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If one takes naturalness seriously and also assumes a weakly coupled extension of the Standard Model (SM) then there are predictions for phenomenology that can be inferred in a model independent framework. The first such prediction is that…

High Energy Physics - Phenomenology · Physics 2008-11-26 Patrick Meade , Matthew Reece

The littlest Higgs model with T-parity, which is called $LHT$ model, predicts the existence of the new particles, such as heavy top quark, heavy gauge bosons, and mirror fermions. We calculate the one-loop contributions of these new…

High Energy Physics - Phenomenology · Physics 2008-12-18 Li Ding , Chong-Xing Yue

The recent ATLAS and CMS experiments show the first observations of a new particle in the search for the Standard Model Higgs boson at the LHC. We revisit the theoretical inconsistency of the fundamental high-energy cutoff with the…

High Energy Physics - Phenomenology · Physics 2015-06-12 She-Sheng Xue

We discuss the role of the top-quark Yukawa coupling $y_t$ concerning the hierarchy problem and construct an alternative scheme to the conventional solutions with top partners. In traditional models, like SUSY or composite Higgs, top…

High Energy Physics - Phenomenology · Physics 2023-09-13 Andreas Bally , Yi Chung , Florian Goertz

We present holographic desciptions of dynamical electroweak symmetry breaking models that incorporate the top mass generation mechanism. The models allow computation of the spectrum in the presence of large anomalous dimensions due to…

High Energy Physics - Phenomenology · Physics 2017-09-20 Will Clemens , Nick Evans , Marc Scott

The twin Higgs mechanism is a solution to the little hierarchy problem in which the top partner is neutral under the Standard Model (SM) gauge group. The simplest mirror twin Higgs (MTH) model -- where a $\mathbf{Z}_2$ symmetry copies each…

High Energy Physics - Phenomenology · Physics 2022-09-13 Keisuke Harigaya , Robert McGehee , Hitoshi Murayama , Katelin Schutz

In models of electroweak symmetry breaking in which the SM fermions get their masses by mixing with composite states, it is natural to expect the top quark to show properties of compositeness. We study the phenomenological viability of…

High Energy Physics - Phenomenology · Physics 2010-03-19 Alex Pomarol , Javi Serra

Anomalously light fermionic partners of the top quark often appear in explicit constructions, such as the 5d holographic models, where the Higgs is a light composite pseudo Nambu-Goldstone boson and its potential is generated radiatively by…

High Energy Physics - Phenomenology · Physics 2015-06-04 Oleksii Matsedonskyi , Giuliano Panico , Andrea Wulzer

New class of models are constructed in which the third family quarks, but not leptons, experience a new SU(2) or U(1) gauge force. Anomaly cancellation enforces the introduction of spectator quarks so that the top and bottom masses are…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. -J. He , T. M. P. Tait , C. -P. Yuan

Collisions of particles at the energy frontier can reveal new particles and forces via localized excesses. However, the initial observation may be consistent with a large variety of theoretical models, especially in sectors with new top…

High Energy Physics - Phenomenology · Physics 2025-02-21 Krish Wu , Brandon Sun , Nitish Polishetty , Justin Kline , Max Fieg , Daniel Whiteson

We consider a model of strong dynamics able to account for the origin of the electroweak symmetry breaking and heavy quark masses. The model is based on a technicolor sector, augmented with topcolor and top-seesaw mechanism to assist in the…

High Energy Physics - Phenomenology · Physics 2012-10-26 Hidenori S. Fukano , Kimmo Tuominen

It now appears phenomenologically that the third family may be essentially different from the first two. Particularly the high value of the top quark mass suggests a special role. In the standard model all three families are treated…

High Energy Physics - Phenomenology · Physics 2007-05-23 Paul H. Frampton

Recently a new class of theories of electroweak symmetry breaking have been constructed. These models, based on deconstruction and the physics of theory space, provide the first alternative to weak-scale supersymmetry with naturally light…

High Energy Physics - Phenomenology · Physics 2011-01-13 N. Arkani-Hamed , A. G. Cohen , T. Gregoire , E. Katz , A. E. Nelson , J. G. Wacker

We consider a theory with composite top quarks but an elementary Higgs boson. The hierarchy problem can be solved by supplementing TeV scale top compositeness with either supersymmetry or Higgs compositeness appearing at the multi-TeV…

High Energy Physics - Phenomenology · Physics 2017-02-01 Aaron Pierce , Yue Zhao

The main challenge faced by Higgsless models of electroweak symmetry breaking is to reconcile the experimental constraints imposed by the precision electroweak data and the top quark phenomenology with the unitarity constraints imposed by…

High Energy Physics - Phenomenology · Physics 2009-11-11 Roshan Foadi , Carl Schmidt

A realization of the composite Higgs scenario in the context of the effective model with the $SU(2)_L\times U(1)_R$ symmetric four-Fermi interactions proposed by Miransky, Tanabashi and Yamawaki is studied. The model implements Nambu's…

High Energy Physics - Phenomenology · Physics 2024-01-19 A. A. Osipov , B. Hiller , A. H. Blin , F. Palanca , J. Moreira , M. Sampaio

The role of the top quark in completing the Standard Model quark sector is reviewed, along with a discussion of production, decay, and theoretical restrictions on the top quark properties. Particular attention is paid to the top quark as a…

High Energy Physics - Phenomenology · Physics 2009-09-29 S. Dawson

In the Minimal Supersymmetric Standard Model, one of the scalar top quarks can be relatively light and its couplings to Higgs bosons strongly enhanced. I will discuss two consequences of this feature: 1) the effects of scalar top loops on…

High Energy Physics - Phenomenology · Physics 2007-05-23 Abdelhak Djouadi

We propose a top hypercharge model with gauge symmetry SU(3)_C x SU(2)_L x U(1)_1 x U(1)_2 where the first two families of the Standard Model (SM) fermions are charged under U(1)_1 while the third family is charged under U(1)_2. The U(1)_1…

High Energy Physics - Phenomenology · Physics 2009-01-06 Cheng-Wei Chiang , Jing Jiang , Tianjun Li , Yong-Rui Wang

We study the production of $t{\bar t}h$ and $t{\bar t}hh$ at hadron colliders, in the minimal Composite Higgs Models, based on the coset $SO(5)/SO(4)$. We explore the fermionic representations ${\bf 5}$ and ${\bf 14}$. A detailed…

High Energy Physics - Phenomenology · Physics 2021-12-22 Carlos Bautista , Leonardo de Lima , Ricardo D. Matheus , Eduardo Pontón , Leônidas A. F. do Prado , Aurore Savoy-Navarro