BPS State Counting Using Wall-Crossing, Holomorphic Anomalies and Modularity

Total Page:16

File Type:pdf, Size:1020Kb

BPS State Counting Using Wall-Crossing, Holomorphic Anomalies and Modularity BPS state counting using wall-crossing, holomorphic anomalies and modularity Dissertation zur Erlangung des Doktorgrades (Dr. rer. nat.) der Mathematisch-Naturwissenschaftlichen Fakultät der Rheinischen Friedrich-Wilhelms-Universität Bonn von Thomas Wotschke aus Iserlohn Bonn 2013 Dieser Forschungsbericht wurde als Dissertation von der Mathematisch-Naturwissenschaftlichen Fakultät der Universität Bonn angenommen und ist auf dem Hochschulschriftenserver der ULB Bonn http://hss.ulb.uni-bonn.de/diss_online elektronisch publiziert. 1. Gutachter: Prof. Dr. Albrecht Klemm 2. Gutachter: Prof. Dr. Hans-Peter Nilles Tag der Promotion: 11.07.2013 Erscheinungsjahr: 2013 Abstract In this thesis we examine the counting of BPS states using wall-crossing, holomorphic anomalies and modularity. We count BPS states that arise in two setups: multiple M5-branes wrapping P × T 2, where P denotes a divisor inside a Calabi-Yau threefold and topological string theory on elliptic Calabi-Yau threefolds. The first setup has a dual description as type IIA string theory via a D4-D2-D0 brane system. Furthermore it leads to two descriptions depending on the size of P and T 2 relative to each other. For the case of a small divisor P this setup is described by the (0; 4) Maldacena-Strominger-Witten conformal field theory of a black hole in M-theory and for the case of small T 2 the setup can by described by N = 4 topological Yang-Mills theory on P. The BPS states are counted by the modified elliptic genus, which can be decomposed into a vector-valued modular form that provides the generating function for the BPS invariants and a Siegel-Narain theta function. In the first part we discuss the holomorphic anomaly of + the modified elliptic genus for the case of two M5-branes and divisors with b2 (P) = 1. Due to the wall-crossing effect the change in the generating function is captured by an indefinite theta function, which is a mock modular form. We use the Kontsevich-Soibelman wall-crossing formula to determine the jumps in the modified elliptic genus. Using the regularisation procedure for mock modular forms of Zwegers, modularity can be restored at the cost of holomorphicity. We show that the non-holomorphic completion is due to bound states of single M5-branes. At the attractor point in the moduli space we prove the holomorphic anomaly equation, which is compatible with the holomorphic anomaly equations observed in the context of N = 4 Yang-Mills theory on P2 and E-strings on a del Pezzo surface. We 2 calculate the generating functions of BPS invariants for the divisors P ; F0; F1 and the del Pezzo surface 1 dP8 and dP9 2 K3 . In the second part we study the quantum geometry of elliptic Calabi-Yau threefolds and examine topological string theory on these spaces. We find a holomorphic anomaly equation for the topological amplitudes with respect to the base that is recursive in the genus and in the base class. The topological amplitudes with respect to the base can be expressed in terms of quasi-modular forms, which resembles the holomorphic anomaly. In particular this generalises a holomorphic anomaly discovered for the 1 2 K3. For genus zero and base F1 we prove the holomorphic anomaly by using mirror symmetry and we motivate our holomorphic anomaly equation by establishing the connection to the holomorphic anomaly equations of Bershadsky-Cecotti-Ooguri-Vafa. Using T-duality allows us to relate this anomaly to the anomaly for the case of D4-D2-D0 BPS state counting. We calculate the generating function of BPS 1 invariants of 2 K3 for higher rank branes in topological string theory and by using algebraic-geometric techniques that were developed in the context of stability of sheaves. iii Danksagungen Walk on walk on with hope in your heart And you’ll never walk alone Zunächst möchte ich meinem Doktorvater Prof. Dr. Albrecht Klemm danken, dass er mir die Möglich- keit gegeben hat in seiner Arbeitsgruppe und dem spannenden Feld der Stringtheorie zu arbeiten. Die Möglichkeit mathematische Erkenntnisse für physikalische Ergebnisse und umgekehrt zu verwenden, haben mich seit meinem Studium fasziniert und insbesondere mein Doktorvater hat meine Faszination in zahlreichen inspirierende Diskussionen und durch seine permanente Unterstützung über die Jahre meiner Doktorarbeit weiter vertieft. Neben den stets guten Möglichkeiten in Bonn, ist auch seine Unter- stützung bei der Teilnahme an verschiedenen Schulen und Konferenzen zu nennen. Prof. Dr. Hans-Peter Nilles danke ich für die Übernahme der Zweitkorrektur. Ohne die zahlreichen Diskussionen mit meinen Kooperationspartnern wäre diese Arbeit nicht mög- lich gewesen. Ich danke Ihnen, dass sie ihre Einsichten mit mir geteilt haben und immer wieder neue Anregungen und Herausforderungen geliefert haben. Somit haben sie wesentlich zu der produktiven At- mosphäre während meiner Doktorarbeit beigetragen. Ich danke Dr. Murad Alim, Dr. Babak Haghighat, Dr. Michael Hecht, Dr. Jan Manschot und Dr. Marco Rauch. Dr. Murad Alim und Dr. Michael Hecht sei besonders für zahlreiche hilfreiche Diskussionen und Aufenthalte in München gedankt. Dr. Marco Rauch danke ich für eine herausragende gemeinsame Zeit während des Studiums, im gemeinsamen Büro während der Promotion und darüber hinaus. Mein Dank gilt ebenfalls den aktuellen und ehemaligen Mitgliedern der Arbeitsgruppe von Prof. Klemm, die stets für Fragen und Anregungen bereit waren. Während meiner Zeit im Büro 104 und im BCTP konnte ich stets auf ein produktives und konstruktives Arbeitsumfeld bauen. Ich danke Dr. Thomas Grimm, Dr. Tae-Won Ha, Dr. Hans Jockers, Dr. Denis Klevers, Dr. Daniel Lopes, Dr. Ma- soud Soroush, Dr. Piotr Sulkowski, Navaneeth Gaddam, Jie Gu, Maximilian Poretschkin, Jonas Reuter und Marc Schiereck. Insbesondere danke ich Maximilian Poretschkin für die gemeinsame Zeit im Büro 2.010 im BCTP, viele anregende Diskussionen und sein stets kollegiales, verlässliches und freundschaft- liches Verhalten. Weiterhin gebührt ihm Dank für das Korrekturlesen meiner Arbeit und viele hilfreiche, konstruktive Vorschläge. Ebenfalls Dr. Maxim Mai sei für seine hilfreichen Anregungen gedankt. Ich danke der Deutsche Telekom Stiftung für die Förderung während meiner Doktorarbeit. Die Stipendiatentreffen, Seminare und weitere Veranstaltungen haben meine Doktorarbeit zu einer einzig- artigen Zeit werden lassen. Ich danke Frau Christiane Frense-Heck für die Betreuung und Prof. Dr. Johann-Dietrich Wörner für seine engagierte Tätigkeit als Mentor. Ebenso danke ich der Bonn-Cologne Graduate School of Physics and Astronomy für die Förderung meiner Doktorarbeit. Meine Zeit während der Promotion wurde auch von vielen Freunden außerhalb der Forschung ge- prägt. Ich danke Dr. Maxim Mai und Konstantin Ottnad für viele Kaffeepausen und die gemeinsame Zeit seit dem Studium. Ich danke Patrick Bavink für viele gute Ratschläge und die gemeinsam erlebten Momente an der Platte und außerhalb. Weiterhin danke ich Christian Burgdorf für zahlreiche Plakate und gemeinsam geleitete Kurse. Meinen Eltern Magdalene und Dieter Wotschke sowie meiner Freundin Christina Cappenberg danke ich vom ganzen Herzen für ihre Unterstützung und Liebe – danke für alles. iv Contents 1 Introduction and Motivation 1 2 Counting BPS states in string theory 13 2.1 BPS states and the supersymmetry algebra . 14 2.2 BPS states and gauge theories . 16 2.3 BPS states and black holes . 19 2.4 Stability of BPS states . 22 2.4.1 Walls of marginal stability and BPS indices . 23 2.4.2 The Kontsevich-Soibelmann wall-crossing formula . 24 2.4.3 Stability conditions . 26 2.4.4 Verification of the Kontsevich-Soibelman wall-crossing formula from physics . 29 2.5 An example: SU(2) Seiberg-Witten theory . 31 2.5.1 The setup and the solution . 31 2.5.2 Quiver description of SU(2) Seiberg-Witten theory . 34 2.6 Modular forms . 35 2.6.1 Elliptic and Siegel modular forms . 35 2.6.2 Mock modularity . 47 2.7 Topological string theory . 57 2.7.1 The chiral ring structure of topological string theory . 57 2.7.2 Deformations . 59 2.7.3 Non-linear sigma model realisation . 59 2.7.4 Topological field theories . 60 2.7.5 Mirror symmetry . 62 2.7.6 Holomorphic anomaly equations . 66 2.7.7 Stable pairs and enumerative invariants . 69 2.8 Counting D4-D2-D0 BPS states . 70 2.8.1 The Maldacena-Strominger-Witten conformal field theory . 71 2.8.2 Counting BPS states a la Gaiotto-Strominger-Yin and using split attractor flows 77 2.8.3 N = 4 Super Yang-Mills, E-strings and bound-states . 79 2.8.4 Counting BPS states via wall-crossing and sheaves . 82 3 Geometries and their construction 85 3.1 Calabi-Yau manifolds as hypersurfaces and complete intersections in weighted project- ive space . 85 3.2 Complex surfaces . 90 v Contents 3.3 Classical geometry of elliptically fibred Calabi-Yau spaces . 90 3.3.1 The classical geometrical data of elliptic fibrations . 92 3.3.2 Realisations in toric ambient spaces . 94 4 Wall-crossing holomorphic anomaly and mock modularity of multiple M5-branes 99 4.1 Generating functions from wall-crossing . 99 4.2 Wall-crossing and mock modularity . 100 4.2.1 D4-D2-D0 wall-crossing . 101 4.2.2 Relation of Kontsevich-Soibelman to Göttsche’s wall-crossing formula . 102 4.2.3 Holomorphic anomaly at rank two . 104 4.3 Applications and extensions . 106 4.3.1 Blow-up formulae and vanishing chambers . 106 + 4.3.2 Applications to surfaces with b2 = 1....................... 107 4.3.3 Extensions to higher rank and speculations . 110 5 Quantum geometry of elliptic fibrations 113 5.1 Quantum cohomology, modularity and the anomaly equations . 113 5.2 The B-model approach to elliptically fibred Calabi-Yau spaces . 116 5.3 Modular subgroup of monodromy group . 118 5.4 Derivation of the holomorphic anomaly equation . 122 5.4.1 The elliptic fibration over F1 ........................... 122 5.4.2 Derivation from BCOV .
Recommended publications
  • Relative Mirror Symmetry and Ramifications of a Formula for Gromov-Witten Invariants
    Relative Mirror Symmetry and Ramifications of a Formula for Gromov-Witten Invariants Thesis by Michel van Garrel In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 2013 (Defended May 21, 2013) ii c 2013 Michel van Garrel All Rights Reserved iii To my parents Curt and Danielle, the source of all virtues that I possess. To my brothers Cl´ement and Philippe, my best and most fun friends. iv Acknowledgements My greatest thanks go to my advisor Professor Tom Graber, whose insights into the workings of algebraic geometry keep astonishing me and whose ideas were of enormous benefit to me during the pursuit of my Ph.D. My special thanks are given to Professor Yongbin Ruan, who initiated the project on relative mirror symmetry and to whom I am grateful many enjoyable discussions. I am grateful that I am able to count on the continuing support of Professor Eva Bayer and Professor James Lewis. Over the past few years I learned a lot from Daniel Pomerleano, who, among others, introduced me to homological mirror symmetry. Mathieu Florence has been a figure of inspiration and motivation ever since he casually introduced me to algebraic geometry. Finally, my thanks go to the innumerable enjoyable math conversations with Roland Abuaf, Dori Bejleri, Adam Ericksen, Anton Geraschenko, Daniel Halpern-Leistner, Hadi Hedayatzadeh, Cl´ement Hongler, Brian Hwang, Khoa Nguyen, Rom Rains, Mark Shoemaker, Zhiyu Tian, Nahid Walji, Tony Wong and Gjergji Zaimi. v Abstract For a toric Del Pezzo surface S, a new instance of mirror symmetry, said relative, is introduced and developed.
    [Show full text]
  • Stringy T3-Fibrations, T-Folds and Mirror Symmetry
    Stringy T 3-fibrations, T-folds and Mirror Symmetry Ismail Achmed-Zade Arnold-Sommerfeld-Center Work to appear with D. L¨ust,S. Massai, M.J.D. Hamilton March 13th, 2017 Ismail Achmed-Zade (ASC) Stringy T 3-fibrations and applications March 13th, 2017 1 / 24 Overview 1 String compactifications and dualities T-duality Mirror Symmetry 2 T-folds The case T 2 The case T 3 3 Stringy T 3-bundles The useful T 4 4 Conclusion Recap Open Problems Ismail Achmed-Zade (ASC) Stringy T 3-fibrations and applications March 13th, 2017 2 / 24 Introduction Target space Super string theory lives on a 10-dimensional pseudo-Riemannian manifold, e.g. 4 6 M = R × T with metric η G = µν GT 6 In general we have M = Σµν × X , with Σµν a solution to Einsteins equation. M is a solution to the supergravity equations of motion. Non-geometric backgrounds X need not be a manifold. Exotic backgrounds can lead to non-commutative and non-associative gravity. Ismail Achmed-Zade (ASC) Stringy T 3-fibrations and applications March 13th, 2017 3 / 24 T-duality Example Somtimes different backgrounds yield the same physics IIA IIB 9 1 2 2 ! 9 1 1 2 R × S ; R dt R × S ; R2 dt More generally T-duality for torus compactifications is an O(D; D; Z)-transformation (T D ; G; B; Φ) ! (T^D ; G^; B^; Φ)^ Ismail Achmed-Zade (ASC) Stringy T 3-fibrations and applications March 13th, 2017 4 / 24 Mirror Symmetry Hodge diamond of three-fold X and its mirror X^ 1 1 0 0 0 0 0 h1;1 0 0 h1;2 0 1 h1;2 h1;2 1 ! 1 h1;1 h1;1 1 0 h1;1 0 0 h1;2 0 0 0 0 0 1 1 Mirror Symmetry This operation induces the following symmetry IIA IIB ! X ; g X^; g^ Ismail Achmed-Zade (ASC) Stringy T 3-fibrations and applications March 13th, 2017 5 / 24 Mirror Symmetry is T-duality!? SYZ-conjecture [Strominger, Yau, Zaslow, '96] Consider singular bundles T 3 −! X T^3 −! X^ ! ? ? S3 S3 Apply T-duality along the smooth fibers.
    [Show full text]
  • Heterotic String Compactification with a View Towards Cosmology
    Heterotic String Compactification with a View Towards Cosmology by Jørgen Olsen Lye Thesis for the degree Master of Science (Master i fysikk) Department of Physics Faculty of Mathematics and Natural Sciences University of Oslo May 2014 Abstract The goal is to look at what constraints there are for the internal manifold in phe- nomenologically viable Heterotic string compactification. Basic string theory, cosmology, and string compactification is sketched. I go through the require- ments imposed on the internal manifold in Heterotic string compactification when assuming vanishing 3-form flux, no warping, and maximally symmetric 4-dimensional spacetime with unbroken N = 1 supersymmetry. I review the current state of affairs in Heterotic moduli stabilisation and discuss merging cosmology and particle physics in this setup. In particular I ask what additional requirements this leads to for the internal manifold. I conclude that realistic manifolds on which to compactify in this setup are severely constrained. An extensive mathematics appendix is provided in an attempt to make the thesis more self-contained. Acknowledgements I would like to start by thanking my supervier Øyvind Grøn for condoning my hubris and for giving me free rein to delve into string theory as I saw fit. It has lead to a period of intense study and immense pleasure. Next up is my brother Kjetil, who has always been a good friend and who has been constantly looking out for me. It is a source of comfort knowing that I can always turn to him for help. Mentioning friends in such an acknowledgement is nearly mandatory. At least they try to give me that impression.
    [Show full text]
  • A Survey of Calabi-Yau Manifolds
    Surveys in Differential Geometry XIII A survey of Calabi-Yau manifolds Shing-Tung Yau Contents 1. Introduction 278 2. General constructions of complete Ricci-flat metrics in K¨ahler geometry 278 2.1. The Ricci tensor of Calabi-Yau manifolds 278 2.2. The Calabi conjecture 279 2.3. Yau’s theorem 279 2.4. Calabi-Yau manifolds and Calabi-Yau metrics 280 2.5. Examples of compact Calabi-Yau manifolds 281 2.6. Noncompact Calabi-Yau manifolds 282 2.7. Calabi-Yau cones: Sasaki-Einstein manifolds 283 2.8. The balanced condition on Calabi-Yau metrics 284 3. Moduli and arithmetic of Calabi-Yau manifolds 285 3.1. Moduli of K3 surfaces 285 3.2. Moduli of high dimensional Calabi-Yau manifolds 286 3.3. The modularity of Calabi–Yau threefolds over Q 287 4. Calabi-Yau manifolds in physics 288 4.1. Calabi-Yau manifolds in string theory 288 4.2. Calabi-Yau manifolds and mirror symmetry 289 4.3. Mathematics inspired by mirror symmetry 291 5. Invariants of Calabi-Yau manifolds 291 5.1. Gromov-Witten invariants 291 5.2. Counting formulas 292 5.3. Proofs of counting formulas for Calabi-Yau threefolds 293 5.4. Integrability of mirror map and arithmetic applications 293 5.5. Donaldson-Thomas invariants 294 5.6. Stable bundles and sheaves 296 5.7. Yau-Zaslow formula for K3 surfaces 296 5.8. Chern-Simons knot invariants, open strings and string dualities 297 c 2009 International Press 277 278 S.-T. YAU 6. Homological mirror symmetry 299 7. SYZ geometric interpretation of mirror symmetry 300 7.1.
    [Show full text]
  • Perspectives on Geometric Analysis
    Surveys in Differential Geometry X Perspectives on geometric analysis Shing-Tung Yau This essay grew from a talk I gave on the occasion of the seventieth anniversary of the Chinese Mathematical Society. I dedicate the lecture to the memory of my teacher S.S. Chern who had passed away half a year before (December 2004). During my graduate studies, I was rather free in picking research topics. I[731] worked on fundamental groups of manifolds with non-positive curva- ture. But in the second year of my studies, I started to look into differential equations on manifolds. However, at that time, Chern was very much inter- ested in the work of Bott on holomorphic vector fields. Also he told me that I should work on Riemann hypothesis. (Weil had told him that it was time for the hypothesis to be settled.) While Chern did not express his opinions about my research on geometric analysis, he started to appreciate it a few years later. In fact, after Chern gave a course on Calabi’s works on affine geometry in 1972 at Berkeley, S.Y. Cheng told me about these inspiring lec- tures. By 1973, Cheng and I started to work on some problems mentioned in Chern’s lectures. We did not realize that the great geometers Pogorelov, Calabi and Nirenberg were also working on them. We were excited that we solved some of the conjectures of Calabi on improper affine spheres. But soon after we found out that Pogorelov [563] published his results right be- fore us by different arguments. Nevertheless our ideas are useful in handling other problems in affine geometry, and my knowledge about Monge-Amp`ere equations started to broaden in these years.
    [Show full text]
  • Download Enumerative Geometry and String Theory Free Ebook
    ENUMERATIVE GEOMETRY AND STRING THEORY DOWNLOAD FREE BOOK Sheldon Katz | 206 pages | 31 May 2006 | American Mathematical Society | 9780821836873 | English | Providence, United States Enumerative Geometry and String Theory Chapter 2. The most accessible portal into very exciting recent material. Topological field theory, primitive forms and related topics : — Nuclear Physics B. Bibcode : PThPh. Bibcode : hep. As an example, consider the torus described above. Enumerative Geometry and String Theory standard analogy for this is to consider a multidimensional object such as a garden hose. An example is the red circle in the figure. This problem was solved by the nineteenth-century German mathematician Hermann Schubertwho found that there are Enumerative Geometry and String Theory 2, such lines. Once these topics are in place, the connection between physics and enumerative geometry is made with the introduction of topological quantum field theory and quantum cohomology. Enumerative Geometry and String Theory mirror symmetry relationship is a particular example of what physicists call a duality. Print Price 1: The book contains a lot of extra material that was not included Enumerative Geometry and String Theory the original fifteen lectures. Increasing the dimension from two to four real dimensions, the Calabi—Yau becomes a K3 surface. This problem asks for the number and construction of circles that are tangent to three given circles, points or lines. Topological Quantum Field Theory. Online Price 1: Online ISBN There are infinitely many circles like it on a torus; in fact, the entire surface is a union of such circles. For other uses, see Mirror symmetry. As an example, count the conic sections tangent to five given lines in the projective plane.
    [Show full text]
  • Syz Mirror Symmetry for Toric Varieties
    SYZ MIRROR SYMMETRY FOR TORIC VARIETIES KWOKWAI CHAN Abstract. We survey recent developments in the study of SYZ mirror sym- metry for compact toric and toric Calabi-Yau varieties, with a special emphasis on works of the author and his collaborators. Contents 1. The SYZ proposal 1 1.1. Semi-flat SYZ: a toy example 2 2. A quick review on toric varieties 5 3. Mirror symmetry for compact toric varieties 6 3.1. Landau-Ginzburg models as mirrors 6 3.2. The SYZ construction 7 3.3. Open mirror theorems 11 4. Mirror symmetry for toric Calabi-Yau varieties 15 4.1. Physicists' mirrors 15 4.2. The SYZ construction 17 4.3. Period integrals and disk counting { a conjecture of Gross-Siebert 21 Acknowledgment 23 References 23 1. The SYZ proposal In 1996, drawing on the new idea of D-branes from string theory, Strominger, Yau and Zaslow [76] made a ground-breaking proposal to explain mirror symmetry geometrically as a Fourier{type transform, known as T-duality. Conjecture 1.1 (The SYZ conjecture [76]). If X and Xˇ are Calabi-Yau manifolds mirror to each other, then (i) both X and Xˇ admit special Lagrangian torus fibrations with sections ρ : X ! B and ρˇ : Xˇ ! B over the same base which are fiberwise dual to each other in the sense that regular fibers ρ−1(b) ⊂ X and ρˇ−1(b) ⊂ Xˇ over the same point b 2 B are dual tori, and (ii) there exist Fourier{type transforms which exchange symplectic-geometric (resp. complex-geometric) data on X with complex-geometric (resp.
    [Show full text]
  • Annual Report 2010 Report Annual IPMU ANNUAL REPORT 2010 April 2010 April – March 2011March
    IPMU April 2010–March 2011 Annual Report 2010 IPMU ANNUAL REPORT 2010 April 2010 – March 2011 World Premier International Institute for the Physics and Mathematics of the Universe (IPMU) Research Center Initiative Todai Institutes for Advanced Study Todai Institutes for Advanced Study The University of Tokyo 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8583, Japan TEL: +81-4-7136-4940 FAX: +81-4-7136-4941 http://www.ipmu.jp/ History (April 2010–March 2011) April • Workshop “Recent advances in mathematics at IPMU II” • Press Release “Shape of dark matter distribution” • Mini-Workshop “Cosmic Dust” May • Shaw Prize to David Spergel • Press Release “Discovery of the most distant cluster of galaxies” • Press Release “An unusual supernova may be a missing link in stellar evolution” June • CL J2010: From Massive Galaxy Formation to Dark Energy • Press Conference “Study of type Ia supernovae strengthens the case for the dark energy” July • Institut d’Astrophysique de Paris Medal (France) to Ken’ichi Nomoto • IPMU Day of Extra-galactic Astrophysics Seminars: Chemical Evolution August • Workshop “Galaxy and cosmology with Thirty Meter Telescope (TMT)” September • Subaru Future Instrumentation Workshop • Horiba International Conference COSMO/CosPA October • The 3rd Anniversary of IPMU, All Hands Meeting and Reception • Focus Week “String Cosmology” • Nishinomiya-Yukawa Memorial Prize to Eiichiro Komatsu • Workshop “Evolution of massive galaxies and their AGNs with the SDSS-III/BOSS survey” • Open Campus Day: Public lecture, mini-lecture and exhibits November
    [Show full text]
  • Black Hole Entropy, Marginal Stability and Mirror Symmetry
    hep-th/0610044 DUKE-CGTP-06-01 SLAC-PUB-12048 October 2006 Black Hole Entropy, Marginal Stability and Mirror Symmetry Paul S. Aspinwall1, Alexander Maloney2 and Aaron Simons3 1 Center for Geometry and Theoretical Physics, Box 90318 Duke University, Durham, NC 27708-0318 2 School of Natural Sciences, Institute for Advanced Study Einstein Dr., Princeton, NJ 08540 3 Department of Physics, Harvard University, Cambridge, MA 02138 Abstract We consider the superconformal quantum mechanics associated to BPS black holes in type IIB Calabi–Yau compactifications. This quantum mechanics describes the dynamics of D- branes in the near-horizon attractor geometry of the black hole. In many cases, the black hole entropy can be found by counting the number of chiral primaries in this quantum mechanics. Both the attractor mechanism and notions of marginal stability play important roles in generating the large number of microstates required to explain this entropy. We compute the microscopic entropy explicitly in a few different cases, where the theory reduces to quantum mechanics on the moduli space of special Lagrangians. Under certain assumptions, the problem may be solved by implementing mirror symmetry as three T-dualities: this is essentially the mirror of a calculation by Gaiotto, Strominger and Yin. In some simple cases, the calculation may be done in greater generality without resorting to conjectures about mirror symmetry. For example, the K3 T 2 case may be studied precisely using the Fourier-Mukai transform. × email: [email protected], [email protected], [email protected] Submitted to Journal of High Energy Physics (JHEP) Work supported in part by Department of Energy contract DE-AC02-76SF00515 SLAC, Stanford Univesity, Stanford, CA 94309 1 Introduction The study of quantum mechanical black holes continues to provide new insights into the basic structure of string theory and quantum gravity.
    [Show full text]
  • JHEP05(2021)013 Springer -Structure May 3, 2021 : March 29, 2021 : -Structure Met- SU(3)
    Published for SISSA by Springer Received: December 21, 2020 Accepted: March 29, 2021 Published: May 3, 2021 Moduli-dependent Calabi-Yau and SU(3)-structure metrics from machine learning JHEP05(2021)013 Lara B. Anderson,a Mathis Gerdes,b James Gray,a Sven Krippendorf,b Nikhil Raghurama and Fabian Ruehlec,d aDepartment of Physics, Robeson Hall, Virginia Tech, Blacksburg, VA 24061, U.S.A. bArnold Sommerfeld Center for Theoretical Physics, Ludwig-Maximilians-Universität, Theresienstr. 37, 80333 Munich, Germany cCERN, Theoretical Physics Department 1, Esplanade des Particules, Geneva 23, CH-1211, Switzerland dRudolf Peierls Centre for Theoretical Physics, University of Oxford, Parks Road, Oxford OX1 3PU, U.K. E-mail: [email protected], [email protected], [email protected], [email protected], [email protected], [email protected] Abstract: We use machine learning to approximate Calabi-Yau and SU(3)-structure met- rics, including for the first time complex structure moduli dependence. Our new methods furthermore improve existing numerical approximations in terms of accuracy and speed. Knowing these metrics has numerous applications, ranging from computations of crucial aspects of the effective field theory of string compactifications such as the canonical nor- malizations for Yukawa couplings, and the massive string spectrum which plays a crucial role in swampland conjectures, to mirror symmetry and the SYZ conjecture. In the case of SU(3) structure, our machine learning approach allows us to engineer metrics with certain torsion properties. Our methods are demonstrated for Calabi-Yau and SU(3)-structure manifolds based on a one-parameter family of quintic hypersurfaces in P4.
    [Show full text]
  • Syz Mirror Symmetry from Witten-Morse Theory
    SYZ MIRROR SYMMETRY FROM WITTEN-MORSE THEORY ZIMING NIKOLAS MA 1. Introduction The celebrated Strominger-Yau-Zaslow (SYZ) conjecture [42] asserts that mirror symmetry is a T-duality, namely, a mirror pair of Calabi-Yau manifolds should admit fibre-wise dual (special) Lagrangian torus fibrations to the same base. This suggests the following construc- tion of a mirror (as a complex manifold): Given a Calabi-Yau manifold X (regarded as a symplectic manifold) equipped with a Lagrangian torus fibration s { (X; !; J) p /B that admits a Lagrangian section s. The base B is then an integral affine manifold with sing singularities, meaning that the smooth locus B0 ⊂ B (whose complement B := B n B0, i.e. the singular locus, is of real codimension at least 1) carries an integral affine structure. sing Restricting p to the smooth locus B0 = B nB , we obtain a semi-flat symplectic Calabi-Yau manifold X0 ,! X which, by Duistermaat's action-angle coordinates [16], can be identified as ∼ ∗ ∗ X0 = T B0=Λ ; ∗ ∗ where Λ ⊂ T B0 is the natural lattice (dual to Λ) locally generated by affine coordinate 1-forms. We can construct a pair of torus bundles over the same base which are fibre-wise dual ˇ X0 X0 p pˇ ~ B0 ; ˇ ∼ ˇ where X0 = TB0=Λ can be equipped with a natural complex structure J0 called the semi- flat complex structure. This, however, does not produce the correct mirror in general.1 The ˇ sing problem is that J0 cannot be extended across the singular points B , so this does not give a complex manifold which fibres over B.
    [Show full text]
  • Mirror Symmetry: Lecture 1
    MIRROR SYMMETRY: LECTURE 1 DENIS AUROUX NOTES BY KARTIK VENKATRAM Goal of the class: this is not always going to be the most rigorous class, but the goal is to tell the story of mirror symmetry. 1. Physical Origins Mirror symmetry comes from statements in supersymmetric string theory. Ba- sic idea of string theory: replace particles with vibrating strings, which propogate through space and form surfaces. We thus get 2-d quantum field theories on these surfaces, called worldsheets, with the fields taking values in some manifolds. Su- persymmetric means that there are lots of symmetries acting here, and physicists have lots of buzzwords here that won't make sense to mathematicians. For in- stance \superconformal field theory" means that the theory depends only on the conformal structure on Σ rather than the Riemannian structure. There are vari- ous flavors of these theories, but the ones more relevant to mirror symmetry are the nonlinear sigma-models 1.1. Non-linear Sigma Models. Here, we look at maps φ :Σ ! X, where X (the \target space") is a Calabi-Yau manifold. Definition 1. A Calabi-Yau manifold is a complex manifold (X; J) (ideally, Vn ∗ ∼ compact, 3-dimensional, maybe b1 = 0) s.t. KX = T X = OX , so 9 a section 0 Ω 2 H (X; KX ), i.e. a holomorphic volume form. On this manifold, we have a complexified K¨ahlerform !C = B + i! which is a closed (1; 1)-form and Im !C = ! is nondegenerate (B is supposed to make the space of symplectic forms a subspace of complex cohomology).
    [Show full text]