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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. -
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. -
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. -
Multipermutations 1.1. Generating Functions
CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector JOURNALOF COMBINATORIALTHEORY, Series A 67, 44-71 (1994) The r- Multipermutations SEUNGKYUNG PARK Department of Mathematics, Yonsei University, Seoul 120-749, Korea Communicated by Gian-Carlo Rota Received October 1, 1992 In this paper we study permutations of the multiset {lr, 2r,...,nr}, which generalizes Gesse| and Stanley's work (J. Combin. Theory Ser. A 24 (1978), 24-33) on certain permutations on the multiset {12, 22..... n2}. Various formulas counting the permutations by inversions, descents, left-right minima, and major index are derived. © 1994 AcademicPress, Inc. 1. THE r-MULTIPERMUTATIONS 1.1. Generating Functions A multiset is defined as an ordered pair (S, f) where S is a set and f is a function from S to the set of nonnegative integers. If S = {ml ..... mr}, we write {m f(mD, .... m f(mr)r } for (S, f). Intuitively, a multiset is a set with possibly repeated elements. Let us begin by considering permutations of multisets (S, f), which are words in which each letter belongs to the set S and for each m e S the total number of appearances of m in the word is f(m). Thus 1223231 is a permutation of the multiset {12, 2 3, 32}. In this paper we consider a special set of permutations of the multiset [n](r) = {1 r, ..., nr}, which is defined as follows. DEFINITION 1.1. An r-multipermutation of the set {ml ..... ran} is a permutation al ""am of the multiset {m~ .... -
40 Chapter 6 the BINOMIAL THEOREM in Chapter 1 We Defined
Chapter 6 THE BINOMIAL THEOREM n In Chapter 1 we defined as the coefficient of an-rbr in the expansion of (a + b)n, and r tabulated these coefficients in the arrangement of the Pascal Triangle: n Coefficients of (a + b)n 0 1 1 1 1 2 1 2 1 3 1 3 3 1 4 1 4 6 4 1 5 1 5 10 10 5 1 6 1 6 15 20 15 6 1 ... n n We then observed that this array is bordered with 1's; that is, ' 1 and ' 1 for n = 0 n 0, 1, 2, ... We also noted that each number inside the border of 1's is the sum of the two closest numbers on the previous line. This property may be expressed in the form n n n%1 (1) % ' . r&1 r r This formula provides an efficient method of generating successive lines of the Pascal Triangle, but the method is not the best one if we want only the value of a single binomial coefficient for a 100 large n, such as . We therefore seek a more direct approach. 3 It is clear that the binomial coefficients in a diagonal adjacent to a diagonal of 1's are the 40 n numbers 1, 2, 3, ... ; that is, ' n. Now let us consider the ratios of binomial coefficients 1 to the previous ones on the same row. For n = 4, these ratios are: (2) 4/1, 6/4 = 3/2, 4/6 = 2/3, 1/4. For n = 5, they are (3) 5/1, 10/5 = 2, 10/10 = 1, 5/10 = 1/2, 1/5. -
Q-Combinatorics
q-combinatorics February 7, 2019 1 q-binomial coefficients n n Definition. For natural numbers n; k,the q-binomial coefficient k q (or just k if there no ambi- guity on q) is defined as the following rational function of the variable q: (qn − 1)(qn−1 − 1) ··· (q − 1) : (1.1) (qk − 1)(qk−1 − 1) ··· (q − 1) · (qn−k − 1)(qn−k−1 − 1) ··· (q − 1) For n = 0, k = 0, or n = k, we interpret the corresponding products 1, as the value of the empty product. If we exclude certain roots of unity from the domain of q, (1.1) is equal to (qn − 1)(qn−1 − 1) ··· (qn−k+1 − 1) (1.2) (qk − 1)(qk−1 − 1) ··· (q − 1) · 1 (qn−1 + ::: + q + 1) ··· (q2 + q + 1)(q + 1) · 1 = : (qk−1 + ::: + q + 1) ··· (q2 + q + 1)(q + 1) · 1(qn−k−1 + ::: + q + 1) ··· (q2 + q + 1)(q + 1) · 1 As the notation starts to be overwhelming, we introduce to q-analogue of the positive integer n, n−1 denoted by [n] or [n]q, as q + ::: + q + 1; and the q-analogue of the factorial of the positive integer n, denoted by [n]! or [n]q!, as [n]q! = [1]q · [2]q ··· [n]q. With this additional notation, we also can say n [n] ! = q ; (1.3) k q [k]q![n − k]q! when we avoid certain roots of unity with q. It is easy too see from (1.1) that n n = = 1 0 q n q and that for every 0 ≤ k ≤ n the symmetry rule n n = k q n − k q holds. -
The Binomial Theorem and Combinatorial Proofs Shagnik Das
The Binomial Theorem and Combinatorial Proofs Shagnik Das Introduction As we live our lives, we are faced with innumerable decisions on a daily basis1. Can I get away with wearing these clothes again before I have to wash them? Which frozen pizza should I have for dinner tonight? What excuse should I use for skipping the gym today? While it may at times seem tiring to be faced with all these choices on a regular basis, it is this exercise of free will that separates us from the machines we live with.2 This multitude of choices, then, provides some measure of our own vitality | the more options we have, the more alive we truly are. What, then, could be more important than being able to count how many options one actually has?4 As we have already seen during our first week of lectures, one of the main protagonists in these counting problems is the binomial coefficient, whose definition is given below. n Definition 1. Given non-negative integers n and k, the binomial coefficient k denotes the number of subsets of size k of a set of n elements. Equivalently, it is the number of unordered choices of k distinct elements from a set of n elements. However, the binomial coefficient leads a double life. Not only does it have the above definition, but also the formula below, which we proved in lecture. Proposition 2. For non-negative integers n and k, n nk n(n − 1)(n − 2) ::: (n − k + 1) n! = = = : k k! k! k!(n − k)! In this note, we will prove several more facts about this most fascinating of creatures. -
Chapter 3.3, 4.1, 4.3. Binomial Coefficient Identities
Chapter 3.3, 4.1, 4.3. Binomial Coefficient Identities Prof. Tesler Math 184A Winter 2019 Prof. Tesler Binomial Coefficient Identities Math 184A / Winter 2019 1 / 36 Table of binomial coefficients n k k = 0 k = 1 k = 2 k = 3 k = 4 k = 5 k = 6 n = 0 1 0 0 0 0 0 0 n = 1 1 1 0 0 0 0 0 n = 2 1 2 1 0 0 0 0 n = 3 1 3 3 1 0 0 0 n = 4 1 4 6 4 1 0 0 n = 5 1 5 10 10 5 1 0 n = 6 1 6 15 20 15 6 1 n n! Compute a table of binomial coefficients using = . k k! (n - k)! We’ll look at several patterns. First, the nonzero entries of each row are symmetric; e.g., row n = 4 is 4 4 4 4 4 0 , 1 , 2 , 3 , 4 = 1, 4, 6, 4, 1 , n n which reads the same in reverse. Conjecture: k = n-k . Prof. Tesler Binomial Coefficient Identities Math 184A / Winter 2019 2 / 36 A binomial coefficient identity Theorem For nonegative integers k 6 n, n n n n = including = = 1 k n - k 0 n First proof: Expand using factorials: n n! n n! = = k k! (n - k)! n - k (n - k)! k! These are equal. Prof. Tesler Binomial Coefficient Identities Math 184A / Winter 2019 3 / 36 Theorem For nonegative integers k 6 n, n n n n = including = = 1 k n - k 0 n Second proof: A bijective proof. We’ll give a bijection between two sets, one counted by the left n n side, k , and the other by the right side, n-k . -
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. -
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. -
8.6 the BINOMIAL THEOREM We Remake Nature by the Act of Discovery, in the Poem Or in the Theorem
pg476 [V] G2 5-36058 / HCG / Cannon & Elich cr 11-30-95 MP1 476 Chapter 8 Discrete Mathematics: Functions on the Set of Natural Numbers (b) Based on your results for (a), guess the minimum number of handshakes. See Exercise 19, page 469. number of moves required if you start with an arbi- Show trary number of n disks. (Hint: Tohelpseeapat- n~n 2 1! tern,add1tothenumberofmovesforn51, 2, 3, f ~n! 5 for every positive integer n. 4.) 2 (c) A legend claims that monks in a remote monastery 56. Suppose n is an odd positive integer not divisible by 3. areworkingtomoveasetof64disks,andthatthe Show that n 2 2 1 is divisible by 24. (Hint: Consider the world will end when they complete their sacred three consecutive integers n 2 1, n, n 1 1. Explain task. Moving one disk per second without error, 24 why the product ~n 2 1!~n 1 1! must be divisible by 3 hours a day, 365 days a year, how long would it take andby8.) to move all 64 disks? 57. Finding Patterns If an 5 Ï24n 1 1, (a) write out 55. Number of Handshakes Suppose there are n people the first five terms of the sequence $an%. (b) What odd at a party and that each person shakes hands with every integers occur in $an%? (c) Explain why $an% contains all other person exactly once. Let f~n! denote the total primes greater than 3. (Hint: UseExercise56.) 8.6 THE BINOMIAL THEOREM We remake nature by the act of discovery, in the poem or in the theorem. -
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.