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Related papers: Inclusive Charm Production in Upsilon(nS) Decay

200 papers

We review the NLL QCD calculations for the branching ratio of B -> X_s gamma in the SM. In particular, we emphasize the problem related to the definition of the charm quark mass which leads to a rather large uncertainty of the NLL…

High Energy Physics - Phenomenology · Physics 2014-11-17 Kay Bieri , Christoph Greub

In recent studies of inclusive $B$ decays, it has been suggested that either $B$ mesons decay much more copiously to final states with no open charm than currently assumed, or $B(D^0 \to K^-\pi^+)$ has to be reduced significantly. This note…

High Energy Physics - Phenomenology · Physics 2015-06-25 Isard Dunietz , Joseph Incandela , Frederick Snider , Hitoshi Yamamoto

We apply perturbative QCD factorization theorems to inclusive heavy hadron decays, and obtain simultaneously a low semileptonic branching ratio $B(B\to Xl\bar{\nu})=10.16%$, the average charm yield $<n_c>=1.17$ per $B$ decay, a small…

High Energy Physics - Phenomenology · Physics 2009-10-31 We-Fu Chang , Hsiang-nan Li , Hoi-Lai Yu

Using Upsilon(2S) and Upsilon(3S) data collected with the CLEO III detector we have searched for decays of chi_bJ to final states with open charm. We fully reconstruct D0 mesons with p_D0 > 2.5 GeV/c in three decay modes (K-pi+, K-pi+pi0,…

High Energy Physics - Experiment · Physics 2010-04-08 CLEO Collaboration , R. A. Briere

Based on an a high statistics e+e- -> ccbar data sample, we report on the inclusive rate for charmed baryons to decay into / particles using charm-event tagging. We select e+e- -> ccbar events which have a clear anti-charm tag and measure…

High Energy Physics - Experiment · Physics 2010-04-08 R. Ammar

We calculate differential energy spectra ($x_F$-distributions) of charmed particles produced in proton-nucleus collisions, assuming the existence of intrinsic heavy quark components in the proton wave function. For the calculation, the…

High Energy Physics - Phenomenology · Physics 2015-03-13 E. V. Bugaev , P. A. Klimai

The cross section for inclusive charm production by a low-energy antiproton beam is calculated using the parton model and next-to-leading order perturbative QCD. For an antiproton beam with a momentum of 15 GeV, the charm cross section at…

High Energy Physics - Phenomenology · Physics 2009-06-30 E. Braaten , P. Artoisenet

We propose a novel method of measuring the CKM matrix element V_ub, via inclusive B decays to "wrong sign" charm. This process is mediated by the quark level decay b -> u cbar s'. When normalized to the inclusive semileptonic decay rate,…

High Energy Physics - Phenomenology · Physics 2011-01-25 Adam F. Falk , Alexey A. Petrov

The effects of the finite charm quark mass on bottom quark mass determinations from $\Upsilon$ sum rules are examined in detail. The charm quark mass effects are calculated at next-to-next-to-leading order in the non-relativistic power…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. H. Hoang

We present the results of a calculation of the intrinsic charm quark contribution to $J/\psi$ plus open charm associated production at large transverse momentum in hadron collisions at high energies. It is shown that the value of the cross…

High Energy Physics - Phenomenology · Physics 2009-10-28 A. P Martynenko , V. A. Saleev

We discuss the impact of the charm quark mass in the CTEQ NNLO global analysis of parton distribution functions of the proton. The $\bar{\rm MS}$ mass $m_c(m_c)$ of the charm quark is extracted in the S-ACOT-$\chi$ heavy-quark factorization…

High Energy Physics - Phenomenology · Physics 2013-07-01 Jun Gao , Marco Guzzi , Pavel M. Nadolsky

We address the nonperturbative effects associated with soft charm quarks in inclusive B decays. Such corrections are allowed by the OPE, but have largely escaped attention so far. The related four-quark `double heavy' expectation values of…

High Energy Physics - Phenomenology · Physics 2008-11-26 I. I. Bigi , N. Uraltsev , R. Zwicky

Inclusive $\chi_{cJ}$ $(J=0,1,2)$ production from $\Upsilon(1S)$ decay is studied within the framework of nonrelativistic QCD (NRQCD) factorization at leading order in $v_Q^2$, which includes the contributions of $b\bar{b}({}^3S_1^{[1]})\to…

High Energy Physics - Phenomenology · Physics 2018-11-14 Zhi-Guo He , Bernd A. Kniehl , Xiang-Peng Wang

We present measurements of the inclusive semileptonic branching fractions of charged and neutral B mesons using 20.6 fb-1 of data measured at the Upsilon(4S) with the BABAR detector. Events are tagged with a fully reconstructed hadronic…

High Energy Physics - Experiment · Physics 2019-08-14 Urs Langenegger

We present a preliminary determination of the CKM matrix element |Vub| based on the analysis of semileptonic B decays from a sample of 88 million Upsilon(4S) decays collected with the BaBar detector at the e+e- storage ring. Charmless…

High Energy Physics - Experiment · Physics 2007-05-23 B. Aubert , The BaBar Collaboration

Our analysis suggests that the charmless yield in B decays is enhanced over traditional estimates. The c c.bar pair produced in b to c c.bar transitions may be seen significantly as light hadrons due to non-perturbative effects. Existing…

High Energy Physics - Phenomenology · Physics 2016-11-03 Isard Dunietz

The ${\Upsilon}(nS)$ ${\to}$ $B_{c}^{\ast}D$ weak decays ($n$ $=$ $1$, $2$, $3$) are investigated with perturbative QCD approach. It is found that the CKM-favored ${\Upsilon}(nS)$ ${\to}$ $B_{c}^{\ast}D_{s}$ decays have branching ratio of…

High Energy Physics - Phenomenology · Physics 2017-09-19 Yueling Yang , Junfeng Sun , Jinshu Huang , Haiyan Li , Gongru Lu , Qin Chang

We determine the leading-order nonrelativistic quantum chromodynamics (NRQCD) matrix element < O_1 >_Upsilon and the ratio < q^2>_Upsilon, for Upsilon=Upsilon(nS) with n=1, 2, and 3 by comparing the measured values for Gamma[Upsilon -> e^+…

High Energy Physics - Phenomenology · Physics 2011-02-16 Hee Sok Chung , Jungil Lee , Chaehyun Yu

We estimate the intrinsic charm contributions to the quark flavor and spin observables of the nucleon in the SU(4) quark meson fluctuation model. In this model, the charm or anticharm reside in the charmed mesons created by the…

High Energy Physics - Phenomenology · Physics 2009-11-07 Xiaotong Song

Using the next-to-leading order QCD-corrected effective Hamiltonian, charmless exclusive nonleptonic decays of the $B_s$ meson into $\eta$ or $\eta'$ are calculated within the generalized factorization approach. Nonfactorizable…

High Energy Physics - Phenomenology · Physics 2009-10-31 B. Tseng