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Related papers: A New Model of Topcolor-Assisted Technicolor

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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. I briefly review the basics of topcolor-assisted technicolor,…

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

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

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 study the constraints on models of topcolor-assisted technicolor arising from measurements of high-$E_T$ jets and high-mass lepton pairs at the Tevatron collider. Existing data can eliminate models that have appeared in the literature.

High Energy Physics - Phenomenology · Physics 2009-10-30 Yumian Su , Gian Franco Bonini , Kenneth Lane

A condensate, $\overline{t}t$, arising from $O(TeV)$ scale ``topcolor,'' in addition to technicolor (and ETC) may naturally explain the gauge hierarchy, the large top quark mass, and contains a rich system of testable consequences. A…

High Energy Physics - Phenomenology · Physics 2011-01-27 Christopher T. Hill

Topcolor and topcolor-assisted technicolor provide examples of dynamical electroweak symmetry breaking which include top-condensation, thereby naturally incorporating a heavy top quark. In this note we discuss the roles of the…

High Energy Physics - Phenomenology · Physics 2009-09-11 R. Sekhar Chivukula , Howard Georgi

We propose and discuss the phenomenology of a Topcolor-assisted Technicolor (TC2) model with a flavor-universal hypercharge sector. After discussing the symmetry breaking pattern and low-energy effective Lagrangian, we examine various…

High Energy Physics - Phenomenology · Physics 2008-11-26 Felix Braam , Michael Flossdorf , R. Sekhar Chivukula , Stefano Di Chiara , Elizabeth H. Simmons

Recently, Hill has proposed a model in which new, potentially low-energy, top-color interactions produce a top-condensate ({\em a la} Nambu---Jona-Lasinio) and accommodate a heavy top quark, while technicolor is responsible for producing…

High Energy Physics - Phenomenology · Physics 2016-09-01 R. S. Chivukula , B. A. Dobrescu , J. Terning

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 calculate the rates for lepton number violating processes via the exchange of the Z' boson occuring in top-color assisted technicolor. The current experimental limits on muon electron conversion in Ti nuclei allow for a mass of the new…

High Energy Physics - Phenomenology · Physics 2016-08-25 Tonguc Rador

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

We review a class of dynamical models in which top condensation occurs at the weak scale, giving rise to the large top quark mass and other phenomena. This typically requires a color embedding, $SU(3)_c \rightarrow SU(3)_1\times SU(3)_2$.…

High Energy Physics - Phenomenology · Physics 2016-09-06 Christopher T. Hill

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

We construct a complete, realistic, and natural UV completion of minimal conformal technicolor that explains the origin of quark and lepton masses and mixing angles. As in "bosonic technicolor", we embed conformal technicolor in a…

High Energy Physics - Phenomenology · Physics 2015-05-20 Jared A. Evans , Jamison Galloway , Markus A. Luty , Ruggero Altair Tacchi

Using precision electroweak data, we put limits on ``natural'' top-color assisted technicolor models. Generically the new $U(1)$ gauge bosons in these models must have masses larger than roughly 2 TeV, although in certain (seemingly…

High Energy Physics - Phenomenology · Physics 2011-01-13 R. S. Chivukula , J. Terning

We present a one-doublet extended technicolor model, with all fermions in fundamental representations. The bare lagrangian has no explicit mass terms but generates masses through gauge symmetry breaking by purely QCD-like dynamics. The…

High Energy Physics - Phenomenology · Physics 2014-11-17 Tom Appelquist , Nick Evans

We have carried out numerical studies of vacuum alignment in technicolor models of electroweak and flavor symmetry breaking. The goal is to understand alignment's implications for strong and weak CP nonconservation in quark interactions. In…

High Energy Physics - Phenomenology · Physics 2009-10-31 Kenneth Lane , Tonguc Rador , Estia Eichten

The nontrivial boundary conditions (BC's) for the Topcolor breaking are investigated in the context of the TeV-scale extra dimension scenario. In the gauge symmetry breaking mechanism via the BC's we do not need to incorporate a dynamical…

High Energy Physics - Phenomenology · Physics 2009-11-10 Michio Hashimoto , Deog Ki Hong

The nontrivial boundary conditions for the Topcolor breaking are investigated in the context of the TeV-scale extra dimension scenario. We present a six dimensional model where the top and bottom quarks in the bulk have the Topcolor charge…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michio Hashimoto

A topcolor model is presented that contains both composite and fundamental scalar fields. Strong dynamics accounts for most of the top quark mass and part of the electroweak symmetry breaking scale. The fundamental scalar is weakly coupled…

High Energy Physics - Phenomenology · Physics 2009-10-31 Alfredo Aranda , Christopher D. Carone
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