Applications of the Octet Baryon Quark-Meson Coupling Model to Hybrid Stars
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Effects of Scalar Mesons in a Skyrme Model with Hidden Local Symmetry
Effects of scalar mesons in a Skyrme model with hidden local symmetry 1, 2, 1, Bing-Ran He, ∗ Yong-Liang Ma, † and Masayasu Harada ‡ 1Department of Physics, Nagoya University, Nagoya, 464-8602, Japan 2Center of Theoretical Physics and College of Physics, Jilin University, Changchun, 130012, China (Dated: March 5, 2018) We study the effects of light scalar mesons on the skyrmion properties by constructing and ex- amining a mesonic model including pion, rho meson, and omega meson fields as well as two-quark and four-quark scalar meson fields. In our model, the physical scalar mesons are defined as mixing states of the two- and four-quark fields. We first omit the four-quark scalar meson field from the model and find that when there is no direct coupling between the two-quark scalar meson and the vector mesons, the soliton mass is smaller and the soliton size is larger for lighter scalar mesons; when direct coupling is switched on, as the coupling strength increases, the soliton becomes heavy, and the radius of the baryon number density becomes large, as the repulsive force arising from the ω meson becomes strong. We then include the four-quark scalar meson field in the model and find that mixing between the two-quark and four-quark components of the scalar meson fields also affects the properties of the soliton. When the two-quark component of the lighter scalar meson is increased, the soliton mass decreases and the soliton size increases. PACS numbers: 11.30.Rd, 12.39.Dc, 12.39.Fe, 14.40.Be I. -
Selfconsistent Description of Vector-Mesons in Matter 1
Selfconsistent description of vector-mesons in matter 1 Felix Riek 2 and J¨orn Knoll 3 Gesellschaft f¨ur Schwerionenforschung Planckstr. 1 64291 Darmstadt Abstract We study the influence of the virtual pion cloud in nuclear matter at finite den- sities and temperatures on the structure of the ρ- and ω-mesons. The in-matter spectral function of the pion is obtained within a selfconsistent scheme of coupled Dyson equations where the coupling to the nucleon and the ∆(1232)-isobar reso- nance is taken into account. The selfenergies are determined using a two-particle irreducible (2PI) truncation scheme (Φ-derivable approximation) supplemented by Migdal’s short range correlations for the particle-hole excitations. The so obtained spectral function of the pion is then used to calculate the in-medium changes of the vector-meson spectral functions. With increasing density and temperature a strong interplay of both vector-meson modes is observed. The four-transversality of the polarisation tensors of the vector-mesons is achieved by a projector technique. The resulting spectral functions of both vector-mesons and, through vector domi- nance, the implications of our results on the dilepton spectra are studied in their dependence on density and temperature. Key words: rho–meson, omega–meson, medium modifications, dilepton production, self-consistent approximation schemes. PACS: 14.40.-n 1 Supported in part by the Helmholz Association under Grant No. VH-VI-041 2 e-mail:[email protected] 3 e-mail:[email protected] Preprint submitted to Elsevier Preprint Feb. 2004 1 Introduction It is an interesting question how the behaviour of hadrons changes in a dense hadronic medium. -
J. Stroth Asked the Question: "Which Are the Experimental Evidences for a Long Mean Free Path of Phi Mesons in Medium?"
J. Stroth asked the question: "Which are the experimental evidences for a long mean free path of phi mesons in medium?" Answer by H. Stroebele ~~~~~~~~~~~~~~~~~~~ (based on the study of several publications on phi production and information provided by the theory friends of H. Stöcker ) Before trying to find an answer to this question, we need to specify what is meant with "long". The in medium cross section is equivalent to the mean free path. Thus we need to find out whether the (in medium) cross section is large (with respect to what?). The reference would be the cross sections of other mesons like pions or more specifically the omega meson. There is a further reference, namely the suppression of phi production and decay described in the OZI rule. A “blind” application of the OZI rule would give a cross section of the phi three orders of magnitude lower than that of the omega meson and correspondingly a "long" free mean path. In the following we shall look at the phi production cross sections in photon+p, pion+p, and p+p interactions. The total photoproduction cross sections of phi and omega mesons were measured in a bubble chamber experiment (J. Ballam et al., Phys. Rev. D 7, 3150, 1973), in which a cross section ratio of R(omega/phi) = 10 was found in the few GeV beam energy region. There are results on omega and phi production in p+p interactions available from SPESIII (Near- Threshold Production of omega mesons in the Reaction p p → p p omega", Phys.Rev.Lett. -
1– N and ∆ RESONANCES Revised May 2015 by V. Burkert
– 1– N AND ∆ RESONANCES Revised May 2015 by V. Burkert (Jefferson Lab), E. Klempt (University of Bonn), M.R. Pennington (Jefferson Lab), L. Tiator (University of Mainz), and R.L. Workman (George Washington University). I. Introduction The excited states of the nucleon have been studied in a large number of formation and production experiments. The Breit-Wigner masses and widths, the pole positions, and the elasticities of the N and ∆ resonances in the Baryon Summary Table come largely from partial-wave analyses of πN total, elastic, and charge-exchange scattering data. The most com- prehensive analyses were carried out by the Karlsruhe-Helsinki (KH80) [1], Carnegie Mellon-Berkeley (CMB80) [2], and George Washington U (GWU) [3] groups. Partial-wave anal- yses have also been performed on much smaller πN reaction data sets to get ηN, KΛ, and KΣ branching fractions (see the Listings for references). Other branching fractions come from analyses of πN ππN data. → In recent years, a large amount of data on photoproduction of many final states has been accumulated, and these data are beginning to tell us much about the properties of baryon resonances. A survey of data on photoproduction can be found in the proceedings of recent conferences [4] and workshops [5], and in recent reviews [6,7]. II. Naming scheme for baryon resonances In the past, when nearly all resonance information came from elastic πN scattering, it was common to label reso- nances with the incoming partial wave L2I,2J , as in ∆(1232)P33 and N(1680)F15. However, most recent information has come from γN experiments. -
Recent Progress on Dense Nuclear Matter in Skyrmion Approaches Yong-Liang Ma, Mannque Rho
Recent progress on dense nuclear matter in skyrmion approaches Yong-Liang Ma, Mannque Rho To cite this version: Yong-Liang Ma, Mannque Rho. Recent progress on dense nuclear matter in skyrmion approaches. SCIENCE CHINA Physics, Mechanics & Astronomy, 2017, 60, pp.032001. 10.1007/s11433-016-0497- 2. cea-01491871 HAL Id: cea-01491871 https://hal-cea.archives-ouvertes.fr/cea-01491871 Submitted on 17 Mar 2017 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. SCIENCE CHINA Physics, Mechanics & Astronomy . Invited Review . Month 2016 Vol. *** No. ***: ****** doi: ******** Recent progress on dense nuclear matter in skyrmion approaches Yong-Liang Ma1 & Mannque Rho2 1Center of Theoretical Physics and College of Physics, Jilin University, Changchun, 130012, China; Email:[email protected] 2Institut de Physique Th´eorique, CEA Saclay, 91191 Gif-sur-Yvette c´edex, France; Email:[email protected] The Skyrme model provides a novel unified approach to nuclear physics. In this approach, single baryon, baryonic matter and medium-modified hadron properties are treated on the same footing. Intrinsic density dependence (IDD) reflecting the change of vacuum by compressed baryonic matter figures naturally in the approach. In this article, we review the recent progress on accessing dense nuclear matter by putting baryons treated as solitons, namely, skyrmions, on crystal lattice with accents on the implications in compact stars. -
Mass Shift of Σ-Meson in Nuclear Matter
Mass shift of σ-Meson in Nuclear Matter J. R. Morones-Ibarra, Mónica Menchaca Maciel, Ayax Santos-Guevara, and Felipe Robledo Padilla. Facultad de Ciencias Físico-Matemáticas, Universidad Autónoma de Nuevo León, Ciudad Universitaria, San Nicolás de los Garza, Nuevo León, 66450, México. Facultad de Ingeniería y Arquitectura, Universidad Regiomontana, 15 de Mayo 567, Monterrey, N.L., 64000, México. April 6, 2010 Abstract The propagation of sigma meson in nuclear matter is studied in the Walecka model, assuming that the sigma couples to a pair of nucleon-antinucleon states and to particle-hole states, including the in medium effect of sigma-omega mixing. We have also considered, by completeness, the coupling of sigma to two virtual pions. We have found that the sigma meson mass decreases respect to its value in vacuum and that the contribution of the sigma omega mixing effect on the mass shift is relatively small. Keywords: scalar mesons, hadrons in dense matter, spectral function, dense nuclear matter. PACS:14.40;14.40Cs;13.75.Lb;21.65.+f 1. INTRODUCTION The study of matter under extreme conditions of density and temperature, has become a very important issue due to the fact that it prepares to understand the physics for some interesting subjects like, the conditions in the early universe, the physics of processes in stellar evolution and in heavy ion collision. Particularly, the study of properties of mesons in hot and dense matter is important to understand which could be the signature for detecting the Quark-Gluon Plasma (QGP) state in heavy ion collision, and to get information about the signal of the presence of QGP and also to know which symmetries are restored [1]. -
Analysis of Pseudoscalar and Scalar $D$ Mesons and Charmonium
PHYSICAL REVIEW C 101, 015202 (2020) Analysis of pseudoscalar and scalar D mesons and charmonium decay width in hot magnetized asymmetric nuclear matter Rajesh Kumar* and Arvind Kumar† Department of Physics, Dr. B. R. Ambedkar National Institute of Technology Jalandhar, Jalandhar 144011 Punjab, India (Received 27 August 2019; revised manuscript received 19 November 2019; published 8 January 2020) In this paper, we calculate the mass shift and decay constant of isospin-averaged pseudoscalar (D+, D0 ) +, 0 and scalar (D0 D0 ) mesons by the magnetic-field-induced quark and gluon condensates at finite density and temperature of asymmetric nuclear matter. We have calculated the in-medium chiral condensates from the chiral SU(3) mean-field model and subsequently used these condensates in QCD sum rules to calculate the effective mass and decay constant of D mesons. Consideration of external magnetic-field effects in hot and dense nuclear matter lead to appreciable modification in the masses and decay constants of D mesons. Furthermore, we also ψ ,ψ ,χ ,χ studied the effective decay width of higher charmonium states [ (3686) (3770) c0(3414) c2(3556)] as a 3 by-product by using the P0 model, which can have an important impact on the yield of J/ψ mesons. The results of the present work will be helpful to understand the experimental observables of heavy-ion colliders which aim to produce matter at finite density and moderate temperature. DOI: 10.1103/PhysRevC.101.015202 I. INTRODUCTION debateable topic. Many theories suggest that the magnetic field produced in HICs does not die immediately due to the Future heavy-ion colliders (HIC), such as the Japan Proton interaction of itself with the medium. -
Kaon Pair Production in Pp, Pd, Dd and Pa Collisions at COSY
Kaon pair production in pp, pd, dd and pA collisions at COSY Michael Hartmann Institut für Kernphysik and Jülich Centre for Hadron Physics, Forschungszentrum Jülich, D-52425 Jülich, Germany E-mail: [email protected] An overview of experiments at the Cooler Synchrotron COSY on kaon-pair production in pp, pd, dd collisions in the close-to-threshold regime is given. These include results on f-meson production, where the meson is detected via its K+K− decay. The study of f production on a range of heavier nuclear targets allows one to deduce a value of the f width in nuclei and its variation with the f momentum. XLIX International Winter Meeting on Nuclear Physics, BORMIO2011 January 24-28, 2011 Bormio, Italy c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence. http://pos.sissa.it/ Kaon pair production at COSY 1. Introduction The cooler synchrotron COSY [1] at the Forschungszentrum Jülich in Germany can accelerate protons and deuterons up to about 3.7 GeV/c. Both polarized and unpolarized beams are available. Excellent beam quality is achieved with the help of electron and/or stochastic cooling. COSY can be used as an accelerator for external target experiments and as a storage ring for internal target experiments. Kaon pair production experiments have been performed at the internal spectrometer ANKE by the COSY-ANKE collaboration, at the internal COSY-11 spectrometer by the COSY-11 collaboration, and at the external BIG KARL spectrograph by the COSY-MOMO collaboration. 103 102 10 pn → dφ total corss section [nb] pp → ppφ 1 pp → ppφ pd → 3Heφ pn → dK+K pp → ppK+K 1 10 pp → ppK+K pp → ppK+K o pp → dK+K pd → 3HeK+K 2 10 dd → 4HeK+K 0 20 40 60 80 100 Excess energy [MeV] Figure 1: World data set on total cross sections for kaon-pair production in terms of the excess energy for each reaction. -
Researcher 2015;7(8)
Researcher 2015;7(8) http://www.sciencepub.net/researcher Curie Particle And The Relation Between The Masses Of Sub-Atomic Particles, Supporting (Bicep2`S) Experiments, Mass Of Neutrino, Present “The Lhcb Collaboration” & “Atlas” Experiments. Nirmalendu Das Life Member (1): THE VON KARMAN SOCIETY for Advanced Study and Research in Mathematical Science (UKS), Old Post Office line, Jalpaiguri, Life Member (2): Indian Science Congress Association, India. Resident Address: MUKUL DEEP, Saratpally, W.No.- 40, 74/48, Meghlal Roy Road Haiderpara, Siliguri – 734006, Dist: Jalpaiguri, West Bengal, India. Mob: +91-9475089337, Email: [email protected], [email protected] Abstract: Light is very sensitive matter. In terms of mass of a photon is important in every field of matter thus for the universe. The scientists of many countries are trying to find the mass of photon by experiment since 1936 and continuing this work in various countries. But the obtained results are differing to each other. So, we cannot consider these mass of a photon. On the other hand matter is made by the photons. We get this idea from the Einstein equation E = mc2. Again, energy is nothing but the bunch of photons. I calculate the mass of a photon (1.6596x10-54 gm) [1] and this mass is applicable to all fields. Here, in this article, we can calculate the mass of “Curie particle” (Unknown to us) by using this mass of photon & is related to Higgs and other sub-atomic particles. The energy of Higgs particle is very low as per BICEP2`s experimental report [2] and I reported about this matter in the year 2011 to “The Authority of CERN, Editor of Press release of CERN and many other places” by emailing, but did not get answer in this regards. -
Vector Meson Production and Nucleon Resonance Analysis in a Coupled-Channel Approach
Vector Meson Production and Nucleon Resonance Analysis in a Coupled-Channel Approach Inaugural-Dissertation zur Erlangung des Doktorgrades der Naturwissenschaftlichen Fakult¨at der Justus-Liebig-Universit¨atGießen Fachbereich 07 – Mathematik, Physik, Geographie vorgelegt von Gregor Penner aus Gießen Gießen, 2002 D 26 Dekan: Prof. Dr. Albrecht Beutelspacher I. Berichterstatter: Prof. Dr. Ulrich Mosel II. Berichterstatter: Prof. Dr. Volker Metag Tag der m¨undlichen Pr¨ufung: Contents 1 Introduction 1 2 The Bethe-Salpeter Equation and the K-Matrix Approximation 7 2.1 Bethe-Salpeter Equation ........................................ 7 2.2 Unitarity and the K-Matrix Approximation ......................... 11 3 The Model 13 3.1 Other Models Analyzing Pion- and Photon-Induced Reactions on the Nucleon 15 3.1.1 Resonance Models: ...................................... 15 3.1.2 Separable Potential Models ................................ 17 3.1.3 Effective Lagrangian Models ............................... 17 3.2 The Giessen Model ............................................ 20 3.3 Asymptotic Particle (Born) Contributions .......................... 23 3.3.1 Electromagnetic Interactions ............................... 23 3.3.2 Hadronic Interactions .................................... 25 3.4 Baryon Resonances ............................................ 28 3.4.1 (Pseudo-)Scalar Meson Decay .............................. 28 3.4.2 Electromagnetic Decays .................................. 32 3.4.3 Vector Meson Decays ................................... -
Mass Generation Via the Higgs Boson and the Quark Condensate of the QCD Vacuum
Pramana – J. Phys. (2016) 87: 44 c Indian Academy of Sciences DOI 10.1007/s12043-016-1256-0 Mass generation via the Higgs boson and the quark condensate of the QCD vacuum MARTIN SCHUMACHER II. Physikalisches Institut der Universität Göttingen, Friedrich-Hund-Platz 1, D-37077 Göttingen, Germany E-mail: [email protected] Published online 24 August 2016 Abstract. The Higgs boson, recently discovered with a mass of 125.7 GeV is known to mediate the masses of elementary particles, but only 2% of the mass of the nucleon. Extending a previous investigation (Schumacher, Ann. Phys. (Berlin) 526, 215 (2014)) and including the strange-quark sector, hadron masses are derived from the quark condensate of the QCD vacuum and from the effects of the Higgs boson. These calculations include the π meson, the nucleon and the scalar mesons σ(600), κ(800), a0(980), f0(980) and f0(1370). The predicted second σ meson, σ (1344) =|ss¯, is investigated and identified with the f0(1370) meson. An outlook is given on the hyperons , 0,± and 0,−. Keywords. Higgs boson; sigma meson; mass generation; quark condensate. PACS Nos 12.15.y; 12.38.Lg; 13.60.Fz; 14.20.Jn 1. Introduction adds a small additional part to the total constituent- quark mass leading to mu = 331 MeV and md = In the Standard Model, the masses of elementary parti- 335 MeV for the up- and down-quark, respectively [9]. cles arise from the Higgs field acting on the originally These constituent quarks are the building blocks of the massless particles. When applied to the visible matter nucleon in a similar way as the nucleons are in the case of the Universe, this explanation remains unsatisfac- of nuclei. -
Masses of Scalar and Axial-Vector B Mesons Revisited
Eur. Phys. J. C (2017) 77:668 DOI 10.1140/epjc/s10052-017-5252-4 Regular Article - Theoretical Physics Masses of scalar and axial-vector B mesons revisited Hai-Yang Cheng1, Fu-Sheng Yu2,a 1 Institute of Physics, Academia Sinica, Taipei 115, Taiwan, Republic of China 2 School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, People’s Republic of China Received: 2 August 2017 / Accepted: 22 September 2017 / Published online: 7 October 2017 © The Author(s) 2017. This article is an open access publication Abstract The SU(3) quark model encounters a great chal- 1 Introduction lenge in describing even-parity mesons. Specifically, the qq¯ quark model has difficulties in understanding the light Although the SU(3) quark model has been applied success- scalar mesons below 1 GeV, scalar and axial-vector charmed fully to describe the properties of hadrons such as pseu- mesons and 1+ charmonium-like state X(3872). A common doscalar and vector mesons, octet and decuplet baryons, it wisdom for the resolution of these difficulties lies on the often encounters a great challenge in understanding even- coupled channel effects which will distort the quark model parity mesons, especially scalar ones. Take vector mesons as calculations. In this work, we focus on the near mass degen- an example and consider the octet vector ones: ρ,ω, K ∗,φ. ∗ ∗0 eracy of scalar charmed mesons, Ds0 and D0 , and its impli- Since the constituent strange quark is heavier than the up or cations. Within the framework of heavy meson chiral pertur- down quark by 150 MeV, one will expect the mass hierarchy bation theory, we show that near degeneracy can be quali- pattern mφ > m K ∗ > mρ ∼ mω, which is borne out by tatively understood as a consequence of self-energy effects experiment.