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Related papers: Multi-meson States in Lattice QCD

200 papers

Quantum Chromodynamics (QCD), the theory of strong interactions, in principle describes the interaction of quark and gluon fields. However, due to the self-coupling of the gluons, quarks and gluons are confined into hadrons and cannot exist…

High Energy Physics - Experiment · Physics 2019-08-13 Fabian Krinner

We analyse in detail the possibility of Bose-Einstein condensation of pions produced in heavy-ion collisions at the beam energy $\sqrt{s_{\rm NN}}$ = 2.76 TeV. Our approach is based on the chemical non-equilibrium thermal model of hadron…

Nuclear Theory · Physics 2015-05-27 Viktor Begun , Wojciech Florkowski

We study baryons of arbitrary isospin in a stringy holographic QCD model. In this D4-D8 holographic setting, the flavor symmetry is promoted to a gauge symmetry in the bulk, and produces, as KK modes of the gauge field, pions and spin one…

High Energy Physics - Theory · Physics 2010-02-03 Jaemo Park , Piljin Yi

We present a new method to evaluate with high precision the isospin breaking effects due to the mass difference between the up and down quarks using lattice QCD. Our proposal is applicable in principle to any hadronic observable which can…

The interplay of strong and weak decay amplitudes for B -> pion-pion-kaon and B -> kaon-antikaon-kaon, with the pion-pion and kaon-antikaon pairs interacting in isospin-0 S-wave, is analyzed for pion-pion effective mass from threshold to…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Loiseau , A. Furman , R. Kaminski , L. Lesniak

The isospin-2 pi pi system provides a useful testing ground for determining elastic hadron scattering parameters from finite-volume spectra obtained using lattice QCD computations. A reliable determination of the excited state spectrum of…

High Energy Physics - Phenomenology · Physics 2012-09-20 Jozef J. Dudek , Robert G. Edwards , Christopher E. Thomas

Recent data of lattice measurements of the gauge-invariant nonlocal scalar quark condensates are analyzed to extract the short--distance correlation length, 1/\lambda_q, and to construct an admissible Ansatz for the condensate behaviour in…

High Energy Physics - Phenomenology · Physics 2009-11-07 A. P. Bakulev , S. V. Mikhailov

We investigate the possible formation of a Bose-Einstein condensed phase of pions in the early Universe at nonvanishing values of lepton flavor asymmetries. A hadron resonance gas model with pion interactions, based on first-principle…

High Energy Physics - Phenomenology · Physics 2021-01-08 Volodymyr Vovchenko , Bastian B. Brandt , Francesca Cuteri , Gergely Endrődi , Fazlollah Hajkarim , Jürgen Schaffner-Bielich

Highly excited states for isospin 1/2 baryons are calculated for the first time using lattice QCD with two flavors of dynamical quarks. Anisotropic lattices are used with two pion masses: 416(36) MeV and 578(29) MeV. The lowest four…

We study multi-particle state contributions to the QCD two-point functions of pseudo-scalar quark bilinears in a finite spatial volume. For sufficiently small quark masses one expects three-meson states with two additional pions at rest to…

High Energy Physics - Lattice · Physics 2013-01-23 Oliver Bar , Maarten Golterman

The holographic Witten-Sakai-Sugimoto model is often employed to describe strongly-coupled baryonic and isospin-asymmetric matter, for example in the context of neutron stars. Here we consider the case of vanishing baryon chemical…

High Energy Physics - Phenomenology · Physics 2024-10-23 Nicolas Kovensky , Andreas Schmitt

In the first part of the talk, I review what we know (or rather do not know) about the structure of the QCD vacuum in the presence of strange quarks. Chiral perturbation theory allows to study reactions of pions and kaons and to further…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ulf-G. Meißner

We present a lattice-QCD calculation of the pion, kaon and $\eta_s$ distribution amplitudes using large-momentum effective theory (LaMET). Our calculation is carried out using three ensembles with 2+1+1 flavors of highly improved staggered…

High Energy Physics - Lattice · Physics 2020-12-30 Rui Zhang , Carson Honkala , Huey-Wen Lin , Jiunn-Wei Chen

The measurements of the Collins and Sivers asymmetries of identified hadrons produced in deep-inelastic scattering of 160 GeV/c muons on a transversely polarised 6LiD target at COMPASS are presented. The results for charged pions and…

High Energy Physics - Experiment · Physics 2011-11-03 The COMPASS Collaboration , M. Alekseev , V. Yu. Alexakhin , Yu. Alexandrov , G. D. Alexeev , A. Amoroso , A. Arbuzov , B. Badełek , F. Balestra , J. Ball , J. Barth , G. Baum , Y. Bedfer , C. Bernet , R. Bertini , M. Bettinelli , R. Birsa , J. Bisplinghoff , P. Bordalo , F. Bradamante , A. Bravar , A. Bressan , G. Brona , E. Burtin , M. P. Bussa , A. Chapiro , M. Chiosso , A. Cicuttin , M. Colantoni , S. Costa , M. L. Crespo , S. Dalla Torre , T. Dafni , S. Das , S. S. Dasgupta , R. De Masi , N. Dedek , O. Yu. Denisov , L. Dhara , V. Diaz , A. M. Dinkelbach , S. V. Donskov , V. A. Dorofeev , N. Doshita , V. Duic , W. Dünnweber , P. D. Eversheim , A. V. Efremov , W. Eyrich , M. Faessler , V. Falaleev , A. Ferrero , L. Ferrero , M. Finger , M. Finger , H. Fischer , C. Franco , J. Franz , J. M. Friedrich , V. Frolov , R. Garfagnini , F. Gautheron , O. P. Gavrichtchouk , R. Gazda , S. Gerassimov , R. Geyer , M. Giorgi , B. Gobbo , S. Goertz , A. M. Gorin , S. Grabmüller , O. A. Grajek , A. Grasso , B. Grube , R. Gushterski , A. Guskov , F. Haas , J. Hannappel , D. von Harrach , T. Hasegawa , J. Heckmann , S. Hedicke , F. H. Heinsius , R. Hermann , C. Heß , F. Hinterberger , M. von Hodenberg , N. Horikawa , S. Horikawa , N. d'Hose , C. Ilgner , A. I. Ioukaev , S. Ishimoto , O. Ivanov , Yu. Ivanshin , T. Iwata , R. Jahn , A. Janata , P. Jasinski , R. Joosten , N. I. Jouravlev , E. Kabuß , D. Kang , B. Ketzer , G. V. Khaustov , Yu. A. Khokhlov , Yu. Kisselev , F. Klein , K. Klimaszewski , S. Koblitz , J. H. Koivuniemi , V. N. Kolosov , E. V. Komissarov , K. Kondo , K. Königsmann , I. Konorov , V. F. Konstantinov , A. S. Korentchenko , A. Korzenev , A. M. Kotzinian , N. A. Koutchinski , O. Kouznetsov , A. Kral , N. P. Kravchuk , Z. V. Kroumchtein , R. Kuhn , F. Kunne , K. Kurek , M. E. Ladygin , M. Lamanna , J. M. Le Goff , A. A. Lednev , A. Lehmann , S. Levorato , J. Lichtenstadt , T. Liska , I. Ludwig , A. Maggiora , M. Maggiora , A. Magnon , G. K. Mallot , A. Mann , C. Marchand , J. Marroncle , A. Martin , J. Marzec , F. Massmann , T. Matsuda , A. N. Maximov , W. Meyer , A. Mielech , Yu. V. Mikhailov , M. A. Moinester , A. Mutter , A. Nagaytsev , T. Nagel , O. Nähle , J. Nassalski , S. Neliba , F. Nerling , S. Neubert , D. P. Neyret , V. I. Nikolaenko , K. Nikolaev , A. G. Olshevsky , M. Ostrick , A. Padee , P. Pagano , S. Panebianco , R. Panknin , D. Panzieri , S. Paul , B. Pawlukiewicz-Kaminska , D. V. Peshekhonov , V. D. Peshekhonov , G. Piragino , S. Platchkov , J. Pochodzalla , J. Polak , V. A. Polyakov , J. Pretz , S. Procureur , C. Quintans , J. -F. Rajotte , S. Ramos , V. Rapatsky , G. Reicherz , D. Reggiani , A. Richter , F. Robinet , E. Rocco , E. Rondio , A. M. Rozhdestvensky , D. I. Ryabchikov , V. D. Samoylenko , A. Sandacz , H. Santos , M. G. Sapozhnikov , S. Sarkar , I. A. Savin , P. Schiavon , C. Schill , L. Schmitt , P. Schönmeier , W. Schröder , O. Yu. Shevchenko , H. -W. Siebert , L. Silva , L. Sinha , A. N. Sissakian , M. Slunecka , G. I. Smirnov , S. Sosio , F. Sozzi , A. Srnka , F. Stinzing , M. Stolarski , V. P. Sugonyaev , M. Sulc , R. Sulej , V. V. Tchalishev , S. Tessaro , F. Tessarotto , A. Teufel , L. G. Tkatchev , G. Venugopal , M. Virius , N. V. Vlassov , A. Vossen , R. Webb , E. Weise , Q. Weitzel , R. Windmolders , S. Wirth , W. Wiślicki , H. Wollny , K. Zaremba , M. Zavertyaev , E. Zemlyanichkina , J. Zhao , R. Ziegler , A. Zvyagin

We present the current status of a non-perturbative lattice calculation of the moments of the pion and kaon distribution amplitudes by the RQCD collaboration. Our investigation is carried out using $N_f=2+1$ dynamical, non-perturbatively…

The three-particle $K$-matrix, $\mathcal{K}_{\mathrm{df},3}$, is a scheme-dependent quantity that parametrizes short-range three-particle interactions in the relativistic-field-theory three-particle finite-volume formalism. In this work, we…

High Energy Physics - Phenomenology · Physics 2023-05-25 Jorge Baeza-Ballesteros , Johan Bijnens , Tomáš Husek , Fernando Romero-López , Stephen R. Sharpe , Mattias Sjö

QCD at finite isospin density is considered for a large number of colors $N_c$. A linear sigma model is used to model the meson content of the theory at low density. At isospin chemical potential $\mu_I << \Lambda_{QCD}$, this matter forms…

High Energy Physics - Phenomenology · Physics 2026-04-08 Larry McLerran

We investigate the QCD phase diagram as a function of isospin chemical potential at a fixed temperature by directly putting large numbers of \pi^+s into the system. Correlation functions of N \pi^+s systems involves N!N! contractions, and…

High Energy Physics - Lattice · Physics 2012-02-15 Zhifeng Shi , William Detmold

Spectra of $q \bar q$ mesons are investigated in the framework of the Hamiltonian obtained from the relativistic path integral in external homogeneous magnetic field. The spectra of all 12 spin-isospin s-wave states generated by $\pi$- and…

High Energy Physics - Phenomenology · Physics 2017-04-05 B. O. Kerbikov , M. A. Andreichikov , Yu. A. Simonov

In this work, we present a first-principles lattice-QCD calculation of the unpolarized quark PDF for the pion and the kaon. The lattice data rely on matrix elements calculated for boosted mesons coupled to non-local operators containing a…

High Energy Physics - Lattice · Physics 2026-05-20 Joshua Miller , Joseph Torsiello , Isaac Anderson , Krzysztof Cichy , Martha Constantinou , Joseph Delmar , Sarah Lampreich