Introduction Co String and Superstrtog Theory II SLAC-PUB--4251 DE87
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String Theory. Volume 1, Introduction to the Bosonic String
This page intentionally left blank String Theory, An Introduction to the Bosonic String The two volumes that comprise String Theory provide an up-to-date, comprehensive, and pedagogic introduction to string theory. Volume I, An Introduction to the Bosonic String, provides a thorough introduction to the bosonic string, based on the Polyakov path integral and conformal field theory. The first four chapters introduce the central ideas of string theory, the tools of conformal field theory and of the Polyakov path integral, and the covariant quantization of the string. The next three chapters treat string interactions: the general formalism, and detailed treatments of the tree-level and one loop amplitudes. Chapter eight covers toroidal compactification and many important aspects of string physics, such as T-duality and D-branes. Chapter nine treats higher-order amplitudes, including an analysis of the finiteness and unitarity, and various nonperturbative ideas. An appendix giving a short course on path integral methods is also included. Volume II, Superstring Theory and Beyond, begins with an introduction to supersym- metric string theories and goes on to a broad presentation of the important advances of recent years. The first three chapters introduce the type I, type II, and heterotic superstring theories and their interactions. The next two chapters present important recent discoveries about strongly coupled strings, beginning with a detailed treatment of D-branes and their dynamics, and covering string duality, M-theory, and black hole entropy. A following chapter collects many classic results in conformal field theory. The final four chapters are concerned with four-dimensional string theories, and have two goals: to show how some of the simplest string models connect with previous ideas for unifying the Standard Model; and to collect many important and beautiful general results on world-sheet and spacetime symmetries. -
Cosmic Accelerated Expansion, Dark Matter and Dark Energy from a Heterotic Superstrings Scenario*
International Journal of Innovation in Science and Mathematics Volume 5, Issue 2, ISSN (Online): 2347–9051 Cosmic Accelerated Expansion, Dark Matter and Dark Energy from a Heterotic Superstrings Scenario* Mohamed S. El Naschie Dept. of Physics, Faculty of Science, University of Alexandria, Egypt. Abstract — Guided by the basic ideas and structure of with a minor twist here and there, we felt it pertinent to heterotic string theory we establish an energy density triality, give here a brief account of the quintessential idea behind which add together to the theoretically expected energy heterotic string theory seen from our “pure dark energy density based on Einstein’s relativity. Thus Einstein’s and dark matter” explanation view point [20-27]. famous formula E = mc2 is found in integer approximation to 1 5 16 2 be the sum of three sectors, namely E mc II. HETEROTIC STRING THEORY FOR DARK 22 ENERGY 2 where E( O ) mc 22 is the ordinary energy density, E( DM ) 5 22 mc2 is the dark matter energy density and We think it is fair to say that what David Gross [18] had 2 in mind when he and his group started work on a new E( PD ) 16 22 mc is the pure dark energy density where heterotic string theory was simply to combine the Green- m is the mass, c is the velocity of light and 16 is the number Schwarz so called Type II, at the time a new ten of heterotic strings extra bosons. We demonstrate further dimensional superstring theory with the relatively older 26 that strictly speaking dark matter is weakly coupled with dimensional bosonic string theory [13-18]. -
Super-Higgs in Superspace
Article Super-Higgs in Superspace Gianni Tallarita 1,* and Moritz McGarrie 2 1 Departamento de Ciencias, Facultad de Artes Liberales, Universidad Adolfo Ibáñez, Santiago 7941169, Chile 2 Deutsches Elektronen-Synchrotron, DESY, Notkestrasse 85, 22607 Hamburg, Germany; [email protected] * Correspondence: [email protected] or [email protected] Received: 1 April 2019; Accepted: 10 June 2019; Published: 14 June 2019 Abstract: We determine the effective gravitational couplings in superspace whose components reproduce the supergravity Higgs effect for the constrained Goldstino multiplet. It reproduces the known Gravitino sector while constraining the off-shell completion. We show that these couplings arise by computing them as quantum corrections. This may be useful for phenomenological studies and model-building. We give an example of its application to multiple Goldstini. Keywords: supersymmetry; Goldstino; superspace 1. Introduction The spontaneous breakdown of global supersymmetry generates a massless Goldstino [1,2], which is well described by the Akulov-Volkov (A-V) effective action [3]. When supersymmetry is made local, the Gravitino “eats” the Goldstino of the A-V action to become massive: The super-Higgs mechanism [4,5]. In terms of superfields, the constrained Goldstino multiplet FNL [6–12] is equivalent to the A-V formulation (see also [13–17]). It is, therefore, natural to extend the description of supergravity with this multiplet, in superspace, to one that can reproduce the super-Higgs mechanism. In this paper we address two issues—first we demonstrate how the Gravitino, Goldstino, and multiple Goldstini obtain a mass. Secondly, by using the Spurion analysis, we write down the most minimal set of new terms in superspace that incorporate both supergravity and the Goldstino multiplet in order to reproduce the super-Higgs mechanism of [5,18] at lowest order in M¯ Pl. -
Workshop Materials
Status and Future of Inflationary Theory August 22-24, 2014 KICP workshop, 2014 Chicago, IL http://kicp-workshops.uchicago.edu/inflation2014/ WORKSHOP MATERIALS http://kicp.uchicago.edu/ http://www.uchicago.edu/ The Kavli Institute for Cosmological Physics (KICP) at the University of Chicago is hosting a workshop this summer on inflationary theory. The goal is to gather a small group of researchers working in inflationary cosmology for several days of informal presentations and discussion relating to the status of theories of the inflationary universe. Topics of particular focus are model building, challenges for inflationary theories, connections to fundamental physics, and prospects for refining our understanding with future datasets. This meeting is a satellite conference of COSMO 2014. The meeting will be complementary to the COSMO conference in that it will be small, informal, and relatively narrow in scope. Invited Speakers Raphael Bousso Robert Brandenberger Cora Dvorkin University of California, Berkeley McGill University Institute for Advanced Study Richard Easther Raphael Flauger Daniel Green University of Auckland Institute for Advanced Study CITA Rich Holman Anna Ijjas Justin Khoury Carnegie Mellon Princeton University University of Pennsylvania Will Kinney Matt Kleban Albion Lawrence SUNY, Buffalo New York University Brandeis University Eugene Lim Emil Martinec Liam McAllister King's College London University of Chicago Cornell University Hiranya Peiris Leonardo Senatore Eva Silverstein University College London Stanford University Stanford University Paul Steinhardt Mark Trodden Princeton University University of Pennsylvania Organizing Committee Peter Adshead Wayne Hu Austin Joyce University of Illinois at Urbana University of Chicago University of Chicago Champaign Marilena LoVerde Emil Martinec University of Chicago University of Chicago Status and Future of Inflationary Theory August 22-24, 2014 @ Chicago, IL List of Participants 1. -
Supersymmetric R4 Actions and Quantum Corrections to Superspace Torsion Constraints
DAMTP-2000-91, NORDITA-2000/87 HE, SPHT-T00/117, hep-th/0010182 SUPERSYMMETRIC R4 ACTIONS AND QUANTUM CORRECTIONS TO SUPERSPACE TORSION CONSTRAINTS K. Peetersa, P. Vanhoveb and A. Westerbergc a CERN, TH-division 1211 Geneva 23, Switzerland b SPHT, Orme des Merisiers, CEA / Saclay, 91191 Gif-sur-Yvette, France c NORDITA, Blegdamsvej 17, DK-2100 Copenhagen Ø, Denmark k.peeters, [email protected], [email protected] We present the supersymmetrisation of the anomaly-related R4 term in eleven dimensions and show that it induces no non-trivial modifications to the on-shell supertranslation algebra and the superspace torsion constraints before inclusion of gauge-field terms.1 1 Higher-derivative corrections and supersymmetry The low-energy supergravity limits of superstring theory as well as D-brane effective actions receive infinite sets of correction terms, proportional to in- 2 creasing powers of α0 = ls and induced by superstring theory massless and massive modes. At present, eleven-dimensional supergravity lacks a corre- sponding microscopic underpinning that could similarly justify the presence of higher-derivative corrections to the classical Cremmer-Julia-Scherk action [1]. Nevertheless, some corrections of this kind are calculable from unitarity argu- ments and super-Ward identities in the massless sector of the theory [2] or by anomaly cancellation arguments [3, 4]. Supersymmetry puts severe constraints on higher-derivative corrections. For example, it forbids the appearance of certain corrections (like, e.g, R3 corrections to supergravity effective actions [5]), and groups terms into var- ious invariants [6–9]. The structure of the invariants that contain anomaly- cancelling terms is of great importance due to the quantum nature of the 1Based on talks given by K.P. -
Introduction to Supersymmetry
Introduction to Supersymmetry Pre-SUSY Summer School Corpus Christi, Texas May 15-18, 2019 Stephen P. Martin Northern Illinois University [email protected] 1 Topics: Why: Motivation for supersymmetry (SUSY) • What: SUSY Lagrangians, SUSY breaking and the Minimal • Supersymmetric Standard Model, superpartner decays Who: Sorry, not covered. • For some more details and a slightly better attempt at proper referencing: A supersymmetry primer, hep-ph/9709356, version 7, January 2016 • TASI 2011 lectures notes: two-component fermion notation and • supersymmetry, arXiv:1205.4076. If you find corrections, please do let me know! 2 Lecture 1: Motivation and Introduction to Supersymmetry Motivation: The Hierarchy Problem • Supermultiplets • Particle content of the Minimal Supersymmetric Standard Model • (MSSM) Need for “soft” breaking of supersymmetry • The Wess-Zumino Model • 3 People have cited many reasons why extensions of the Standard Model might involve supersymmetry (SUSY). Some of them are: A possible cold dark matter particle • A light Higgs boson, M = 125 GeV • h Unification of gauge couplings • Mathematical elegance, beauty • ⋆ “What does that even mean? No such thing!” – Some modern pundits ⋆ “We beg to differ.” – Einstein, Dirac, . However, for me, the single compelling reason is: The Hierarchy Problem • 4 An analogy: Coulomb self-energy correction to the electron’s mass A point-like electron would have an infinite classical electrostatic energy. Instead, suppose the electron is a solid sphere of uniform charge density and radius R. An undergraduate problem gives: 3e2 ∆ECoulomb = 20πǫ0R 2 Interpreting this as a correction ∆me = ∆ECoulomb/c to the electron mass: 15 0.86 10− meters m = m + (1 MeV/c2) × . -
Generalised Geometry and Supergravity Backgrounds
Imperial College, London Department of Physics MSc dissertation Generalised geometry and supergravity backgrounds Author: Supervisor: Daniel Reilly Prof. Daniel Waldram September 30, 2011 Submitted in partial fulfilment of the requirements for the degree of Master of Science of Imperial College London Abstract We introduce the topcic of generalised geometry as an extension of differential geomentry on the bundle TM ⊕ T ∗M. An algebraic structure is built that leads to the formation of the generalised tangent bundle. We place a generalised Riemannian metric on this space and show that it is compatible with the metric for a generalised K¨ahlerstructure. We investigate the nature of supersymmetric backgrounds in type II supergravity by discussing the usual and generalised Calabi-Yau structure. From this we show how the formalism of generalised geometry may be used to describe a manifold with such a structure. It's unique appeal to physicists lies in its unification of the fields in NS-NS sector of supergravity. 1 Contents 1 Introduction 4 1.1 Early work . 4 1.2 Generalised geometry . 6 2 The Courant bracket 8 2.1 Lie algebroids . 8 2.2 Courant bracket . 10 2.3 Twisted Courant barcket . 12 3 Generalised tangent bundle 14 3.1 Linear structure . 14 3.2 Courant algebroid . 17 4 Metric on TM ⊕ T ∗M 19 4.1 Dirac structure . 19 4.2 Generalised metric . 20 4.3 Complex structure . 21 4.4 Generalised complex structure . 23 4.5 Generalised K¨ahlerstructure . 24 5 Spinors on TM ⊕ T ∗M 28 5.1 Clifford algebra . 28 5.2 Generalised Calbi-Yau structure . -
Interpreting Supersymmetry
Interpreting Supersymmetry David John Baker Department of Philosophy, University of Michigan [email protected] October 7, 2018 Abstract Supersymmetry in quantum physics is a mathematically simple phenomenon that raises deep foundational questions. To motivate these questions, I present a toy model, the supersymmetric harmonic oscillator, and its superspace representation, which adds extra anticommuting dimensions to spacetime. I then explain and comment on three foundational questions about this superspace formalism: whether superspace is a sub- stance, whether it should count as spatiotemporal, and whether it is a necessary pos- tulate if one wants to use the theory to unify bosons and fermions. 1 Introduction Supersymmetry{the hypothesis that the laws of physics exhibit a symmetry that transforms bosons into fermions and vice versa{is a long-standing staple of many popular (but uncon- firmed) theories in particle physics. This includes several attempts to extend the standard model as well as many research programs in quantum gravity, such as the failed supergravity program and the still-ascendant string theory program. Its popularity aside, supersymmetry (SUSY for short) is also a foundationally interesting hypothesis on face. The fundamental equivalence it posits between bosons and fermions is prima facie puzzling, given the very different physical behavior of these two types of particle. And supersymmetry is most naturally represented in a formalism (called superspace) that modifies ordinary spacetime by adding Grassmann-valued anticommuting coordinates. It 1 isn't obvious how literally we should interpret these extra \spatial" dimensions.1 So super- symmetry presents us with at least two highly novel interpretive puzzles. Only two philosophers of science have taken up these questions thus far. -
Black Holes and Thermodynamics of Non-Gravitational Theories
EFI-99-26 hep-th/9906044 Black Holes and Thermodynamics of Non-Gravitational Theories Vatche Sahakian1 2 Enrico Fermi Inst. and Dept. of Physics University of Chicago 5640 S. Ellis Ave., Chicago, IL 60637, USA Abstract arXiv:hep-th/9906044v1 4 Jun 1999 This is a thesis/review article that combines some of the results of [1, 2, 3] with a short discussion of introductory background material; an attempt has been made to present the work in a self-contained manner. The first chapter mostly targets readers who are vaguely familiar with traditional and contemporary string theory. Chapter two discusses in detail the thermodynamics of the 0 + 1 dimensional Super Yang-Mills (SYM) theory as an illustrative example of the main ideas of the work. The third chapter outlines the phase structures of p + 1 dimensional SYM theories on tori for 1 p 5, and that of the D1D5 system; we avoid presenting the technical details of the construction of these phase≤ diagrams,≤ focusing instead on the physics of the final results. The last chapter discusses the dynamics of the formation of boosted black holes in strongly coupled SYM theory. [email protected] 2Address after August 1, 1999: Laboratory of Nuclear Studies, Cornell University, Ithaca, NY 14853 2 Acknowledgments The work presented in this thesis is a compilation of the papers [1, 2, 3]; it was submitted to the division of Physical Sciences at the University of Chicago as a PhD thesis. I thank my collaborators Emil Martinec and Miao Li for many fruitful discussions and a pleasant atmosphere of collaboration. -
25. Hu2019.Pdf
Superfield Component Decompositions and the Scan for Prepotential Supermultiplets in High Dimensional Superspaces Yangrui Hu Dec 16, Miami 2019 Conference Based on the work with S.J. Gates, Jr. and S.-N. Hazel Mak [arXiv: 1911.00807], [arXiv: 1912.xxxx], and [arXiv: 1912.xxxx] Motivation An irreducible (even a reducible) off-shell formulation containing a finite number of component fields for the ten and eleven dimensional supergravity multiplet has not been presented. Our purpose: reducible off-shell formulation Scalar superfield: compensator Prepotential candidates [1] S.J. Gates, Jr., Y. Hu,, H. Jiang, and , S.-N. Hazel Mak, A codex on linearized Nordström supergravity in eleven and ten dimensional superspaces, JHEP 1907 (2019) 063, DOI: 10.1007/ JHEP07(2019)063 2 Linearized Nordström SUGRA: In Nordström theory, only non-conformal spin-0 part of graviton and non-conformal spin-1/2 part of gravitino show up All component fields of Nordström SG are obtained from spin-0 graviton, spin-1/2 gravitino, and all possible spinorial derivatives to the field strength Gαβ [1] S.J. Gates, Jr., Y. Hu,, H. Jiang, and , S.-N. Hazel Mak, A codex on linearized Nordström supergravity in eleven and ten dimensional superspaces, JHEP 1907 (2019) 063, DOI: 10.1007/ JHEP07(2019)063 3 Scalar Superfield Decomposition in 10D, � = 1 Breitenlohner 10D, � = 2A 10D, � = 2B Approach [2] 9D to 5D minimal 11D, � = 1 scalar superfield decomp prepotential 10D YM candidates supermultiplet Young Tableau Approach Branching Rule Approach [2] P. Breitenlohner, “A Geometric Interpretation of Local Supersymmetry,” Phys. Lett. 67B (1977) 49, DOI: 10.1016/0370-2693(77)90802-4. -
Effective Dynamics of the Schwarzschild Black Hole Interior
Effective dynamics of the Schwarzschild black hole interior with inverse triad corrections Hugo A. Morales-Técotl,1, 2, ∗ Saeed Rastgoo,3, 1, 4, y and Juan C. Ruelas1, z 1Departamento de Física, Universidad Autónoma Metropolitana - Iztapalapa San Rafael Atlixco 186, Ciudad de Mexico 09340, Mexico 2Departamento de Física, Escuela Superior de Física y Matemáticas del Instituto Politécnico Nacional Unidad Adolfo López Mateos, Edificio 9, 07738 Ciudad de México, Mexico 3School of Sciences and Engineering Monterrey Institute of Technology (ITESM), Campus León Av. Eugenio Garza Sada, León, Guanajuato 37190, Mexico 4Department of Physics and Astronomy, York University 4700 Keele Street, Toronto, Ontario M3J 1P3, Canada (Dated: January 22, 2021) We reconsider the study of the interior of the Schwarzschild black hole now in- cluding inverse triad quantum corrections within loop quantization. We derive these corrections and show that they are are related to two parameters δb; δc associated to the minimum length in the radial and angular directions, that enter Thiemann’s trick for quantum inverse triads. Introduction of such corrections may lead to non- invariance of physical results under rescaling of the fiducial volume needed to compute the dynamics, due to noncompact topology of the model. So, we put forward two prescriptions to resolve this issue. These prescriptions amount to interchange δb; δc in classical computations in Thiemann’s trick. By implementing the inverse triad cor- rections we found, previous results such as singularity resolution and black-to-white hole bounce hold with different values for the minimum radius-at-bounce, and the mass of the white hole. I. INTRODUCTION As one of the most fascinating predictions of general relativity, black holes have been arXiv:1806.05795v3 [gr-qc] 21 Jan 2021 the subject of much analysis and explorations. -
Lectures on Supersymmetry
Lectures on Supersymmetry Matteo Bertolini SISSA June 9, 2021 1 Foreword This is a write-up of a course on Supersymmetry I have been giving for several years to first year PhD students attending the curriculum in Theoretical Particle Physics at SISSA, the International School for Advanced Studies of Trieste. There are several excellent books on supersymmetry and many very good lecture courses are available on the archive. The ambition of this set of notes is not to add anything new in this respect, but to offer a set of hopefully complete and self- consistent lectures, which start from the basics and arrive to some of the more recent and advanced topics. The price to pay is that the material is pretty huge. The advantage is to have all such material in a single, possibly coherent file, and that no prior exposure to supersymmetry is required. There are many topics I do not address and others I only briefly touch. In particular, I discuss only rigid supersymmetry (mostly focusing on four space-time dimensions), while no reference to supergravity is given. Moreover, this is a the- oretical course and phenomenological aspects are only briefly sketched. One only chapter is dedicated to present basic phenomenological ideas, including a bird eyes view on models of gravity and gauge mediation and their properties, but a thorough discussion of phenomenological implications of supersymmetry would require much more. There is no bibliography at the end of the file. However, each chapter contains its own bibliography where the basic references (mainly books and/or reviews available on-line) I used to prepare the material are reported { including explicit reference to corresponding pages and chapters, so to let the reader have access to the original font (and to let me give proper credit to authors).