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Related papers: $\sigma(e^+e^-\to{hadrons})$ and the Heavy Quark M…

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We measure the cross section for e^+e^- -> \psi(3770) -> hadrons at Ecm=3773 MeV to be (6.38+-0.08^{+0.41}_{-0.30}) nb using the CLEO detector at the CESR e^+e^- collider. The difference between this and the e^+e^- -> \psi(3770) -> DD-bar…

High Energy Physics - Experiment · Physics 2010-04-15 D. Besson

We review lattice determinations of the charm and bottom quark masses and the strong coupling constant obtained by different methods. We explain how effective field theory approaches, such as Non-Relativistic QCD (NRQCD), potential…

High Energy Physics - Lattice · Physics 2020-07-15 Javad Komijani , Peter Petreczky , Johannes Heinrich Weber

We present the first direct determination of the running top-quark mass based on the total cross section of top-quark pair-production as measured at the Tevatron. Our theory prediction for the cross section includes various…

High Energy Physics - Phenomenology · Physics 2009-09-24 U. Langenfeld , S. Moch , P. Uwer

Using the CLEO III detector, we measure absolute cross sections for e+e- -> hadrons at seven center-of-mass energies between 6.964 and 10.538 GeV. R, the ratio of hadronic and muon pair production cross sections, is measured at these…

High Energy Physics - Experiment · Physics 2008-11-26 Sheldon Stone

We present an analysis of charm quark fragmentation at 10.6 GeV, based on a data sample of 103 fb collected by the Belle detector at the KEKB accelerator. We consider fragmentation into the main charmed hadron ground states, namely \DZ,…

High Energy Physics - Experiment · Physics 2008-11-26 R. Seuster

The production of beauty and charm quarks in ep interactions has been studied with the ZEUS detector at HERA for exchanged four-momentum squared 5 < Q^2 < 1000 GeV^2 using an integrated luminosity of 354 pb^{-1}. The beauty and charm…

High Energy Physics - Experiment · Physics 2014-10-22 ZEUS collaboration , H. Abramowicz , I. Abt , L. Adamczyk , M. Adamus , R. Aggarwal , S. Antonelli , O. Arslan , V. Aushev , Y. Aushev , O. Bachynska , A. N. Barakbaev , N. Bartosik , O. Behnke , J. Behr , U. Behrens , A. Bertolin , S. Bhadra , I. Bloch , V. Bokhonov , E. G. Boos , K. Borras , I. Brock , R. Brugnera , A. Bruni , B. Brzozowska , P. J. Bussey , A. Caldwell , M. Capua , C. D. Catterall , J. Chwastowski , J. Ciborowski , R. Ciesielski , A. M. Cooper-Sarkar , M. Corradi , F. Corriveau , G. D'Agostini , R. K. Dementiev , R. C. E. Devenish , G. Dolinska , V. Drugakov , S. Dusini , J. Ferrando , J. Figiel , B. Foster , G. Gach , A. Garfagnini , A. Geiser , A. Gizhko , L. K. Gladilin , O. Gogota , Yu. A. Golubkov , J. Grebenyuk , I. Gregor , G. Grzelak , O. Gueta , M. Guzik , W. Hain , G. Hartner , D. Hochman , R. Hori , Z. A. Ibrahim , Y. Iga , M. Ishitsuka , A. Iudin , F. Januschek , I. Kadenko , S. Kananov , T. Kanno , U. Karshon , M. Kaur , P. Kaur , L. A. Khein , D. Kisielewska , R. Klanner , U. Klein , N. Kondrashova , O. Kononenko , Ie. Korol , I. A. Korzhavina , A. Kotański , U. Kötz , N. Kovalchuk , H. Kowalski , O. Kuprash , M. Kuze , B. B. Levchenko , A. Levy , V. Libov , S. Limentani , M. Lisovyi , E. Lobodzinska , W. Lohmann , B. Löhr , E. Lohrmann , A. Longhin , D. Lontkovskyi , O. Yu. Lukina , J. Maeda , I. Makarenko , J. Malka , J. F. Martin , S. Mergelmeyer , F. Mohamad Idris , K. Mujkic , V. Myronenko , K. Nagano , A. Nigro , T. Nobe , D. Notz , R. J. Nowak , K. Olkiewicz , Yu. Onishchuk , E. Paul , W. Perlański , H. Perrey , N. S. Pokrovskiy , A. S. Proskuryakov , M. Przybycień , A. Raval , P. Roloff , I. Rubinsky , M. Ruspa , V. Samojlov , D. H. Saxon , M. Schioppa , W. B. Schmidke , U. Schneekloth , T. Schörner-Sadenius , J. Schwartz , L. M. Shcheglova , R. Shehzadi , R. Shevchenko , O. Shkola , I. Singh , I. O. Skillicorn , W. Słomiński , V. Sola , A. Solano , A. Spiridonov , L. Stanco , N. Stefaniuk , A. Stern , T. P. Stewart , P. Stopa , J. Sztuk-Dambietz , D. Szuba , J. Szuba , E. Tassi , T. Temiraliev , K. Tokushuku , J. Tomaszewska , A. Trofymov , V. Trusov , T. Tsurugai , M. Turcato , O. Turkot , T. Tymieniecka , A. Verbytskyi , O. Viazlo , R. Walczak , W. A. T. Wan Abdullah , K. Wichmann , M. Wing , G. Wolf , S. Yamada , Y. Yamazaki , N. Zakharchuk , A. F. Żarnecki , L. Zawiejski , O. Zenaiev , B. O. Zhautykov , N. Zhmak , D. S. Zotkin

We present preliminary results for the charm quark mass in the $N_f=4$ RGI scheme. These were obtained using $N_f=2+1$ CLS ensembles with $\mathcal{O}(a)$ non-perturbatively improved Wilson fermions. We employed five different lattice…

High Energy Physics - Lattice · Physics 2022-06-10 Gunnar Bali , Sjoerd Bouma , Sara Collins , Wolfgang Söldner

We compute two-loop corrections to the vector current matching coefficient involving two heavy quark masses. The result is applied to the computation of the $\Upsilon(1S)$ decay width into an electron or muon pair. We complement the…

High Energy Physics - Phenomenology · Physics 2021-10-04 Manuel Egner , Matteo Fael , Jan Piclum , Kay Schoenwald , Matthias Steinhauser

I outline the basic strategies for the computation of charm and bottom quark masses by means of lattice QCD, where particular emphasis is placed on the non-perturbative renormalization of the effective theory for the b-quark in heavy-light…

High Energy Physics - Lattice · Physics 2011-01-27 Jochen Heitger

By using QCD sum rules, the mass of the hidden charm tetraquark $[cu][\bar{c}\bar{d}]$ state with $I^{G} (J^{P}) = 1^+ (1^{+})$ (HCTV) is estimated, which presumably will turn out to be the newly observed charmonium-like resonance…

High Energy Physics - Phenomenology · Physics 2015-06-16 Cong-Feng Qiao , Liang Tang

Heavy-light meson system is investigated using the relativistic heavy quark action on the 2+1 dynamical flavor PACS-CS configurations at the lattice spacing $a^{-1}=2.2$ GeV and the spatial extent L=3 fm. Dynamical up-down and strange quark…

High Energy Physics - Lattice · Physics 2019-08-14 Y. Namekawa

A method for computing electromagnetic properties of hadrons in lattice QCD is described. The electromagnetic field is introduced dynamically, using a noncompact formulation. Employing enhanced electric charges, the dependence of the…

High Energy Physics - Lattice · Physics 2009-10-28 A. Duncan , E. Eichten , H. Thacker

In present work, we systematically calculate the mass spectra of open charm and bottom tetraquarks $q q\bar q \bar Q$ within an extended relativized quark model. The four-body relativized Hamiltonians including the Coulomb potential,…

High Energy Physics - Phenomenology · Physics 2020-11-04 Qi-Fang Lü , Dian-Yong Chen , Yu-Bing Dong

QCD inequalities are derived for the masses of mesons and baryons containing a single heavy quark using the heavy quark effective field theory. A rigorous lower bound is obtained for the $\bar\Lambda$ parameters of the heavy quark effective…

High Energy Physics - Phenomenology · Physics 2011-01-25 Zachary Guralnik , Aneesh V. Manohar

Using recent CLEO III results for the cross section for $e^+e^- \to {\rm hadrons}$ at seven centre-of-mass energies between 6.964 and 10.538 GeV, we derive a value for the strong coupling constant…

High Energy Physics - Phenomenology · Physics 2008-11-26 Johann H. Kuhn , Matthias Steinhauser , Thomas Teubner

We present preliminary results on the light, charmed and bottom baryon spectra using overlap valence quarks on the background of 2+1+1 flavours HISQ gauge configurations of the MILC collaboration. These calculations are performed on three…

High Energy Physics - Lattice · Physics 2018-04-18 Sourav Mondal , M. Padmanath , Nilmani Mathur

We have studied the determination of the running b-quark mass, $m_b(M_Z)$, using $Z^0$ decays into 3 or more hadronic jets. We calculated the ratio of $\geq3$-jet fractions in $e^+e^-\to b\bar{b}$ vs. $e^+e^-\to q_l\bar{q_l}$ ($q_l$ = u or…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Brandenburg , P. N. Burrows , D. Muller , N. Oishi , P. Uwer

Recent results from studies using half the perturbative mass of heavy quark-antiquark n=1, ${}^3S_1$ quarkonium as a new heavy quark mass definition for problems where the characteristic scale is smaller than or of the same order as the…

High Energy Physics - Phenomenology · Physics 2011-01-25 A. H. Hoang

The processes of D^{(*)}-mesons and \Lambda_c-baryons production in e^+e^--annihilation at 10.58 GeV and 91.18 GeV energies are concerned. At the 10.58 GeV energy the production of charmed particles via the B-mesons decays is also…

High Energy Physics - Phenomenology · Physics 2010-12-30 Alexey Novoselov

Recently the ALICE Collaboration has published a few data of charm hadrons in Pb + Pb collisions at the CERN Large Hadron Collider (LHC). We extend the quark combination to the charm sector and point out that the measurement of charm hadron…

High Energy Physics - Phenomenology · Physics 2015-03-05 Rui-qin Wang , Jun Song , Feng-lan Shao
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