Selfbreaking technicolor

technicolor gauge interaction which also manages to break itself completely. The technicolor gauge bosons and technifermions are not confined by the technicolor force, but get large masses. Starting with a single technidoublet, one emerges with a complete standard model family of technifermions after the symmetry breaking is complete. This suggests a broad new avenue for model building. A few variations on the theme are mentioned.

model: technicolor
spontaneous symmetry breaking
gauge field theory: SU(4)
gauge field theory: SU(3) x SU(2) x U(1)
mass generation
fermion: condensation
renormalization: beta function

References(31)

Figures(0)

Implications of Dynamical Symmetry Breaking

Steven Weinberg
(
- Harvard U.
)

- Phys.Rev.D 13 (1976) 974-996,
- Phys.Rev.D 19 (1979) 1277-1280 (addendum),
- Also in *Farhi, E. (ed.), Jackiw, R. (ed.): Dynamical Gauge Symmetry Breaking*, 127-149
•
DOI:
- 10.1103/PhysRevD.19.1277

Dynamics of Spontaneous Symmetry Breaking in the Weinberg-Salam Theory

Leonard Susskind
(
- SLAC
)

- Phys.Rev.D 20 (1979) 2619-2625,
- Also in *Farhi, E. (ed.), Jackiw, R. (ed.): Dynamical Gauge Symmetry Breaking*, 154-160
•
DOI:
- 10.1103/PhysRevD.20.2619

Mass Without Scalars

Savas Dimopoulos
(
- Columbia U.
)
,
Leonard Susskind
(
- Stanford U., ITP
)

- Nucl.Phys.B 155 (1979) 237-252,
- Also in *Farhi, E. (ed.), Jackiw, R. (ed.): Dynamical Gauge Symmetry Breaking*, 161-176,
•
DOI:
- 10.1016/0550-3213(79)90364-X

Dynamical Breaking of Weak Interaction Symmetries

Estia Eichten
(
- Harvard U.
)
,
Kenneth D. Lane
(
- Harvard U.
)

- Phys.Lett.B 90 (1980) 125-130,
- Also in *Farhi, E. (ed.), Jackiw, R. (ed.): Dynamical Gauge Symmetry Breaking*, 177-182
•
DOI:
- 10.1016/0370-2693(80)90065-9

Challenges for Extended Technicolor Theories

Savas Dimopoulos
(
- Stanford U., Phys. Dept.
)
,
John R. Ellis
(
- CERN
)

- Nucl.Phys.B 182 (1982) 505-528,
- Also in *Farhi, E. (ed.), Jackiw, R. (ed.): Dynamical Gauge Symmetry Breaking*, 321-344
•
DOI:
- 10.1016/0550-3213(81)90132-2

Raising the Sideways Scale

Bob Holdom
(
- Harvard U. and
- Texas U.
)

- Phys.Rev.D 24 (1981) 1441
•
DOI:
- 10.1103/PhysRevD.24.1441

Techniodor

Bob Holdom
(
- Toronto U. and
- Santa Barbara, KITP
)

- Phys.Lett.B 150 (1985) 301-305
•
DOI:
- 10.1016/0370-2693(85)91015-9

Dynamics of Spontaneous Chiral Symmetry Breaking and Continuum Limit in Quantum Electrodynamics

V.A. Miransky
(
- BITP, Kiev
)

- Nuovo Cim.A 90 (1985) 149-170
•
DOI:
- 10.1007/BF02724229

Chiral Hierarchies and the Flavor Changing Neutral Current Problem in Technicolor

- Phys.Rev.Lett. 57 (1986) 957
•
DOI:
- 10.1103/PhysRevLett.57.957

DISCRIMINATING TECHNICOLOR THEORIES THROUGH FLAVOR CHANGING NEUTRAL CURRENTS: WALKING OR STANDING COUPLING CONSTANTS?

Masako Bando
(
- Kyoto U.
)
,
Takuya Morozumi
(
- Kyoto U.
)
,
Hiroto So
(
- Kyoto U., Yukawa Inst., Kyoto
)
,
Koichi Yamawaki
(
- Nagoya U.
)

- Phys.Rev.Lett. 59 (1987) 389
•
DOI:
- 10.1103/PhysRevLett.59.389

Higher Mass Scales and Mass Hierarchies

- Phys.Lett.B 220 (1989) 223-228
•
DOI:
- 10.1016/0370-2693(89)90041-5

Dynamical Electroweak Symmetry Breaking with Large Anomalous Dimension and t Quark Condensate

- Phys.Lett.B 221 (1989) 177-183
•
DOI:
- 10.1016/0370-2693(89)91494-9

Topcolor: Top quark condensation in a gauge extension of the standard model

Christopher T. Hill
(
- Fermilab
)

- Phys.Lett.B 266 (1991) 419-424
•
DOI:
- 10.1016/0370-2693(91)91061-Y

A Tumbling top quark condensate model

Stephen P. Martin
(
- Florida U.
)

- Phys.Rev.D 46 (1992) 2197-2202
•
e-Print:
- hep-ph/9204204
•
DOI:
- 10.1103/PhysRevD.46.2197

Renormalizable top quark condensate models

Stephen P. Martin
(
- Florida U.
)

- Phys.Rev.D 45 (1992) 4283-4293
•
DOI:
- 10.1103/PhysRevD.45.4283

Top condensation from very massive strongly coupled gauge bosons

Manfred Lindner
(
- CERN
)
,
Douglas Ross
(
- CERN
)

- Nucl.Phys.B 370 (1992) 30-50
•
DOI:
- 10.1016/0550-3213(92)90343-A

Top Quark and Higgs Masses in the Sp(6)-l X U(1)-y Family Model

- Phys.Lett.B 248 (1990) 119-122
•
DOI:
- 10.1016/0370-2693(90)90025-2

Dynamical symmetry breaking solution to the problem of flavor

Stephen F. King
(
- Southampton U.
)

- Phys.Rev.D 45 (1992) 990-992
•
DOI:
- 10.1103/PhysRevD.45.990

Minimal Dynamical Symmetry Breaking of the Standard Model

- Phys.Rev.D 41 (1990) 1647
•
DOI:
- 10.1103/PhysRevD.41.1647

Electroweak Radiative Corrections with an Effective Lagrangian: Four Fermion Processes

D.C. Kennedy
(
- Stanford U., ITP and
- SLAC
)
,
B.W. Lynn
(
- Stanford U., ITP and
- SLAC
)

- Nucl.Phys.B 322 (1989) 1-54
•
DOI:
- 10.1016/0550-3213(89)90483-5

Global symmetry properties of electroweak heavy physics parameters

D.C. Kennedy
(
- Pennsylvania U.
)

- Phys.Lett.B 268 (1991) 86-88
•
DOI:
- 10.1016/0370-2693(91)90927-I

Estimation of oblique electroweak corrections

Michael E. Peskin
(
- SLAC
)
,
Tatsu Takeuchi
(
- SLAC
)

- Phys.Rev.D 46 (1992) 381-409
•
DOI:
- 10.1103/PhysRevD.46.381

Dynamical Model of Elementary Particles Based on an Analogy with Superconductivity. 1.

Yoichiro Nambu
(
- Chicago U., EFI
)
,
G. Jona-Lasinio
(
- Chicago U., EFI
)

- Phys.Rev. 122 (1961) 345-358,
- Also in *Lai, C. H. (Ed.): Gauge Theory Of Weak and Electromagnetic Interactions*, 104-117,
•
DOI:
- 10.1103/PhysRev.122.345

Electroweak symmetry breaking by fourth generation condensates and the neutrino spectrum

Christopher T. Hill
(
- Fermilab
)
,
Markus A. Luty
(
- Chicago U., EFI and
- Chicago U.
)
,
Emmanuel A. Paschos
(
- Dortmund U.
)

- Phys.Rev.D 43 (1991) 3011-3025
•
DOI:
- 10.1103/PhysRevD.43.3011

Group Theory for Unified Model Building

R. Slansky
(
- Los Alamos
)

- Phys.Rept. 79 (1981) 1-128
•
DOI:
- 10.1016/0370-1573(81)90092-2

1-25 of 31
1
2
25 / page