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Abachi, S.; Abbott, B.; Abolins, M.; Acharya, B. S.; Адам, И.; Adams, T.; Adams, M. R.; Ahn, Shihyun; Aihara, H.; Álvarez, G.; Alves, G. A.; Amidi, E.; Amos, N.; Anderson, E. W.; Aronson, S. H.; Astur, R.; Avery, R. E.; Baden, A.; Balamurali, V.; Balderston, J.; Baldin, B.; Bantly, J.; Bartlett, J. F.; Bazizi, K.; Behnke, T.; Bendich, J.; Beri, S. B.; Bertram, I.; Bezzubov, V. A.; Bhat, P. C.; Bhatnagar, V.; Bhattacharjee, M.; Bischoff, A.; Biswas, N. N.; Blazey, G.; Blessing, S.; Boehnlein, A.; Bojko, N. I.; Borcherding, F.; Borders, J.; Boswell, C.; Brandt, A.; Brock, R.; Bross, A.; Buchholz, D.; Буртовой, В. С.; Butler, J. M.; Callot, O.; Casey, D.; Castilla‐Valdez, H.; Chakraborty, D.; Chang, S. M.; Chekulaev, S. V.; Chen, L. P.; Chen, W.; Chevalier, L.; Chopra, S.; Choudhary, B. C.; Christenson, J. H.; Chung, M.; Claes, D. R.; Clark, A. R.; Cobau, W. G.; Cochran, J.; Cooper, W. E.; Cretsinger, C.; Cullen-Vidal, D.; Cummings, M. A.C.; Cussonneau, J. P.; Ćutts, D.; Dahl, O. 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doi:10.1103/physrevlett.74.3548

Cited by 110 publications

(40 citation statements)

References 13 publications

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“…The observed shapes of distributions and correlations are reasonably well explained by perturbative QCD. However, the observed cross-sections at the Tevatron (Run I) are larger than QCD predictions [204][205][206][207][208][209][210][211] which is confirmed by Run II data. Similar effects are observed in γ p collisions at HERA [212][213][214][215][216][217][218] and in γ γ interactions at LEP [219,220].…”

Section: Inclusive B-quark Productionmentioning

confidence: 73%

CMS Physics Technical Design Report, Volume II: Physics Performance

Bayatian¹,

Chatrchyan²,

Hmayakyan³

et al. 2007

J. Phys. G: Nucl. Part. Phys.

715

161

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CMS is a general purpose experiment, designed to study the physics of pp collisions at 14 TeV at the Large Hadron Collider (LHC). It currently involves more than 2000 physicists from more than 150 institutes and 37 countries. The LHC will provide extraordinary opportunities for particle physics based on its unprecedented collision energy and luminosity when it begins operation in 2007.The principal aim of this report is to present the strategy of CMS to explore the rich physics programme offered by the LHC. This volume demonstrates the physics capability of the CMS experiment. The prime goals of CMS are to explore physics at the TeV scale and to study the mechanism of electroweak symmetry breaking-through the discovery of the Higgs particle or otherwise. To carry out this task, CMS must be prepared to search for new particles, such as the Higgs boson or supersymmetric partners of the Standard Model particles, from the start-up of the LHC since new physics at the TeV scale may manifest itself with modest data samples of the order of a few fb −1 or less. The analysis tools that have been developed are applied to study in great detail and with all the methodology of performing an analysis on CMS data specific benchmark processes upon which to gauge the performance of CMS. These processes cover several Higgs boson decay channels, the production and decay of new particles such as Z and supersymmetric particles, B s production and processes in heavy ion collisions. The simulation of these benchmark processes includes subtle effects such as possible detector miscalibration and misalignment. Besides these benchmark processes, the physics reach of CMS is studied for a large number of signatures arising in the Standard Model and also in theories beyond the Standard Model for integrated luminosities ranging from 1 fb −1 to 30 fb −1 . The Standard Model processes include QCD, B-physics, diffraction, detailed studies of the top quark properties, and electroweak physics topics such as the W and Z 0 boson properties. The production and decay of the Higgs particle is studied for many observable decays, and the precision with which the Higgs boson properties can be derived is determined. About ten different supersymmetry benchmark points are analysed using full simulation. The CMS discovery reach is evaluated in the SUSY parameter space covering a large variety of decay signatures.

show abstract

Section: Inclusive B-quark Productionmentioning

confidence: 73%

CMS Physics Technical Design Report, Volume II: Physics Performance

Bayatian¹,

Chatrchyan²,

Hmayakyan³

et al. 2007

J. Phys. G: Nucl. Part. Phys.

715

161

View full text Add to dashboard Cite

show abstract

“…The first measurements were performed more than two decades ago by the UA1 Collaboration at the CERN S " ppS collider [1] operating at a center-of-mass energy of ffiffiffi S p ¼ 0:63 TeV. More recent measurements were made by the CDF and D0 collaborations at the Fermilab Tevatron running at ffiffiffi S p ¼ 1:8 TeV [2,3] and 1.96 TeV [4]. Just recently, the CMS Collaboration at the CERN LHC collider published first results for inclusive B þ - [5], B 0 - [6], and B s -meson [7] production in pp collisions at ffiffiffi S p ¼ 7 TeV.…”

Section: Introductionmentioning

confidence: 99%

InclusiveB-meson production at the LHC in the general-mass variable-flavor-number scheme

et al. 2011

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We calculate the next-to-leading-order cross section for the inclusive production of B mesons in pp collisions in the general-mass variable-flavor-number scheme, an approach that takes into account the finite mass of the b quarks. We use realistic evolved nonperturbative fragmentation functions obtained from fits to e þ e À data and compare our results for the transverse-momentum and rapidity distributions at a center-of-mass energy of 7 TeV with recent data from the CMS Collaboration at the CERN LHC. We find good agreement, in particular, at large values of p T .

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“…At the CERN Sp" pS, the UA1 experiment measured beauty production via single muons (10 < p t < 40 GeV=c) at ffiffi ffi s p ¼ 630 GeV [13], while the UA2 experiment used single electrons (0:5 < p t < 2 GeV=c) to measure the charm production cross section [14]. At the Tevatron, both the CDF and D0 experiments measured beauty production via single electrons (7 < p t < 60 GeV=c) [15] and single muons (3:5 < p t < 60 GeV=c) [16], respectively.…”

Section: Introductionmentioning

confidence: 99%

Measurement of electrons from semileptonic heavy-flavor hadron decays inppcollisions ats=7 TeV

Abelev¹,

Adam²,

Adamová³

et al. 2012

Phys. Rev. D

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The differential production cross section of electrons from semileptonic heavy-flavor hadron decays has been measured at midrapidity (jyj < 0:5) in proton-proton collisions at ffiffi ffi s p ¼ 7 TeV with ALICE at the LHC. Electrons were measured in the transverse momentum range 0:5 < p t < 8 GeV=c. Predictions from a fixed-order perturbative QCD calculation with next-to-leading-log resummation agree with the data within the theoretical and experimental uncertainties.

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Inclusiveμandb-Quark Production Cross Sections inpp¯

Cited by 110 publications

References 13 publications

CMS Physics Technical Design Report, Volume II: Physics Performance

CMS Physics Technical Design Report, Volume II: Physics Performance

InclusiveB-meson production at the LHC in the general-mass variable-flavor-number scheme

Measurement of electrons from semileptonic heavy-flavor hadron decays inppcollisions ats=7 TeV

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