Calabi-Yau Compactification of Type II String Theories Sibasish Banerjee
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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. -
Lectures on D-Branes
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server CPHT/CL-615-0698 hep-th/9806199 Lectures on D-branes Constantin P. Bachas1 Centre de Physique Th´eorique, Ecole Polytechnique 91128 Palaiseau, FRANCE [email protected] ABSTRACT This is an introduction to the physics of D-branes. Topics cov- ered include Polchinski’s original calculation, a critical assessment of some duality checks, D-brane scattering, and effective worldvol- ume actions. Based on lectures given in 1997 at the Isaac Newton Institute, Cambridge, at the Trieste Spring School on String The- ory, and at the 31rst International Symposium Ahrenshoop in Buckow. June 1998 1Address after Sept. 1: Laboratoire de Physique Th´eorique, Ecole Normale Sup´erieure, 24 rue Lhomond, 75231 Paris, FRANCE, email : [email protected] Lectures on D-branes Constantin Bachas 1 Foreword Referring in his ‘Republic’ to stereography – the study of solid forms – Plato was saying : ... for even now, neglected and curtailed as it is, not only by the many but even by professed students, who can suggest no use for it, never- theless in the face of all these obstacles it makes progress on account of its elegance, and it would not be astonishing if it were unravelled. 2 Two and a half millenia later, much of this could have been said for string theory. The subject has progressed over the years by leaps and bounds, despite periods of neglect and (understandable) criticism for lack of direct experimental in- put. To be sure, the construction and key ingredients of the theory – gravity, gauge invariance, chirality – have a firm empirical basis, yet what has often catalyzed progress is the power and elegance of the underlying ideas, which look (at least a posteriori) inevitable. -
String Theory University of Cambridge Part III Mathematical Tripos
Preprint typeset in JHEP style - HYPER VERSION January 2009 String Theory University of Cambridge Part III Mathematical Tripos Dr David Tong Department of Applied Mathematics and Theoretical Physics, Centre for Mathematical Sciences, Wilberforce Road, Cambridge, CB3 OWA, UK http://www.damtp.cam.ac.uk/user/tong/string.html [email protected] –1– Recommended Books and Resources J. Polchinski, String Theory • This two volume work is the standard introduction to the subject. Our lectures will more or less follow the path laid down in volume one covering the bosonic string. The book contains explanations and descriptions of many details that have been deliberately (and, I suspect, at times inadvertently) swept under a very large rug in these lectures. Volume two covers the superstring. M. Green, J. Schwarz and E. Witten, Superstring Theory • Another two volume set. It is now over 20 years old and takes a slightly old-fashioned route through the subject, with no explicit mention of conformal field theory. How- ever, it does contain much good material and the explanations are uniformly excellent. Volume one is most relevant for these lectures. B. Zwiebach, A First Course in String Theory • This book grew out of a course given to undergraduates who had no previous exposure to general relativity or quantum field theory. It has wonderful pedagogical discussions of the basics of lightcone quantization. More surprisingly, it also has some very clear descriptions of several advanced topics, even though it misses out all the bits in between. P. Di Francesco, P. Mathieu and D. S´en´echal, Conformal Field Theory • This big yellow book is a↵ectionately known as the yellow pages. -
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. -
Introduction to String Theory
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Introduction to String Theory Thomas Mohaupt Friedrich-Schiller Universit¨at Jena, Max-Wien-Platz 1, D-07743 Jena, Germany Abstract. We give a pedagogical introduction to string theory, D-branes and p-brane solutions. 1 Introductory remarks These notes are based on lectures given at the 271-th WE-Haereus-Seminar ‘Aspects of Quantum Gravity’. Their aim is to give an introduction to string theory for students and interested researches. No previous knowledge of string theory is assumed. The focus is on gravitational aspects and we explain in some detail how gravity is described in string theory in terms of the graviton excitation of the string and through background gravitational fields. We include Dirichlet boundary conditions and D-branes from the beginning and devote one section to p-brane solutions and their relation to D-branes. In the final section we briefly indicate how string theory fits into the larger picture of M-theory and mention some of the more recent developments, like brane world scenarios. The WE-Haereus-Seminar ‘Aspects of Quantum Gravity’ covered both main approaches to quantum gravity: string theory and canonical quantum gravity. Both are complementary in many respects. While the canonical approach stresses background independence and provides a non-perturbative framework, the cor- nerstone of string theory still is perturbation theory in a fixed background ge- ometry. Another difference is that in the canonical approach gravity and other interactions are independent from each other, while string theory automatically is a unified theory of gravity, other interactions and matter. -
Classical String Theory
PROSEMINAR IN THEORETICAL PHYSICS Classical String Theory ETH ZÜRICH APRIL 28, 2013 written by: DAVID REUTTER Tutor: DR.KEWANG JIN Abstract The following report is based on my talk about classical string theory given at April 15, 2013 in the course of the proseminar ’conformal field theory and string theory’. In this report a short historical and theoretical introduction to string theory is given. This is fol- lowed by a discussion of the point particle action, leading to the postulation of the Nambu-Goto and Polyakov action for the classical bosonic string. The equations of motion from these actions are derived, simplified and generally solved. Subsequently the Virasoro modes appearing in the solution are discussed and their algebra under the Poisson bracket is examined. 1 Contents 1 Introduction 3 2 The Relativistic String4 2.1 The Action of a Classical Point Particle..........................4 2.2 The General p-Brane Action................................6 2.3 The Nambu Goto Action..................................7 2.4 The Polyakov Action....................................9 2.5 Symmetries of the Action.................................. 11 3 Wave Equation and Solutions 13 3.1 Conformal Gauge...................................... 13 3.2 Equations of Motion and Boundary Terms......................... 14 3.3 Light Cone Coordinates................................... 15 3.4 General Solution and Oscillator Expansion......................... 16 3.5 The Virasoro Constraints.................................. 19 3.6 The Witt Algebra in Classical String Theory........................ 22 2 1 Introduction In 1969 the physicists Yoichiro Nambu, Holger Bech Nielsen and Leonard Susskind proposed a model for the strong interaction between quarks, in which the quarks were connected by one-dimensional strings holding them together. However, this model - known as string theory - did not really succeded in de- scribing the interaction. -
Arxiv:Hep-Th/0110227V1 24 Oct 2001 Elivrac Fpbae.Orcnieain a Eextended Be Can Considerations Branes
REMARKS ON WEYL INVARIANT P-BRANES AND Dp-BRANES J. A. Nieto∗ Facultad de Ciencias F´ısico-Matem´aticas de la Universidad Aut´onoma de Sinaloa, C.P. 80010, Culiac´an Sinaloa, M´exico Abstract A mechanism to find different Weyl invariant p-branes and Dp-branes actions is ex- plained. Our procedure clarifies the Weyl invariance for such systems. Besides, by consid- ering gravity-dilaton effective action in higher dimensions we also derive a Weyl invariant action for p-branes. We argue that this derivation provides a geometrical scenario for the arXiv:hep-th/0110227v1 24 Oct 2001 Weyl invariance of p-branes. Our considerations can be extended to the case of super-p- branes. Pacs numbers: 11.10.Kk, 04.50.+h, 12.60.-i October/2001 ∗[email protected] 1 1.- INTRODUCTION It is known that, in string theory, the Weyl invariance of the Polyakov action plays a central role [1]. In fact, in string theory subjects such as moduli space, Teichmuler space and critical dimensions, among many others, are consequences of the local diff x Weyl symmetry in the partition function associated to the Polyakov action. In the early eighties there was a general believe that the Weyl invariance was the key symmetry to distinguish string theory from other p-branes. However, in 1986 it was noticed that such an invariance may be also implemented to any p-brane and in particular to the 3-brane [2]. The formal relation between the Weyl invariance and p-branes was established two years later independently by a number of authors [3]. -
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 -
Arxiv:Hep-Th/9508143V5 10 Jun 1997 1 Okspotdi Atb H ..Dp.O Nryudrgrant Under Energy of Dept
CALT-68-2013 hep-th/9508143 An SL(2,Z) Multiplet of Type IIB Superstrings1 John H. Schwarz California Institute of Technology, Pasadena, CA 91125, USA Abstract An SL(2, Z) family of string solutions of type IIB supergravity in ten dimensions is constructed. The solutions are labeled by a pair of relatively prime integers, which characterize charges of the three-form field strengths. The string tensions depend on these charges in an SL(2, Z) covariant way. Compactifying on a circle and identifying with eleven-dimensional supergravity compactified on a torus implies that the modulus of the IIB theory should be equated to the modular arXiv:hep-th/9508143v5 10 Jun 1997 parameter of the torus. 1Work supported in part by the U.S. Dept. of Energy under Grant No. DE-FG03-92-ER40701. Among the various conjectured duality symmetries of superstring theories, the proposed SL(2, Z) symmetry of the type IIB superstring theory in ten dimensions is especially inter- esting [1, 2]. Like the SL(2, Z) S duality of the N =4 D = 4 heterotic string [3, 4], it relates weak and strong coupling. However, unlike the heterotic example in which the symmetry relates electrically and magnetically charged states of the same gauge field, the IIB duality relates electrically charged states of two different gauge fields. In this respect it is more like a T duality [5]. Combined with ordinary T dualities, the IIB SL(2, Z) duality implies the complete U duality symmetry of toroidally compactified type II strings in dimensions D< 10 [1, 6]. -
Hagedorn Behavior of Little String Theories1
CORE Metadata, citation and similar papers at core.ac.uk Provided by CERN Document Server NBI-HE-00-35 SPIN-2000/25 ITF-UU-00/27 hep-th/0010169 HAGEDORN BEHAVIOR OF LITTLE STRING THEORIES1 T. Harmark1 and N.A. Obers2;3 1 Niels Bohr Institute, Blegdamsvej 17, DK-2100 Copenhagen, Denmark, 2 Spinoza Institute, Utrecht University, 3584 CE Utrecht, The Netherlands 3 Institute for Theoretical Physics, Utrecht Universty 3508 TA Utrecht, The Netherlands We examine the Hagedorn behavior of little string theory using its conjectured duality with near-horizon NS5-branes. In particular, by studying the string- corrected NS5-brane supergravity solution, it is shown that tree-level corrections to the temperature vanish, while the leading one-loop string correction generates the correct temperature dependence of the entropy near the Hagedorn tempera- ture. Finally, the Hagedorn behavior of ODp-brane theories, which are deformed versions of little string theory, is considered via their supergravity duals. 1TALK PRESENTED BY N.O. AT CONFERENCE "QUANTIZATION, GAUGE THEORY, AND STRINGS", DEDICATED TO THE MEMORY OF PROF. E. FRADKIN, MOSCOW, RUSSIA, JUNE 5-10. 1 Introduction The near-horizon limit of NS5-branes is conjectured to be dual to Little String Theory (LST) with 16 supercharges [1]. LST is a 5+1 dimensional non- gravitational and non-local theory of strings [2] (see also [3]). As for any string theory, the statistical mechanics description of LST breaks down at a certain temperature, known as the Hagedorn temperature [4] (see also e.g. [5]). This raises the question whether it is possible to observe, via the con- jectured near-horizon-NS5/LST duality, Hagedorn behavior of LST from the thermodynamics of near-horizon NS5-branes. -
D-Brane Actions and N = 2 Supergravity Solutions
D-Brane Actions and N =2Supergravity Solutions Thesis by Calin Ciocarlie In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 2004 (Submitted May 20 , 2004) ii c 2004 Calin Ciocarlie All Rights Reserved iii Acknowledgements I would like to express my gratitude to the people who have taught me Physics throughout my education. My thesis advisor John Schwarz has given me insightful guidance and invaluable advice. I benefited a lot by collaborating with outstanding colleagues: Iosif Bena, Iouri Chepelev, Peter Lee, Jongwon Park. I have also bene- fited from interesting discussions with Vadim Borokhov, Jaume Gomis, Prof. Anton Kapustin, Tristan McLoughlin, Yuji Okawa, and Arkadas Ozakin. I am also thankful to my Physics teacher Violeta Grigorie who’s enthusiasm for Physics is contagious and to my family for constant support and encouragement in my academic pursuits. iv Abstract Among the most remarkable recent developments in string theory are the AdS/CFT duality, as proposed by Maldacena, and the emergence of noncommutative geometry. It has been known for some time that for a system of almost coincident D-branes the transverse displacements that represent the collective coordinates of the system become matrix-valued transforming in the adjoint representation of U(N). From a geometrical point of view this is rather surprising but, as we will see in Chapter 2, it is closely related to the noncommutative descriptions of D-branes. A consequence of the collective coordinates becoming matrix-valued is the ap- pearance of a “dielectric” effect in which D-branes can become polarized into higher- dimensional fuzzy D-branes. -
Arxiv:Hep-Th/9611050V2 23 Apr 1997
TASI LECTURES ON D-BRANES JOSEPH POLCHINSKI Institute for Theoretical Physics University of California, Santa Barbara, CA 93106-4030 This is an introduction to the properties of D-branes, topological defects in string theory on which string endpoints can live. D-branes provide a simple description of various nonperturbative objects required by string duality, and give new insight into the quantum mechanics of black holes and the nature of spacetime at the shortest distances. The first two thirds of these lectures closely follow the earlier ITP lectures hep-th/9602052, written with S. Chaudhuri and C. Johnson. The final third includes more extensive applications to string duality. D-branes are extended objects, topological defects in a sense, defined by the property that strings can end on them. One way to see that these objects must be present in string theory is by studying the R 0 limit of open string theory, where the different behaviors of open and clos→ed strings lead to a seeming paradox.1 From the study of this limit one can argue that the usual Type I, Type IIA and Type IIB string theories are different states in a single theory, which also contains states with arbitrary configurations of D-branes. Moreover this argument is purely perturbative, in that it does not require any strong-coupling continuation or use of the BPS property. However, this subject remained obscure until the advent of string duality. It was then observed that D-branes have precisely the correct properties to fill out duality multiplets,2 whose other members are fundamental string states and ordinary field-theoretic solitons.