SCALE-INVARIANT HYPERCOLOR MODEL AND A DILATON

[1] BARDEEN WA, UNPUB SPONTANEOUS SY

[2] BARDEEN WA, UNPUB DILATON CHIRAL

[3] CHIRAL SYMMETRY-BREAKING IN LATTICE ELECTRODYNAMICS [J]. NUCLEAR PHYSICS B, 1984, 230 (02) : 222 - 240

[4] MASS WITHOUT SCALARS [J]. NUCLEAR PHYSICS B, 1979, 155 (01) : 237 - 252

[5] DYNAMICAL BREAKING OF WEAK INTERACTION SYMMETRIES [J]. PHYSICS LETTERS B, 1980, 90 (1-2) : 125 - 130

[6] Farhi E., 1981, Physics Reports, V74, P277, DOI 10.1016/0370-1573(81)90173-3

[7] FORMIN PI, 1983, RIV NUOVO CIMENTO SO, V6, P1

[8] SCHWINGER-DYSON EQUATION FOR MASSLESS VECTOR THEORY AND ABSENCE OF A FERMION POLE [J]. NUCLEAR PHYSICS B, 1976, 117 (01) : 250 - 264

[9] UNEXTENDED HYPERCOLOR AND UNIFICATION [J]. PHYSICAL REVIEW LETTERS, 1981, 47 (21) : 1511 - 1513

[10] SOME TESTS FOR WHETHER A NARROW NEUTRAL RESONANCE CAN BE A HIGGS PARTICLE [J]. PHYSICS LETTERS B, 1984, 135 (1-3) : 196 - 202

[1] BARDEEN WA, UNPUB SPONTANEOUS SY

[2] BARDEEN WA, UNPUB DILATON CHIRAL

[3] CHIRAL SYMMETRY-BREAKING IN LATTICE ELECTRODYNAMICS [J]. NUCLEAR PHYSICS B, 1984, 230 (02) : 222 - 240

[4] MASS WITHOUT SCALARS [J]. NUCLEAR PHYSICS B, 1979, 155 (01) : 237 - 252

[5] DYNAMICAL BREAKING OF WEAK INTERACTION SYMMETRIES [J]. PHYSICS LETTERS B, 1980, 90 (1-2) : 125 - 130

[6] Farhi E., 1981, Physics Reports, V74, P277, DOI 10.1016/0370-1573(81)90173-3

[7] FORMIN PI, 1983, RIV NUOVO CIMENTO SO, V6, P1

[8] SCHWINGER-DYSON EQUATION FOR MASSLESS VECTOR THEORY AND ABSENCE OF A FERMION POLE [J]. NUCLEAR PHYSICS B, 1976, 117 (01) : 250 - 264

[9] UNEXTENDED HYPERCOLOR AND UNIFICATION [J]. PHYSICAL REVIEW LETTERS, 1981, 47 (21) : 1511 - 1513

[10] SOME TESTS FOR WHETHER A NARROW NEUTRAL RESONANCE CAN BE A HIGGS PARTICLE [J]. PHYSICS LETTERS B, 1984, 135 (1-3) : 196 - 202