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Related papers: A Tumbling Top-Quark Condensate Model

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Standard Model (SM) with 15 Weyl fermions per family (lacking the 16th, the sterile right-handed neutrino $\nu_R$) suffers from mixed gauge-gravitational anomalies tied to baryon number plus or minus lepton number ${\bf B} \pm {\bf L}$…

High Energy Physics - Theory · Physics 2025-03-14 Juven Wang

Flavor changing neutral current (FCNC) interactions for a top quark $t$ decays into $Xq$ with $X$ represents a neutral gauge or Higgs boson, and $q$ a up- or charm-quark are highly suppressed in the Standard Model (SM) due to the…

High Energy Physics - Phenomenology · Physics 2018-03-14 P. Q. Hung , Yu-Xiang Lin , Chrisna Setyo Nugroho , Tzu-Chiang Yuan

We construct a purely fermionic system with spontaneously broken supersymmetry that shares the common feature with a fracton phase of matter. Our model is gapless due to the Nambu-Goldstone mechanism. It shows a ground-state degeneracy with…

High Energy Physics - Theory · Physics 2022-08-24 Hosho Katsura , Yu Nakayama

We study an SU(3)^2 axigluon model introduced by Frampton, Shu, and Wang to explain the recent Fermilab Tevatron observation of a significant positive enhancement in the top quark forward-backward asymmetry relative to standard model…

High Energy Physics - Phenomenology · Physics 2010-12-13 R. Sekhar Chivukula , Elizabeth H. Simmons , C. -P. Yuan

We consider the generation of fermion masses in an emergent model of electroweak symmetry breaking with composite $W,Z$ gauge bosons. A universal bulk fermion profile in a warped extra dimension is used for all fermion flavors. Electroweak…

High Energy Physics - Phenomenology · Physics 2011-01-04 Yanou Cui , Tony Gherghetta , James Stokes

We present a new model based on the SU(3)xSU(2)xU(1) symmetry, in which there is a new consistent set of chiral fermion fields that renders the model free from anomalies. The new fermions do not share the usual family structure of the…

High Energy Physics - Phenomenology · Physics 2013-07-23 Alexandre Alves , E. Ramirez Barreto , D. A. Camargo , A. G. Dias

The Standard Model flavor structure can be explained in theories where the fermions are localized on different points in a compact extra dimension. We show that models with two bulk scalars compactified on an orbifold can produce such…

High Energy Physics - Phenomenology · Physics 2014-11-17 Yuval Grossman , Gilad Perez

We study the properties of vectorlike fermions that have the same gauge charges as the Standard Model lepton doublets, but opposite lepton number. These antileptons undergo decays mediated by heavier scalar leptoquarks, while the symmetries…

High Energy Physics - Phenomenology · Physics 2024-03-25 Innes Bigaran , Bogdan A. Dobrescu , Alessandro Russo

If the gauge fields of the Standard Model propagate in TeV-size extra dimensions, they rapidly become strongly coupled and can form scalar bound states of quarks and leptons. If the quarks and leptons of the third generation propagate in 6…

High Energy Physics - Phenomenology · Physics 2014-11-17 Nima Arkani-Hamed , Hsin-Chia Cheng , Bogdan A. Dobrescu , Lawrence J. Hall

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

While pure Yang-Mills theory feature the centre symmetry, this symmetry is explicitly broken by the presence of dynamical matter. We study the impact of the centre symmetry in such QCD-like theories. In the analytically solvable Schwinger…

High Energy Physics - Lattice · Physics 2012-02-07 Kurt Langfeld , Andreas Wipf

The top quark is one of the least well-studied components of the standard model. In these lectures I discuss the expected properties of the top quark, which will be tested at the Fermilab Tevatron and the CERN Large Hadron Collider. I begin…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Willenbrock

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

The phase diagram of non-compact lattice QED in four dimensions with staggered fermions of charges 1 and $-1/2$ is investigated. The renormalized charges are determined and found to be in agreement with perturbation theory. This is an…

High Energy Physics - Lattice · Physics 2009-10-28 A. Ali Khan

The top quark decay process $\tcups$ is studied in the Standard Model and the Minimal Supersymmetric Standard Model with conserved and violated $R-$parity. In dealing with the heavy quarkonium, $\ups$, production, we take both color-singlet…

High Energy Physics - Phenomenology · Physics 2008-11-26 L. T. Handoko , C. -F. Qiao

We explore corrections to electroweak parameters in the context of Extended Technicolor (ETC) models in which the ETC gauge-boson which generates the top-quark mass carries weak $SU(2)$ charge. For $m_t \sim 150$ GeV there exist potentially…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. S. Chivukula , E. H. Simmons , J. Terning

We study unconventional decays of the top-quark in the framework of SUSY models with spontaneously broken R-parity. In particular we discuss an effective theory which consists of the MSSM plus bilinearly broken R-parity. We demonstrate that…

High Energy Physics - Phenomenology · Physics 2009-09-17 L. Navarro , W. Porod , J. W. F. Valle

An extension of the Standard Model is presented that leads to the possible existence of new gauge bosons with masses in the range of a few TeV. Due to the fact that their couplings to Standard Model fermions are strongly suppressed, it is…

High Energy Physics - Phenomenology · Physics 2018-10-31 Carlos Alvarado , Alfredo Aranda

We consider a minimal renormalizable non-supersymmetric $E_6$ Grand Unified Theory using fundamental representation $27$ for fermions and scalars. The scalar with adjoint representation ${78}$ is also taken for direct breaking of $E_{6}$ to…

High Energy Physics - Phenomenology · Physics 2024-02-07 Chandini Dash , Snigdha Mishra , Sudhanwa Patra , Purushottam Sahu

We analyze the implications of the light gluino scenario for the unification of gauge and Yukawa couplings within the minimal supersymmetric standard model. Within this scheme all fermionic supersymmetric particles are naturally light,…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Carena , L. Clavelli , D. Matalliotakis , H. P. Nilles , C. E. M. Wagner