UNIVERSITY of CALIFORNIA SAN DIEGO Aspects of Scale Invariant

Total Page:16

File Type:pdf, Size:1020Kb

UNIVERSITY of CALIFORNIA SAN DIEGO Aspects of Scale Invariant UNIVERSITY OF CALIFORNIA SAN DIEGO Aspects of Scale Invariant Quantum Field Theory A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Physics by Sridip Pal Committee in charge: Professor Kenneth Intriligator, Chair Professor Benjamin Grinstein, Co-Chair Professor Tarun Grover Professor John McGreevy Professor James Mckernan 2019 Copyright Sridip Pal, 2019 All rights reserved. The dissertation of Sridip Pal is approved, and it is accept- able in quality and form for publication on microfilm and electronically: Co-Chair Chair University of California San Diego 2019 iii DEDICATION To my parents and my friends Ahanjit, Brato, Shouvik for being there Always . iv EPIGRAPH The career of a young theoretical physicist consists of treating the harmonic oscillator in ever-increasing levels of abstraction. —Sydney Coleman v TABLE OF CONTENTS Signature Page....................................... iii Dedication.......................................... iv Epigraph...........................................v Table of Contents...................................... vi List of Figures........................................x List of Tables........................................ xii Acknowledgements..................................... xiii Vita............................................. xviii Abstract of the Dissertation................................. xix Chapter 1 Introduction.................................1 Chapter 2 Weyl Consistency Conditions in Non-Relativistic Quantum Field Theory. 13 2.1 Introduction.............................. 13 2.2 Generalities.............................. 17 2.2.1 Dynamical exponent..................... 25 2.3 d = 2, z = 2 Non Relativistic theory................. 28 2.3.1 Listing out terms....................... 28 2.3.2 Using counter-terms..................... 31 2.3.3 Consistency conditions and vanishing anomalies...... 34 2.3.4 Applications......................... 35 2.4 Generalisation to arbitrary z value.................. 38 2.5 A candidate for a C-theorem in d + 1D............... 39 2.6 Summary and Discussion....................... 46 Chapter 3 On the Heat Kernel and Weyl Anomaly of Schrodinger¨ invariant theory. 49 3.1 Introduction.............................. 50 3.2 Newton-Cartan Structure & Weyl Anomaly............. 53 3.3 Discrete Light Cone Quantization (DLCQ) & its cousin Lightcone Reduction (LCR)........................... 57 3.4 Heat Kernel for a Galilean CFT with z = 2.............. 61 3.4.1 Preliminaries: Heat Kernel, Zeta Regularisation....... 61 3.4.2 Heat Kernel in Flat Space-time................ 66 3.4.3 Heat Kernel in Curved spacetime.............. 70 vi 3.5 Perturbative proof of Vanishing anomaly............... 73 3.6 Modified LCR and Generalisation.................. 77 3.6.1 Proving the heat kernel prescription............. 77 3.6.2 Generalisation........................ 78 3.7 Summary, Discussion and Future directions............. 83 Chapter 4 Unitarity and Universality in non relativistic Conformal Field theory... 87 4.1 Introduction.............................. 87 4.2 Unitarity bounds & Null conditions................. 90 4.3 Non Unitarity in non integer dimensions.............. 96 4.4 Universality.............................. 98 4.5 Discussion & Outlook........................ 101 4.6 Acknowledgments.......................... 104 Chapter 5 Existence and Construction of Galilean invariant z 6= 2 Theories...... 106 5.1 Introduction.............................. 107 5.2 Generalized Schrodinger¨ algebra and its Representation....... 110 5.3 Null reduction and Embedding into Conformal group........ 116 5.4 Explicit d + 1 dimensional examples................. 117 5.4.1 z = 0............................. 117 2` 5.4.2 z = `+1 ;` 2 Z, ` ≥ 1..................... 118 5.5 Conclusion.............................. 119 Chapter 6 Hilbert Series and Operator Basis for NRQED and NRQCD/HQET.... 121 6.1 Introduction.............................. 121 6.2 Effective Theory for a Nonrelativistic Fermion............ 123 6.3 Hilbert series for a nonrelativistic theory............... 125 6.4 NRQED................................ 128 6.5 NRQCD/HQET............................ 131 6.6 Discussion and Conclusions..................... 133 Chapter 7 Conformal Structure of the Heavy Particle EFT Operator Basis...... 137 7.1 Introduction.............................. 137 7.2 Operator Basis for Heavy Particle EFTs............... 139 7.3 Operator Basis and the Schrodinger¨ Algebra............. 142 7.4 Discussion and Conclusions..................... 149 Chapter 8 Nonrelativistic Conformal Field Theories in the Large Charge Sector... 152 8.1 Introduction and Summary...................... 152 8.2 Lightning Review of Schrodinger¨ Algebra.............. 157 8.3 Lightning Review of Coset Construction............... 159 8.4 Schrodinger¨ Superfluid from Coset Construction.......... 162 8.5 Superfluid Hydrodynamics...................... 166 8.5.1 Superfluid in a Harmonic Trap................ 167 vii 8.6 Operator Dimensions......................... 169 8.6.1 Ground State Energy & Scaling of Operator Dimension... 169 8.6.2 Excited State Spectrum.................... 171 8.7 Correlation Functions......................... 173 8.7.1 Two Point Function...................... 173 8.7.2 Three Point Function..................... 173 8.8 Conclusions and Future Directions.................. 175 Chapter 9 The Spinful Large Charge Sector of Non-Relativistic CFTs: From Phonons to Vortex Crystals.............................. 178 9.1 Introduction and Summary...................... 178 9.2 Superfluid Hydrodynamics and Large Charge NRCFT........ 182 9.3 Phonons................................ 185 9.4 Single Vortex in the Trap....................... 188 9.4.1 Single vortex in d = 2.................... 190 9.4.2 Single vortex in d = 3.................... 191 9.5 Multi-Vortex Profile.......................... 193 9.6 Conclusions and Future Directions.................. 198 Chapter 10 Modular Invariance and Cardy Formula.................. 200 Chapter 11 Bounds on density of states and spectral gap in CFT2 ........... 212 11.1 The premise and the results...................... 212 11.2 Derivation of the improvement.................... 216 11.3 Bound on bounds........................... 221 11.4 Bound on spectral gap: towards optimality.............. 225 11.5 Brief discussion............................ 231 Appendix A Weyl Consistency Conditions in Non Relativistic Quantum Field Theory. 233 A.1 Consistency Conditions for 2 + 1d NRCFT............. 233 A.2 Anomaly ambiguities......................... 236 2 A.2.1 ¶t Sector........................... 236 2 A.2.2 ¶t∇ Sector.......................... 236 A.2.3 ∇4 Sector........................... 238 A.3 S-theorem: 0 + 1D conformal quantum mechanics.......... 240 Appendix B On the Heat Kernel and Weyl Anomaly of Schrodinger¨ invariant theory. 244 B.1 Technical Aspects of Heat Kernel for one time derivative theory.. 244 B.2 Riemann normal co-ordinate and coincident limit.......... 245 B.3 Explicit Perturbative Calculation of h-regularized Heat Kernel... 249 viii Appendix C Unitarity and Universality in non relativistic Conformal Field theory... 255 C.1 SL(2;R) invariant field theory.................... 255 C.2 Schrodinger¨ algebra, Primaries and Quasi-primaries......... 258 C.3 Time reversal and Parity....................... 260 C.4 Free Schrodinger¨ Field theory & Its Euclidean avatar........ 263 Appendix D Existence and Construction of Galilean invariant z 6= 2 Theories..... 268 D.1 Diagonalizable and finite dimensional dilatation generator..... 268 Appendix E Hilbert Series and Operator Basis for NRQED and NRQCD/HQET.... 273 E.1 Characters and Haar Measures.................... 273 Appendix F Conformal Structure of the Heavy Particle EFT Operator Basis...... 275 F.1 Normalsize Symmetries of Non-Relativistic Systems........ 275 F.2 Symmetries, Operators, and States.................. 279 F.3 Constraints from Algebra and Unitarity bound............ 283 Appendix G Nonrelativistic Conformal Field Theories in the Large Charge Sector... 287 G.1 Appendix A: Phonons in the Trap.................. 287 G.2 Appendix B: Correlation Functions in Oscillator Frame....... 289 G.2.1 Two point function...................... 289 G.2.2 Three point function..................... 290 Appendix H The Spinful Large Charge Sector of Non-Relativistic CFTs: From Phonons to Vortex Crystals.............................. 291 H.1 Particle-Vortex Duality........................ 291 H.2 A Contour integral.......................... 294 Bibliography........................................ 296 ix LIST OF FIGURES Figure 1.1: The rotation of a sphere with a dot, without the dot, the two scenarios are exactly the same................................2 Figure 1.2: The image of a fractal............................3 Figure 2.1: Self energy correction to propagator at one loop. The ingoing momenta is denoted by (E;k) while the internal loop momenta is given by the variable p. 26 Figure 4.1: Unitarity bound on (a;D) plane: the projection of the region bounded by two curves onto the Y axis excludes D < 0. The blue thick curve is D+ = 1 q 1 1 q 1 −a − 2 + a + 4 while the orange dashed curve is D− = −a − 2 − a + 4 . 92 Figure 4.2: Unitarity bound on (b;D) plane: the projection of the region bounded by the d ellipse onto the Y axis excludes D 2 −1; 2 . Here d = 10. The blue thick db−1 1 p 2 curve is D+ = 2 + 2 1 + 2db − 2db while the orange dashed curve is db−1 1 p 2 D− = 2 − 2 1 + 2db − 2db ......................
Recommended publications
  • Supergravity and Its Legacy Prelude and the Play
    Supergravity and its Legacy Prelude and the Play Sergio FERRARA (CERN – LNF INFN) Celebrating Supegravity at 40 CERN, June 24 2016 S. Ferrara - CERN, 2016 1 Supergravity as carved on the Iconic Wall at the «Simons Center for Geometry and Physics», Stony Brook S. Ferrara - CERN, 2016 2 Prelude S. Ferrara - CERN, 2016 3 In the early 1970s I was a staff member at the Frascati National Laboratories of CNEN (then the National Nuclear Energy Agency), and with my colleagues Aurelio Grillo and Giorgio Parisi we were investigating, under the leadership of Raoul Gatto (later Professor at the University of Geneva) the consequences of the application of “Conformal Invariance” to Quantum Field Theory (QFT), stimulated by the ongoing Experiments at SLAC where an unexpected Bjorken Scaling was observed in inclusive electron- proton Cross sections, which was suggesting a larger space-time symmetry in processes dominated by short distance physics. In parallel with Alexander Polyakov, at the time in the Soviet Union, we formulated in those days Conformal invariant Operator Product Expansions (OPE) and proposed the “Conformal Bootstrap” as a non-perturbative approach to QFT. S. Ferrara - CERN, 2016 4 Conformal Invariance, OPEs and Conformal Bootstrap has become again a fashionable subject in recent times, because of the introduction of efficient new methods to solve the “Bootstrap Equations” (Riccardo Rattazzi, Slava Rychkov, Erik Tonni, Alessandro Vichi), and mostly because of their role in the AdS/CFT correspondence. The latter, pioneered by Juan Maldacena, Edward Witten, Steve Gubser, Igor Klebanov and Polyakov, can be regarded, to some extent, as one of the great legacies of higher dimensional Supergravity.
    [Show full text]
  • Hep-Ph/9811291
    CERN-TH/98-354 hep-ph/9811291 Quantum Gravity and Extra Dimensions at High-Energy Colliders Gian F. Giudice, Riccardo Rattazzi, and James D. Wells Theory Division, CERN CH-1211 Geneva 23, Switzerland Abstract Recently it has been pointed out that the characteristic quantum-gravity scale could be as low as the weak scale in theories with gravity propagating in higher dimensions. The observed smallness of Newton’s constant is a consequence of the large compactified volume of the extra dimensions. We investigate the consequences of this supposition for high-energy collider experiments. We do this by first compactifying the higher dimen- sional theory and constructing a 3 + 1-dimensional low-energy effective field theory of the graviton Kaluza-Klein excitations and their interactions with ordinary matter. We then consider graviton production processes, and select γ+ E and jet+ E signatures 6 6 for careful study. We find that both a 1 TeV e+e− collider and the CERN LHC will be able to reliably and perturbatively probe the fundamental gravity scale up to several arXiv:hep-ph/9811291v2 13 Mar 2000 TeV, with the precise value depending on the number of extra dimensions. Similarly, searches at LEP2 and the Tevatron are able to probe this scale up to approximately 1 TeV. We also discuss virtual graviton exchange, which induces local dimension-eight operators associated with the square of the energy-momentum tensor. We estimate the size of such operators and study their effects on ff¯ γγ observables. → CERN-TH/98-354 November 1998 Contents 1 Introduction 1 2 The Kaluza-Klein Excitations of the Graviton 7 3 Feynman Rules 14 4 Graviton Production Processes 18 5 Virtual Graviton Exchange 21 6 Graviton Production and Collider Experiments 24 6.1 e+e− andMuonColliders............................
    [Show full text]
  • Exact Null Tachyons from Renormalization Group Flows
    Exact null tachyons from renormalization group flows The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Adams, Allan , Albion Lawrence, and Ian Swanson. “Exact null tachyons from renormalization group flows.” Physical Review D 80.10 (2009): 106005. © 2009 The American Physical Society As Published http://dx.doi.org/10.1103/PhysRevD.80.106005 Publisher American Physical Society Version Final published version Citable link http://hdl.handle.net/1721.1/52507 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. PHYSICAL REVIEW D 80, 106005 (2009) Exact null tachyons from renormalization group flows Allan Adams,1 Albion Lawrence,2 and Ian Swanson1 1Center for Theoretical Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA 2Theory Group, Martin Fisher School of Physics, Brandeis University, MS057, 415 South Street, Waltham, Massachusetts 02454, USA (Received 11 August 2009; published 20 November 2009) We construct exact two-dimensional conformal field theories, corresponding to closed string tachyon and metric profiles invariant under shifts in a null coordinate, which can be constructed from any two- dimensional renormalization group flow. These solutions satisfy first order equations of motion in the conjugate null coordinate. The direction along which the tachyon varies is identified precisely with the world sheet scale, and the tachyon equations of motion are the renormalization group flow equations. DOI: 10.1103/PhysRevD.80.106005 PACS numbers: 11.25.Àw, 11.10.Hi I.
    [Show full text]
  • Jhep05(1999)013
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Received: March 30, 1999, Accepted: May 11, 1999 HYPER VERSION Sparticle masses from the superconformal anomaly Alex Pomarol∗ Theory Division, CERN CH-1211 Geneva 23, Switzerland JHEP05(1999)013 E-mail: [email protected] Riccardo Rattazzi INFN and Scuola Normale Superiore I-56100 Pisa, Italy E-mail: [email protected] Abstract: We discuss a recently proposed scenario where the sparticle masses are purely mediated by gravity through the superconformal anomaly. This scenario ele- gantly evades the supersymmetric flavor problem since soft masses, like the anomaly, are not directly sensitive to ultraviolet physics. However, its minimal incarnation fails by predicting tachyonic sleptons. We study the conditions for decoupling of heavy threshold effects and how these conditions are evaded. We use these results to build a realistic class of models where the non-decoupling effects of ultra-heavy vectorlike matter fields eliminate the tachyons. These models have a flavor invariant superspectrum similar to that of gauge mediated models. They, however, differ in several aspects: the gaugino masses are not unified, the colored sparticles are not much heavier than the others, the µ problem is less severe and the gravitino mass is well above the weak scale, m3=2 & 10 TeV. We also show that in models where an R-symmetry can be gauged, the associated D-term gives rise to soft terms that are similarly insensitive to the ultraviolet. Keywords: Supersymmetry Breaking, Supergravity Models, Supersymmetric Standard Model. ∗On leave of absence from IFAE, Universitat Aut`onoma de Barcelona, E-08193 Bellaterra, Barcelona.
    [Show full text]
  • Dark Matter and Collider Phenomenology of Non-Universal Gaugino Masses
    Dark Matter and Collider Phenomenology of Non-Universal Gaugino Masses A dissertation presented by Michael Holmes to The Department of Physics In partial fulfillment of the requirements for the degree of Doctor of Philosophy in the field of Physics Northeastern University Boston, Massachusetts April, 2010 1 c Michael Holmes, 2010 ALL RIGHTS RESERVED 2 Dark Matter and Collider Phenomenology of Non-Universal Gaugino Masses by Michael Holmes ABSTRACT OF DISSERTATION Submitted in partial fulfillment of the requirement for the degree of Doctor of Philosophy in Physics in the Graduate School of Arts and Sciences of Northeastern University, April, 2010 3 Abstract Signals of minimal supersymmetric models with non-universalities in the gaugino sector of the theory are analyzed at the CERN Large Hadron Collider (LHC) and in experiments searching for dark matter. Signals of dark matter including direct and indirect detection are investigated at depth in various supersymmetric frameworks. The parameter space of deflected mirage mediation, in which the soft terms receive contributions from the three main supersymmetry breaking mediation mechanisms, is investigated with emphasis on the neutralino sector and dark matter signals. The potential for non-universal gaugino masses to explain the recent CDMS II data is studied and possible implications for indirect dark matter detection experiments and LHC signatures are considered. Collider implications of non- universalities in the gaugino sector are examined with attention paid to specific signatures which are targeted to track the non-universalities. Further, the complementarity of dark matter and collider measurements is discussed with emphasis on breaking model degeneracies which may arise in LHC data.
    [Show full text]
  • Dynamical Spacetimes from Numerical Hydrodynamics
    MIT-CTP-4607 Dynamical Spacetimes from Numerical Hydrodynamics Allan Adams,1 Nathan Benjamin,1, 2 Arvin Moghaddam,1, 3 and Wojciech Musial1, 3 1Center for Theoretical Physics, Massachusetts Institute of Technology, Cambridge, MA 02139 2Stanford Institute for Theoretical Physics, Stanford University, Stanford, CA 94305 3Center for Theoretical Physics, University of California, Berkeley, Berkeley, CA 94720 We numerically construct dynamical asymptotically-AdS4 metrics by evaluating the fluid/gravity metric on numerical solutions of dissipative hydrodynamics in (2+1) dimensions. The resulting numerical metrics satisfy Einstein's equations in (3+1) dimensions to high accuracy. Holography provides a precise relationship between Review of Fluid/Gravity black holes in AdSd+1 and QFTs in d-dimensions at fi- nite density and temperature. When the QFT state lies We begin by recalling the essential features of the in a hydrodynamic regime (i.e. when d-dimensional gra- fluid/gravity correspondence for a (2+1) fluid as given dients are sufficiently small that the stress-tensor may in [1{4]. At equilibrium, a fluid moving with constant 3- µ be expanded as a power-series in derivatives), the dual velocity u at temperature T is dual to an asymptotically spacetime metric may also be so expanded, leading to an AdS4 black brane described by the metric [10] analytic “fluid/gravity" map between solutions of hydro- ds2 = −2u dxµdr−r2f(br) u u dxµdxν +r2P dxµdxν ; dynamics in d dimensions and dynamical asymptotically- µ µ ν µν AdSd+1 solutions of the Einstein equations. 3 where b = 4πT is the rescaled inverse temperature, This suggests a simple strategy for constructing nu- P µν =ηµν +uµuν projects onto directions transverse to merical solutions of the Einstein equations in asymptot- µ 1 u , and f(ρ) = 1 − ρ3 is the emblackening factor.
    [Show full text]
  • Yonatan F. Kahn, Ph.D
    Yonatan F. Kahn, Ph.D. Contact Loomis Laboratory 415 E-mail: [email protected] Information Urbana, IL 61801 USA Website: yfkahn.physics.illinois.edu Research High-energy theoretical physics (phenomenology): direct, indirect, and collider searches for sub-GeV Interests dark matter, laboratory and astrophysical probes of ultralight particles Positions Assistant professor August 2019 { present University of Illinois Urbana-Champaign Urbana, IL USA Current research: • Sub-GeV dark matter: new experimental proposals for direct detection • Axion-like particles: direct detection, indirect detection, laboratory searches • Phenomenology of new light weakly-coupled gauge forces: collider searches and effects on low-energy observables • Neural networks: physics-inspired theoretical descriptions of autoencoders and feed-forward networks Postdoctoral fellow August 2018 { July 2019 Kavli Institute for Cosmological Physics (KICP) University of Chicago Chicago, IL USA Postdoctoral research associate September 2015 { August 2018 Princeton University Princeton, NJ USA Education Massachusetts Institute of Technology September 2010 { June 2015 Cambridge, MA USA Ph.D, physics, June 2015 • Thesis title: Forces and Gauge Groups Beyond the Standard Model • Advisor: Jesse Thaler • Thesis committee: Jesse Thaler, Allan Adams, Christoph Paus University of Cambridge October 2009 { June 2010 Cambridge, UK Certificate of Advanced Study in Mathematics, June 2010 • Completed Part III of the Mathematical Tripos in Applied Mathematics and Theoretical Physics • Essay topic: From Topological Strings to Matrix Models Northwestern University September 2004 { June 2009 Evanston, IL USA B.A., physics and mathematics, June 2009 • Senior thesis: Models of Dark Matter and the INTEGRAL 511 keV line • Senior thesis advisor: Tim Tait B.Mus., horn performance, June 2009 Mentoring Graduate students • Siddharth Mishra-Sharma, Princeton (Ph.D.
    [Show full text]
  • Arxiv:1808.00010V3 [Hep-Ph] 20 Dec 2019
    USTC-ICTS-18-13 Positivity bounds on vector boson scattering at the LHC Cen Zhang Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China Shuang-Yong Zhou Interdisciplinary Center for Theoretical Study, University of Science and Technology of China, Hefei, Anhui 230026, China Weak vector boson scattering (VBS) is a sensitive probe of new physics effects in the electroweak symmetry breaking. Currently, experimental results at the LHC are interpreted in the effective field theory approach, where possible deviations from the Standard Model in the quartic-gauge-boson couplings are often described by 18 dimension-8 operators. By assuming that a UV completion exists, we derive a new set of theoretical constraints on the coefficients of these operators, i.e. certain combinations of coefficients must be positive. These constraints imply that the current effective approach to VBS has a large redundancy: only about 2% of the full parameter space leads to a UV completion. By excluding the remaining unphysical region of the parameter space, these constraints provide guidance for future VBS studies and measurements. Introduction.| After the discovery of the Higgs bo- values. Recently, a novel approach has been developed son [1, 2], the focus of particle physics has turned to the to set theoretical bounds on the Wilson coefficients of mechanism of electroweak symmetry breaking and be- a generic EFT that can be UV completed. Going un- yond. At the Large Hadron Collider (LHC), vector bo- der the name of positivity bounds, this approach only son scattering (VBS) is among the processes most sen- requires a minimum set of assumptions, which are noth- sitive to the electroweak and the Higgs sectors.
    [Show full text]
  • Physics Beyond the Standard Model
    CERN-PH-TH/2006-042 hep-ph/0607058 Physics Beyond the Standard Model Riccardo Rattazzi Department of Physics, CERN, CH-1211 Geneva 23, Switzerland Abstract I review recent theoretical work on electroweak symmetry breaking. International Europhysics Conference on High Energy Physics July 21st - 27th 2005 Lisboa, Portugal arXiv:hep-ph/0607058v1 5 Jul 2006 1 1 Introduction I have been assigned this broad title but my talk will be mostly concerned with the origin of the electroweak scale. I will attempt to give an overview of the theoretical ‘laborings’ that came up after the end of the LEP era and in preparation to the commissioning of the LHC. An appropriate subtitle for my talk could thus be ‘Electroweak Symmetry Breaking after LEP/SLC’. There are two different sides from which to regard the legacy of LEP/SLC, and forming what is also known as the LEP paradox [1]. From one side it is an impressive triumph of human endeavour: the Standard Model (SM) is a complete theory of fundamental processes successfully tested at the per-mille precision. That means that small quantum corrections to the Born approximation are essential in the comparison between theory and experiment. However, when regarded from the other side, this great success becomes a huge conceptual bafflement, because the hierarchy problem, which inspired theoretical speculations for the last three decades, suggested that the SM should be overthrown right at the weak scale. That did not happen, so we must now understand why. I will discuss the paradoxical LEP/SLC legacy in the first part of my talk.
    [Show full text]
  • Brane-To-Brane Mediation of Supersymmetry Breaking in Presence of D-Type Breaking 1
    Institute of Physics Publishing Journal of Physics: Conference Series 53 (2006) 635–642 doi:10.1088/1742-6596/53/1/039 Corfu Summer Institute on Elementary Particle Physics Brane-to-brane mediation of supersymmetry breaking in presence of D-type breaking 1 Thomas Gr´egoire Physics department Boston University Boston MA, 02215 1. Introduction As it is well known, supersymmetry is a very attractive option for physics beyond the Standard Model (SM). While it has not been discovered at LEP and the Tevatron, it will still be extensively looked for at the LHC, and many remain hopeful that it will be seen there. An important feature of supersymmetry is that it guarantees the absence of quadratic divergence in the renormalization of scalar masses, in the case of interest the Higgs mass. This property holds even if supersymmetry is broken softly, that is by operators of dimension two or three. The minimal extension of the SM into such a theory is called the minimal supersymmetric standard model (MSSM). It contains renormalizable supersymmetric interactions as well as a set of super- renormalizable, supersymmetry-breaking interactions dubbed the soft masses: L L 2 u u d d e d u d = kin + d θ yijQiUjH + yijQiDjH + yijLiEjH + μH H (1) 2 ∗ a a a u u u d ··· +mijqi qj + m1/2λ λ + yijAuqiujh + Bμh h + , 2 a where mij are scalar soft masses squared, m1/2 gaugino masses and A trilinear scalar terms. The dots denote similar terms. The value of these soft masses are very constrained by experiment. One constraint comes from the fact that supersymmetry has not yet been discovered, which requires the superpartners to be somewhat heavy.
    [Show full text]
  • The Dawn of the Post-Naturalness Era Arxiv:1710.07663V1 [Physics.Hist-Ph]
    CERN-TH-2017-205 The Dawn of the Post-Naturalness Era Gian Francesco Giudice CERN, Theoretical Physics Department, Geneva, Switzerland Abstract In an imaginary conversation with Guido Altarelli, I express my views on the status of particle physics beyond the Standard Model and its future prospects. Contribution to the volume \From My Vast Repertoire" { The Legacy of Guido Altarelli. 1 A Master and a Friend Honour a king in his own land; honour a wise man everywhere. | Tibetan proverb [1] Guido Altarelli was an extraordinary theoretical physicist. Not only was Guido one of the heroes of the Standard Model, but he incarnated the very essence of that theory: a perfect synthesis of pure elegance and brilliance. With his unique charisma, he had a great influence on CERN and contributed much in promoting the role of theoretical physics in the life of the laboratory. With the right mixture of vision, authority, and practical common sense, he led the Theory Division from 2000 to 2004. I have always admired Guido for his brilliance, humour, knowledge, leadership, and intellectual integrity. I learned much from his qualities and his example is a precious legacy for me and for all of his colleagues. Guido had a very pragmatic attitude towards scientific theories. He was not attracted arXiv:1710.07663v1 [physics.hist-ph] 18 Oct 2017 by elaborate mathematical constructions, but wanted to understand the essence behind the formalism and get straight to the concept. In physics, I would define him as a conservative revolutionary or as an optimistic skeptical. One episode illustrates the meaning of this definition.
    [Show full text]
  • Theoretical Particle Physics Laboratory (LPTP)
    TP - IV Theoretical Particle Physics Laboratory (LPTP) Riccardo Rattazzi Relativity Quantum Mechanics instantenous action at a Discrete nature of distance is not possible microworld need fields permeating all of space wave of smallest intensity: particle interaction carried by waves in the fields Relativity Quantum Field Theory Quantum Mechanics Explanation of existence of matter, forces and their properties Standard Model: specific QFT describing/explaining basicaly all that we see EM weak strong gravity Higgs geometric bizarre Relativity Quantum Field Theory Quantum Mechanics Explanation of existence of matter, forces and their properties Standard Model: specific QFT describing/explaining basicaly all that we see EM weak strong gravity Higgs geometric bizarre • Most precisely tested theory in science (g-2 of electron, 1ppb) • Atomic and Nuclear physics “just” complex corollaries of simple principles • Satisfies all particle physics tests so far ...yet big mysteries persist (and deepened with Higgs discovery) The mysteries (some of them) • The origin of matter/antimatter symmetry in the universe • What is Dark Matter made up of? • .... • .... • The incredible properties of the vacuum Quantum mechanically the vacuum is very active Higgs force and The curvature radius its boson should of universe should plausibly be plausibly be less than confined to 10-3 mm distances of (Dark Energy order 10-30 cm puzzle) (Hierarchy puzzle) Quantum mechanically the vacuum is very active Higgs force and The curvature radius its boson should of universe should
    [Show full text]