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Related papers: Final-state interaction in the process $e^{+}e^{-}…

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Electromagnetic form factors of hyperons ($\Lambda$, $\Sigma$, $\Xi$) in the timelike region, accessible in the reaction $e^+e^- \to \bar YY$, are studied. The focus is on energies close to the reaction thresholds, where the properties of…

Nuclear Theory · Physics 2021-02-03 Johann Haidenbauer , Ulf-G. Meißner , Ling-Yun Dai

Motivated by recent BESIII measurements of the $\Lambda p \to \Lambda p$ and $\bar{\Lambda} p \to \bar{\Lambda} p$ scattering processes, we investigate these reactions within the framework of the quasipotential Bethe-Salpeter equation using…

High Energy Physics - Phenomenology · Physics 2025-07-25 Yaning Chen , Jun He

Measurements of hadronic final states in $e^{+}e^{-}$ collisions at centre-of-mass (CM) energies below the Z peak can notably extend the FCC-ee physics reach in terms of precision quantum chromodynamics (QCD) studies. Hadronic final states…

High Energy Physics - Experiment · Physics 2026-04-01 David d'Enterria , Pier Francesco Monni , Peter Skands , Andrii Verbytskyi

Multiple phases occurring in a Bose gas with finite-range interaction are investigated. In the vicinity of the onset of Bose-Einstein condensation (BEC) the chemical potential and the pressure show a van-der-Waals like behavior indicating a…

Quantum Gases · Physics 2013-05-24 M. Männel , K. Morawetz , P. Lipavský

The contribution of rescattering to final state interactions in the (e,e'p) cross section is studied using a semiclassical model. This approach considers a two-step process with the propagation of an intermediate nucleon and uses Glauber…

Nuclear Theory · Physics 2007-05-23 C. Barbieri , L. Lapikas

A model of the DN interaction is presented which is developed in close analogy to the meson-exchange KbarN potential of the Juelich group utilizing SU(4) symmetry constraints. The main ingredients of the interaction are provided by vector…

Nuclear Theory · Physics 2011-07-26 J. Haidenbauer , G. Krein , Ulf-G. Meißner , L. Tolos

The effects of isotopic invariance violation in the processes $e^{+}e^{-}\to B\bar{B}$, $e^{+}e^{-}\to B^{*}\bar{B}$, and $e^{+}e^{-}\to B^{*}\bar{B}^{*}$ are considered in the energy range between the thresholds of $B^{+}B^{-}$ and…

High Energy Physics - Phenomenology · Physics 2026-02-10 S. G. Salnikov , A. I. Milstein

A procedure is proposed which accounts for final state interaction corrections for near threshold meson production in nucleon-nucleon scattering. In analogy with the Watson-Migdal approximation, it is shown that in the limit of extremely…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Moalem , L. Razdolskaja , E. Gedalin

We outline a relativistic and unfactorized framework to treat the final-state interactions in quasi-elastic A(e,e'p) reactions for four-momentum transfers Q$^{2} \gtrsim 0.3$ (GeV/c)$^{2}$. The model, which relies on the eikonal…

Nuclear Theory · Physics 2009-11-07 D. Debruyne , J. Ryckebusch , S. Janssen , T. Van Cauteren

It is notoriously difficult to make quantitative theoretical predictions of the superconducting $T_c$, either from first-principles or even from a knowledge of normal state properties. Ultimately, this reflects the fact that the energy…

Superconductivity · Physics 2019-01-15 I. Esterlis , S. A. Kivelson , D. J. Scalapino

I examine the role of final state interactions in cold nuclear matter in modifying hadron production on nuclear targets with leptonic or hadronic beams. I demonstrate the extent to which available experimental data in electron-nucleus…

Nuclear Theory · Physics 2008-11-26 Alberto Accardi

Motivated by the large cross section of $e^+e^-\to \eta J/\psi$ process measured by the BESIII and Belle Collaborations recently, we evaluate this process at $\mathcal{O}(\alpha_s^4)$ accuracy in the framework of nonrelativistic QCD. We…

High Energy Physics - Phenomenology · Physics 2015-06-19 Cong-Feng Qiao , Rui-Lin Zhu

We report measurements of production cross sections for $\rho^+$, $\rho^0$, $\omega$, $K^{*+}$, $K^{*0}$, $\phi$, $\eta$, $K_S^0$, $f_0(980)$, $D^+$, $D^0$, $D_s^+$, $D^{*+}$, $D^{*0}$, and $D^{*+}_s$ in $e^+e^-$ collisions at a…

High Energy Physics - Experiment · Physics 2025-03-14 Belle Collaboration , R. Seidl , I. Adachi , H. Aihara , T. Aushev , R. Ayad , Sw. Banerjee , K. Belous , J. Bennett , M. Bessner , B. Bhuyan , D. Biswas , D. Bodrov , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , K. Chilikin , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , S. Das , G. De Nardo , G. De Pietro , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , D. Dossett , P. Ecker , T. Ferber , B. G. Fulsom , V. Gaur , A. Giri , P. Goldenzweig , E. Graziani , Y. Guan , K. Gudkova , C. Hadjivasiliou , T. Hara , H. Hayashii , D. Herrmann , W. -S. Hou , C. -L. Hsu , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , S. Jia , Y. Jin , K. K. Joo , A. B. Kaliyar , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , P. Kodyš , A. Korobov , S. Korpar , P. Križan , P. Krokovny , D. Kumar , K. Kumara , Y. -J. Kwon , T. Lam , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , D. Liventsev , Y. Ma , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , K. Miyabayashi , R. Mussa , M. Nakao , A. Natochii , M. Niiyama , S. Nishida , S. Ogawa , H. Ono , G. Pakhlova , S. Pardi , J. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , G. Russo , S. Sandilya , L. Santelj , V. Savinov , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , W. Shan , J. -G. Shiu , B. Shwartz , J. B. Singh , E. Solovieva , M. Starič , M. Sumihama , M. Takizawa , K. Tanida , F. Tenchini , T. Uglov , Y. Unno , S. Uno , Y. Usov , C. Van Hulse , A. Vinokurova , A. Vossen , M. -Z. Wang , B. D. Yabsley , W. Yan , Y. Yook , C. Z. Yuan , L. Yuan , Z. P. Zhang , V. Zhilich

The effects of meson-exchange currents (MEC) are computed for the one-particle one-hole transverse response function for finite nuclei at high momentum transfers $q$ in the region of the quasielastic peak. A semi-relativistic shell model is…

Nuclear Theory · Physics 2010-04-06 J. E. Amaro , M. B. Barbaro , J. A. Caballero , T. W. Donnelly , C. Maieron , J. M. Udias

The associative charm particles production in nucleon-nucleon collisions $N+N\to \Lambda_c(\Sigma_c)+\bar{D}+N$, is described in a general way and the spin and isospin structure of the corresponding matrix elements are derived. Using an…

Nuclear Theory · Physics 2007-05-23 Michail P. Rekalo Egle Tomasi-Gustafsson

We consider a system of two-dimensional electrons strongly localized by disorder. Interactions create a gap in the average tunneling density of states $\nu(E)$ at energies, E, close to the Fermi level. We derive a system of self-consistent…

Mesoscale and Nanoscale Physics · Physics 2009-10-31 Ya. M. Blanter , M. E. Raikh

In this review we give a perspective of the theoretical work done recently on the interpretation of results from $B$, $D$, $\Lambda_b$, $\Lambda_c$ weak decays into final states that contain interacting hadrons, and how it is possible to…

We study the effect of final state interactions at the threshold of Higgs boson pair production in the Glashow-Weinberg-Salam model. We consider three major processes of the pair production in the model: lepton pair annihilation, ZZ fusion,…

High Energy Physics - Phenomenology · Physics 2015-10-28 Zhentao Zhang

The missing mass spectrum measured in high resolution studies of the reaction pp -> K^+X is analyzed with respect to the strong final state interaction near the Lambda p production threshold. The observed spectrum can be described by…

Nuclear Experiment · Physics 2009-11-10 F. Hinterberger , A. Sibirtsev