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Dimuon production in neutrino-nucleus collisions, an important constraint of strangeness in global parton distribution function analyses, is typically calculated by assuming it to be proportional to inclusive charm production. This approach…

High Energy Physics - Phenomenology · Physics 2025-11-04 Ilkka Helenius , Hannu Paukkunen , Sami Yrjänheikki

The production rates of D*+-, Ds*+-, D+-, D0 / D0bar, Ds+, and Lambda_c in Z to ccbar decays are measured using the LEP I data sample recorded by the ALEPH detector. The fractional energy spectrum of the D*+- is well described as the sum of…

High Energy Physics - Experiment · Physics 2012-08-27 ALEPH Collaboration

It is well known that large nonfragmentational contributions to inclusive production of charmed particles appear at low energies. In the case of charm production in $B$-meson decays these contributions arise from the participation of the…

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

We calculate the transverse-momentum (p_T) distribution for the inclusive hadroproduction of B mesons at intermediate values of p_T at next-to-leading order (NLO) in a dedicated finite-mass scheme using realistic non-perturbative…

High Energy Physics - Phenomenology · Physics 2008-11-26 B. A. Kniehl , G. Kramer , I. Schienbein , H. Spiesberger

Chiral thermodynamics of charmed mesons is formulated at finite temperature within a $2+1+1$-flavored effective Lagrangian incorporating heavy quark symmetry. The charmed-meson mean fields act as an extra source which breaks the chiral…

High Energy Physics - Phenomenology · Physics 2015-06-22 Chihiro Sasaki

The production of D^*+, D^0, D^+, D_s^+ and Lambda_c^+ charm hadrons and their antiparticles in ep scattering at HERA was measured with the ZEUS detector using an integrated luminosity of 79 pb^-1. The measurement has been performed in the…

High Energy Physics - Experiment · Physics 2012-08-27 ZEUS Collaboration

We present nonperturbative fragmentation functions (FFs) for bottom-flavored ($B$) hadrons both at next-to-leading (NLO) and, for the first time, at next-to-next-to-leading order (NNLO) in the $\overline{\mathrm{MS}}$ factorization scheme…

High Energy Physics - Phenomenology · Physics 2019-06-12 Maral Salajegheh , S. Mohammad Moosavi Nejad , Hamzeh Khanpour , Bernd A. Kniehl , Maryam Soleymaninia

We present a new model for the description of heavy-flavor hadronization in relativistic heavy-ion collisions. We explore its effect on the charmed hadron yields and kinematic distributions once the latter is applied at the end of transport…

High Energy Physics - Phenomenology · Physics 2023-03-22 Andrea Beraudo , Arturo De Pace , Daniel Pablos Alfonso , Francesco Prino , Marco Monteno , Marzia Nardi

We present hadron-level predictions from the Monte Carlo generator Cascade and numerical calculations of charm and beauty production at the Fermilab Tevatron within the framework of the $k_T$-factorization QCD approach. Our consideration is…

High Energy Physics - Phenomenology · Physics 2011-01-25 H. Jung , M. Kraemer , A. V. Lipatov , N. P. Zotov

Recent data for the masses of $D$ and $D^*$ mesons determined using methods of lattice QCD for several values of the charm quark mass different from its physical mass are analysed in Heavy Quark Effective Theory. Nonperturbative parameters…

High Energy Physics - Lattice · Physics 2024-05-24 Alexey Nefediev

The ALICE experiment will be able to detect hadrons containing charm and beauty quarks in proton-proton and heavy ion collisions in the new energy regime of the CERN Large Hadron Collider (LHC). Open charmed mesons are a powerful tool to…

Nuclear Experiment · Physics 2009-07-14 Renu Bala

The CLEO-c experiment at the CESR e+ e- storage ring has collected data with E_cm = 3.77 GeV and E_cm ~ 4.17 GeV to study the decays of charmed mesons. This paper discusses results on the hadronic branching fractions of the D0, D+, and Ds+.

High Energy Physics - Experiment · Physics 2019-08-14 Peter Onyisi

We improve upon previous explicit estimates of charm rescattering contributions to the decay $B^0\to K^0\bar{\ell}\ell$ by including contributions from dipole interactions with the intermediate charm-meson states, and by further…

High Energy Physics - Phenomenology · Physics 2025-11-07 Gino Isidori , Zachary Polonsky , Arianna Tinari

I review some recent results on hadronic decays of charmed mesons. These decays illuminate a wide range of physics, including the absolute normalizations of b and c decays, the understanding of D^0 mixing, the coupling of heavy mesons to…

High Energy Physics - Experiment · Physics 2008-10-21 P. U. E. Onyisi

The total decay widths of the charmed baryons are calculated by means of the $^3P_0$ model. Our calculations consider in the final states: the charmed baryon-(vector/pseudoscalar) meson pairs and the (octet/ decuplet)…

High Energy Physics - Phenomenology · Physics 2023-03-08 H. Garcia-Tecocoatzi , A. Giachino , J. Li , A. Ramirez-Morales , E. Santopinto

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

Recent $p_{\rm T}$-integrated cross section measurements of the ground-state charm mesons and baryons, D$^{\rm 0}$, D$^+$, D$_{\rm s}^{+}$, $\Lambda_{\rm c}^{+}$, and $\Xi_{\rm c}^0$, are used to evaluate the charm fragmentation fractions…

Nuclear Experiment · Physics 2022-02-07 ALICE Collaboration

Fragmentation of heavy quarks into heavy-flavoured hadrons receives both perturbative and non-perturbative contributions. We consider perturbative QCD corrections to heavy quark production in $e^+e^-$ collisions to next-to-next-to-leading…

High Energy Physics - Phenomenology · Physics 2024-06-12 Leonardo Bonino , Matteo Cacciari , Giovanni Stagnitto

The study of heavy-flavour mesons and baryons in hadronic collisions provides unique access to the properties of heavy-quark hadronisation in the presence of large partonic densities, where new mechanisms of hadron formation beyond…

High Energy Physics - Experiment · Physics 2023-12-18 Jianhui Zhu

Effects of final-state interactions in nonleptonic decays of charmed mesons are studied in the framework of quark-diagram approach. For the case of u-d-s flavour symmetry we discuss how the inelastic coupled-channel rescattering effects…

High Energy Physics - Phenomenology · Physics 2007-05-23 Piotr Zenczykowski
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