String Theory and Applications to Phenomenology and Cosmology
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Particles-Versus-Strings.Pdf
Particles vs. strings http://insti.physics.sunysb.edu/~siegel/vs.html In light of the huge amount of propaganda and confusion regarding string theory, it might be useful to consider the relative merits of the descriptions of the fundamental constituents of matter as particles or strings. (More-skeptical reviews can be found in my physics parodies.A more technical analysis can be found at "Warren Siegel's research".) Predictability The main problem in high energy theoretical physics today is predictions, especially for quantum gravity and confinement. An important part of predictability is calculability. There are various levels of calculations possible: 1. Existence: proofs of theorems, answers to yes/no questions 2. Qualitative: "hand-waving" results, answers to multiple choice questions 3. Order of magnitude: dimensional analysis arguments, 10? (but beware hidden numbers, like powers of 4π) 4. Constants: generally low-energy results, like ground-state energies 5. Functions: complete results, like scattering probabilities in terms of energy and angle Any but the last level eventually leads to rejection of the theory, although previous levels are acceptable at early stages, as long as progress is encouraging. It is easy to write down the most general theory consistent with special (and for gravity, general) relativity, quantum mechanics, and field theory, but it is too general: The spectrum of particles must be specified, and more coupling constants and varieties of interaction become available as energy increases. The solutions to this problem go by various names -- "unification", "renormalizability", "finiteness", "universality", etc. -- but they are all just different ways to realize the same goal of predictability. -
JHEP10(2009)051 3 3 2), | S 1 Ads , (1 × 3 Heory P SU August 10, 2009 October 20, 2009 : : September 20, 2009 : Ads Received , Published Unting in D1-D5 Systems
Published by IOP Publishing for SISSA Received: August 10, 2009 Accepted: September 20, 2009 Published: October 20, 2009 3 Asymptotic symmetries of string theory on AdS3 × S JHEP10(2009)051 with Ramond-Ramond fluxes Sujay K. Ashok,a,b Raphael Benichouc and Jan Troostc aInstitute of Mathematical Sciences, C.I.T Campus, Taramani, Chennai, 600113 India bPerimeter Institute for Theoretical Physics, Waterloo, Ontario, ON N2L2Y5, Canada cLaboratoire de Physique Th´eorique, Unit´eMixte du CRNS et de l’Ecole´ Normale Sup´erieure associ´ee `al’Universit´ePierre et Marie Curie 6, UMR 8549, 24 Rue Lhomond, Paris 75005, France E-mail: [email protected], [email protected], [email protected] Abstract: String theory on AdS3 space-times with boundary conditions that allow for black hole states has global asymptotic symmetries which include an infinite dimensional conformal algebra. Using the conformal current algebra for sigma-models on P SU(1, 1 2), | we explicitly construct the R-symmetry and Virasoro charges in the worldsheet theory describing string theory on AdS S3 with Ramond-Ramond fluxes. We also indicate how 3 × to construct the full boundary superconformal algebra. The boundary superconformal algebra plays an important role in classifying the full spectrum of string theory on AdS3 with Ramond-Ramond fluxes, and in the microscopic entropy counting in D1-D5 systems. Keywords: AdS-CFT Correspondence, Conformal Field Models in String Theory ArXiv ePrint: 0907.1242 c SISSA 2009 doi:10.1088/1126-6708/2009/10/051 Contents 1 Introduction 1 3 -
Exercise 3 — Supersymmetry for Superstrings
Arash Ardehali String Theory | Prof. Sheikh-Jabbari Exercise 3 | Supersymmetry for Superstrings 1. SUSY generalities (suggested reading : Vafa et. al., Mirror symmetry, Ch 10) Supersymmetry often leads to: I) stability of quantum systems, and II) control over the non-perturbative regime of quantum systems. As for item I, in string theory supersymmetry allows removing the bosonic string tachyon in Minkowski background. (Question: do you remember the masses of the open and closed bosonic string tachyons in Minkowski background?) In other words, the superstring spectrum, unlike the bosonic spectrum, does not signal a perturbative instability in the system. The fact that supersymmetry (SUSY) removes the tachyon (after GSO, of course), is in accord with the general wisdom that supersymmetry often stabilizes quantum systems. • Write down the N = (1; 1) SUSY algebra (in terms of Hilbert-space operators) in 1+0, 1+1, and 1+3 dimensional quantum field theories. [Hint: ask Google.] Make sure you understand the role of y. Show that in all cases the SUSY algebra implies a positive semi-definite energy. [Hint: write the expectation value of the Hamiltonian in terms of the supercharge operators.] • Write down the SUSY algebra in 1+1 dimensional conformal field theory (CFT). This CFT could be the one living on the worldsheet of superstrings. Does the algebra imply a positivity constraint on the spectrum? Task: read about Witten's SUSY-inspired proof of the positive energy theorem in clas- sical GR. As for item II, in string theory supersymmetry allows understanding various strong- weak dualities between the five superstring theories and M-theory. -
Modular Constraints on Superconformal Field Theories
KIAS-P18096 Modular Constraints on Superconformal Field Theories Jin-Beom Bae, Sungjay Lee, and Jaewon Song Korea Institute for Advanced Study 85 Hoegiro, Dongdaemun-Gu, Seoul 02455, Korea Abstract We constrain the spectrum of N = (1; 1) and N = (2; 2) superconformal field theories in two-dimensions by requiring the NS-NS sector partition function to be invariant under the Γθ congruence subgroup of the full modular group SL(2; Z). We employ semi-definite programming to find constraints on the allowed spectrum of operators with or without U(1) charges. Especially, the arXiv:1811.00976v1 [hep-th] 2 Nov 2018 upper bounds on the twist gap for the non-current primaries exhibit interest- ing peaks, kinks, and plateau. We identify a number of candidate rational (S)CFTs realized at the numerical boundaries and find that they are realized as the solutions to modular differential equations associated to Γθ. Some of the candidate theories have been discussed by H¨ohnin the context of self-dual ex- tremal vertex operator (super)algebra. We also obtain bounds for the charged operators and study their implications to the weak gravity conjecture in AdS3. Contents 1 Introduction 1 2 Preliminaries 7 2.1 Representations of N = 1 Superconformal Algebra . .7 2.2 Representations of N = 2 Superconformal Algebra . .9 2.3 Semi-Definite Programming . 12 3 Charge Independent Bounds 14 3.1 Spin-independent bounds on the gap . 14 3.2 Spin-dependent Bounds for N = (1; 1) SCFT . 16 3.3 Spin-dependent Bounds for N = (2; 2) SCFT . 26 4 Charge Dependent Bounds 29 4.1 HFK-type Bound for the Charged States . -
Prospects from Strings and Branes
Prospects from strings and branes Alexander Sevrin Vrije Universiteit Brussel and The International Solvay Institutes for Physics and Chemistry http://tena4.vub.ac.be/ Moriond 2004 Strings and branes… Moriond, March 24, 2004 1 References Not-too-technical review paper, including numerous references: Strings, Gravity and Particle Physics by Augusto Sagnotti and AS In the proceedings of 37th Rencontres de Moriond on Electroweak Interactions and Unified Theories, 2002. e-Print Archive: hep-ex/0209011 Strings and branes… Moriond, March 24, 2004 2 Contents • Dirichlet-branes • D-branes and gauge theories - Worldvolume point of view -AdS/CFT • D-branes and black holes •Cosmology • Some conclusions Strings and branes… Moriond, March 24, 2004 3 Branes Solitons: solutions of the equations of motion with a finite energy(-density) and a mass inversely proportional to the coupling constant. E.g. Scalar field in d = 1 + 1: kink. 12m3 mass = λ Other example in d = 3 + 1: magnetic monopole: 1 mass ∝ 2 gYM Strings and branes… Moriond, March 24, 2004 4 Solitons in string theory: Dirichlet branes Besides the “conventional” fields, such as e.g., gµν (x)=gνµ(x): metric = graviton Φ(x): dilaton, one has RR- potentials as well. E.g. vector potential, A µ : Fµν = ∂µAν − ∂ν Aµ, Aµ → Aµ − ∂µf, Fµν → Fµν . Couples to particles: µ S = q dτ x˙ (τ)Aµ(x(τ)). Z Strings and branes… Moriond, March 24, 2004 5 E.g. 2-form potential, A µ ν = − A ν µ : Fµνρ = ∂µAνρ + ∂ν Aρµ + ∂ρAµν , Aµν → Aµν − ∂µfν + ∂ν fµ,Fµνρ → Fµνρ. Couples to strings: µ ν S = q dτdσ x˙(τ, σ) x0(τ, σ) Aµν (x(τ, σ)). -
Comments on String Theory on Adss
© 1998 International Press Adv. Theor. Math. Phys. 2 (1998) 733-782 Comments on String Theory on AdSs Amit Giveona, David Kutasovb, Nathan Seibergc aRacah Institute of Physics The Hebrew University Jerusalem 91904, Israel b Department of Physics University of Chicago 5640 S. Ellis Av. Chicago, IL 60637, USA ^Department of Physics of Elementary Particles Weizmann Institute of Science Rehovot, Israel cSchool of Natural Sciences Institute for Advanced Study Olden Lane Princeton, NJ, USA Abstract We study string propagation on AdSs times a compact space from an "old fashioned" worldsheet point of view of perturbative string theory. We derive the spacetime CFT and its Virasoro and current algebras, thus establishing the conjectured AdS/CFT correspondence for this case in the full string theory. Our results have implications for the extreme IR limit of the Dl - D5 system, as well as to 2+1 dimensional BTZ black holes and their Bekenstein-Hawking entropy. e-print archive: http://xxx.lanl.gov/abs/hep-th/9806194 734 COMMENTS ON STRING THEORY ON AdSz 1 Introduction The purpose of this paper is to study string propagation on curved spacetime manifolds that include AdS^. We will mostly discuss the Euclidean version also known as H^ = 51/(2, C)/SU(2) (in Appendix A we will comment on the Lorentzian signature version of AdS^, which is the SX(2, R) group man- ifold) . At low energies the theory reduces to 2 + 1 dimensional gravity with a negative cosmological constant coupled (in general) to a large collection of matter fields. The low energy action is but we will go beyond this low energy approximation. -
String Theory 101 Lectures at the International School of Strings and Fundamental Physics
String Theory 101 Lectures at the International School of Strings and Fundamental Physics Munich July 26 - August 6 2010 Neil Lambert Theory Division CERN 1211 Geneva 23 Switzerland Email: [email protected] 1 Contents 1 Introduction: Why String Theory? 3 2 Classical and Quantum Dynamics of Point Particles 4 2.1 Classical Action . 4 2.2 Electromagnetic field . 7 2.3 Quantization . 8 3 Classical and Quantum Dynamics of Strings 10 3.1 Classical Action . 10 3.2 Spacetime Symmetries and Conserved Charges . 13 3.3 Quantization . 14 3.4 Open Strings . 23 3.5 Closed Strings . 27 4 Light-cone gauge 31 4.1 D = 26, a =1................................. 33 4.2 Partition Function . 34 5 Curved Spacetime and an Effective Action 36 5.1 Strings in Curved Spacetime . 36 5.2 A Spacetime Effective Action . 38 6 Superstrings 39 6.1 Type II strings . 39 6.2 Type I and Heterotic String . 44 6.3 The Spacetime Effective Action . 46 2 1 Introduction: Why String Theory? The so-called Standard Model of Particle Physics is the most successful scientific theory of Nature in the sense that no other theory has such a high level of accuracy over such a complete range of physical phenomena using such a modest number of assumptions and parameters. It is unreasonably good and was never intended to be so successful. Since its formulation around 1970 there has not been a single experimental result that has produced even the slightest disagreement. Nothing, despite an enormous amount of effort. But there are skeletons in the closet. -
The Early Years of String Theory: a Personal Perspective
CALT-68-2657 THE EARLY YEARS OF STRING THEORY: A PERSONAL PERSPECTIVE John H. Schwarz California Institute of Technology Pasadena, CA 91125, USA Abstract arXiv:0708.1917v3 [hep-th] 3 Apr 2009 This article surveys some of the highlights in the development of string theory through the first superstring revolution in 1984. The emphasis is on topics in which the author was involved, especially the observation that critical string theories provide consistent quantum theories of gravity and the proposal to use string theory to construct a unified theory of all fundamental particles and forces. Based on a lecture presented on June 20, 2007 at the Galileo Galilei Institute 1 Introduction I am happy to have this opportunity to reminisce about the origins and development of string theory from 1962 (when I entered graduate school) through the first superstring revolution in 1984. Some of the topics were discussed previously in three papers that were written for various special events in 2000 [1, 2, 3]. Also, some of this material was reviewed in the 1985 reprint volumes [4], as well as the string theory textbooks [5, 6]. In presenting my experiences and impressions of this period, it is inevitable that my own contributions are emphasized. Some of the other early contributors to string theory have presented their recollections at the Galileo Galilei Institute meeting on “The Birth of String Theory” in May 2007. Since I was unable to attend that meeting, my talk was given at the GGI one month later. Taken together, the papers in this collection should -
Introduction to Superstring Theory
Introduction to Superstring theory Carmen Nunez Instituto de Astronomia y Física del Espacio C.C. 67 - Sue. 28, 1428 Buenos Aires, Argentina and Physics Department, University of Buenos Aires [email protected] Abstract 1 Overview The bosonic string theory, despite all its beautiful features, has a number of short comings. The most obvious of these are the absence of fermions and the presence of tachyons in spacetime. The tachyon is not an actual physical inconsistency; it indicates at least that the calculations are being performed in an unstable vacuum state. More over, tachyon exchange contributes infrarred divergences in loop diagrams and these divergences make it hard to isolate the ultraviolet behaviour of the "unified quan tum theory" the bosonic string theory gives rise to and determine whether it is really satisfactory. Historically, the solution to the tachyon problem appeared with the solution to the other problem, the absence of fermions. The addition of a new ingredient, supersym- metry on the world-sheet, improves substantially the general picture. In 1977 Gliozzi, Scherk and Olive showed that it was possible to get a model with no tachyons and with equal masses and multiplicities for bosons and fermions. In 1980, Green and Schwarz proved that this model had spacetime supersymmetry. In the completely consisten- t tachyon free form of the superstring theory it was then possible to show that the one-loop diagrams were completely finite and free of ultraviolet divergences. While most workers on the subject believe that the finiteness will also hold to all orders of perturbation theory, complete and universally accepted proofs have not appeared so far. -
The Conformal Bootstrap and Super W-Algebras
THE CONFORMAL BOOTSTRAP AND SUPER W -ALGEBRAS Jose´ M. Figueroa-O’Farrill\ and Stany Schrans] Instituut voor Theoretische Fysica, Universiteit Leuven Celestijnenlaan 200 D, B–3001 Heverlee, BELGIUM ABSTRACT We undertake a systematic study of the possible extensions of the N = 1 super Vi- 1 7 rasoro algebra by a superprimary field of spin 2 ≤ ∆ ≤ 2 . Besides new extensions which exist only for specific values of the central charge, we find a new non-linear algebra (super W2) generated by a spin 2 superprimary which is associative for all values of the central charge. Furthermore, the spin 3 extension is argued to be the symmetry algebra of the m = 6 super Virasoro unitary minimal model, by exhibiting the (A7,D4)-type modular invariant as diagonal in terms of extended characters. \ e-mail: [email protected] ] Onderzoeker I.I.K.W., Belgium; e-mail: [email protected] §1 Introduction Extended conformal and superconformal algebras have received a great deal of attention lately[1],[2],[3]. Their study is relevant for the classification problem of rational conformal field theories[4] (RCFTs) since every RCFT is by definition a minimal model of its chiral algebra (the operator subalgebra generated by its holomorphic fields) which, since it contains the Virasoro algebra as a subalgebra, extends it. As shown by Cardy[5], a conformal field theory (CFT) which is ra- tional relative to the Virasoro algebra (i.e. , which contains a finite number of Virasoro primaries) must necessarily have c < 1. Similar arguments show that a superconformal field theory (SCFT) which is rational relative to the N = 1 super 3 Virasoro algebra must have c < 2 . -
Thesis in Amsterdam
UvA-DARE (Digital Academic Repository) The physics and mathematics of microstates in string theory: And a monstrous Farey tail de Lange, P. Publication date 2016 Document Version Final published version Link to publication Citation for published version (APA): de Lange, P. (2016). The physics and mathematics of microstates in string theory: And a monstrous Farey tail. General rights It is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulations If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: https://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. UvA-DARE is a service provided by the library of the University of Amsterdam (https://dare.uva.nl) Download date:10 Oct 2021 P a u A dissertation that delves l The Physics & d into physical and e L mathematical aspects of a Microstates Mathematics of n g string theory. In the first e part ot this book, Microstates in T microscopic porperties of h Moonshine e string theoretic black String Theory P h holes are investigated. -
Introduction to Superstring Theory
Introduction to Superstring Theory Carmen N´u~nez IAFE (UBA-CONICET) & PHYSICS DEPT. (University of Buenos Aires) VI ICTP LASS 2015 Mexico, 26 October- 6 November 2015 . Programme Class 1: The classical fermionic string Class 2: The quantized fermionic string Class 3: Partition Function Class 4: Interactions . Outline Class 1: The classical fermionic string The action and its symmetries Gauge fixing and constraints Equations of motion and boundary conditions Oscillator expansions . The spectra of bosonic strings contain a tachyon ! it might indicate the vacuum has been incorrectly identified. The mass squared of a particle T is the quadratic term in the 2 @2V (T ) j − 4 ) action: M = @T 2 T =0 = α0 = we are expanding around a maximum of V . If there is some other stable vacuum, this is not an actual inconsistency. Why superstrings? . The mass squared of a particle T is the quadratic term in the 2 @2V (T ) j − 4 ) action: M = @T 2 T =0 = α0 = we are expanding around a maximum of V . If there is some other stable vacuum, this is not an actual inconsistency. Why superstrings? The spectra of bosonic strings contain a tachyon ! it might indicate the vacuum has been incorrectly identified. If there is some other stable vacuum, this is not an actual inconsistency. Why superstrings? The spectra of bosonic strings contain a tachyon ! it might indicate the vacuum has been incorrectly identified. The mass squared of a particle T is the quadratic term in the 2 @2V (T ) j − 4 ) action: M = @T 2 T =0 = α0 = we are expanding around a maximum of V .