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Heavier fermions and fine-tuning problem in top condensate scheme

Abstract

The analysis in the bubble approximation indicates that a heavier quark-lepton generation with the degenerate mass m{sub U} in the range of 163-353 GeV added in the top condensate scheme could make the momentum cut-off {Lambda} come down to 10{sup 6}-5x10{sup 3} GeV when m{sub t} = 160 GeV is taken. This could greatly alleviate the fine-tuning problem. The Higgs boson {Phi}{sup 0}{sub s}{sup 0} will obey the mass constraint 2 m{sub t}
Authors:
Publication Date:
Sep 01, 1992
Product Type:
Technical Report
Report Number:
IC-92/288
Reference Number:
SCA: 662210; PA: AIX-24:020296; SN: 93000946071
Resource Relation:
Other Information: PBD: Sep 1992
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; UNIFIED GAUGE MODELS; LEPTONS; QUARKS; COUPLING CONSTANTS; HIGGS BOSONS; LAGRANGIAN FUNCTION; MASS; PROPAGATOR; SYMMETRY BREAKING; 662210; UNIFIED THEORIES AND MODELS
OSTI ID:
10126222
Research Organizations:
International Centre for Theoretical Physics (ICTP), Trieste (Italy)
Country of Origin:
IAEA
Language:
English
Other Identifying Numbers:
Other: ON: DE93616861; TRN: XA9333245020296
Availability:
OSTI; NTIS (US Sales Only); INIS
Submitting Site:
INIS
Size:
[10] p.
Announcement Date:
Jul 04, 2005

Citation Formats

Bangrong, Zhou. Heavier fermions and fine-tuning problem in top condensate scheme. IAEA: N. p., 1992. Web.
Bangrong, Zhou. Heavier fermions and fine-tuning problem in top condensate scheme. IAEA.
Bangrong, Zhou. 1992. "Heavier fermions and fine-tuning problem in top condensate scheme." IAEA.
@misc{etde_10126222,
title = {Heavier fermions and fine-tuning problem in top condensate scheme}
author = {Bangrong, Zhou}
abstractNote = {The analysis in the bubble approximation indicates that a heavier quark-lepton generation with the degenerate mass m{sub U} in the range of 163-353 GeV added in the top condensate scheme could make the momentum cut-off {Lambda} come down to 10{sup 6}-5x10{sup 3} GeV when m{sub t} = 160 GeV is taken. This could greatly alleviate the fine-tuning problem. The Higgs boson {Phi}{sup 0}{sub s}{sup 0} will obey the mass constraint 2 m{sub t}
place = {IAEA}
year = {1992}
month = {Sep}
}