Renormalization Group Flows in Gauge-Yukawa Theories, Compositeness & the Higgs
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Arxiv:1406.7795V2 [Hep-Ph] 24 Apr 2017 Mass Renormalization in a Toy Model with Spontaneously Broken Symmetry
UWThPh-2014-16 Mass renormalization in a toy model with spontaneously broken symmetry W. Grimus∗, P.O. Ludl† and L. Nogu´es‡ University of Vienna, Faculty of Physics Boltzmanngasse 5, A–1090 Vienna, Austria April 24, 2017 Abstract We discuss renormalization in a toy model with one fermion field and one real scalar field ϕ, featuring a spontaneously broken discrete symmetry which forbids a fermion mass term and a ϕ3 term in the Lagrangian. We employ a renormalization scheme which uses the MS scheme for the Yukawa and quartic scalar couplings and renormalizes the vacuum expectation value of ϕ by requiring that the one-point function of the shifted field is zero. In this scheme, the tadpole contributions to the fermion and scalar selfenergies are canceled by choice of the renormalization parameter δv of the vacuum expectation value. However, δv and, therefore, the tadpole contributions reenter the scheme via the mass renormalization of the scalar, in which place they are indispensable for obtaining finiteness. We emphasize that the above renormalization scheme provides a clear formulation of the hierarchy problem and allows a straightforward generalization to an arbitrary number of fermion and arXiv:1406.7795v2 [hep-ph] 24 Apr 2017 scalar fields. ∗E-mail: [email protected] †E-mail: [email protected] ‡E-mail: [email protected] 1 1 Introduction Our toy model is described by the Lagrangian 1 1 = iχ¯ γµ∂ χ + y χT C−1χ ϕ + H.c. + (∂ ϕ)(∂µϕ) V (ϕ) (1) L L µ L 2 L L 2 µ − with the scalar potential 1 1 V (ϕ)= µ2ϕ2 + λϕ4. -
A Chiral Symmetric Calculation of Pion-Nucleon Scattering
. s.-q3 4 4t' A Chiral Symmetric Calculation of Pion-Nucleon Scattering UNeOo M Sc (Rangoon University) A thesis submitted in fulfillment of the requirements for the degree of Doctor of Philosophy at the University of Adelaide Department of Physics and Mathematical Physics University of Adelaide South Australia February 1993 Aword""l,. ng3 Contents List of Figures v List of Tables IX Abstract xt Acknowledgements xll Declaration XIV 1 Introduction 1 2 Chiral Symmetry in Nuclear Physics 7 2.1 Introduction . 7 2.2 Pseudoscalar and Pseudovector pion-nucleon interactions 8 2.2.1 The S-wave interaction 8 2.3 Soft-pion Theorems L2 2.3.1 Partially Conserved Axial Current(PCAC) T2 2.3.2 Adler's Consistency condition l4 2.4 The Sigma Model 16 2.4.I The Linear Sigma, Mocìel 16 2.4.2 Broken Symmetry Mode 18 2.4.3 Correction to the S-wave amplitude . 19 2.4.4 The Non-linear sigma model 2.5 Summary 3 Relativistic Two-Body Propagators 3.1 Introduction . 3.2 Bethe-Salpeter Equation 3.3 Relativistic Two Particle Propagators 3.3.1 Blankenbecler-Sugar Method 3.3.2 Instantaneous-interaction approximation 3.4 Short Range Structure in the Propagators 3.5 Smooth Propagators 3.6 The One Body Limit 3.7 One Body Limit, the R factor 3.8 Application to the zr.lú system 3.9 Summary 4 The Formalisrn 4.r Introduction - 4.2 Interactions in the Cloudy Bag Model . 4.2.1 Vertex Functions 4.2.2 The Weinberg-Tomozawa Term 4.3 Higher order graphs 4.3.1 The Cross Box Interaction 4.3.2 Loop diagram 4.3.3 The Chiral Partner of the Sigma Diagram 4.3.4 Sigma like diagrams 4.3.5 The Contact Interaction 4.3.6 The Interaction for Diagram h . -
``Topcolor''; Invited Talk Presented At" Strongly Coupled Gauge Theories
FERMILAB-Conf-97/032-T TOPCOLOR1 CHRISTOPHER T. HILL Fermi National Accelerator Laboratory P.O. Box 500, Batavia, Illinois, 60510, USA 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) SU(3)1 SU(3)2, ergo “Topcolor.” Topcolor suggests c → × a novel route to technicolor models in which sequential quarks condense under the Topcolor interaction to break electroweak symmetries. 1 Top Quark Condensation 1.1 Preliminary The top quark has arrived with a mass of 175 GeV. This is remarkably ∼ large in comparison to all other known fundamental particles, and coin- cidently equals the natural scale of electroweak interactions, 1/ 2√2GF . The top quark mass may be dynamically generated, analogousq to a con- stituent quark mass in QCD. Then the relevant question becomes: “Are arXiv:hep-ph/9702320v1 12 Feb 1997 there new strong interactions that are revealing themselves through the large top mass?” If the answer is no, then the most sensible scenario for physics beyond the standard model is something like the minimal supersymmetric standard model (MSSM). In this case the top quark mass is given by the infra–red renormalization group fixed point [1], and many of the successful predictions of unification are tied to this fact [2]. By itself, this is remarkable, because the infra–red renormalization group fixed point is really a consequence of the approximate scale invariance of the unified theory over the range of 1Invited Talk presented at Strongly Coupled Gauge Theories ‘96, Nagoya, Nov. -
Two Composite Higgs Doublets: Is It the Low Energy Limit of A
Two Composite Higgs Doublets: Is it the Low Energy Limit of a Natural Strong Electroweak Symmetry Breaking Sector ? Alfonso R. Zerwekh∗ Centro de Estudios Subat´omicos and Instituto de F´ısica, Facultad de Ciencias, Universidad Austral de Chile, Casilla 567, Valdivia,Chile Abstract In this paper, we propose an effective model scheme that describes the electroweak symmetry breaking sector by means of composite Higgs- like scalars, following the ideas of Minimal Walking Technicolor (MWT). We argue that, because of the general failure of Extended Technicolor (ETC) to explain the mass of the top quark, it is necessary to introduce two composite Higgs bosons: one of them originated by a MWT-ETC sector and the other one produced by a Topcolor sector. We focus on the phenomenological differences between the light composite Higgs present in our model and the fundamental Higgs boson predicted by the Standard Model and their production at the LHC. We show that in this scheme the main production channel of the lighter Higgs boson are the associated production with a gauge boson and WW fusion but not the gluon-gluon fusion channel which is substantially suppressed. 1 Introduction arXiv:0907.4690v3 [hep-ph] 25 Dec 2009 High Energy Physics is at the dawn of a new era. In the very near future the LHC will allow us to explore, for the first time, the physics responsible for the electroweak symmetry breaking. We are quite sure that something different to the minimal Higgs sector of the Standard Model will be found, but the conjectured alternatives, far from being unique, are varied and very different among them, going from Higgsless models to Supersymmetry. -
Higgs Bosons Strongly Coupled to the Top Quark
CERN-TH/97-331 SLAC-PUB-7703 hep-ph/9711410 November 1997 Higgs Bosons Strongly Coupled to the Top Quark Michael Spiraa and James D. Wellsb aCERN, Theory Division, CH-1211 Geneva, Switzerland bStanford Linear Accelerator Center Stanford University, Stanford, CA 94309† Abstract Several extensions of the Standard Model require the burden of electroweak sym- metry breaking to be shared by multiple states or sectors. This leads to the possibility of the top quark interacting with a scalar more strongly than it does with the Stan- dard Model Higgs boson. In top-quark condensation this possibility is natural. We also discuss how this might be realized in supersymmetric theories. The properties of a strongly coupled Higgs boson in top-quark condensation and supersymmetry are described. We comment on the difficulties of seeing such a state at the Tevatron and LEPII, and study the dramatic signatures it could produce at the LHC. The four top quark signature is especially useful in the search for a strongly coupled Higgs boson. We also calculate the rates of the more conventional Higgs boson signatures at the LHC, including the two photon and four lepton signals, and compare them to expectations in the Standard Model. CERN-TH/97-331 SLAC-PUB-7703 hep-ph/9711410 November 1997 †Work supported by the Department of Energy under contract DE-AC03-76SF00515. 1 Introduction Electroweak symmetry breaking and fermion mass generation are both not understood. The Standard Model (SM) with one Higgs scalar doublet is the simplest mechanism one can envision. The strongest arguments in support of the Standard Model Higgs mechanism is that no experiment presently refutes it, and that it allows both fermion masses and electroweak symmetry breaking. -
Model-Independent Constraints on Topcolor from Rb
MADPH-97-984 TUM-HEP-267/97 hep-ph/9702265 Model-independent Constraints on Topcolor from Rb Gustavo Burdman∗ Department of Physics, University of Wisconsin, Madison, WI 53706, USA and Dimitris Kominis† Institut f¨ur Theoretische Physik, Technische Universit¨at M¨unchen, James-Franck-Straße, 85748 Garching, Germany Abstract arXiv:hep-ph/9702265v2 8 May 1997 We identify and compute the main corrections to Rb in Topcolor theories. They are due to the top-pions, the pseudo-Goldstone bosons associated with the chiral symmetry breaking responsible for the top quark mass, and amount to (1 4)%, − − independent of the details of the Topcolor model. We show that the cancellation of this effect against the contributions from Topcolor vector and scalar resonances is unlikely, given the inherently distinct character of the two scales governing the potentially cancelling terms. The resulting value of Rb leads to severe constraints on Topcolor theories. ∗e-mail address: [email protected] †e-mail address: [email protected] 1 Introduction The large value of the top-quark mass has led to speculation that the properties of the top quark may be fundamentally different from those of the other known fermions. In theories of top condensation, for example, a new strong gauge interaction (Topcolor), which couples to the t-quark and perhaps to other fermions as well, drives the formation of a tt¯ condensate and imparts a large dynamical mass to the top quark. In the process, h i the chiral symmetries associated with the strongly interacting fermions are spontaneously broken and at least three Goldstone bosons emerge. -
Strongly Coupled Fermions on the Lattice
Syracuse University SURFACE Dissertations - ALL SURFACE December 2019 Strongly coupled fermions on the lattice Nouman Tariq Butt Syracuse University Follow this and additional works at: https://surface.syr.edu/etd Part of the Physical Sciences and Mathematics Commons Recommended Citation Butt, Nouman Tariq, "Strongly coupled fermions on the lattice" (2019). Dissertations - ALL. 1113. https://surface.syr.edu/etd/1113 This Dissertation is brought to you for free and open access by the SURFACE at SURFACE. It has been accepted for inclusion in Dissertations - ALL by an authorized administrator of SURFACE. For more information, please contact [email protected]. Abstract Since its inception with the pioneering work of Ken Wilson, lattice field theory has come a long way. Lattice formulations have enabled us to probe the non-perturbative structure of theories such as QCD and have also helped in exploring the phase structure and classification of phase transitions in a variety of other strongly coupled theories of interest to both high energy and condensed matter theorists. The lattice approach to QCD has led to an understanding of quark confinement, chiral sym- metry breaking and hadronic physics. Correlation functions of hadronic operators and scattering matrix of hadronic states can be calculated in terms of fundamental quark and gluon degrees of freedom. Since lat- tice QCD is the only well-understood method for studying the low-energy regime of QCD, it can provide a solid foundation for the understanding of nucleonic structure and interaction directly from QCD. Despite these successes problems remain. In particular, the study of chiral gauge theories on the lattice is an out- standing problem of great importance owing to its theoretical implications and for its relevance to the electroweak sector of the Standard Model. -
Optimized Probes of the CP Nature of the Top Quark Yukawa Coupling at Hadron Colliders
S S symmetry Article Optimized Probes of the CP Nature of the Top Quark Yukawa Coupling at Hadron Colliders Darius A. Faroughy 1, Blaž Bortolato 2, Jernej F. Kamenik 2,3,* , Nejc Košnik 2,3 and Aleks Smolkoviˇc 2 1 Physik-Institut, Universitat Zurich, CH-8057 Zurich, Switzerland; [email protected] 2 Jozef Stefan Institute, Jamova 39, 1000 Ljubljana, Slovenia; [email protected] (B.B.); [email protected] (N.K.); [email protected] (A.S.) 3 Faculty of Mathematics and Physics, University of Ljubljana, Jadranska 19, 1000 Ljubljana, Slovenia * Correspondence: [email protected] Abstract: We summarize our recent proposals for probing the CP-odd ik˜t¯g5th interaction at the LHC and its projected upgrades directly using associated on-shell Higgs boson and top quark or top quark pair production. We first recount how to construct a CP-odd observable based on top quark polarization in Wb ! th scattering with optimal linear sensitivity to k˜. For the corresponding hadronic process pp ! thj we then present a method of extracting the phase-space dependent weight function that allows to retain close to optimal sensitivity to k˜. For the case of top quark pair production in association with the Higgs boson, pp ! tth¯ , with semileptonically decaying tops, we instead show how one can construct manifestly CP-odd observables that rely solely on measuring the momenta of the Higgs boson and the leptons and b-jets from the decaying tops without having to distinguish the charge of the b-jets. Finally, we introduce machine learning (ML) and non-ML techniques to study the phase-space optimization of such CP-odd observables. -
Outlook Post-Higgs
Outlook Post-Higgs Christopher T. Hill Fermilab UCLA Higgs Workshop March 22, 2013 A dynamical “Higgs” mechanism was supposed to explain the origin of electroweak mass A dynamical “Higgs” mechanism was supposed to explain the origin of electroweak mass We now know that, evidently, a fundamental Higgs Boson exists and explains the masses of quarks, leptons, W and Z A dynamical “Higgs” mechanism was supposed to explain the origin of electroweak mass We now know that, evidently, a fundamental Higgs Boson exists and explains the masses of quarks, leptons, W and Z The Higgs Boson does NOT explain the origin of the electroweak mass-scale A dynamical “Higgs” mechanism was supposed to explain the origin of electroweak mass We now know that, evidently, a fundamental Higgs Boson exists and explains the masses of quarks, leptons, W and Z The Higgs Boson does NOT explain the origin of the electroweak mass-scale i.e., what is the origin of the Higgs Boson mass itself? A dynamical “Higgs” mechanism was supposed to explain the origin of electroweak mass We now know that, evidently, a fundamental Higgs Boson exists and explains the masses of quarks, leptons, W and Z The Higgs Boson does NOT explain the origin of the electroweak mass-scale i.e., what is the origin of the Higgs Boson mass itself? This may present opportunities for a deeper understanding QCD beautifully explains the origin of strong mass : The magnificent scale anomaly: The scale current: = 0 in a scale invariant theory The magnificent scale anomaly: The scale current: = 0 in a scale invariant -
Single Top Production Associated with a Neutral Scalar at LHC in Topcolor-Assisted Technicolor
Chinese Physics C (HEP & NP) Vol. 32, No. 9, Sep., 2008 Single top production associated with a neutral scalar at LHC in topcolor-assisted technicolor LIU Guo-Li(7Iw)1 ZHANG Huan-Jun(Ü)2;1) 1 (Department of Physics, Zhengzhou University, Henan 450052, China) 2 (Department of Physics, Henan Normal University, Xinxiang 453007, China) Abstract The topcolor-assisted technicolor (TC2) model predicts a number of neutral scalars like the top-pion 0 0 (πt ) and the top-Higgs (ht ). These scalars have flavor-changing neutral-current (FCNC) top quark couplings, among which the top-charm transition couplings may be sizable. Such FCNC couplings induce single top productions associated with a neutral scalar at the CERN Large Hadron Collider (LHC) through the parton ! 0 ! 0 processes cg tπt and cg tht . In this paper we examine these productions and find their production rates can exceed the 3σ sensitivity of the LHC in a large part of parameter space. Since in the Standard Model and the minimal supersymmetric model such rare productions have unobservably small production rates at the LHC, these rare processes will serve as a good probe for the TC2 model. Key words top quark, technicolor, LHC PACS 14.65.Ha, 12.60.Fr, 12.60.Jv As the heaviest fermion in the Standard Model ated with a neutral scalar at the LHC through the 0 0 (SM), the top quark may be a sensitive probe of new parton processes cg tπt and cg tht . In this pa- [1] ! ! physics . So far there remain plenty of room for new per we examine these productions and figure out if physics in top quark sector due to the small statis- their rates can exceed the 3σ sensitivity of the LHC. -
Symmetry Breaking and Generational Mixing in Topcolor--Assisted
BUHEP–96–2 hep-ph/9602221 Symmetry Breaking and Generational Mixing in Topcolor–Assisted Technicolor Kenneth Lane† Department of Physics, Boston University 590 Commonwealth Avenue, Boston, MA 02215 Abstract 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 heavy and light generations while breaking the strong topcolor interactions near 1 TeV. I argue that these phenomena, as well as electroweak symmetry breaking, are intimately connected and I arXiv:hep-ph/9602221v1 4 Feb 1996 present a scenario for them based on nontrivial patterns of technifermion condensation. I also exhibit a class of models realizing this scenario. This picture leads to a rich phe- nomenology, especially in hadron and lepton collider experiments in the few hundred GeV to few TeV region and in precision electroweak tests at the Z0, atomic parity violation, and polarized Møller scattering. 2/96 † [email protected] 1. Introduction Topcolor–assisted technicolor (TC2) was proposed by Hill [1] to overcome major shortcomings of top–condensate models of electroweak symmetry breaking [2], [3] and of technicolor models of dynamical electroweak and flavor symmetry breaking [4], [5]. Technicolor and extended technicolor (ETC) have been unable to provide a natural and plausible understanding of why the top quark mass is so large [6]. On the other hand, models in which strong topcolor interactions drive top–quark condensation and elec- troweak symmetry breaking are unnatural. To reproduce the one–Higgs–doublet standard model consistent with precision electroweak measurements (especially of the parameter 2 2 2 ρ = M /M cos θW 1), the topcolor energy scale must be much greater than the W Z ≃ electroweak scale of (1 TeV). -
Yukawa Potential Orbital Energy: Its Relation to Orbital Mean Motion As Well to the Graviton Mediating the Interaction in Celestial Bodies
Hindawi Advances in Mathematical Physics Volume 2019, Article ID 6765827, 10 pages https://doi.org/10.1155/2019/6765827 Research Article Yukawa Potential Orbital Energy: Its Relation to Orbital Mean Motion as well to the Graviton Mediating the Interaction in Celestial Bodies Connor Martz,1 Sheldon Van Middelkoop,2 Ioannis Gkigkitzis,3 Ioannis Haranas ,4 and Ilias Kotsireas4 1 University of Waterloo, Department of Physics and Astronomy, Waterloo, ON, N2L-3G1, Canada 2University of Western Ontario, Department of Physics and Astronomy, London, ON N6A-3K7, Canada 3NOVA, Department of Mathematics, 8333 Little River Turnpike, Annandale, VA 22003, USA 4Wilfrid Laurier University, Department of Physics and Computer Science, Waterloo, ON, N2L-3C5, Canada Correspondence should be addressed to Ioannis Haranas; [email protected] Received 25 September 2018; Revised 25 November 2018; Accepted 4 December 2018; Published 1 January 2019 Academic Editor: Eugen Radu Copyright © 2019 Connor Martz et al. Tis is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Research on gravitational theories involves several contemporary modifed models that predict the existence of a non-Newtonian Yukawa-type correction to the classical gravitational potential. In this paper we consider a Yukawa potential and we calculate the time rate of change of the orbital energy as a function of the orbital mean motion for circular and elliptical orbits. In both cases we fnd that there is a logarithmic dependence of the orbital energy on the mean motion. Using that, we derive an expression for the mean motion as a function of the Yukawa orbital energy, as well as specifc Yukawa potential parameters.