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Topcolor--assisted technicolor provides a dynamical explanation for electroweak and flavor symmetry breaking and for the large mass of the top quark without unnatural fine tuning. A major challenge is to generate the observed mixing between…

High Energy Physics - Phenomenology · Physics 2016-08-24 Kenneth Lane

I present a model of topcolor-assisted technicolor that can have topcolor breaking of the desired pattern, hard masses for all quarks and leptons, mixing among the heavy and light generations, and explicit breaking of all technifermion…

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

In this talk we review the physics of top-quark mass generation in models of dynamical electroweak symmetry breaking and the constraints on this physics arising from limits on the deviation of the weak interaction $\rho$-parameter from one.…

High Energy Physics - Phenomenology · Physics 2011-03-02 R. Sekhar Chivukula , Bogdan Dobrescu , John Terning

We propose a new mechanism in which all of the electroweak symmetry breaking is driven by a natural top quark condensate, produced by topcolor interactions at a multi-TeV scale. The scheme allows the observed top quark mass, and acceptable…

High Energy Physics - Phenomenology · Physics 2009-10-30 Bogdan A. Dobrescu , Christopher T. Hill

Technicolor, with extended technicolor, is the theory of dynamical electroweak and flavor symmetry breaking at energies far below the Planck scale. To motivate it, I describe the most important difficulties of the standard electroweak model…

High Energy Physics - Phenomenology · Physics 2016-09-01 Kenneth Lane

The motivations for studying dynamical scenarios of electroweak and flavor symmetry breaking are reviewed and the latest ideas, especially topcolor-assisted technicolor, are summarized. Several technicolor signatures at the Tevatron and…

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

We construct a prototype of topcolor--assisted technicolor in which, although both top and bottom quarks acquire some mass from extended technicolor, strong $U(1)$ couplings of technifermions are isospin symmetric and all gauge anomalies…

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

We present a model of dynamical electroweak symmetry breaking in which the splitting between the top and bottom quark masses arises naturally. The W and Z masses are produced by a minimal technicolor sector, the top quark mass is given by…

High Energy Physics - Phenomenology · Physics 2016-08-25 Bogdan A. Dobrescu , Elizabeth H. Simmons

We review the status of and recent developments in dynamical electroweak symmetry breaking, concentrating on the ideas of technicolour and top quark condensates. The emphasis is on the essential physical ideas and experimental implications…

High Energy Physics - Phenomenology · Physics 2010-12-17 Stephen F King

After briefly remarking on alternatives for breaking the electroweak symmetry, I discuss the implication that recent precision experiments at LEP have for the symmetry breaking sector. The difficulties associated with generating fermion…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. D. Peccei

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 this note I provide a brief description of models of dynamical electroweak symmetry breaking, including walking technicolor, top-color assisted technicolor, the top-quark seesaw model, and little higgs theories.

High Energy Physics - Phenomenology · Physics 2007-05-23 R. Sekhar Chivukula

We consider a supersymmetric QCD with soft supersymmetry breaking terms as the dynamics for the electroweak symmetry breaking. We find various advantages compared to the non-supersymmetric models, such as a natural incorporation of the…

High Energy Physics - Phenomenology · Physics 2011-01-28 Hiraku Fukushima , Ryuichiro Kitano , Masahiro Yamaguchi

Technicolor and other theories of dynamical electroweak symmetry breaking invoke chiral symmetry breaking triggered by strong gauge-dynamics, analogous to that found in QCD, to explain the observed W, Z, and fermion masses. In this talk we…

High Energy Physics - Lattice · Physics 2011-05-18 R. Sekhar Chivukula , Elizabeth H. Simmons

We describe a class of models of electroweak symmetry breaking that involves strong dynamics and top quark condensation. A new scheme based upon a seesaw mechanism appears particularly promising. Various implications for the first-stage…

High Energy Physics - Phenomenology · Physics 2009-10-31 Christopher T. Hill

We report first results from the investigation on probing dynamical mechanism of the electroweak symmetry breaking using top quark. We consider the case where the top mass originates from a fermion-antifermion pair condensate, which…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. Asaka , N. Maekawa , T. Moroi , Y. Shobuda , Y. Sumino

In strong dynamical schemes for electroweak symmetry breaking the third generation must be treated in a special manner, owing to the heavy top quark. This potentially leads to new flavor physics involving the members of the third generation…

High Energy Physics - Phenomenology · Physics 2009-10-09 G. Buchalla , G. Burdman , C. T. Hill , D. Kominis

In these lectures we present the motivation for dynamical electroweak symmetry breaking and its most popular realization, technicolor. We introduce the basic ideas of technicolor and its companion theory of flavor, extended technicolor. We…

High Energy Physics - Phenomenology · Physics 2016-10-26 Kenneth Lane

Models of top condensation can provide both a compelling solution to the hierarchy problem as well as an explanation of why the top-quark mass is large. The spectrum of such models, in particular topcolor-assisted technicolor, includes…

High Energy Physics - Phenomenology · Physics 2015-05-28 Yanou Cui , Zhenyu Han , Matthew D. Schwartz

We argue that extended technicolor augmented with topcolor requires that all mixing between the third and the first two quark generations resides in the mixing matrix of left-handed down quarks. Then, the anti-B_d--B_d mixing that occurs in…

High Energy Physics - Phenomenology · Physics 2009-10-31 Gustavo Burdman , Kenneth Lane , Tonguc Rador
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