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
algebraic quantum field theory (perturbative, on curved spacetimes, homotopical)
quantum mechanical system, quantum probability
interacting field quantization
In the plain minimally supersymmetric standard model (MSSM), baryon/lepton number would not need to be preserved. Since however experimental observation indicates that these quantum observables are preserved to high accuracy, a common ad hoc solution in bottom-up model-building is to impose a certain Z/2-action on the MSSM as a global symmetry, called R-parity, which does enforce baryon/lepton number conservation.
From a top-down model building-perspective there is the rough idea that R-parity may be thought of as a discrete remnant of R-symmetry (e.g. Chamseddine-Dreiner 96, p. 2, Frugiuele-Gregoire 11)
There remain speculations that even if MSSM-like models are realistic, R-parity might in fact be violated in nature after all, such as as possibly indicated by the apparent flavour anomalies (Wang-Yang-Yuan 19).
The original articles are
Savas Dimopoulos, Howard Georgi, Softly broken supersymmetry and , Nuclear Physics B Volume 193, Issue 1, 21 1981 (doi:10.1016/0550-3213(81)90522-8)
N. Z. Sakai, Naturalnes in supersymmetric GUTS Zeitschrift für Physik C Particles and Fields (1981) 11: 153 (doi:10.1007/BF01573998)
Hans-Peter Nilles, Stuart Raby, Supersymmetry and the strong CP problem, Nuclear Physics B Volume 198, Issue 1, 26 April 1982 (doi:10.1016/0550-3213(82)90547-8)
N. Sakai, Tsutomu Yanagida, Proton decay in a class of supersymmetric grand unified models, Nuclear Physics B Volume 197, Issue 3, 12 April 1982, Pages 533-542 (doi:10.1016/0550-3213(82)90457-6)
Savas Dimopoulos, Stuart Raby, Frank Wilczek, Proton decay in supersymmetric models, Physics Letters B Volume 112, Issue 2, 6 May 1982, Pages 133-136 (doi:10.1016/0370-2693(82)90313-6)
See also
Discussion of possible relation to R-symmetry:
Ali Chamseddine, Herbi Dreiner, Anomaly-Free Gauged R-Symmetry in Local Supersymmetry, Nucl.Phys. B458 (1996) 65-89 (arXiv:hep-ph/9504337)
Claudia Frugiuele, Thomas Gregoire, Making the Sneutrino a Higgs with a Lepton Number, PhysRev D.85.015016 (arXiv:1107.4634)
In SemiSpin(32)-heterotic string phenomenology:
Suggestion that the MSSM with R-parity violation could explain the flavour anomalies:
Dong-Yang Wang, Ya-Dong Yang, Xing-Bo Yuan, decays in supersymmetry with R-parity violation (arXiv:1905.08784)
Quan-Yi Hu, Lin-Lin Huang, Explaining data by sneutrinos in the R-parity violating MSSM (arXiv:1912.03676)
Quan-Yi Hu, Ya-Dong Yang, Min-Di Zheng, Revisiting the B-physics anomalies in R-parity violating MSSM (arXiv:2002.09875)
Wolfgang Altmannshofer, P. S. Bhupal Dev, Amarjit Soni, Yicong Sui, Addressing , , muon and ANITA anomalies in a minimal R-parity violating supersymmetric framework (arXiv:2002.12910)
Last revised on March 2, 2020 at 10:55:41. See the history of this page for a list of all contributions to it.