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Standard model without Higgs particles

Abstract

A modification of the standard model of electroweak interactions with the nonlocal Higgs sector is proposed. Proper form of nonlocality makes Higgs particles unobservable after the electroweak symmetry breaking. They appear only as a virtual state because their propagator is an entire function. We discuss some specific consequences of this approach comparing it with the conventional standard model. (author). 12 refs.
Authors:
Publication Date:
Oct 01, 1992
Product Type:
Technical Report
Report Number:
IC-92/368
Reference Number:
SCA: 662210; PA: AIX-24:020299; SN: 93000946074
Resource Relation:
Other Information: PBD: Oct 1992
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; WEINBERG LEPTON MODEL; YUKAWA NONLOCAL THEORY; HIGGS BOSONS; HIGGS MODEL; PROPAGATOR; SYMMETRY BREAKING; 662210; UNIFIED THEORIES AND MODELS
OSTI ID:
10126236
Research Organizations:
International Centre for Theoretical Physics (ICTP), Trieste (Italy)
Country of Origin:
IAEA
Language:
English
Other Identifying Numbers:
Other: ON: DE93616864; TRN: XA9333255020299
Availability:
OSTI; NTIS (US Sales Only); INIS
Submitting Site:
INIS
Size:
[10] p.
Announcement Date:
Jul 04, 2005

Citation Formats

Kovalenko, S G. Standard model without Higgs particles. IAEA: N. p., 1992. Web.
Kovalenko, S G. Standard model without Higgs particles. IAEA.
Kovalenko, S G. 1992. "Standard model without Higgs particles." IAEA.
@misc{etde_10126236,
title = {Standard model without Higgs particles}
author = {Kovalenko, S G}
abstractNote = {A modification of the standard model of electroweak interactions with the nonlocal Higgs sector is proposed. Proper form of nonlocality makes Higgs particles unobservable after the electroweak symmetry breaking. They appear only as a virtual state because their propagator is an entire function. We discuss some specific consequences of this approach comparing it with the conventional standard model. (author). 12 refs.}
place = {IAEA}
year = {1992}
month = {Oct}
}