1998/10/28 by Stephen Godfrey, Tao Han, Pat Kalyniak
Physics and Astronomy · #Crystallography #Electroweak interaction #High-Energy Particle Collisions Research #Luminosity #Omega #Particle physics #Particle physics theoretical and experimental studies #Physics #Production (economics) #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #hep-ph
paper · pdf · doi:10.1103/physrevd.59.095006
published as Phys.Rev. D59 (1999) 095006 · LaTex file uses revtex, epsfig, 9 pages with 7 postscript figures
arxiv created 1998/10/28 · openalex publication_date 1999/04/01 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
In a strongly interacting electroweak sector with an isosinglet vector state, such as the techni-omega, \ensuremathωT, the direct \ensuremathωTZ\ensuremathγ coupling implies that an \ensuremathωT can be produced by Z\ensuremathγ fusion in e\ensuremathγ collisions. This is a unique feature for high energy e+e^\ensuremath- or e^\ensuremath-e^\ensuremath- colliders operating in an e\ensuremathγ mode. We consider the processes e^\ensuremath-\stackrel\ensuremath→\ensuremathγe^\ensuremath-Z\ensuremathγ and e^\ensuremath-\stackrel\ensuremath→\ensuremathγe^\ensuremath-W+W^\ensuremath-Z, both of which proceed via an intermediate \ensuremathωT. We find that at a 1.5 TeV e+e^\ensuremath- linear collider operating in an e\ensuremathγ mode with an integrated luminosity of 200 fb^\ensuremath-1, an \ensuremathωT can be discovered for a broad range of masses and widths.