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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

Extended technicolor (ETC) theories typically require ETC gauge bosons lighter than of order 1 TeV, to perturbatively generate the $t$ quark mass. We point out that explicit models of $t-b$ mass splitting also typically contain additional…

High Energy Physics - Phenomenology · Physics 2009-10-28 Thomas Appelquist , Nick Evans , Stephen B. Selipsky

The extended technicolor theory is a candidate of the physics beyond the standard model. To explain the mass hierarchy of the quarks and leptons, the extended technicolor gauge symmetry must hierarchically break to the technicolor gauge…

High Energy Physics - Phenomenology · Physics 2007-05-23 Noriaki Kitazawa

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

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

We present the determination of the charm quark mass, the masses, and decay constants of charmed mesons using thirteen 2+1 flavor gauge ensembles at five different lattice spacings $a\in[0.05,0.11]$ fm, 8 pion masses $m_{\pi}\in(130,360)$…

High Energy Physics - Lattice · Physics 2025-01-10 Hai-Yang Du , Bolun Hu , Mengchu Cai , Ying Chen , Heng-Tong Ding , Xiangyu Jiang , Chuan Liu , Liuming Liu , Yu Meng , Peng Sun , Ji-Hao Wang , Yi-Bo Yang , Dian-Jun Zhao

When technicolor (TC), QCD, extended technicolor (ETC) and other interactions become coupled through their different Schwinger-Dyson equations, the solution of these equations are modified compared to those of the isolated equations. The…

High Energy Physics - Phenomenology · Physics 2020-07-22 A. A. Natale , A. Doff

We analyze two versions of the extended technicolor (ETC) incorporating the top quark condensate via the flavor-universal coloron type topcolor $SU(3)_1 \times SU(3)_2$: A straightforward top-mode ETC having quarks and techniquarks assigned…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hidenori Fukano , Koichi Yamawaki

The origin of mass must lie in physics beyond the Standard Model. Dynamical electroweak symmetry breaking models like technicolor can generate masses for the W and Z bosons. Providing the large top quark mass and large top-bottom mass…

High Energy Physics - Phenomenology · Physics 2007-05-23 Elizabeth H. Simmons

We consider constraints on models in which a top quark mass is generated through unenhanced extended technicolor interactions. The deviation in the $\rho$ parameter from unity and $B$--$\overline{B}$ mixing could be large, but given the…

High Energy Physics - Phenomenology · Physics 2009-09-15 L. Randall

LEP precision measurements of the $Zb\bar{b}$ vertex coupling are sufficiently accurate to see the non-oblique corrections from the heavy gauge boson responsible for the large top mass in standard extended tecnicolour models. If the ETC…

High Energy Physics - Phenomenology · Physics 2009-10-28 Nick Evans

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

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 consider a minimal technicolor model in which the ordinary and technicolor sectors are coupled by a {\it massless} scalar doublet. When technicolor interactions become strong, the resulting technicolor condensate not only breaks the…

High Energy Physics - Phenomenology · Physics 2009-09-11 Christopher D. Carone , Howard Georgi

We point out that the flavor problem in theories with dynamical electroweak symmetry breaking can be effectively decoupled if the physics above the TeV scale is strongly conformal, and the electroweak order parameter has a scaling dimension…

High Energy Physics - Phenomenology · Physics 2009-11-10 Markus A. Luty , Takemichi Okui

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

We consider the question of vacuum alignment in the recently proposed "composite technicolor" (CTC) models. In order for these models to work, an "ultrafermion" condensate must align in a particular way, driven by the competition between…

High Energy Physics - Phenomenology · Physics 2009-10-22 Markus A. Luty

I describe a technicolor model (without walking) of all interactions up to energies of the order of 1000~TeV. The low energy extended technicolor model has the CTSM form. But at intermediate energy scales, additional interactions are…

High Energy Physics - Phenomenology · Physics 2009-09-11 Howard Georgi

I propose a resolution of the strong CP problem of quarks based on vacuum alignment in theories of dynamically broken electroweak and flavor symmetries. Mixing in the neutral B and K--meson systems is used to restrict the form of quark mass…

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