fields and particles in particle physics
and in the standard model of particle physics:
matter field fermions (spinors, Dirac fields)
flavors of fundamental fermions in the standard model of particle physics: | |||
---|---|---|---|
generation of fermions | 1st generation | 2nd generation | 3d generation |
quarks () | |||
up-type | up quark () | charm quark () | top quark () |
down-type | down quark () | strange quark () | bottom quark () |
leptons | |||
charged | electron | muon | tauon |
neutral | electron neutrino | muon neutrino | tau neutrino |
bound states: | |||
mesons | light mesons: pion () ρ-meson () ω-meson () f1-meson a1-meson | strange-mesons: ϕ-meson (), kaon, K*-meson (, ) eta-meson () charmed heavy mesons: D-meson (, , ) J/ψ-meson () | bottom heavy mesons: B-meson () ϒ-meson () |
baryons | nucleons: proton neutron |
(also: antiparticles)
hadrons (bound states of the above quarks)
minimally extended supersymmetric standard model
bosinos:
dark matter candidates
Exotica
In the standard model of particle physics a B-meson is a meson which is a bound state of a bottom quark and any other quark from the first two generations of fermions (up quark or down quark or strange quark or charm quark).
Hence the class of B-mesons goes along side that of K-mesons (light mnesons with a strange quark) and D-mesons (light meson with a charm quark).
flavors of fundamental fermions in the standard model of particle physics: | |||
---|---|---|---|
generation of fermions | 1st generation | 2nd generation | 3d generation |
quarks () | |||
up-type | up quark () | charm quark () | top quark () |
down-type | down quark () | strange quark () | bottom quark () |
leptons | |||
charged | electron | muon | tauon |
neutral | electron neutrino | muon neutrino | tau neutrino |
bound states: | |||
mesons | light mesons: pion () ρ-meson () ω-meson () f1-meson a1-meson | strange-mesons: ϕ-meson (), kaon, K*-meson (, ) eta-meson () charmed heavy mesons: D-meson (, , ) J/ψ-meson () | bottom heavy mesons: B-meson () ϒ-meson () |
baryons | nucleons: proton neutron |
Current experiments studying B-meson physics are the \
All these are increasingly seeing flavour anomalies (see there) in -meson decays at high statistical significance, pointing to physics beyond the standard model of particle physics.
B-meson experiments
observations
See also
Review:
R. Casalbuoni, A. Deandrea, N.Di Bartolomeo, F. Feruglio, R. Gatto, G. Nardulli, Phenomenology of Heavy Meson Chiral Lagrangians, Phys. Rept. 281:145-238, 1997 (arXiv:hep-ph/9605342)
Jochen Dingfelder, Thomas Mannel, Leptonic and semileptonic decays of mesons, Rev. Mod. Phys. 88 (2016) 3, 035008 (spire:1488176, doi:10.1103/RevModPhys.88.035008)
See also
J. P. Lees et al. (BABAR Collaboration), Measurement of the branching fraction with semileptonically tagged B mesons, Phys. Rev. D 88, 072006 (2013) (doi:10.1103/PhysRevD.88.072006)
Xian-Wei Kang, Tao Luo, Yi Zhang, Ling-Yun Dai, Chao Wang, Semileptonic and decays involving scalar and axial-vector mesons, Eur. Phys. J. C 78, 909 (2018) (doi:10.1140/epjc/s10052-018-6385-9)
Inclusion of heavy flavors into the Skyrme model for quantum hadrodynamics:
Inclusion of strange quarks/kaons into the Skyrme model:
Curtis Callan, Igor Klebanov, Bound-state approach to strangeness in the Skyrme model, Nuclear Physics B Volume 262, Issue 2, 16 December 1985, Pages 365-382 (doi10.1016/0550-3213(85)90292-5)
Curtis Callan, K. Hornbostel, Igor Klebanov, Baryon masses in the bound state approach to strangeness in the skyrme model, Physics Letters B Volume 202, Issue 2, 3 March 1988, Pages 269-275 (doi10.1016/0370-2693(88)90022-6)
Norberto Scoccola, D. P. Min, H. Nadeau, Mannque Rho, The strangeness problem: An skyrmion with vector mesons, Nuclear Physics A Volume 505, Issues 3–4, 25 December 1989, Pages 497-524 (doi:10.1016/0375-9474(89)90029-8)
Review:
Igor Klebanov, section 6 of: Strangeness in the Skyrme model, in: D. Vauthrin, F. Lenz, J. W. Negele, Hadrons and Hadronic Matter, Plenum Press 1989 (doi:10.1007/978-1-4684-1336-6)
Mannque Rho, Section 2.2 of: Cheshire Cat Hadrons, Phys. Rept. 240 (1994) 1-142 (arXiv:hep-ph/9310300, doi:10.1016/0370-1573(94)90002-7)
Inclusion of charm quarks/D-mesons into the Skyrme model:
Mannque Rho, D. O. Riska, Norberto Scoccola, Charmed baryons as soliton - D meson bound states, Phys. Lett.B 251 (1990) 597-602 (spire:297771, doi:10.1016/0370-2693(90)90802-D)
Yongseok Oh, Dong-Pil Min, Mannque Rho, Norberto Scoccola, Massive-quark baryons as skyrmions: Magnetic moments, Nuclear Physics A Volume 534, Issues 3–4 (1991) Pages 493-512 (doi:10.1016/0375-9474(91)90458-I)
Inclusion of further heavy flavors beyond strange quark/kaons, namely charm quarks/D-mesons and bottom quarks/B-mesons, into the Skyrme model:
Mannque Rho, D. O. Riska, Norberto Scoccola, The energy levels of the heavy flavour baryons in the topological soliton model, Zeitschrift für Physik A Hadrons and Nuclei volume 341, pages 343–352 (1992) (doi:10.1007/BF01283544)
Arshad Momen, Joseph Schechter, Anand Subbaraman, Heavy Quark Solitons: Strangeness and Symmetry Breaking, Phys. Rev. D49:5970-5978, 1994 (arXiv:hep-ph/9401209)
Yongseok Oh, Byung-Yoon Park, Dong-Pil Min, Heavy Baryons as Skyrmion with Corrections, Phys. Rev. D49 (1994) 4649-4658 (arXiv:hep-ph/9402205)
Review:
Mannque Rho, Massive-quark baryons as Skyrmions, Modern Physics Letters A, Vol. 06, No. 23 (1991) (doi:10.1142/S0217732391002268)
Norberto Scoccola, Heavy quark skyrmions, (arXiv:0905.2722, doi:10.1142/9789814280709_0004), Chapter 4 in: The Multifaceted Skyrmion, World Scientific 2016 (doi:10.1142/9710)
Discussion in holographic light front QCD:
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