| 10. |
THE PHYSICS OF ELEMENTARY PARTICLES AND FIELDS (for cosmic rays, see 96.50.S- in astronomy; for experimental methods and instrumentation for elementary-particle physics, see section 29) |
|
| 11. |
General theory of fields and particles (see also 03.65.-w Quantum mechanics and 03.70.+k Theory of quantized fields) |
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| 11.10.-z |
Field theory (for gauge field theories, see 11.15.-q) |
|
| 11.10.Cd |
Axiomatic approach |
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| 11.10.Ef |
Lagrangian and Hamiltonian approach |
|
| 11.10.Gh |
Renormalization |
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| 11.10.Hi |
Renormalization group evolution of parameters |
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| 11.10.Jj |
Asymptotic problems and properties |
|
| 11.10.Kk |
Field theories in dimensions other than four (see also 04.50.+h Gravity in more than four dimensions; 04.60.Kz Lower dimensional models in quantum gravity) |
|
| 11.10.Lm |
Nonlinear or nonlocal theories and models (see also 11.27.+d Extended classical solutions; cosmic strings, domain walls, texture) |
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| 11.10.Nx |
Noncommutative field theory |
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| 11.10.St |
Bound and unstable states; Bethe–Salpeter equations |
|
| 11.10.Wx |
Finite-temperature field theory |
| ... ... ... | Relativistic wave equations, see 03.65.Pm |
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| 11.15.-q |
Gauge field theories |
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| 11.15.Bt |
General properties of perturbation theory |
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| 11.15.Ex |
Spontaneous breaking of gauge symmetries |
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| 11.15.Ha |
Lattice gauge theory (see also 12.38.Gc Lattice QCD calculations) |
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| 11.15.Kc |
Classical and semiclassical techniques |
|
| 11.15.Me |
Strong-coupling expansions |
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| 11.15.Pg |
Expansions for large numbers of components (e.g., 1/Nc expansions) |
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| 11.15.Tk |
Other nonperturbative techniques |
|
| 11.25.-w |
Strings and branes (for cosmic strings, see 98.80.Cq in cosmology; see also 11.27.+d Extended classical solutions; cosmic strings, domain walls, texture) |
|
| 11.25.Db |
Properties of perturbation theory |
|
| 11.25.Hf |
Conformal field theory, algebraic structures |
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| 11.25.Mj |
Compactification and four-dimensional models |
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| 11.25.Pm |
Noncritical string theory |
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| 11.25.Sq |
Nonperturbative techniques; string field theory |
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| 11.25.Tq |
Gauge/string duality |
|
| 11.25.Uv |
D branes |
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| 11.25.Wx |
String and brane phenomenology |
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| 11.25.Yb |
M theory |
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| 11.27.+d |
Extended classical solutions; cosmic strings, domain walls, texture (see also 98.80.Cq in cosmology; 11.25.-w Strings and branes) |
|
| 11.30.-j |
Symmetry and conservation laws (see also 02.20.-a Group theory) |
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| 11.30.Cp |
Lorentz and Poincare invariance |
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| 11.30.Er |
Charge conjugation, parity, time reversal, and other discrete symmetries |
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| 11.30.Fs |
Global symmetries (e.g., baryon number, lepton number) |
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| 11.30.Hv |
Flavor symmetries |
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| 11.30.Ly |
Other internal and higher symmetries |
|
| 11.30.Na |
Nonlinear and dynamical symmetries (spectrum-generating symmetries) |
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| 11.30.Pb |
Supersymmetry (see also 12.60.Jv Supersymmetric models) |
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| 11.30.Qc |
Spontaneous and radiative symmetry breaking |
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| 11.30.Rd |
Chiral symmetries |
|
| 11.40.-q |
Currents and their properties |
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| 11.40.Dw |
General theory of currents |
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| 11.40.Ex |
Formal properties of current algebras (see also 12.39.Fe Chiral Lagrangians) |
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| 11.40.Ha |
Partially conserved axial-vector currents |
|
| 11.55.-m |
S-matrix theory; analytic structure of amplitudes |
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| 11.55.Bq |
Analytic properties of S matrix |
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| 11.55.Ds |
Exact S matrices |
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| 11.55.Fv |
Dispersion relations |
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| 11.55.Hx |
Sum rules |
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| 11.55.Jy |
Regge formalism (see also 12.40.Nn in strong interactions) |
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| 11.80.-m |
Relativistic scattering theory |
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| 11.80.Cr |
Kinematical properties (helicity and invariant amplitudes, kinematic singularities, etc.) |
|
| 11.80.Et |
Partial-wave analysis |
|
| 11.80.Fv |
Approximations (eikonal approximation, variational principles, etc.) |
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| 11.80.Gw |
Multichannel scattering |
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| 11.80.Jy |
Many-body scattering and Faddeev equation |
|
| 11.80.La |
Multiple scattering |
|
| 11.90.+t |
Other topics in general theory of fields and particles (restricted to new topics in section 11) |
|
| 12. |
Specific theories and interaction models; particle systematics |
|
| 12.10.-g |
Unified field theories and models (see also 04.50.+h-in general relativity and gravitation, 11.25.Mj Compactification and four-dimensional models) |
|
| 12.10.Dm |
Unified theories and models of strong and electroweak interactions |
|
| 12.10.Kt |
Unification of couplings; mass relations |
|
| 12.15.-y |
Electroweak interactions |
| ... ... ... | Extensions of gauge or Higgs sector, see 12.60.Cn or 12.60.Fr |
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| 12.15.Ff |
Quark and lepton masses and mixing (see also 14.60.Pq Neutrino mass and mixing) |
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| 12.15.Hh |
Determination of Kobayashi-Maskawa matrix elements |
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| 12.15.Ji |
Applications of electroweak models to specific processes |
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| 12.15.Lk |
Electroweak radiative corrections (see also 13.40.Ks Electromagnetic corrections to strong- and weak-interaction processes) |
|
| 12.15.Mm |
Neutral currents |
|
| 12.20.-m |
Quantum electrodynamics |
|
| 12.20.Ds |
Specific calculations |
|
| 12.20.Fv |
Experimental tests (for optical tests in quantum electrodynamics, see 42.50.Xa) |
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| 12.38.-t |
Quantum chromodynamics |
| ... ... ... | Quarks, gluons, and QCD in nuclei and nuclear processes, see 24.85.+p |
|
| 12.38.Aw |
General properties of QCD (dynamics, confinement, etc.) |
|
| 12.38.Bx |
Perturbative calculations |
|
| 12.38.Cy |
Summation of perturbation theory |
|
| 12.38.Gc |
Lattice QCD calculations (see also 11.15.Ha Lattice gauge theory) |
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| 12.38.Lg |
Other nonperturbative calculations |
|
| 12.38.Mh |
Quark-gluon plasma (see also 25.75.Nq Quark deconfinement, quark-gluon plasma production and phase transitions in relativistic heavy ion collisions) |
|
| 12.38.Qk |
Experimental tests |
|
| 12.39.-x |
Phenomenological quark models |
|
| 12.39.Ba |
Bag model |
|
| 12.39.Dc |
Skyrmions |
|
| 12.39.Fe |
Chiral Lagrangians |
|
| 12.39.Hg |
Heavy quark effective theory |
|
| 12.39.Jh |
Nonrelativistic quark model |
|
| 12.39.Ki |
Relativistic quark model |
|
| 12.39.Mk |
Glueball and nonstandard multi-quark/gluon states |
|
| 12.39.Pn |
Potential models |
|
| 12.39.St |
Factorization |
|
| 12.40.-y |
Other models for strong interactions |
|
| 12.40.Ee |
Statistical models |
|
| 12.40.Nn |
Regge theory, duality, absorptive/optical models (see also 11.55.Jy Regge formalism) |
|
| 12.40.Vv |
Vector-meson dominance |
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| 12.40.Yx |
Hadron mass models and calculations |
|
| 12.60.-i |
Models beyond the standard model |
| ... ... ... | Unified field theories and models, see 12.10.-g |
|
| 12.60.Cn |
Extensions of electroweak gauge sector |
|
| 12.60.Fr |
Extensions of electroweak Higgs sector |
|
| 12.60.Jv |
Supersymmetric models (see also 04.65.+e Supergravity) |
|
| 12.60.Nz |
Technicolor models |
|
| 12.60.Rc |
Composite models |
|
| 12.90.+b |
Miscellaneous theoretical ideas and models (restricted to new topics in section 12) |
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| 13. |
Specific reactions and phenomenology |
|
| 13.15.+g |
Neutrino interactions |
|
| 13.20.-v |
Leptonic, semileptonic, and radiative decays of mesons |
|
| 13.20.Cz |
Decays of pi mesons |
|
| 13.20.Eb |
Decays of K mesons |
|
| 13.20.Fc |
Decays of charmed mesons |
|
| 13.20.Gd |
Decays of J/psi, Upsilon, and other quarkonia |
|
| 13.20.He |
Decays of bottom mesons |
|
| 13.20.Jf |
Decays of other mesons |
|
| 13.25.-k |
Hadronic decays of mesons |
|
| 13.25.Cq |
Decays of pi mesons |
|
| 13.25.Es |
Decays of K mesons |
|
| 13.25.Ft |
Decays of charmed mesons |
|
| 13.25.Gv |
Decays of J/psi, Upsilon, and other quarkonia |
|
| 13.25.Hw |
Decays of bottom mesons |
|
| 13.25.Jx |
Decays of other mesons |
|
| 13.30.-a |
Decays of baryons |
|
| 13.30.Ce |
Leptonic, semileptonic, and radiative decays |
|
| 13.30.Eg |
Hadronic decays |
|
| 13.35.-r |
Decays of leptons |
|
| 13.35.Bv |
Decays of muons |
|
| 13.35.Dx |
Decays of taus |
|
| 13.35.Hb |
Decays of heavy neutrinos |
|
| 13.38.-b |
Decays of intermediate bosons |
|
| 13.38.Be |
Decays of W bosons |
|
| 13.38.Dg |
Decays of Z bosons |
|
| 13.40.-f |
Electromagnetic processes and properties |
|
| 13.40.Dk |
Electromagnetic mass differences |
|
| 13.40.Em |
Electric and magnetic moments |
|
| 13.40.Gp |
Electromagnetic form factors |
|
| 13.40.Hq |
Electromagnetic decays |
|
| 13.40.Ks |
Electromagnetic corrections to strong- and weak-interaction processes |
|
| 13.60.-r |
Photon and charged-lepton interactions with hadrons (for neutrino interactions, see 13.15.+g) |
|
| 13.60.Fz |
Elastic and Compton scattering |
|
| 13.60.Hb |
Total and inclusive cross sections (including deep-inelastic processes) |
|
| 13.60.Le |
Meson production |
|
| 13.60.Rj |
Baryon production |
|
| 13.66.-a |
Lepton-lepton interactions |
|
| 13.66.Bc |
Hadron production in e-e+ interactions |
|
| 13.66.De |
Lepton production in e-e+ interactions |
|
| 13.66.Fg |
Gauge and Higgs boson production in e-e+ interactions |
|
| 13.66.Hk |
Production of non-standard model particles in ee+ interactions |
|
| 13.66.Jn |
Precision mesurements in e-e+ interactions |
|
| 13.66.Lm |
Processes in other lepton-lepton interactions |
|
| 13.75.-n |
Hadron-induced low- and intermediate-energy reactions and scattering (energy(less-than-or-equal-to)10 GeV) (for higher energies, see 13.85.-t) |
|
| 13.75.Cs |
Nucleon-nucleon interactions (including antinucleons, deuterons, etc.) (for N-N interactions in nuclei, see 21.30.-x) |
|
| 13.75.Ev |
Hyperon-nucleon interactions |
|
| 13.75.Gx |
Pion-baryon interactions |
|
| 13.75.Jz |
Kaon-baryon interactions |
|
| 13.75.Lb |
Meson-meson interactions |
|
| 13.85.-t |
Hadron-induced high- and super-high-energy interactions (energy>10 GeV) (for low energies, see 13.75.-n) |
|
| 13.85.Dz |
Elastic scattering |
|
| 13.85.Fb |
Inelastic scattering: two-particle final states |
|
| 13.85.Hd |
Inelastic scattering: many-particle final states |
|
| 13.85.Lg |
Total cross sections |
|
| 13.85.Ni |
Inclusive production with identified hadrons |
|
| 13.85.Qk |
Inclusive production with identified leptons, photons, or other nonhadronic particles |
|
| 13.85.Rm |
Limits on production of particles |
|
| 13.85.Tp |
Cosmic-ray interactions (see also 96.50.S- Cosmic rays in interplanetary physics) |
|
| 13.87.-a |
Jets in large-Q2 scattering |
|
| 13.87.Ce |
Production |
|
| 13.87.Fh |
Fragmentation into hadrons |
|
| 13.88.+e |
Polarization in interactions and scattering |
|
| 13.90.+i |
Other topics in specific reactions and phenomenology of elementary particles (restricted to new topics in section 13) |
|
| 14. |
Properties of specific particles |
|
| 14.20.-c |
Baryons (including antiparticles) |
|
| 14.20.Dh |
Protons and neutrons |
|
| 14.20.Gk |
Baryon resonances with S=0 |
|
| 14.20.Jn |
Hyperons |
|
| 14.20.Lq |
Charmed baryons |
|
| 14.20.Mr |
Bottom baryons |
|
| 14.20.Pt |
Dibaryons |
|
| 14.40.-n |
Mesons |
|
| 14.40.Aq |
pi, K, and eta mesons |
|
| 14.40.Cs |
Other mesons with S=C=0, mass<2.5 GeV |
|
| 14.40.Ev |
Other strange mesons |
|
| 14.40.Gx |
Mesons with S=C=B=0, mass>2.5 GeV (including quarkonia) |
|
| 14.40.Lb |
Charmed mesons |
|
| 14.40.Nd |
Bottom mesons |
|
| 14.60.-z |
Leptons |
|
| 14.60.Cd |
Electrons (including positrons) |
|
| 14.60.Ef |
Muons |
|
| 14.60.Fg |
Taus |
|
| 14.60.Hi |
Other charged heavy leptons |
|
| 14.60.Lm |
Ordinary neutrinos (nue, numu, nutau) |
|
| 14.60.Pq |
Neutrino mass and mixing (see also 12.15.Ff Quark and lepton masses and mixing) |
|
| 14.60.St |
Non-standard-model neutrinos, right-handed neutrinos, etc. |
|
| 14.65.-q |
Quarks |
|
| 14.65.Bt |
Light quarks |
|
| 14.65.Dw |
Charmed quarks |
|
| 14.65.Fy |
Bottom quarks |
|
| 14.65.Ha |
Top quarks |
|
| 14.70.-e |
Gauge bosons |
|
| 14.70.Bh |
Photons |
|
| 14.70.Dj |
Gluons |
|
| 14.70.Fm |
W bosons |
|
| 14.70.Hp |
Z bosons |
|
| 14.70.Pw |
Other gauge bosons |
|
| 14.80.-j |
Other particles (including hypothetical) |
|
| 14.80.Bn |
Standard-model Higgs bosons |
|
| 14.80.Cp |
Non-standard-model Higgs bosons |
|
| 14.80.Hv |
Magnetic monopoles |
|
| 14.80.Ly |
Supersymmetric partners of known particles |
|
| 14.80.Mz |
Axions and other Nambu-Goldstone bosons (Majorons, familons, etc.) |
|