C
- Chhibra SS
- Clerbaux B
- Cornelis T
- D'Hondt J
- Darwish MR
- David P
- De Clercq J
- De Lentdecker G
- De Wolf EA
- Delaere C
- Delannoy H
- Delcourt M
- Di Croce D
- Dobur D
- Dorney B
- Dragicevic M
- Drugakov V
- Erö J
- Escalante Del Valle A
- Favart L
- Flechl M
- FrĂŒhwirth R
- Giammanco A
- Grebenyuk A
- Janssen X
- Jeitler M
- Kalsi AK
- Khvastunov I
- Krammer N
- KrÀtschmer I
- Lauwers J
- Lelek A
- Lemaitre V
- Liko D
- Lontkovskyi D
- Lowette S
- Luetic J
- Madlener T
- Magitteri A
- Marchesini I
- Mikulec I
- Moortgat S
- Moreels L
- Mossolov V
- Pieters M
- Popov A
- Postiau N
- Prisciandaro J
- Python Q
- Rad N
- Rejeb Sfar H
- Roskas C
- Saggio A
- Schieck J
- Schöfbeck R
- Sirunyan AM
- Skovpen K
- Spanring M
- Spitzbart D
- Starling E
- Suarez Gonzalez J
- Tavernier S
- Thomas L
- Trocino D
- Tumasyan A
- Tytgat M
- Van Doninck W
- Van Haevermaet H
- Van Mechelen P
- Van Mulders P
- Van Parijs I
- Van Putte S
- Van Remortel N
- Vander Velde C
- Vanlaer P
- Vannerom D
- Verbeke W
- Vermassen B
- Vidal Marono M
- Vischia P
- Vit M
- Waltenberger W
- Wang Q
- Wittmann J
- Wulz CE
- Zaganidis N
- Zarucki M
- Zobec J
- Publication venue
- eScholarship, University of California
- Publication date
- 17/10/2019
- Field of study
Results are presented for an extraction of the top quark Yukawa coupling from top quark-antiquark (tt) kinematic distributions in the lepton plus jets final state in proton-proton collisions, based on data collected by the CMS experiment at the LHC at s=13 TeV, corresponding to an integrated luminosity of 35.8 fb-1. Corrections from weak boson exchange, including Higgs bosons, between the top quarks can produce large distortions of differential distributions near the energy threshold of tt production. Therefore, precise measurements of these distributions are sensitive to the Yukawa coupling. Top quark events are reconstructed with at least three jets in the final state, and a novel technique is introduced to reconstruct the tt system for events with one missing jet. This technique enhances the experimental sensitivity in the low invariant mass region, Mtt. The data yields in Mtt, the rapidity difference |yt-yt|, and the number of reconstructed jets are compared with distributions representing different Yukawa couplings. These comparisons are used to measure the ratio of the top quark Yukawa coupling to its standard model predicted value to be 1.07-0.43+0.34 with an upper limit of 1.67 at the 95% confidence level
Search for a heavy Higgs boson decaying to a pair of W bosons in proton-proton collisions at âs = 13 TeV
- Author
- Adam W
- Alves FL
- Ambrogi F
- Beghin D
- Bergauer T
- Bilin B
- Blekman F
- Bols ES
- Bondu O
- Brandstetter J
- Brun H
- Bruno G
- Caputo C
- Chhibra SS
- Clerbaux B
- Cornelis T
- Darwish MR
- David P
- De Clercq J
- De Lentdecker G
- De Wolf EA
- Delaere C
- Delannoy H
- Delcourt M
- Di Croce D
- Dobur D
- Dorney B
- Dragicevic M
- Drugakov V
- DâHondt J
- Erö J
- Escalante Del Valle A
- Favart L
- Flechl M
- FrĂŒhwirth R
- Giammanco A
- Grebenyuk A
- Janssen X
- Jeitler M
- Kalsi AK
- Khvastunov I
- Krammer N
- KrÀtschmer I
- Lauwers J
- Lelek A
- Lemaitre V
- Liko D
- Lontkovskyi D
- Lowette S
- Luetic J
- Madlener T
- Magitteri A
- Marchesini I
- Mikulec I
- Moortgat S
- Moreels L
- Mossolov V
- Niedziela M
- Pieters M
- Popov A
- Postiau N
- Prisciandaro J
- Python Q
- Rad N
- Rejeb Sfar H
- Roskas C
- Saggio A
- Schieck J
- Schöfbeck R
- Sirunyan AM
- Skovpen K
- Spanring M
- Spitzbart D
- Starling E
- Suarez Gonzalez J
- Tavernier S
- Thomas L
- Trocino D
- Tumasyan A
- Tytgat M
- Van Doninck W
- Van Haevermaet H
- Van Mechelen P
- Van Mulders P
- Van Parijs I
- Van Putte S
- Van Remortel N
- Vander Velde C
- Vanlaer P
- Vannerom D
- Verbeke W
- Vermassen B
- Vidal Marono M
- Vischia P
- Vit M
- Waltenberger W
- Wulz CE
- Zaganidis N
- Zarucki M
- Zobec J
- Publication venue
- eScholarship, University of California
- Publication date
- 01/03/2020
- Field of study
A search for a heavy Higgs boson in the mass range from 0.2 to 3.0 TeV, decaying to a pair of W bosons, is presented. The analysis is based on proton-proton collisions at s = 13 TeV recorded by the CMS experiment at the LHC in 2016, corresponding to an integrated luminosity of 35.9 fbâ1. The W boson pair decays are reconstructed in the 2â2Îœ and âÎœ2q final states (with â = e or ÎŒ). Both gluon fusion and vector boson fusion production of the signal are considered. Interference effects between the signal and background are also taken into account. The observed data are consistent with the standard model (SM) expectation. Combined upper limits at 95% confidence level on the product of the cross section and branching fraction exclude a heavy Higgs boson with SM-like couplings and decays up to 1870 GeV. Exclusion limits are also set in the context of a number of two-Higgs-doublet model formulations, further reducing the allowed parameter space for SM extensions. [Figure not available: see fulltext.
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- 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
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
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- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boimska B
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- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
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- Bornheim A
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- Bortoletto D
- Bose S
- Bose T
- Bostock F
- Botta C
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- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Broccolo G
- Brochero Cifuentes JA
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmann MA
- Buchmuller O
- Bunkowski K
- Bunn J
- Buontempo S
- Burgmeier A
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
- Campbell A
- Camporesi T
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
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- Carlsmith D
- Carrillo Moreno S
- Carroll R
- Cartiglia N
- Carvalho W
- Casal B
- Casimiro Linares E
- Castaldi R
- Castello R
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- Castro A
- Castro E
- Caudron J
- Caulfield M
- Cavallari F
- Cavallo FR
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- Ceard L
- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
- Chen M
- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Cho Y
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cooper W
- Cornelis T
- Correa Martins Junior M
- Cortezon EP
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
- David A
- Davids M
- Davies G
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Troconiz JF
- De Visscher S
- De Wolf EA
- Deisher A
- Deiters K
- Dejardin M
- del Arbol PMR
- Del Re D
- Delaere C
- Delgado Peris A
- Deliomeroglu M
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demortier L
- Denegri D
- Deniz M
- Depasse P
- Dermenev A
- Dero V
- Dhingra N
- Di Giovanni GP
- Di Guida S
- Di Marco E
- Di Matteo L
- Diamond B
- Dias FA
- Diemoz M
- Dierlamm A
- Dietz C
- Dietz-Laursonn E
- Diez Pardos C
- Dimitrov A
- Dinardo ME
- Dirkes G
- Dissertori G
- Dittmar M
- Djordjevic M
- Dobrzynski L
- Dobson M
- Dobur D
- Doesburg R
- Dogangun O
- Dolen J
- Dominguez Vazquez D
- Dominguez A
- Dominik W
- Don CKK
- Dorigo T
- Dorney B
- Doroba K
- Dozen C
- Draeger J
- Dragicevic M
- Dragoiu C
- Drell BR
- Dremin I
- Drouhin F
- Drozdetskiy A
- du Pree T
- Duarte Campderros J
- Duarte J
- Dubinin M
- Dudero PR
- Dudko L
- Duenser M
- Dugad S
- Duggan D
- Dumanoglu I
- Dupont-Sagorin N
- Duric S
- Duris J
- Durkin LS
- Duru F
- Dutta D
- Dutta S
- Dutta V
- Dzelalija M
- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
- Eerola P
- Efron J
- Eggert N
- Ekmedzic M
- El Mamouni H
- Elgammal S
- Elliott-Peisert A
- Ellison J
- Elmer P
- Elvira VD
- Enderle H
- Engh D
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erfle J
- Erhan S
- Ero J
- Erofeeva M
- Ershov A
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- Eshaq Y
- Eskut E
- Etesami SM
- Eugster J
- Eusebi R
- Evangelou I
- Evans D
- Everaerts P
- Everett A
- Evstyukhin S
- Fabbri F
- Fabbri F
- Fabbricatore P
- Fabbro B
- Fabjan C
- Fabozzi F
- Faccioli P
- Fahim A
- Falkiewicz A
- Fanelli C
- Fanfani A
- Fano L
- Fantasia C
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- Yilmaz Y
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- Zalewski P
- Zanetti M
- Zang J
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- Zeinali M
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- 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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- Yilmaz Y
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- Yumiceva F
- Yun JC
- Zabel J
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Zoeller MH
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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
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
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- Wardle N
- Wasserbaech S
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- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
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- Yang F
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- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- 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
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
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- Ujvari B
- Ulmer KA
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- Uzunian A
- Vaandering EW
- Valls N
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- Veszpremi V
- Vesztergombi G
- Veverka J
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- Villella I
- Vinogradov A
- Virdee T
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- Virto AL
- Vischia P
- Vishnevskiy D
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- Vizan Garcia JM
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- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
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- Vorobyev A
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- Vuosalo C
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- Wehrli L
- Weiler T
- Weinberg M
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- Wickramage N
- Widl E
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- Williams G
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- Winer BL
- 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
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
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- Zhukov V
- Zhukova V
- 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
- âŠ