Supergauge invariant extension of the Higgs mechanism and a model for the electron and its neutrino
about
Supersymmetry at ordinary energies. II. R invariance, Goldstone bosons, and gauge-fermion massesPseudo-scalar Higgs boson production at N[Formula: see text]LO[Formula: see text]+N[Formula: see text]LL[Formula: see text].Lower limits on R-parity-violating couplings in supersymmetric models with light squarks.Search for Baryon-Number Violating Ξ_{b}^{0} Oscillations.Is the CNMSSM more credible than the CMSSM?ULTRAHIGH ENERGY COSMIC RAYS: THE STATE OF THE ART BEFORE THE AUGER OBSERVATORYSearch for Supersymmetry in pp Collisions at sqrt[s]=13 TeV in the Single-Lepton Final State Using the Sum of Masses of Large-Radius JetsSearch for supersymmetry with razor variables inppcollisions ats=7 TeVSearches for electroweak neutralino and chargino production in channels with Higgs,Z, andWbosons inppcollisions at 8 TeVSearch for neutral MSSM Higgs bosons decaying to a pair of tau leptons in pp collisionsInclusive Search for Supersymmetry Using Razor Variables inppCollisions ats=7 TeVInclusive search for squarks and gluinos inppcollisions ats=7 TeVSearch for a light charged Higgs boson in top quark decays in pp collisions at $ \sqrt {s} = 7\;TeV $Search for new physics in same-sign dilepton events in proton-proton collisions at [Formula: see text]Search for electroweak production of charginos and neutralinos in WH events in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeVSearch for new phenomena with the $$M_{\mathrm {T2}}$$ M T 2 variable in the all-hadronic final state produced in proton–proton collisions at $$\sqrt{s} = 13$$ s = 13 $$\,\text {TeV}$$ TeVSearch for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeVSearch for top squark pair production in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV using single lepton eventsSearch for new phenomena with multiple charged leptons in proton–proton collisions at $$\sqrt{s}= 13$$ s = 13 $$\,\text {TeV}$$ TeVSearch for physics beyond the standard model in events with two leptons of same sign, missing transverse momentum, and jets in proton–proton collisions at $$\sqrt{s} = 13\,\text {TeV} $$ s = 13 TeVSearch for supersymmetry in multijet events with missing transverse momentum in proton-proton collisions at 13 TeVSearch for supersymmetry in the all-hadronic final state using top quark tagging in pp collisions at s=13 TeVSearch for supersymmetry in events with one lepton and multiple jets in proton-proton collisions at s=13 TeVInclusive search for supersymmetry using razor variables in pp collisions at s=13 TeVSearch for dark matter particles in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using the razor variablesSearch for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeVPhenomenological MSSM interpretation of CMS searches in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeVSearch for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeVSearch for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jetsSearch for supersymmetry inppcollisions ats=8 TeVin final states with boostedWbosons andbjets using razor variablesSearch for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeVSearch for a light charged Higgs boson decaying to c s ¯ $$ \mathrm{c}\overline{\mathrm{s}} $$ in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeVSearch for a charged Higgs boson in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeVSearch for supersymmetry using razor variables in events withb-tagged jets inppcollisions ats=8 TeVSearch forR-Parity Violating Supersymmetry Using Like-Sign Dielectrons inpp¯Collisions at√s=1.8TeVSupersymmetry and fundamental interactions in the region of the fermi scaleSupersymmetry (fermi-bose symmetry): A new invariance of quantum field theorySummary of the searches for squarks and gluinos using s = 8 $$ \sqrt{s}=8 $$ TeV pp collisions with the ATLAS experiment at the LHCProbing the μνSSM with light scalars, pseudoscalars and neutralinos from the decay of a SM-like Higgs boson at the LHCSearch for Pair Production of Scalar Top Quarks inR-Parity Violating Decay Modes inpp¯Collisions ats=1.8 TeV
P2860
Q27350471-4D388505-31CA-4971-AE32-1EF4D6D67216Q42141335-F6A4BD78-19DB-4056-8757-043707FC5DDDQ49255089-2F9616BB-E325-4655-A361-509320F5F102Q50011643-F676DF95-8E47-42DC-A38E-5833FCE83C56Q55966595-B6D3CAA1-B320-4CFE-8B5F-24854C186646Q56083158-C203697C-51F2-4C9C-A289-9C792C5CA0F5Q56481568-4DAEF7F0-10AD-4014-BA04-E86BC0C28EC9Q56635661-8C0621F3-D7F6-46F2-A714-CF6F41154AA1Q56637227-F2967E0B-69DE-485B-B94D-6E41988B2C9DQ56640847-3CFB6E8E-A7FF-4BD0-A889-9FDC622B1CDDQ56698688-743AD9B7-4C48-4B95-A388-36D5EA97A7C5Q56742465-F0CB8FBF-45B3-4A61-B0CA-EADF47242EB7Q56742834-0C078EF0-4ACB-40E5-A63E-9A8C468CF8B8Q56881512-7F68B596-F88F-4B60-887C-AEFE173BBAFFQ56896777-1A9A406A-4A64-450E-8B33-54DE74FC0CB2Q56896888-B93DC5B6-6EBD-455D-A87A-A06B6B55B9CFQ56897026-50560112-ECCA-4624-8101-E6310CF571A2Q56897140-A827F49F-60B3-4107-9383-8B558D16095AQ56897238-A731C5CD-4D7F-49B7-ABBB-5D57AC7DF87DQ56897487-0C47AB3E-4371-4283-9F32-6213F06D773EQ56897510-0DBBC75B-17E0-4042-B678-24ACDCE0FDA4Q56897754-B9CBBCDA-BB6A-4C1F-9013-E160FB7CF5DBQ56898969-2900B0D0-9653-4FC3-B1B3-7F332CFE0F97Q56899174-BF763932-CBAF-454C-9F64-4749CB196E41Q56899275-8ED33947-6468-4404-9FE1-AE837AE0A982Q56899492-9A3EEA4F-6004-4DC3-B4E1-CEFAF4BF0898Q56899635-19A4D3B2-15A5-41D9-9471-D2C9D3D9FC78Q56899741-0A1AF5B7-6137-499C-9ED9-D4A82F2D6B0BQ56900118-2624EF18-ECD0-4087-9501-F571D2947316Q56900671-FBCE7C00-44AE-4A0B-AD21-A28907E9DC70Q56901688-9CDB5DFE-86AB-4F88-B87A-3A6C410B2C44Q56901841-4346D34E-86F2-4288-8EE9-7B809D687581Q56902000-47BFFEC3-B042-44FA-928B-7157E6FB015DQ56903356-32DD1EC1-4DAE-456D-A2BD-0C744B5CE979Q56942618-16284FEE-6D27-4658-99D6-FD092418F3B9Q56973718-ECD3E3CD-504C-48C8-A8E7-113B8D48EE1BQ56973949-9AFDF7FE-DC32-4157-ABA3-98F54DAEB6E8Q57007758-8C20F812-2168-4D9B-A861-3BF95A09FCC9Q57722923-0D7DEC13-ABD3-487B-A97B-9627812E36D9Q57741778-4411C386-B63D-4DE2-9FCB-35CAF3AC41F4
P2860
Supergauge invariant extension of the Higgs mechanism and a model for the electron and its neutrino
description
article
@en
im Januar 1975 veröffentlichter wissenschaftlicher Artikel
@de
wetenschappelijk artikel
@nl
наукова стаття, опублікована в січні 1975
@uk
ലേഖനം
@ml
name
Supergauge invariant extension ...... the electron and its neutrino
@en
Supergauge invariant extension ...... the electron and its neutrino
@nl
type
label
Supergauge invariant extension ...... the electron and its neutrino
@en
Supergauge invariant extension ...... the electron and its neutrino
@nl
prefLabel
Supergauge invariant extension ...... the electron and its neutrino
@en
Supergauge invariant extension ...... the electron and its neutrino
@nl
P1433
P1476
Supergauge invariant extension ...... the electron and its neutrino
@en
P2093
Pierre Fayet
P304
P356
10.1016/0550-3213(75)90636-7
P577
1975-01-01T00:00:00Z