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We propose a new algorithm for the identification of the production flavor of neutral $D$ mesons in the Belle II experiment. The algorithm exploits the correlation between the flavor of a reconstructed neutral $D$ meson (signal $D$ meson)…

High Energy Physics - Experiment · Physics 2023-07-03 Belle II Collaboration , I. Adachi , L. Aggarwal , H. Ahmed , H. Aihara , N. Akopov , A. Aloisio , N. Anh Ky , D. M. Asner , H. Atmacan , T. Aushev , V. Aushev , M. Aversano , V. Babu , H. Bae , S. Bahinipati , P. Bambade , Sw. Banerjee , M. Barrett , J. Baudot , M. Bauer , A. Baur , A. Beaubien , J. Becker , P. K. Behera , J. V. Bennett , F. U. Bernlochner , V. Bertacchi , M. Bertemes , E. Bertholet , M. Bessner , S. Bettarini , B. Bhuyan , F. Bianchi , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , A. Bolz , A. Bondar , J. Borah , A. Bozek , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , S. Bussino , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , J. Cerasoli , M. -C. Chang , P. Chang , R. Cheaib , P. Cheema , V. Chekelian , B. G. Cheon , K. Chilikin , K. Chirapatpimol , H. -E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , S. Choudhury , L. Corona , L. M. Cremaldi , S. Das , F. Dattola , E. De La Cruz-Burelo , S. A. De La Motte , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , M. Destefanis , A. De Yta-Hernandez , R. Dhamija , A. Di Canto , F. Di Capua , J. Dingfelder , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , M. Dorigo , K. Dort , S. Dreyer , S. Dubey , G. Dujany , P. Ecker , M. Eliachevitch , P. Feichtinger , T. Ferber , D. Ferlewicz , T. Fillinger , C. Finck , G. Finocchiaro , A. Fodor , F. Forti , A. Frey , B. G. Fulsom , A. Gabrielli , E. Ganiev , M. Garcia-Hernandez , G. Gaudino , V. Gaur , A. Gaz , A. Gellrich , G. Ghevondyan , D. Ghosh , G. Giakoustidis , R. Giordano , A. Giri , B. Gobbo , R. Godang , P. Goldenzweig , W. Gradl , T. Grammatico , S. Granderath , E. Graziani , D. Greenwald , Z. Gruberová , T. Gu , Y. Guan , K. Gudkova , S. Halder , Y. Han , T. Hara , K. Hayasaka , H. Hayashii , S. Hazra , C. Hearty , M. T. Hedges , I. Heredia de la Cruz , M. Hernández Villanueva , A. Hershenhorn , T. Higuchi , E. C. Hill , M. Hoek , M. Hohmann , C. -L. Hsu , T. Iijima , K. Inami , G. Inguglia , N. Ipsita , A. Ishikawa , S. Ito , R. Itoh , M. Iwasaki , P. Jackson , W. W. Jacobs , D. E. Jaffe , E. -J. Jang , Q. P. Ji , S. Jia , Y. Jin , A. Johnson , K. K. Joo , H. Junkerkalefeld , H. Kakuno , A. B. Kaliyar , J. Kandra , K. H. Kang , S. Kang , G. Karyan , T. Kawasaki , F. Keil , C. Ketter , C. Kiesling , C. -H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Koga , S. Kohani , A. Korobov , S. Korpar , E. Kovalenko , R. Kowalewski , T. M. G. Kraetzschmar , P. Križan , P. Krokovny , M. Kumar , K. Kumara , T. Kunigo , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , Y. -T. Lai , T. Lam , J. S. Lange , M. Laurenza , K. Lautenbach , R. Leboucher , F. R. Le Diberder , P. Leitl , D. Levit , C. Li , L. K. Li , J. Libby , Q. Y. Liu , Z. Q. Liu , S. Longo , A. Lozar , T. Lueck , C. Lyu , Y. Ma , M. Maggiora , R. Maiti , S. Maity , G. Mancinelli , R. Manfredi , E. Manoni , A. C. Manthei , M. Mantovano , D. Marcantonio , S. Marcello , C. Marinas , L. Martel , C. Martellini , A. Martini , T. Martinov , L. Massaccesi , M. Masuda , D. Matvienko , S. K. Maurya , J. A. McKenna , R. Mehta , F. Meier , M. Merola , F. Metzner , M. Milesi , C. Miller , M. Mirra , K. Miyabayashi , R. Mizuk , G. B. Mohanty , N. Molina-Gonzalez , S. Mondal , S. Moneta , H. -G. Moser , R. Mussa , I. Nakamura , Y. Nakazawa , A. Narimani Charan , M. Naruki , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , G. Nazaryan , M. Niiyama , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , Y. Onuki , P. Oskin , E. R. Oxford , P. Pakhlov , G. Pakhlova , A. Paladino , A. Panta , E. Paoloni , S. Pardi , K. Parham , H. Park , S. -H. Park , B. Paschen , S. Patra , S. Paul , T. K. Pedlar , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , P. L. M. Podesta-Lerma , T. Podobnik , S. Pokharel , L. Polat , C. Praz , S. Prell , E. Prencipe , M. T. Prim , H. Purwar , N. Rad , P. Rados , G. Raeuber , S. Raiz , M. Reif , S. Reiter , I. Ripp-Baudot , G. Rizzo , L. B. Rizzuto , S. H. Robertson , M. Roehrken , J. M. Roney , A. Rostomyan , N. Rout , D. A. Sanders , S. Sandilya , A. Sangal , L. Santelj , Y. Sato , V. Savinov , B. Scavino , M. Schnepf , C. Schwanda , Y. Seino , A. Selce , K. Senyo , J. Serrano , M. E. Sevior , C. Sfienti , W. Shan , C. Sharma , X. D. Shi , T. Shillington , J. -G. Shiu , D. Shtol , A. Sibidanov , F. Simon , J. B. Singh , J. Skorupa , R. J. Sobie , M. Sobotzik , A. Soffer , A. Sokolov , E. Solovieva , S. Spataro , B. Spruck , M. Starič , S. Stefkova , Z. S. Stottler , R. Stroili , M. Sumihama , W. Sutcliffe , H. Svidras , M. Takahashi , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , A. Thaller , O. Tittel , R. Tiwary , D. Tonelli , E. Torassa , K. Trabelsi , I. Tsaklidis , M. Uchida , I. Ueda , T. Uglov , K. Unger , Y. Unno , K. Uno , S. Uno , P. Urquijo , Y. Ushiroda , S. E. Vahsen , R. van Tonder , G. S. Varner , K. E. Varvell , A. Vinokurova , V. S. Vismaya , L. Vitale , V. Vobbilisetti , B. Wach , M. Wakai , H. M. Wakeling , S. Wallner , E. Wang , M. -Z. Wang , X. L. Wang , Z. Wang , A. Warburton , M. Watanabe , S. Watanuki , M. Welsch , C. Wessel , E. Won , X. P. Xu , B. D. Yabsley , S. Yamada , W. Yan , S. B. Yang , J. H. Yin , Y. M. Yook , K. Yoshihara , C. Z. Yuan , Y. Yusa , L. Zani , V. Zhilich , J. S. Zhou , Q. D. Zhou , V. I. Zhukova

We use a recently completed O(alpha_s^2) fixed-order calculation of the heavy-flavour production cross section in e+e- collisions to compute the heavy-quark fragmentation function. We fit the result of our calculation, convoluted with a…

High Energy Physics - Phenomenology · Physics 2009-10-31 Paolo Nason , Carlo Oleari

We report recent experimental and theoretical progress concerning the heavy-quark electro-production in the context of the ABM11 parton distribution function (PDF) fit. In the updated ABM11 analysis, including the recent combined HERA charm…

High Energy Physics - Phenomenology · Physics 2013-07-30 S. Alekhin , J. Blümlein , S. Moch

Nonperturbative effects in $D$-meson production in pion-nucleon and proton-nucleon collisions are investigated within the recombination model. The coalescence of perturbatively created charm quarks with sea- and valence-quarks from…

High Energy Physics - Phenomenology · Physics 2009-11-10 R. Rapp , E. V. Shuryak

Recent experiments at Fermilab and CERN have observed a strong asymmetry between the hadroproduction cross sections of leading $D$ mesons, containing projectile valence quarks, and nonleading charmed mesons, without projectile valence…

High Energy Physics - Phenomenology · Physics 2009-09-25 R. Vogt , S. J. Brodsky

Fragmentation functions are one of the key components of the factorisation theorem used to calculate heavy-flavour hadron production cross sections. The non-perturbative nature of fragmentation functions necessitates that they are…

High Energy Physics - Experiment · Physics 2023-10-24 Antonio Palasciano

After the completion of data taking at HERA-2, a large data set is at hand to study the photoproduction of charm and beauty quarks in ep collisions. New measurements of charm production based on D^* meson tagging and beauty production based…

High Energy Physics - Experiment · Physics 2019-08-14 Benno List

Fragmentation functions for D mesons, based on the convolution of a perturbative part, related to the heavy quark perturbative showering, and a non-perturbative model for its hadronization into the meson, are used to describe D^* production…

High Energy Physics - Phenomenology · Physics 2014-11-17 Matteo Cacciari , Mario Greco

The observed $D^{**}$ mesons have $c\bar q$ flavor quantum numbers and spin-parity of the light degrees of freedom $s_\ell^{\pi_{\ell}} = 3/2^+$. In the $m_c \rightarrow \infty$ limit the spin of the charm quark is conserved and the $c…

High Energy Physics - Phenomenology · Physics 2009-10-28 Yu-Qi Chen , Mark B. Wise

Using 13.6/fb of continuum two-jet e+e- -> ccbar events collected with the CLEO detector, we have searched for baryon number correlations at the primary quark level. We have measured the likelihood for a /\c+ charmed baryon to be produced…

High Energy Physics - Experiment · Physics 2010-04-08 A. Bornheim

Leading charm hadrons produced in hadron-nucleus interactions cannot be adequately described within the parton fusion model. Recent results on charm baryon production in $\Sigma^- A$ interactions at 330 GeV with the WA89 detector disagree…

High Energy Physics - Phenomenology · Physics 2014-11-17 T. Gutierrez , R. Vogt

The experimental data of BELLE Collaboration on the exclusive charmed meson pair production in the process of monophotonic $e^+e^-$-annihilation ($e^+e^-\to \gamma^* \to D\bar D$) has been studied. It has been shown that these data is…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. V. Berezhnoy , A. K. Likhoded

The C-parameter event-shape distribution for e+e- annihilation into hadrons is computed in the framework of SCET including input from fixed-order perturbation theory. We calculate all missing ingredients for achieving N3LL resummation…

High Energy Physics - Phenomenology · Physics 2016-02-17 Andre H. Hoang , Daniel W. Kolodrubetz , Vicent Mateu , Iain W. Stewart

We examine the production of open charm in antiproton annihilation on finite nuclei. The enhancement of the subthreshold production cross section, even in a nucleus as light as carbon, should provide a clean signature of the reduction in…

Nuclear Theory · Physics 2010-02-17 A. Sibirtsev , K. Tsushima , A. W. Thomas

A perturbative QCD calculation of heavy flavor quark fragmentation into heavy flavor baryons is developed along the lines of corresponding heavy meson models. The non-perturbative formation of the baryon is accomplished by implementing the…

High Energy Physics - Phenomenology · Physics 2009-10-30 Anatoly D. Adamov , Gary R. Goldstein

Within the framework of nonrelativistic QCD (NRQCD), we calculate the fragmentation function for a charm quark into an $S$-wave fully-charmed tetraquark, denoted as $T_{4c}$. The charm-to-$T_{4c}$ fragmentation function is expressed as a…

High Energy Physics - Phenomenology · Physics 2024-09-04 Xiao-Wei Bai , Feng Feng , Chang-Man Gan , Yingsheng Huang , Wen-Long Sang , Hong-Fei Zhang

A selection of topics on open heavy quark production at HERA are reviewed here. Measurements of charm fragmentation parameters will be presented together with developments in the study of D* di-jet angular distributions. Charm production in…

High Energy Physics - Experiment · Physics 2007-05-23 Andrea Longhin

The coefficient functions for heavy-flavour production in deeply inelastic electron-hadron scattering have been calculated previously. Analytic expressions are impossible to publish due to their length. Therefore we have tabulated them as…

High Energy Physics - Phenomenology · Physics 2011-07-19 S. Riemersma , J. Smith , W. L. van Neerven

e present measurements on $D^0$ meson production via direct reconstruction of its hadronic decay channel $D^0\to K\pi$ in minimum bias $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV with $p_T$ up to $\sim$3 GeV/$c$. Non-photonic…

Nuclear Experiment · Physics 2009-11-11 Haibin Zhang

Using e+e- collision data in the sqrt{s} = 4 GeV energy region, CLEO-c has made extensive studies of semileptonic and leptonic decays of the D0, D+, and Ds+ charmed mesons. We report recent measurements of absolute branching fractions, form…

High Energy Physics - Experiment · Physics 2019-08-13 Werner M. Sun
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