Orbifold Cohomology of Torus Quotients
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PCMI Summer 2015 Undergraduate Lectures on Flag Varieties 0. What
PCMI Summer 2015 Undergraduate Lectures on Flag Varieties 0. What are Flag Varieties and Why should we study them? Let's start by over-analyzing the binomial theorem: n X n (x + y)n = xmyn−m m m=0 has binomial coefficients n n! = m m!(n − m)! that count the number of m-element subsets T of an n-element set S. Let's count these subsets in two different ways: (a) The number of ways of choosing m different elements from S is: n(n − 1) ··· (n − m + 1) = n!=(n − m)! and each such choice produces a subset T ⊂ S, with an ordering: T = ft1; ::::; tmg of the elements of T This realizes the desired set (of subsets) as the image: f : fT ⊂ S; T = ft1; :::; tmgg ! fT ⊂ Sg of a \forgetful" map. Since each preimage f −1(T ) of a subset has m! elements (the orderings of T ), we get the binomial count. Bonus. If S = [n] = f1; :::; ng is ordered, then each subset T ⊂ [n] has a distinguished ordering t1 < t2 < ::: < tm that produces a \section" of the forgetful map. For example, in the case n = 4 and m = 2, we get: fT ⊂ [4]g = ff1; 2g; f1; 3g; f1; 4g; f2; 3g; f2; 4g; f3; 4gg realized as a subset of the set fT ⊂ [4]; ft1; t2gg. (b) The group Perm(S) of permutations of S \acts" on fT ⊂ Sg via f(T ) = ff(t) jt 2 T g for each permutation f : S ! S This is an transitive action (every subset maps to every other subset), and the \stabilizer" of a particular subset T ⊂ S is the subgroup: Perm(T ) × Perm(S − T ) ⊂ Perm(S) of permutations of T and S − T separately. -
A Space-Time Orbifold: a Toy Model for a Cosmological Singularity
hep-th/0202187 UPR-981-T, HIP-2002-07/TH A Space-Time Orbifold: A Toy Model for a Cosmological Singularity Vijay Balasubramanian,1 ∗ S. F. Hassan,2† Esko Keski-Vakkuri,2‡ and Asad Naqvi1§ 1David Rittenhouse Laboratories, University of Pennsylvania Philadelphia, PA 19104, U.S.A. 2Helsinki Institute of Physics, P.O.Box 64, FIN-00014 University of Helsinki, Finland Abstract We explore bosonic strings and Type II superstrings in the simplest time dependent backgrounds, namely orbifolds of Minkowski space by time reversal and some spatial reflections. We show that there are no negative norm physi- cal excitations. However, the contributions of negative norm virtual states to quantum loops do not cancel, showing that a ghost-free gauge cannot be chosen. The spectrum includes a twisted sector, with strings confined to a “conical” sin- gularity which is localized in time. Since these localized strings are not visible to asymptotic observers, interesting issues arise regarding unitarity of the S- matrix for scattering of propagating states. The partition function of our model is modular invariant, and for the superstring, the zero momentum dilaton tad- pole vanishes. Many of the issues we study will be generic to time-dependent arXiv:hep-th/0202187v2 19 Apr 2002 cosmological backgrounds with singularities localized in time, and we derive some general lessons about quantizing strings on such spaces. 1 Introduction Time-dependent space-times are difficult to study, both classically and quantum me- chanically. For example, non-static solutions are harder to find in General Relativity, while the notion of a particle is difficult to define clearly in field theory on time- dependent backgrounds. -
Deformations of G2-Structures, String Dualities and Flat Higgs Bundles Rodrigo De Menezes Barbosa University of Pennsylvania, [email protected]
University of Pennsylvania ScholarlyCommons Publicly Accessible Penn Dissertations 2019 Deformations Of G2-Structures, String Dualities And Flat Higgs Bundles Rodrigo De Menezes Barbosa University of Pennsylvania, [email protected] Follow this and additional works at: https://repository.upenn.edu/edissertations Part of the Mathematics Commons, and the Quantum Physics Commons Recommended Citation Barbosa, Rodrigo De Menezes, "Deformations Of G2-Structures, String Dualities And Flat Higgs Bundles" (2019). Publicly Accessible Penn Dissertations. 3279. https://repository.upenn.edu/edissertations/3279 This paper is posted at ScholarlyCommons. https://repository.upenn.edu/edissertations/3279 For more information, please contact [email protected]. Deformations Of G2-Structures, String Dualities And Flat Higgs Bundles Abstract We study M-theory compactifications on G2-orbifolds and their resolutions given by total spaces of coassociative ALE-fibrations over a compact flat Riemannian 3-manifold Q. The afl tness condition allows an explicit description of the deformation space of closed G2-structures, and hence also the moduli space of supersymmetric vacua: it is modeled by flat sections of a bundle of Brieskorn-Grothendieck resolutions over Q. Moreover, when instanton corrections are neglected, we obtain an explicit description of the moduli space for the dual type IIA string compactification. The two moduli spaces are shown to be isomorphic for an important example involving A1-singularities, and the result is conjectured to hold in generality. We also discuss an interpretation of the IIA moduli space in terms of "flat Higgs bundles" on Q and explain how it suggests a new approach to SYZ mirror symmetry, while also providing a description of G2-structures in terms of B-branes. -
Jhep05(2019)105
Published for SISSA by Springer Received: March 21, 2019 Accepted: May 7, 2019 Published: May 20, 2019 Modular symmetries and the swampland conjectures JHEP05(2019)105 E. Gonzalo,a;b L.E. Ib´a~neza;b and A.M. Urangaa aInstituto de F´ısica Te´orica IFT-UAM/CSIC, C/ Nicol´as Cabrera 13-15, Campus de Cantoblanco, 28049 Madrid, Spain bDepartamento de F´ısica Te´orica, Facultad de Ciencias, Universidad Aut´onomade Madrid, 28049 Madrid, Spain E-mail: [email protected], [email protected], [email protected] Abstract: Recent string theory tests of swampland ideas like the distance or the dS conjectures have been performed at weak coupling. Testing these ideas beyond the weak coupling regime remains challenging. We propose to exploit the modular symmetries of the moduli effective action to check swampland constraints beyond perturbation theory. As an example we study the case of heterotic 4d N = 1 compactifications, whose non-perturbative effective action is known to be invariant under modular symmetries acting on the K¨ahler and complex structure moduli, in particular SL(2; Z) T-dualities (or subgroups thereof) for 4d heterotic or orbifold compactifications. Remarkably, in models with non-perturbative superpotentials, the corresponding duality invariant potentials diverge at points at infinite distance in moduli space. The divergence relates to towers of states becoming light, in agreement with the distance conjecture. We discuss specific examples of this behavior based on gaugino condensation in heterotic orbifolds. We show that these examples are dual to compactifications of type I' or Horava-Witten theory, in which the SL(2; Z) acts on the complex structure of an underlying 2-torus, and the tower of light states correspond to D0-branes or M-theory KK modes. -
A Quasideterminantal Approach to Quantized Flag Varieties
A QUASIDETERMINANTAL APPROACH TO QUANTIZED FLAG VARIETIES BY AARON LAUVE A dissertation submitted to the Graduate School—New Brunswick Rutgers, The State University of New Jersey in partial fulfillment of the requirements for the degree of Doctor of Philosophy Graduate Program in Mathematics Written under the direction of Vladimir Retakh & Robert L. Wilson and approved by New Brunswick, New Jersey May, 2005 ABSTRACT OF THE DISSERTATION A Quasideterminantal Approach to Quantized Flag Varieties by Aaron Lauve Dissertation Director: Vladimir Retakh & Robert L. Wilson We provide an efficient, uniform means to attach flag varieties, and coordinate rings of flag varieties, to numerous noncommutative settings. Our approach is to use the quasideterminant to define a generic noncommutative flag, then specialize this flag to any specific noncommutative setting wherein an amenable determinant exists. ii Acknowledgements For finding interesting problems and worrying about my future, I extend a warm thank you to my advisor, Vladimir Retakh. For a willingness to work through even the most boring of details if it would make me feel better, I extend a warm thank you to my advisor, Robert L. Wilson. For helpful mathematical discussions during my time at Rutgers, I would like to acknowledge Earl Taft, Jacob Towber, Kia Dalili, Sasa Radomirovic, Michael Richter, and the David Nacin Memorial Lecture Series—Nacin, Weingart, Schutzer. A most heartfelt thank you is extended to 326 Wayne ST, Maria, Kia, Saˇsa,Laura, and Ray. Without your steadying influence and constant comraderie, my time at Rut- gers may have been shorter, but certainly would have been darker. Thank you. Before there was Maria and 326 Wayne ST, there were others who supported me. -
GROMOV-WITTEN INVARIANTS on GRASSMANNIANS 1. Introduction
JOURNAL OF THE AMERICAN MATHEMATICAL SOCIETY Volume 16, Number 4, Pages 901{915 S 0894-0347(03)00429-6 Article electronically published on May 1, 2003 GROMOV-WITTEN INVARIANTS ON GRASSMANNIANS ANDERS SKOVSTED BUCH, ANDREW KRESCH, AND HARRY TAMVAKIS 1. Introduction The central theme of this paper is the following result: any three-point genus zero Gromov-Witten invariant on a Grassmannian X is equal to a classical intersec- tion number on a homogeneous space Y of the same Lie type. We prove this when X is a type A Grassmannian, and, in types B, C,andD,whenX is the Lagrangian or orthogonal Grassmannian parametrizing maximal isotropic subspaces in a com- plex vector space equipped with a non-degenerate skew-symmetric or symmetric form. The space Y depends on X and the degree of the Gromov-Witten invariant considered. For a type A Grassmannian, Y is a two-step flag variety, and in the other cases, Y is a sub-maximal isotropic Grassmannian. Our key identity for Gromov-Witten invariants is based on an explicit bijection between the set of rational maps counted by a Gromov-Witten invariant and the set of points in the intersection of three Schubert varieties in the homogeneous space Y . The proof of this result uses no moduli spaces of maps and requires only basic algebraic geometry. It was observed in [Bu1] that the intersection and linear span of the subspaces corresponding to points on a curve in a Grassmannian, called the kernel and span of the curve, have dimensions which are bounded below and above, respectively. -
Arxiv:Hep-Th/9404101V3 21 Nov 1995
hep-th/9404101 April 1994 Chern-Simons Gauge Theory on Orbifolds: Open Strings from Three Dimensions ⋆ Petr Horavaˇ ∗ Enrico Fermi Institute University of Chicago 5640 South Ellis Avenue Chicago IL 60637, USA ABSTRACT Chern-Simons gauge theory is formulated on three dimensional Z2 orbifolds. The locus of singular points on a given orbifold is equivalent to a link of Wilson lines. This allows one to reduce any correlation function on orbifolds to a sum of more complicated correlation functions in the simpler theory on manifolds. Chern-Simons theory on manifolds is known arXiv:hep-th/9404101v3 21 Nov 1995 to be related to 2D CFT on closed string surfaces; here I show that the theory on orbifolds is related to 2D CFT of unoriented closed and open string models, i.e. to worldsheet orb- ifold models. In particular, the boundary components of the worldsheet correspond to the components of the singular locus in the 3D orbifold. This correspondence leads to a simple identification of the open string spectra, including their Chan-Paton degeneration, in terms of fusing Wilson lines in the corresponding Chern-Simons theory. The correspondence is studied in detail, and some exactly solvable examples are presented. Some of these examples indicate that it is natural to think of the orbifold group Z2 as a part of the gauge group of the Chern-Simons theory, thus generalizing the standard definition of gauge theories. E-mail address: [email protected] ⋆∗ Address after September 1, 1994: Joseph Henry Laboratories, Princeton University, Princeton, New Jersey 08544. 1. Introduction Since the first appearance of the notion of “orbifolds” in Thurston’s 1977 lectures on three dimensional topology [1], orbifolds have become very appealing objects for physicists. -
An Introduction to Orbifolds
An introduction to orbifolds Joan Porti UAB Subdivide and Tile: Triangulating spaces for understanding the world Lorentz Center November 2009 An introduction to orbifolds – p.1/20 Motivation • Γ < Isom(Rn) or Hn discrete and acts properly discontinuously (e.g. a group of symmetries of a tessellation). • If Γ has no fixed points ⇒ Γ\Rn is a manifold. • If Γ has fixed points ⇒ Γ\Rn is an orbifold. An introduction to orbifolds – p.2/20 Motivation • Γ < Isom(Rn) or Hn discrete and acts properly discontinuously (e.g. a group of symmetries of a tessellation). • If Γ has no fixed points ⇒ Γ\Rn is a manifold. • If Γ has fixed points ⇒ Γ\Rn is an orbifold. ··· (there are other notions of orbifold in algebraic geometry, string theory or using grupoids) An introduction to orbifolds – p.2/20 Examples: tessellations of Euclidean plane Γ= h(x, y) → (x + 1, y), (x, y) → (x, y + 1)i =∼ Z2 Γ\R2 =∼ T 2 = S1 × S1 An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) 2 2 An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) 2 2 2 2 2 2 2 2 2 2 2 2 An introduction to orbifolds – p.3/20 Example: tessellations of hyperbolic plane Rotations of angle π, π/2 and π/3 around vertices (order 2, 4, and 6) An introduction to orbifolds – p.4/20 Example: tessellations of hyperbolic plane Rotations of angle π, π/2 and π/3 around vertices (order 2, 4, and 6) 2 4 2 6 An introduction to orbifolds – p.4/20 Definition Informal Definition • An orbifold O is a metrizable topological space equipped with an atlas modelled on Rn/Γ, Γ < O(n) finite, with some compatibility condition. -
Ads Orbifolds and Penrose Limits
IPM/P-2002/061 UCB-PTH-02/54 LBL-51767 hep-th/yymmnnn AdS orbifolds and Penrose limits Mohsen Alishahihaa, Mohammad M. Sheikh-Jabbarib and Radu Tatarc a Institute for Studies in Theoretical Physics and Mathematics (IPM) P.O.Box 19395-5531, Tehran, Iran e-mail: [email protected] b Department of Physics, Stanford University 382 via Pueblo Mall, Stanford CA 94305-4060, USA e-mail: [email protected] c Department of Physics, 366 Le Conte Hall University of California, Berkeley, CA 94720 and Lawrence Berkeley National Laboratory Berkeley, CA 94720 email:[email protected] Abstract In this paper we study the Penrose limit of AdS5 orbifolds. The orbifold can be either in the pure spatial directions or space and time directions. For the AdS =¡ S5 spatial orbifold we observe that after the Penrose limit we 5 £ obtain the same result as the Penrose limit of AdS S5=¡. We identify the 5 £ corresponding BMN operators in terms of operators of the gauge theory on R £ S3=¡. The semi-classical description of rotating strings in these backgrounds have also been studied. For the spatial AdS orbifold we show that in the quadratic order the obtained action for the fluctuations is the same as that in S5 orbifold, however, the higher loop correction can distinguish between two cases. 1 Introduction In the past ¯ve years important results have been obtained relating closed and open string theories, in particular the AdS/CFT correspondence [1] had important impact into the understanding between these two sectors. The main problem in testing the conjecture beyond the supergravity level is the fact that we do not know how to quantize string theory in the presence of RR-fluxes. -
K3 Surfaces and String Duality
RU-96-98 hep-th/9611137 November 1996 K3 Surfaces and String Duality Paul S. Aspinwall Dept. of Physics and Astronomy, Rutgers University, Piscataway, NJ 08855 ABSTRACT The primary purpose of these lecture notes is to explore the moduli space of type IIA, type IIB, and heterotic string compactified on a K3 surface. The main tool which is invoked is that of string duality. K3 surfaces provide a fascinating arena for string compactification as they are not trivial spaces but are sufficiently simple for one to be able to analyze most of their properties in detail. They also make an almost ubiquitous appearance in the common statements concerning string duality. We arXiv:hep-th/9611137v5 7 Sep 1999 review the necessary facts concerning the classical geometry of K3 surfaces that will be needed and then we review “old string theory” on K3 surfaces in terms of conformal field theory. The type IIA string, the type IIB string, the E E heterotic string, 8 × 8 and Spin(32)/Z2 heterotic string on a K3 surface are then each analyzed in turn. The discussion is biased in favour of purely geometric notions concerning the K3 surface itself. Contents 1 Introduction 2 2 Classical Geometry 4 2.1 Definition ..................................... 4 2.2 Holonomy ..................................... 7 2.3 Moduli space of complex structures . ..... 9 2.4 Einsteinmetrics................................. 12 2.5 AlgebraicK3Surfaces ............................. 15 2.6 Orbifoldsandblow-ups. .. 17 3 The World-Sheet Perspective 25 3.1 TheNonlinearSigmaModel . 25 3.2 TheTeichm¨ullerspace . .. 27 3.3 Thegeometricsymmetries . .. 29 3.4 Mirrorsymmetry ................................. 31 3.5 Conformalfieldtheoryonatorus . ... 33 4 Type II String Theory 37 4.1 Target space supergravity and compactification . -
International Theoretical Physics
INTERNATIONAL THEORETICAL PHYSICS INTERACTION OF MOVING D-BRANES ON ORBIFOLDS INTERNATIONAL ATOMIC ENERGY Faheem Hussain AGENCY Roberto Iengo Carmen Nunez UNITED NATIONS and EDUCATIONAL, Claudio A. Scrucca SCIENTIFIC AND CULTURAL ORGANIZATION CD MIRAMARE-TRIESTE 2| 2i CO i IC/97/56 ABSTRACT SISSAREF-/97/EP/80 We use the boundary state formalism to study the interaction of two moving identical United Nations Educational Scientific and Cultural Organization D-branes in the Type II superstring theory compactified on orbifolds. By computing the and velocity dependence of the amplitude in the limit of large separation we can identify the International Atomic Energy Agency nature of the different forces between the branes. In particular, in the Z orbifokl case we THE ABDUS SALAM INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS 3 find a boundary state which is coupled only to the N = 2 graviton multiplet containing just a graviton and a vector like in the extremal Reissner-Nordstrom configuration. We also discuss other cases including T4/Z2. INTERACTION OF MOVING D-BRANES ON ORBIFOLDS Faheem Hussain The Abdus Salam International Centre for Theoretical Physics, Trieste, Italy, Roberto Iengo International School for Advanced Studies, Trieste, Italy and INFN, Sezione di Trieste, Trieste, Italy, Carmen Nunez1 Instituto de Astronomi'a y Fisica del Espacio (CONICET), Buenos Aires, Argentina and Claudio A. Scrucca International School for Advanced Studies, Trieste, Italy and INFN, Sezione di Trieste, Trieste, Italy. MIRAMARE - TRIESTE February 1998 1 Regular Associate of the ICTP. The non-relativistic dynamics of Dirichlet branes [1-3], plays an essential role in the coordinate satisfies Neumann boundary conditions, dTX°(T = 0, a) = drX°(r = I, a) = 0. -
Totally Positive Toeplitz Matrices and Quantum Cohomology of Partial Flag Varieties
JOURNAL OF THE AMERICAN MATHEMATICAL SOCIETY Volume 16, Number 2, Pages 363{392 S 0894-0347(02)00412-5 Article electronically published on November 29, 2002 TOTALLY POSITIVE TOEPLITZ MATRICES AND QUANTUM COHOMOLOGY OF PARTIAL FLAG VARIETIES KONSTANZE RIETSCH 1. Introduction A matrix is called totally nonnegative if all of its minors are nonnegative. Totally nonnegative infinite Toeplitz matrices were studied first in the 1950's. They are characterized in the following theorem conjectured by Schoenberg and proved by Edrei. Theorem 1.1 ([10]). The Toeplitz matrix ∞×1 1 a1 1 0 1 a2 a1 1 B . .. C B . a2 a1 . C B C A = B .. .. .. C B ad . C B C B .. .. C Bad+1 . a1 1 C B C B . C B . .. .. a a .. C B 2 1 C B . C B .. .. .. .. ..C B C is totally nonnegative@ precisely if its generating function is of theA form, 2 (1 + βit) 1+a1t + a2t + =exp(tα) ; ··· (1 γit) i Y2N − where α R 0 and β1 β2 0,γ1 γ2 0 with βi + γi < . 2 ≥ ≥ ≥···≥ ≥ ≥···≥ 1 This beautiful result has been reproved many times; see [32]P for anP overview. It may be thought of as giving a parameterization of the totally nonnegative Toeplitz matrices by ~ N N ~ (α;(βi)i; (~γi)i) R 0 R 0 R 0 i(βi +~γi) < ; f 2 ≥ × ≥ × ≥ j 1g i X2N where β~i = βi βi+1 andγ ~i = γi γi+1. − − Received by the editors December 10, 2001 and, in revised form, September 14, 2002. 2000 Mathematics Subject Classification. Primary 20G20, 15A48, 14N35, 14N15.