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Related papers: Technicolor Signatures at the High Energy Muon Col…

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In multiscale and topcolor-assisted models of walking technicolor, relatively light spin-one technihadrons $\rho_T$ and $\omega_T$ exist and are expected to decay as $\rho_T \to W \pi_T, Z \pi_T$ and $\omega_T \to \gamma \pi_T$. For…

High Energy Physics - Phenomenology · Physics 2011-01-13 Estia Eichten , Kenneth Lane , John Womersley

The motivations for studying dynamical scenarios of electroweak and flavor symmetry breaking are reviewed and the latest ideas, especially topcolor-assisted technicolor, are summarized. Technicolor's observable low-energy signatures are…

High Energy Physics - Phenomenology · Physics 2009-10-31 Kenneth Lane

In modern technicolor models, there exist very narrow spin-zero and spin-one neutral technihadrons---$pi^0_T$, $rho^0_T$ and $omega_T$---with masses of a few 100 GeV. The large coupling of $\pi^0_T$ to $\mu^+\mu^-$, the direct coupling of…

High Energy Physics - Phenomenology · Physics 2009-10-31 Estia Eichten , Kenneth Lane , John Womersley

New strong dynamics at the energy scale ~ 1 TeV is an attractive and elegant theoretical ansatz for the origin of electroweak symmetry breaking. We review here the theoretical models for strong dynamics, particularly, technicolor theories…

High Energy Physics - Phenomenology · Physics 2009-10-31 Pushpalatha Bhat , Estia Eichten

Muon colliders might greatly extend the energy frontier of collider physics. One can contemplate circular colliders with center-of-mass energies in excess of 10 TeV. Some physics issues that might be relevant at such a machine are…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. S. Berger

This paper extends an earlier one describing the Higgs boson $H$ as a light composite scalar in a strong extended technicolor model of electroweak symmetry breaking. The Higgs mass $M_H$ is made much smaller than $\Lambda_{ETC}$ by tuning…

High Energy Physics - Phenomenology · Physics 2017-07-04 Kenneth Lane , Lukas Pritchett

We consider the implications of an extended color group, $SU\left( 3\right) _I\times SU\left( 3\right) _{II}$, spontaneously broken to $SU\left( 3\right) _c$ at a TeV or lower scale, for the hadronic colliders. The associated massive color…

High Energy Physics - Phenomenology · Physics 2009-10-28 D. A. Dicus , B. Dutta , S. Nandi

While it is natural for supersymmetric particles to be well within the mass range of the large hadron collider, it is possible that the sparticle masses could be very heavy. Signatures are examined at a very high energy hadron collider and…

High Energy Physics - Phenomenology · Physics 2007-05-23 I Hinchliffe , F. E. Paige

Pair-production of heavy top quarks at the Tevatron Collider is significantly enhanced by the color--octet technipion, $\eta_T$, occurring in multiscale models of walking technicolor. We discuss $\bar tt$ rates for $m_t = 170$ GeV and…

High Energy Physics - Phenomenology · Physics 2009-10-28 Estia Eichten , Kenneth Lane

We analyze collider signatures of massive color-octet bosons whose couplings to quarks are suppressed. Gauge invariance forces the octets to couple at tree level only in pairs to gluons, with a strength set by the QCD gauge coupling. For a…

High Energy Physics - Phenomenology · Physics 2009-02-18 Bogdan A. Dobrescu , Kyoungchul Kong , Rakhi Mahbubani

Muon colliders offer special opportunities to discover and study new physics. With the high intensity source of muons at the front end, orders of magnitude improvements would be realized in searches for rare muon processes, in deep…

High Energy Physics - Phenomenology · Physics 2009-10-31 V. Barger

In multiscale and topcolor-assisted models of walking technicolor, light, spin-one technihadrons can exist with masses of a few hundred GeV; they are expected to decay as rho_T -> W pi_T. For technirho masses ~200 GeV and technipion masses…

High Energy Physics - Phenomenology · Physics 2009-10-31 Stephen Mrenna , John Womersley

Muon Colliders have unique technical and physics advantages and disadvantages when compared with both hadrons and electron machines. They should be regarded as complementary. Parameters are given of a 4 TeV high luminosity muon-muon…

Accelerator Physics · Physics 2008-11-26 R. B. Palmer , J. C. Gallardo

We briefly review the basic structure of modern--day technicolor theories. We then discuss the signatures for technicolor as they were in its early days, the searches that have been recently performed at the Tevatron and LEP colliders, and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Kenneth Lane

Precision electroweak data, a light higgs and LHC searches for new spin one particles are all very constraining on technicolor models. We use a holographic model of walking techicolor (WTC) gauge dynamics, tuned to produce a light higgs and…

High Energy Physics - Phenomenology · Physics 2019-05-15 Alexander Belyaev , Azaria Coupe , Nick Evans , Marc Scott

It is shown that at muon colliders with the energy in the region of 100 TeV the process of coherent pair creation by the muon in the field of the opposing beam becomes important and imposes some limitations on collider parameters.

High Energy Physics - Experiment · Physics 2009-10-31 Valery Telnov

Parameters are given of 4 TeV and 0.5 TeV (c-of-m) high luminosity muon-muon Colliders. We discuss the various systems, starting from the proton accelerator needed to generate the muons and proceeding through muon cooling, acceleartion and…

Accelerator Physics · Physics 2009-09-25 R. B. Palmer , J. C. Gallardo

Muon colliders offer the possibility to go to very high energies with relatively small circular colliders, energies up to 10 or 14 TeV are envisioned. Due to their very clean collider environment they provide a fantastic tool to search for…

High Energy Physics - Phenomenology · Physics 2023-05-23 Jürgen Reuter

We study the signatures for new TeV resonances that couple to top or bottom quarks both at the Tevatron Run II and at the LHC. We find that it is possible to study these resonances when they are produced in association with a pair of heavy…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tao Han , German Valencia , Yili Wang

We discuss the phenomenology of the lightest SU(3)_C singlet and non-singlet technihadrons in the Straw Man Model of low-scale technicolor (TCSM). The technihadrons are assumed to be those arising in topcolor--assisted technicolor models in…

High Energy Physics - Phenomenology · Physics 2011-01-13 Kenneth Lane , Stephen Mrenna
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