104 research outputs found
Measurement of D-s(+) and D-s(*+) production in B meson decays and from continuum e(+)e(-) annihilation at âs=10.6 GeV
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Andress JC
- Angelini C
- Anjomshoaa A
- Anthony PL
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- Azzopardi DE
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baird K
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Benayoun M
- Berger N
- Beringer J
- Bernard D
- Bernet R
- Best D
- Bettarini S
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom E
- Bloom P
- Blouw J
- Bona M
- Bondioli M
- Bonneaud GR
- Borean C
- Borgland AW
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandt T
- Brau B
- Brau J
- Breon AB
- Briand H
- Bright-Thomas PG
- Brigljevic V
- Brochard F
- Brose J
- Brown CM
- Brown D
- Brown DN
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Bulos F
- Burchat PR
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Cahn RN
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Carroll M
- Cartaro C
- Cavallo N
- Cavoto G
- Chao M
- Charles E
- Chauveau J
- Chen E
- Chen GP
- Chen JC
- Cheng CH
- Chevalier N
- Christ S
- Chun S
- Clark AR
- Clark PJ
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colberg T
- Colecchia F
- Contri R
- Convery MR
- Copty N
- Cottingham WN
- Coupal DP
- Cowan G
- Cowan R
- Coward DH
- Crawley HB
- Cremaldi L
- Crosetti G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dasu S
- Dauncey PD
- David P
- Davis CL
- De Groot N
- de la Vaissiere C
- de Lesquen A
- de Monchenault GH
- De Nardo G
- de Sangro R
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- Devmal S
- Di Lodovico F
- Dickopp M
- Dima MO
- Dittongo S
- Dixon P
- Dorfan DE
- Dorfan J
- Dorigo A
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- Dubois-Felsmann GP
- Dunwoodie W
- Dvoretskii A
- Dyce N
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
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- Eschenburg V
- Eschrich I
- Fabozzi F
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- Falbo M
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- Luitz S
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- Lynch HL
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- Smith AJS
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- Spanier SM
- Speziali V
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- Stark J
- Steinke M
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- Swain JE
- T'Jampens S
- Tanaka HA
- Taras P
- Taylor F
- Tehrani FS
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- Telnov VI
- Thiebaux C
- Thiessen D
- Tinslay J
- Tisserand V
- Toki WH
- Torassa E
- Tosi S
- Touramanis C
- Treadwell E
- Triggiani G
- Trincaz-Duvoid S
- Tumanov A
- Turnbull L
- Turri M
- Va'vra J
- Vaitsas G
- van Bibber K
- van Hoek WC
- Varnes EW
- Vasileiadis G
- Vasseur G
- Verderi M
- Verkerke W
- Versille S
- Vidal PB
- Voci C
- Voena C
- von Wimmersperg-Toeller JH
- Vuagnin G
- Wagner DL
- Wagner SR
- Wagoner DE
- Waldi R
- Walkowiak W
- Wallom D
- Walsh J
- Wang P
- Watson AT
- Watson NK
- Weatherall JH
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams MI
- Willocq S
- Wilson FF
- Wilson MG
- Wilson RJ
- Wisniewski WJ
- Witherell M
- Wormser G
- Wright DH
- Wright DM
- Wu SL
- Xella SM
- Xie Y
- Yamamoto RK
- Yang S
- Yeche C
- Yellin S
- Young CC
- Yu Z
- Yumiceva FX
- Yushkov AN
- Zacek V
- Zallo A
- Zhang J
- Zhu RY
- Zhu YS
- Zito M
- Publication venue
- American Physical Society
- Publication date
- 01/01/2002
- Field of study
This is the pre-print version of the Article. The official published version can be accessed from the links below. Copyright @ 2002 APSNew measurements of Ds+ and Ds*+ meson production rates from B decays and from qqÌ
continuum events near the ΄(4S) resonance are presented. Using 20.8 fb-1 of data on the ΄(4S) resonance and 2.6 fb-1 off-resonance, we find the inclusive branching fractions B(BâDs+X)=(10.93±0.19±0.58±2.73)% and B(BâDs*+X)=(7.9±0.8±0.7±2.0)%, where the first error is statistical, the second is systematic, and the third is due to the Ds+âÏÏ+ branching fraction uncertainty. The production cross sections Ï(e+e-âDs+X)ĂB(Ds+âÏÏ+)=7.55±0.20±0.34pb and Ï(e+e-âDs*±X)ĂB(Ds+âÏÏ+)=5.8±0.7±0.5pb are measured at center-of-mass energies about 40 MeV below the ΄(4S) mass. The branching fractions ÎŁB(BâDs(*)+D(*))=(5.07±0.14±0.30±1.27)% and ÎŁB(BâDs*+D(*))=(4.1±0.2±0.4±1.0)% are determined from the Ds(*)+ momentum spectra. The mass difference m(Ds+)-m(D+)=98.4±0.1±0.3MeV/c2 is also measured.This work was supported by DOE and NSF (USA), NSERC (Canada), IHEP (China), CEA and CNRS-IN2P3 (France), BMBF (Germany), INFN (Italy), NFR (Norway), MIST (Russia), and PPARC (United Kingdom). Individuals have received support from the Swiss NSF, A. P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
Evidence for the h_b(1P) meson in the decay Upsilon(3S) --> pi0 h_b(1P)
- Author
- Adametz A.
- Adye T.
- Ahmed H.
- Alam M. S.
- Albert J.
- Allen M. T.
- Alwyn K. E.
- Andreassen R.
- Angelini C.
- Anh TV
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- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini-Ferroli R.
- Band H. R.
- Banerjee Sw.
- Bard D. J.
- Barlow R. J.
- Bartoldus R.
- Batignani G.
- Behera P. K.
- Bellis M.
- Ben-Haim E.
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
- Bettarini S.
- Bettoni D.
- Bevan A. J.
- Bhuyan B.
- Bianchi F.
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- Biassoni P.
- Bingham I.
- Blinov V. E.
- Bloom P. C.
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- Castanheira MTD
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- Tartarelli GF
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- Temming KK
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- Yarritu A. K.
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- Zucchelli S.
- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Using a sample of 122 million Upsilon(3S) events recorded with the BaBar
detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we search for
the hbâ(1P) spin-singlet partner of the P-wave chi_{bJ}(1P) states in the
sequential decay Upsilon(3S) --> pi0 h_b(1P), h_b(1P) --> gamma eta_b(1S). We
observe an excess of events above background in the distribution of the recoil
mass against the pi0 at mass 9902 +/- 4(stat.) +/- 2(syst.) MeV/c^2. The width
of the observed signal is consistent with experimental resolution, and its
significance is 3.1sigma, including systematic uncertainties. We obtain the
value (4.3 +/- 1.1(stat.) +/- 0.9(syst.)) x 10^{-4} for the product branching
fraction BF(Upsilon(3S)-->pi0 h_b) x BF(h_b-->gamma eta_b).Comment: 8 pages, 4 postscript figures, submitted to Phys. Rev. D (Rapid
Communications
Measurement of the Ratio of b Quark Production Cross Sections in Antiproton-Proton Collisions at 630 GeV and 1800 GeV
- Author
- Acosta D
- Adam I
- Adye T
- Affolder T
- Ahsan A
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- Yumiceva FX
- Yun JC
- Yushkov AN
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- Zallo A
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- Zetti F
- Zhang J
- Zhu RY
- Zito M
- Zucchelli Stison TS
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2002
- Field of study
We report a measurement of the ratio of the bottom quark production cross
section in antiproton-proton collisions at 630 GeV to 1800 GeV using bottom
quarks with transverse momenta greater than 10.75 GeV identified through their
semileptonic decays and long lifetimes. The measured ratio
sigma(630)/sigma(1800) = 0.171 +/- .024 +/- .012 is in good agreement with
next-to-leading order (NLO) quantum chromodynamics (QCD)
Search for the X(5568) State Decaying into B-s(0)pi(+/-) in Proton-Proton Collisions at root s=8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
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- Acosta JG
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- Ălvarez FernĂĄndez A
- Publication venue
- Publication date
- 01/01/2017
- Field of study
A search for resonancelike structures in the B-s(0)pi(+/-) invariant mass spectrum is performed using proton-proton collision data collected by the CMS experiment at the LHC at root s = 8 TeV, corresponding to an integrated luminosity of 19.7 fb(-1). The B-s(0) mesons are reconstructed in the decay chain B-s(0) -> J/Psi phi, with J/Psi -> mu(+) mu(-) and phi -> K+K-. The B-s(0)pi(+/-) invariant mass distribution shows no statistically significant peaks for different selection requirements on the reconstructed B-s(0) and pi(+/-) candidates. Upper limits are set on the relative production rates of the X(5568) and B-s(0) states times the branching fraction of the decay X(5568)(+/-) -> B-s(0)pi(+/-). In addition, upper limits are obtained as a function of the mass and the natural width of possible exotic states decaying into B-s(0)pi(+/-).Peer reviewe
Measurement of inclusive very forward jet cross sections in proton-lead collisions at \sqrt{sNN} = 5:02 TeV
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- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
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- Yetkin EA
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yusli MN
- Zabel J
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zevi Della Porta G
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
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- Zhang Z
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- Zhaozhong S
- Zhiltsov V
- Zhokin A
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- Zhu RY
- Zhukov V
- Zientek M
- Zito G
- Zobec J
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
Measurements of differential cross sections for inclusive very forward jet production in proton-lead collisions as a function of jet energy are presented. The data were collected with the CMS experiment at the LHC in the laboratory pseudorapidity range â6.6 < η < â5.2. Asymmetric beam energies of 4 TeV for protons and 1.58 TeV per nucleon for Pb nuclei were used, corresponding to a center-of-mass energy per nucleon pair of \sqrt{sNN} = 5:02 TeV. Collisions with either the proton (p+Pb) or the ion (Pb+p) traveling towards the negative η hemisphere are studied. The jet cross sections are unfolded to stable-particle level cross sections with p_{T} âł 3 GeV, and compared to predictions from various Monte Carlo event generators. In addition, the cross section ratio of p+Pb and Pb+p data is presented. The results are discussed in terms of the saturation of gluon densities at low fractional parton momenta. None of the models under consideration describes all the data over the full jet-energy range and for all beam configurations. Discrepancies between the differential cross sections in data and model predictions of more than two orders of magnitude are observed
A rule-based model of insulin signalling pathway
- Author
- A Rowland
- A Sedaghat
- A Smith
- A Sonntag
- A Tsuchiya
- Azzurra Carlon
- B Camillo Di
- B Kholodenko
- Barbara Di Camillo
- BB Aldridge
- C BrÀnnmark
- C BrÀnnmark
- C Luni
- C Sawyers
- D Hu
- E Jacinto
- E Kwei
- E Nyman
- EY Skolnik
- F Tremblay
- F Xiao
- Federica Eduati
- G Cedersund
- Gianna Maria Toffolo
- H Kitano
- H Kitano
- J Copp
- J Faeder
- J Papin
- KD Copps
- L Pearce
- M Blinov
- M Freeman
- MI Stefan
- MK Morris
- MS Creamer
- N Borisov
- N NovĂšre Le
- P Dalle Pezze
- P Gual
- P Vinod
- R Chen
- R Zoncu
- RJ Orton
- S Hoops
- T Perumal
- U Bhalla
- V Danos
- V Danos
- V Villaamil
- VV Kiselyov
- W Hlavacek
- Y Zick
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of prompt Ï(2S) production cross sections in protonâlead and protonâproton collisions at âsNN = 5.02 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Acosta MV
- Adam W
- Adams MR
- Adams T
- Adzic R
- Agapitos A
- Agaras MN
- Aggleton R
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- Wu Z
- Wulsin HW
- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
- Xu Z
- Yagil A
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- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- You C
- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yuldashev BS
- Yumiceva F
- Yusli MN
- Zabel J
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhaozhong S
- Zhiltsov V
- Zhokin A
- Zhu DH
- Zhu RY
- Zhukov V
- Zientek M
- Zito G
- Zobec J
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 10/03/2019
- Field of study
Measurements of prompt Ï(2S) meson production cross sections in protonâlead (pPb) and protonâproton
(pp) collisions at a nucleonânucleon center-of-mass energy of âsNN = 5.02 TeV are reported. The results
are based on pPb and pp data collected by the CMS experiment at the LHC, corresponding to integrated
luminosities of 34.6 nbâ1 and 28.0 pbâ1, respectively. The nuclear modification factor RpPb is measured
for prompt Ï(2S) in the transverse momentum range 4 < pT < 30 GeV/c and the center-of-mass rapidity
range â2.4 < yCM < 1.93. The results on Ï(2S) RpPb are compared to the corresponding modification
factor for prompt J/Ï mesons. The results point to different nuclear effects at play in the production of
the excited charmonium state compared to the ground state, in the region of backward rapidity and for
pT < 10 GeV/c
Search for resonant ttÂŻ production in proton-proton collisions at sâ=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Ali MABM
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JDR
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asilar E
- Askew A
- Atakisi IO
- Atay S
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baffioni S
- Baginyan A
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Ball AH
- Ball F
- Ban Y
- Band R
- Banerjee S
- Banerjee S
- Bani L
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barker A
- Barnes VE
- Barney D
- Baron O
- Barone L
- Barria P
- Barrio Luna M
- Bartek R
- Barth C
- Bartok M
- Bartosik N
- Baselga M
- Baskakov A
- Bat A
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baur S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerra DAS
- Beck L
- Beernaert K
- Beghin D
- Behera PK
- Behnke O
- Behrens U
- Bein S
- Beirao Da Cruz E Silva C
- Belchior Batista Das Chagas E
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benussi L
- Benvenuti AC
- Beretvas A
- Bergauer T
- Berger P
- Beri SB
- Bernardes CA
- Bernet C
- Berry D
- Berryhill J
- Bertl W
- Bertsche D
- Besancon M
- Beschi A
- Betts RR
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- Wulsin HW
- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
- Xu Z
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yilmaz Y
- Yohay R
- Yonamine R
- Yoo HD
- Yoo J
- You C
- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yuldashev BS
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zhukov V
- Zientek M
- Zito G
- Zobec J
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 03/04/2019
- Field of study
A search for a heavy resonance decaying into a top quark and antiquark (ttÂŻ) pair is performed using proton-proton collisions at sâ=13 TeV. The search uses the data set collected with the CMS detector in 2016, which corresponds to an integrated luminosity of 35.9 fbâ1. The analysis considers three exclusive final states and uses reconstruction techniques that are optimized for top quarks with high Lorentz boosts, which requires the use of nonisolated leptons and jet substructure techniques. No significant excess of events relative to the expected yield from standard model processes is observed. Upper limits on the production cross section of heavy resonances decaying to a ttÂŻ pair are calculated. Limits are derived for a leptophobic topcolor ZâČ resonance with widths of 1, 10, and 30%, relative to the mass of the resonance, and exclude masses up to 3.80, 5.25, and 6.65 TeV, respectively. Kaluza-Klein excitations of the gluon in the Randall-Sundrum model are excluded up to 4.55 TeV. To date, these are the most stringent limits on ttÂŻ resonances
Measurement of the mass of the top quark in decays with a J/Ï meson in pp collisions at 8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
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- Akgun B
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- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- AldĂĄ JĂșnior WL
- Aleksandrov A
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- Ali MAB Md
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- Andrews MB
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- Carrillo Montoya CA
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
Search for lepton flavour violating decays of a neutral heavy Higgs boson to ÎŒÏ and eÏ in proton-proton collisions at sâ = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams MR
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- Adzic P
- Agapitos A
- Agarwal G
- Aggleton R
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- Ahmad A
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- Ahmad M
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- Ăzçelik Ă
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2020
- Field of study
A search for lepton flavour violating decays of a neutral non-standard-model Higgs boson in the ÎŒÏ and eÏ decay modes is presented. The search is based on proton-proton collisions at a center of mass energy sâ = 13 TeV collected with the CMS detector in 2016, corresponding to an integrated luminosity of 35.9 fbâ1. The Ï leptons are reconstructed in the leptonic and hadronic decay modes. No signal is observed in the mass range 200â900 GeV. At 95% confidence level, the observed (expected) upper limits on the production cross section multiplied by the branching fraction vary from 51.9 (57.4) fb to 1.6 (2.1) fb for the ÎŒÏ and from 94.1 (91.6) fb to 2.3 (2.3) fb for the eÏ decay modes
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