Introduction to String Theory
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Band Spectrum Is D-Brane
Prog. Theor. Exp. Phys. 2016, 013B04 (26 pages) DOI: 10.1093/ptep/ptv181 Band spectrum is D-brane Koji Hashimoto1,∗ and Taro Kimura2,∗ 1Department of Physics, Osaka University, Toyonaka, Osaka 560-0043, Japan 2Department of Physics, Keio University, Kanagawa 223-8521, Japan ∗E-mail: [email protected], [email protected] Received October 19, 2015; Revised November 13, 2015; Accepted November 29, 2015; Published January 24 , 2016 Downloaded from ............................................................................... We show that band spectrum of topological insulators can be identified as the shape of D-branes in string theory. The identification is based on a relation between the Berry connection associated with the band structure and the Atiyah–Drinfeld–Hitchin–Manin/Nahm construction of solitons http://ptep.oxfordjournals.org/ whose geometric realization is available with D-branes. We also show that chiral and helical edge states are identified as D-branes representing a noncommutative monopole. ............................................................................... Subject Index B23, B35 1. Introduction at CERN - European Organization for Nuclear Research on July 8, 2016 Topological insulators and superconductors are one of the most interesting materials in which theo- retical and experimental progress have been intertwined each other. In particular, the classification of topological phases [1,2] provided concrete and rigorous argument on stability and the possibility of topological insulators and superconductors. The key to finding the topological materials is their electron band structure. The existence of gapless edge states appearing at spatial boundaries of the material signals the topological property. Identification of possible electron band structures is directly related to the topological nature of topological insulators. It is important, among many possible appli- cations of topological insulators, to gain insight into what kind of electron band structure is possible for topological insulators with fixed topological charges. -
Introductory Lectures on Quantum Field Theory
Introductory Lectures on Quantum Field Theory a b L. Álvarez-Gaumé ∗ and M.A. Vázquez-Mozo † a CERN, Geneva, Switzerland b Universidad de Salamanca, Salamanca, Spain Abstract In these lectures we present a few topics in quantum field theory in detail. Some of them are conceptual and some more practical. They have been se- lected because they appear frequently in current applications to particle physics and string theory. 1 Introduction These notes are based on lectures delivered by L.A.-G. at the 3rd CERN–Latin-American School of High- Energy Physics, Malargüe, Argentina, 27 February–12 March 2005, at the 5th CERN–Latin-American School of High-Energy Physics, Medellín, Colombia, 15–28 March 2009, and at the 6th CERN–Latin- American School of High-Energy Physics, Natal, Brazil, 23 March–5 April 2011. The audience on all three occasions was composed to a large extent of students in experimental high-energy physics with an important minority of theorists. In nearly ten hours it is quite difficult to give a reasonable introduction to a subject as vast as quantum field theory. For this reason the lectures were intended to provide a review of those parts of the subject to be used later by other lecturers. Although a cursory acquaintance with the subject of quantum field theory is helpful, the only requirement to follow the lectures is a working knowledge of quantum mechanics and special relativity. The guiding principle in choosing the topics presented (apart from serving as introductions to later courses) was to present some basic aspects of the theory that present conceptual subtleties. -
TASI Lectures on String Compactification, Model Building
CERN-PH-TH/2005-205 IFT-UAM/CSIC-05-044 TASI lectures on String Compactification, Model Building, and Fluxes Angel M. Uranga TH Unit, CERN, CH-1211 Geneve 23, Switzerland Instituto de F´ısica Te´orica, C-XVI Universidad Aut´onoma de Madrid Cantoblanco, 28049 Madrid, Spain angel.uranga@cern,ch We review the construction of chiral four-dimensional compactifications of string the- ory with different systems of D-branes, including type IIA intersecting D6-branes and type IIB magnetised D-branes. Such models lead to four-dimensional theories with non-abelian gauge interactions and charged chiral fermions. We discuss the application of these techniques to building of models with spectrum as close as possible to the Stan- dard Model, and review their main phenomenological properties. We finally describe how to implement the tecniques to construct these models in flux compactifications, leading to models with realistic gauge sectors, moduli stabilization and supersymmetry breaking soft terms. Lecture 1. Model building in IIA: Intersecting brane worlds 1 Introduction String theory has the remarkable property that it provides a description of gauge and gravitational interactions in a unified framework consistently at the quantum level. It is this general feature (beyond other beautiful properties of particular string models) that makes this theory interesting as a possible candidate to unify our description of the different particles and interactions in Nature. Now if string theory is indeed realized in Nature, it should be able to lead not just to `gauge interactions' in general, but rather to gauge sectors as rich and intricate as the gauge theory we know as the Standard Model of Particle Physics. -
Arxiv:Hep-Th/0006117V1 16 Jun 2000 Oadmarolf Donald VERSION HYPER - Style
Preprint typeset in JHEP style. - HYPER VERSION SUGP-00/6-1 hep-th/0006117 Chern-Simons terms and the Three Notions of Charge Donald Marolf Physics Department, Syracuse University, Syracuse, New York 13244 Abstract: In theories with Chern-Simons terms or modified Bianchi identities, it is useful to define three notions of either electric or magnetic charge associated with a given gauge field. A language for discussing these charges is introduced and the proper- ties of each charge are described. ‘Brane source charge’ is gauge invariant and localized but not conserved or quantized, ‘Maxwell charge’ is gauge invariant and conserved but not localized or quantized, while ‘Page charge’ conserved, localized, and quantized but not gauge invariant. This provides a further perspective on the issue of charge quanti- zation recently raised by Bachas, Douglas, and Schweigert. For the Proceedings of the E.S. Fradkin Memorial Conference. Keywords: Supergravity, p–branes, D-branes. arXiv:hep-th/0006117v1 16 Jun 2000 Contents 1. Introduction 1 2. Brane Source Charge and Brane-ending effects 3 3. Maxwell Charge and Asymptotic Conditions 6 4. Page Charge and Kaluza-Klein reduction 7 5. Discussion 9 1. Introduction One of the intriguing properties of supergravity theories is the presence of Abelian Chern-Simons terms and their duals, the modified Bianchi identities, in the dynamics of the gauge fields. Such cases have the unusual feature that the equations of motion for the gauge field are non-linear in the gauge fields even though the associated gauge groups are Abelian. For example, massless type IIA supergravity contains a relation of the form dF˜4 + F2 H3 =0, (1.1) ∧ where F˜4, F2,H3 are gauge invariant field strengths of rank 4, 2, 3 respectively. -
Two-Dimensional Instantons with Bosonization and Physics of Adjoint QCD2
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Preprint ITEP–TH–21/96 Two-Dimensional Instantons with Bosonization and Physics of Adjoint QCD2. A.V. Smilga ITEP, B. Cheremushkinskaya 25, Moscow 117259, Russia Abstract We evaluate partition functions ZI in topologically nontrivial (instanton) gauge sectors in the bosonized version of the Schwinger model and in a gauged WZNW model corresponding to QCD2 with adjoint fermions. We show that the bosonized model is equivalent to the fermion model only if a particular form of the WZNW action with gauge-invariant integrand is chosen. For the exact correspondence, it is necessary to 2 integrate over the ways the gauge group SU(N)/ZN is embedded into the full O(N −1) group for the bosonized matter field. For even N, one should also take into account the 2 n contributions of both disconnected components in O(N − 1). In that case, ZI ∝ m 0 for small fermion masses where 2n0 coincides with the number of fermion zero modes in n a particular instanton background. The Taylor expansion of ZI /m 0 in mass involves only even powers of m as it should. The physics of adjoint QCD2 is discussed. We argue that, for odd N, the discrete chiral symmetry Z2 ⊗Z2 present in the action is broken spontaneously down to Z2 and the fermion condensate < λλ¯ >0 is formed. The system undergoes a first order phase transition at Tc = 0 so that the condensate is zero at an arbitrary small temperature. -
Five-Branes in Heterotic Brane-World Theories
SUSX-TH/01-037 HUB-EP-01/34 hep-th/0109173 Five-Branes in Heterotic Brane-World Theories Matthias Br¨andle1∗ and Andr´eLukas2§ 1Institut f¨ur Physik, Humboldt Universit¨at Invalidenstraße 110, 10115 Berlin, Germany 2Centre for Theoretical Physics, University of Sussex Falmer, Brighton BN1 9QJ, UK Abstract The effective action for five-dimensional heterotic M-theory in the presence of five-branes is systemat- ically derived from Hoˇrava-Witten theory coupled to an M5-brane world-volume theory. This leads to a 1 five-dimensional N = 1 gauged supergravity theory on S /Z2 coupled to four-dimensional N = 1 theories residing on the two orbifold fixed planes and an additional bulk three-brane. We analyse the properties of this action, particularly the four-dimensional effective theory associated with the domain-wall vacuum state. arXiv:hep-th/0109173v2 8 Oct 2001 The moduli K¨ahler potential and the gauge-kinetic functions are determined along with the explicit relations between four-dimensional superfields and five-dimensional component fields. ∗email: [email protected] §email: [email protected] 1 Introduction A large class of attractive five-dimensional brane-world models can be constructed by reducing Hoˇrava-Witten theory [1, 2, 3] on Calabi-Yau three-folds. This procedure has been first carried out in Ref. [4, 5, 6] and it leads 1 to gauged five-dimensional N = 1 supergravity on the orbifold S /Z2 coupled to N = 1 gauge and gauge matter multiplets located on the two four-dimensional orbifold fixed planes. It has been shown [7]–[13] that a phenomeno- logically interesting particle spectrum on the orbifold planes can be obtained by appropriate compactifications. -
Flux Tubes, Domain Walls and Orientifold Planar Equivalence
Flux tubes, domain walls and orientifold planar equivalence Agostino Patella CERN GGI, 5 May 2011 Agostino Patella (CERN) Tubes and walls GGI, 5/5/11 1 / 19 Introduction Orientifold planar equivalence Orientifold planar equivalence OrQCD 2 SU(N) gauge theory (λ = g N fixed) with Nf Dirac fermions in the antisymmetric representation is equivalent in the large-N limit and in a common sector to AdQCD 2 SU(N) gauge theory (λ = g N fixed) with Nf Majorana fermions in the adjoint representation if and only if C-symmetry is not spontaneously broken. Agostino Patella (CERN) Tubes and walls GGI, 5/5/11 2 / 19 2 Z Z ff e−N W(J) = DADψDψ¯ exp −S(A, ψ, ψ¯) + N2 J(x)O(x)d4x Introduction Orientifold planar equivalence Gauge-invariant common sector AdQCD BOSONIC C-EVEN FERMIONIC C-EVEN BOSONIC C-ODD FERMIONIC C-ODD ~ w OrQCD BOSONIC C-EVEN BOSONIC C-ODD COMMON SECTOR Agostino Patella (CERN) Tubes and walls GGI, 5/5/11 3 / 19 Introduction Orientifold planar equivalence Gauge-invariant common sector AdQCD BOSONIC C-EVEN FERMIONIC C-EVEN BOSONIC C-ODD FERMIONIC C-ODD ~ w OrQCD BOSONIC C-EVEN BOSONIC C-ODD COMMON SECTOR 2 Z Z ff e−N W(J) = DADψDψ¯ exp −S(A, ψ, ψ¯) + N2 J(x)O(x)d4x lim WOr(J) = lim WAd(J) N→∞ N→∞ Agostino Patella (CERN) Tubes and walls GGI, 5/5/11 3 / 19 Introduction Orientifold planar equivalence Gauge-invariant common sector AdQCD BOSONIC C-EVEN FERMIONIC C-EVEN BOSONIC C-ODD FERMIONIC C-ODD ~ w OrQCD BOSONIC C-EVEN BOSONIC C-ODD COMMON SECTOR 2 Z Z ff e−N W(J) = DADψDψ¯ exp −S(A, ψ, ψ¯) + N2 J(x)O(x)d4x hO(x ) ··· O(xn)i hO(x ) ··· -
Flux Backgrounds, Ads/CFT and Generalized Geometry Praxitelis Ntokos
Flux backgrounds, AdS/CFT and Generalized Geometry Praxitelis Ntokos To cite this version: Praxitelis Ntokos. Flux backgrounds, AdS/CFT and Generalized Geometry. Physics [physics]. Uni- versité Pierre et Marie Curie - Paris VI, 2016. English. NNT : 2016PA066206. tel-01620214 HAL Id: tel-01620214 https://tel.archives-ouvertes.fr/tel-01620214 Submitted on 20 Oct 2017 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. THÈSE DE DOCTORAT DE L’UNIVERSITÉ PIERRE ET MARIE CURIE Spécialité : Physique École doctorale : « Physique en Île-de-France » réalisée à l’Institut de Physique Thèorique CEA/Saclay présentée par Praxitelis NTOKOS pour obtenir le grade de : DOCTEUR DE L’UNIVERSITÉ PIERRE ET MARIE CURIE Sujet de la thèse : Flux backgrounds, AdS/CFT and Generalized Geometry soutenue le 23 septembre 2016 devant le jury composé de : M. Ignatios ANTONIADIS Examinateur M. Stephano GIUSTO Rapporteur Mme Mariana GRAÑA Directeur de thèse M. Alessandro TOMASIELLO Rapporteur Abstract: The search for string theory vacuum solutions with non-trivial fluxes is of particular importance for the construction of models relevant for particle physics phenomenology. In the framework of the AdS/CFT correspondence, four-dimensional gauge theories which can be considered to descend from N = 4 SYM are dual to ten- dimensional field configurations with geometries having an asymptotically AdS5 factor. -
Dirac Equation for Strings in Minkowski Space-Time and Then Study the Radial Vibrations of the String
Dirac equation for strings Maciej Trzetrzelewski ∗ M. Smoluchowski Institute of Physics, Jagiellonian University, Lojasiewicza, St. 11, 30-348 Krak´ow, Poland Abstract Starting with a Nambu-Goto action, a Dirac-like equation can be constructed by taking the square-root of the momentum constraint. The eigenvalues of the resulting Hamiltonian are real and correspond to masses of the excited string. In particular there are no tachyons. A special case of radial oscillations of a closed string in Minkowski space-time admits exact solutions in terms of wave functions of the harmonic oscillator. 1 Introduction In 1962 Dirac considered the possibility that leptons may be described arXiv:1302.5907v3 [hep-th] 14 Feb 2018 by extended objects of spherical topology [1, 2]. In this way one could understand the muon as an excitation of the ground state of the membrane - the electron. Anticipating Nambu [3] and Goto [4] by almost a decade he introduced what is now known as a generalization of the Nambu-Goto action to the case of membranes. Using Bohr- Sommerfeld approximation for the Hamiltonian corresponding to the radial mode, one can then show [1] that the mass of the first excitation is about 53me where me is the mass of the electron. This is about a quarter of the observed mass of the muon. In fact, when instead of ∗e-mail: [email protected] 1 the Bohr-Sommerfeld approximation one uses, more precise, numeri- cal methods one finds that the correct value of the first excitation is about 43me [5, 6]. Therefore Dirac’s model ”explains” 1/5th of the actual value of the muon mass. -
HEP-TH-9408163 Address After Sept
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server SNUTP-94-73 CALT-68-1944 TOPOLOGY OF A NONTOPOLOGICAL MAGNETIC MONOPOLE Cho onkyu Lee Department of Physics and Center for Theoretical Physics Seoul National University, Seoul 151-742, Korea 12 Piljin Yi California Institute of Technology, Pasadena, CA 91125, U.S.A. ABSTRACT Certain nontop ological magnetic monop oles, recently found by Lee and Wein- b erg, are reinterpreted as top ological solitons of a non-Ab elian gauged Higgs mo del. Our study makes the nature of the Lee-Weinb erg monop oles more transparent, esp ecially with regard to their singularity structure. Submitted to Physics Letters B. HEP-TH-9408163 1 e-mail address: [email protected] 2 Address after Sept. 1, 1994: Physics Department, Columbia University, New York, NY 10027, U.S.A. When Dirac [1] founded the theory of magnetic monop oles in 1931, the monop ole was not something that p eople could not live without. Things changed a great deal in the seventies when 't Ho oft and Polyakov [2] showed that magnetic monop oles inevitably o ccur as solitons of sp ontaneously broken non-Ab elian gauge theories; such as all grand uni ed theories where an internal semi-simple gauge symmetry is sp ontaneously broken to U (1). Their existence is understo o d in terms of the nontrivial top ology of the vacuum manifold, and as such the non-Ab elian nature of the original gauge group plays a crucial role. -
Low Energy Physics from Type IIB String Theory
Katholieke Universiteit Leuven Faculteit der Wetenschapp en Instituut vo or Theoretische Fysica Low energy physics from typ e IIB string theory Frederik Denef Promotor Prof Dr W Tro ost Pro efschrift ingediend voor het b ehalen van de graad van Do ctor in de Wetenschapp en Deze thesis kwam tot stand met de nanciele steun van het Fonds voor Wetenschapp elijk Onderzo ek Een geest een en al logica is als een mes dat een en al lemmet is Het doet de hand die het gebruikt bloeden Tagore De wijze waarop het eten wordt opgediend is minstens even belangrijk als de wijze waarop het wordt toebereid Ons Kookboek KVLV Vo orwo ord Een thesis schrijf je niet alleen Ik b en daarom iedereen die de vo orbije zes entwintig jaar heeft bijgedragen tot het tot stand komen van dit werk bijzonder dankbaar In de eerste plaats denk ik daarbij natuurlijk aan mijn promotor Walter Tro ost voor het op gang brengen en aanwakkeren van mijn interesse in string theorie en theoretische fysica in het algemeen vo or zijn advies hulp en aanmo edi ging en om me te laten meegenieten van zijn scherp e fysische inzichten humor en relativeringsvermogen Ook Toine Van Pro eyen zou ik sp eciaal willen bedanken omwille van wat hij mij op wetenschapp elijk en menselijk vlak heeft bijgebracht voor de internationale contacten en vo or zijn no oit tanende gedrevenheid waaraan het instituut wellicht een gro ot deel van haar huidige internationale uitstraling te danken heeft Heel wat collegafysici ben ik bovendien dankbaar voor de soms verduisterende maar meestal verhelderende uiteenzettingen -
Electromagnetic Duality for Children
Electromagnetic Duality for Children JM Figueroa-O'Farrill [email protected] Version of 8 October 1998 Contents I The Simplest Example: SO(3) 11 1 Classical Electromagnetic Duality 12 1.1 The Dirac Monopole ....................... 12 1.1.1 And in the beginning there was Maxwell... 12 1.1.2 The Dirac quantisation condition . 14 1.1.3 Dyons and the Zwanziger{Schwinger quantisation con- dition ........................... 16 1.2 The 't Hooft{Polyakov Monopole . 18 1.2.1 The bosonic part of the Georgi{Glashow model . 18 1.2.2 Finite-energy solutions: the 't Hooft{Polyakov Ansatz . 20 1.2.3 The topological origin of the magnetic charge . 24 1.3 BPS-monopoles .......................... 26 1.3.1 Estimating the mass of a monopole: the Bogomol'nyi bound ........................... 27 1.3.2 Saturating the bound: the BPS-monopole . 28 1.4 Duality conjectures ........................ 30 1.4.1 The Montonen{Olive conjecture . 30 1.4.2 The Witten e®ect ..................... 31 1.4.3 SL(2; Z) duality ...................... 33 2 Supersymmetry 39 2.1 The super-Poincar¶ealgebra in four dimensions . 40 2.1.1 Some notational remarks about spinors . 40 2.1.2 The Coleman{Mandula and Haag{ÃLopusza¶nski{Sohnius theorems .......................... 42 2.2 Unitary representations of the supersymmetry algebra . 44 2.2.1 Wigner's method and the little group . 44 2.2.2 Massless representations . 45 2.2.3 Massive representations . 47 No central charges .................... 48 Adding central charges . 49 1 [email protected] draft version of 8/10/1998 2.3 N=2 Supersymmetric Yang-Mills .