Vacuum Moduli Spaces of Supersymmetric Quiver Gauge Theories with 8 Supercharges
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JHEP05(2015)095 ) Gauge Springer N May 4, 2015 May 19, 2015 : : February 11, 2015
Published for SISSA by Springer Received: February 11, 2015 Accepted: May 4, 2015 Published: May 19, 2015 Defects and quantum Seiberg-Witten geometry JHEP05(2015)095 Mathew Bullimore,a Hee-Cheol Kimb and Peter Koroteevb aInstitute for Advanced Study, Einstein Dr., Princeton, NJ 08540, U.S.A. bPerimeter Institute for Theoretical Physics, 31 Caroline Street North, Waterloo, Ontario N2L2Y5, Canada E-mail: [email protected], [email protected], [email protected] Abstract: We study the Nekrasov partition function of the five dimensional U(N) gauge theory with maximal supersymmetry on R4 S1 in the presence of codimension two defects. × The codimension two defects can be described either as monodromy defects, or by coupling to a certain class of three dimensional quiver gauge theories on R2 S1. We explain how × these computations are connected with both classical and quantum integrable systems. We check, as an expansion in the instanton number, that the aforementioned partition functions are eigenfunctions of an elliptic integrable many-body system, which quantizes the Seiberg-Witten geometry of the five-dimensional gauge theory. Keywords: Supersymmetric gauge theory, Duality in Gauge Field Theories, Integrable Equations in Physics, Differential and Algebraic Geometry ArXiv ePrint: 1412.6081 Open Access, c The Authors. ⃝ doi:10.1007/JHEP05(2015)095 Article funded by SCOAP3. Contents 1 Introduction 1 2 Twisted chiral rings 3 2.1 The Nekrasov-Shatashvili correspondence 4 2.2 Quantum/classical duality 6 2.2.1 Electric frame -
Matrix Factorizations, D-Branes and Homological Mirror Symmetry W.Lerche, KITP 03/2009
Matrix Factorizations, D-branes and Homological Mirror Symmetry W.Lerche, KITP 03/2009 • Motivation, general remarks • Mirror symmetry and D-branes • Matrix factorizations and LG models • Toy example: eff. superpotential for intersecting branes, applications much more diverse instantons than for closed strings (world-sheet and D-brane instantons) 1 Part I Motivation: D-brane worlds Typical brane + flux configuration on a Calabi-Yau space closed string (bulk) moduli t open string (brane location + bundle) moduli u 3+1 dim world volume with effective N=1 SUSY theory What are the exact effective superpotential, the vacuum states, gauge couplings, etc ? (Φ, t, u) = ? Weff 2 Quantum geometry of D-branes Classical geometry ("branes wrapping p-cycles", gauge bundle configurations on top of them) makes sense only at weak coupling/large radius! M In fact, practically all of string Classical geometry: phenomenology deals with the cycles, gauge (“bundle”) boundary of the moduli space configurations on them (weak coupling, large radius) 3 Quantum geometry of D-branes Classical geometry ("branes wrapping p-cycles", gauge bundle configurations on top of them) makes sense only at weak coupling/large radius! “Gepner point” (CFT description) typ. symmetry between M 0,2,4,6 cycles ? “conifold point” extra massles states Classical geometry: Quantum corrected geometry: cycles, gauge (“bundle”) (instanton) corrections wipe out configurations on them notions of classical geometry 4 Quantum geometry of D-branes Classical geometry ("branes wrapping p-cycles", gauge bundle configurations on top of them) makes sense only at weak coupling/large radius! Need to develop formalism capable of describing the physics of general D-brane configurations (here: topological B-type D-branes), incl their continuous deformation families over the moduli space ....well developed techniques (mirror symmetry) mostly for non-generic (non-compact, non-intersecting, integrable) brane configurations branes only ! 5 Intersecting branes: eff. -
Intersecting Surface Defects and 3D Superconformal Indices
Published for SISSA by Springer Received: February 2, 2021 Accepted: April 19, 2021 Published: May 18, 2021 JHEP05(2021)155 Intersecting surface defects and 3d superconformal indices Junfeng Liu, Yiwen Pan and Hong-Hao Zhang School of Physics, Sun Yat-Sen University, Guangzhou 510275, China E-mail: [email protected], [email protected], [email protected] Abstract: We compute the 3d N = 2 superconformal indices for 3d/1d coupled systems, which arise as the worldvolume theories of intersecting surface defects engineered by Higgsing 5d N = 1 gauge theories. We generalize some known 3d dualities, including non-Abelian 3d mirror symmetry and 3d/3d correspondence, to some of the simple 3d/1d coupled systems. Finally we propose a q-Virasoro construction for the superconformal indices. Keywords: Duality in Gauge Field Theories, Supersymmetry and Duality ArXiv ePrint: 2101.05689 Open Access , c The Authors. https://doi.org/10.1007/JHEP05(2021)155 Article funded by SCOAP3. Contents 1 Introduction1 2 Higgsing and surface defects3 3 Intersecting surface defects on S4 × S1 6 3.1 Higgsing6 3.2 Index of intersecting gauge theory 10 JHEP05(2021)155 3.2.1 Reduction to 2d 12 4 3d dualities 13 4.1 3d mirror symmetry 13 4.1.1 U(1) 1 theory 14 4.1.2 3d mirror2 symmetry from fiber-base duality 16 4.2 3d/3d correspondence 21 5 q-Virasoro construction 24 A Special functions 28 B Instanton partition function 29 C Factorization of 3d index 31 1 Introduction Since the seminal work by Pestun [1], numerous exact results have been derived using the technique of supersymmetric localization for supersymmetric theories in different dimensions. -
Extremal Chiral Ring States in Ads/CFT Are Described by Free Fermions for A
DAMTP-2015-7 Extremal chiral ring states in AdS/CFT are described by free fermions for a generalized oscillator algebra David Berenstein Department of Applied Math and Theoretical Physics, Wilbeforce Road, Cambridge, CB3 0WA, UK and Department of Physics, University of California at Santa Barbara, CA 93106 Abstract This paper studies a special class of states for the dual conformal field theories associated with supersymmetric AdS X compactifications, where X is a Sasaki-Einstein manifold with additional 5 × U(1) symmetries. Under appropriate circumstances, it is found that elements of the chiral ring that maximize the additional U(1) charge at fixed R-charge are in one to one correspondence with multitraces of a single composite field. This is also equivalent to Schur functions of the composite field. It is argued that in the formal zero coupling limit that these dual field theories have, the different Schur functions are orthogonal. Together with large N counting arguments, one predicts that various extremal three point functions are identical to those of = 4 SYM, except for a N single normalization factor, which can be argued to be related to the R-charge of the composite word. The leading and subleading terms in 1/N are consistent with a system of free fermions for a generalized oscillator algebra. One can further test this conjecture by constructing coherent states arXiv:1504.05389v2 [hep-th] 4 Aug 2015 for the generalized oscillator algebra that can be interpreted as branes exploring a subset of the moduli space of the field theory and use these to compute the effective K¨ahler potential on this subset of the moduli space. -
Quiver Asymptotics: Free Chiral Ring
Journal of Physics A: Mathematical and Theoretical PAPER • OPEN ACCESS Quiver asymptotics: free chiral ring To cite this article: S Ramgoolam et al 2020 J. Phys. A: Math. Theor. 53 105401 View the article online for updates and enhancements. This content was downloaded from IP address 131.169.5.251 on 26/02/2020 at 00:58 IOP Journal of Physics A: Mathematical and Theoretical J. Phys. A: Math. Theor. Journal of Physics A: Mathematical and Theoretical J. Phys. A: Math. Theor. 53 (2020) 105401 (18pp) https://doi.org/10.1088/1751-8121/ab6fc6 53 2020 © 2020 The Author(s). Published by IOP Publishing Ltd Quiver asymptotics: = 1 free chiral ring N JPHAC5 S Ramgoolam1,3, Mark C Wilson2 and A Zahabi1,3 1 Centre for Research in String Theory, School of Physics and Astronomy, 105401 Queen Mary University of London, United Kingdom 2 Department of Computer Science, University of Auckland, Auckland, New Zealand 3 S Ramgoolam et al National Institute for Theoretical Physics, School of Physics and Mandelstam Institute for Theoretical Physics, University of the Witwatersrand, Johannesburg, South Africa Quiver asymptotics: = 1 free chiral ring N E-mail: [email protected], [email protected] and [email protected] Printed in the UK Received 23 August 2019, revised 21 January 2020 Accepted for publication 24 January 2020 JPA Published 20 February 2020 Abstract 10.1088/1751-8121/ab6fc6 The large N generating functions for the counting of chiral operators in = 1, four-dimensional quiver gauge theories have previously been obtained N Paper in terms of the weighted adjacency matrix of the quiver diagram. -
Brane Brick Models and Their Elliptic Genera
2016 Current Topics in String Theory : CFT Brane Brick Models and their Elliptic Genera Dongwook Ghim Seoul National University 2016. 12. 15 @ KIAS, Seoul 2016. 12. 15. KIAS This talk is based on … • 1506.03818 – Construction of theories SF, DG, SL, RKS, DY • 1510.01744 – Brane Brick SF, SL, RKS • 1602.01834 – (0,2) Triality SF, SL, RKS • 1609.01723 – Mirror perspective SF, SL, RKS, CV • 1609.07144 – Orbifold reduction SF, SL, RKS • 1612. to appear – Elliptic genus SF, DG, SL, RKS Collaborators: Sebastian Franco (CUNY), Sangmin Lee (SNU), Rak-Kyeong Seong (Uppsala), Daisuke Yokoyama (King’s college), Cumrun Vafa (Harvard) 2016. 12. 15. KIAS 2 Brane Brick Model 2d (0,2) gauge theory as a world-volume theory of D1-branes probing toric Calabi Yau 4-fold cones 2d (0,2) quiver gauge theory with U(N) gauge groups Quiver diagram N D1-branes toric CY 4-fold Brane configuration Toric diagram 2016. 12. 15. KIAS 3 Relatives and ancestors D(9-2n)-branes In type-IIB string theory, D(9-2n)-branes probing toric CY n-folds toric CYn dim, T-dual Symmetry n # of SUSY configuration 2 6d, N=(1,0) Necklace quiver - 3 4d, N=1 Brane tiling Seiberg duality 4 2d, N=(0,2) Brane brick GGP triality 2016. 12. 15. KIAS 4 2d (0,2) quiver gauge theories Gauge Theory SUSY multiplets of 2d (0,2) theories multiplets superfield component fields vector V (va, χ , χ ,D) − − chiral Φij (φ, +) Quiver diagrams of Fermi ⇤ij (λ ,G) − 2d (0,2) gauge theories • 2d (0,2) field-strength multiplet with U(N) gauge group + + + Y = χ i✓ (D iF01) i✓ ✓ @+χ − − − − − Φ • 2d (0,2) chiral ij • 2d (0,2) Fermi ⇤ij J-term E-term For SUSY, 2016. -
3D Mirror Symmetry As a Canonical Transformation
3d mirror symmetry as a canonical transformation Nadav Drukkera and Jan Felixb Department of Mathematics, King's College London The Strand, WC2R 2LS, London, UK Abstract We generalize the free Fermi-gas formulation of certain 3d = 3 supersymmetric Chern-Simons-matter theories by allowing Fayet-Iliopoulos couplingsN as well as mass terms for bifundamental matter fields. The resulting partition functions are given by simple modifications of the argument of the Airy function found previously. With these extra parameters it is easy to see that mirror-symmetry corresponds to linear canonical transformations on the phase space (or operator algebra) of the 1-dimensional fermions. arXiv:1501.02268v2 [hep-th] 13 Oct 2015 [email protected] [email protected] 1 Introduction and summary Supersymmetric localization leads to a dramatic simplification of the calculation of sphere partition functions (and some other observables) by reducing the infinite dimensional path integral to a finite dimensional matrix model [1,2] This matrix model can then be solved (sometimes) by a variety of old and new techniques to yield exact results. A particular application of this is to check dualities | two theories which are equivalent (or flow to the same IR fixed point) should have the same partition function. In practice, it is often very hard to solve the matrix models exactly, so dualities are checked by comparing the matrix models of the two theories and using integral identities to relate them. The first beautiful realization of this is in the Alday-Gaiotto-Tachikawa (AGT) correspondence, where the matrix models evaluating the partition functions of 4d = 2 theories were shown to be essentially identical to correlation functions of Liouville theoryN as expressed via the conformal bootstrap in a specific channel. -
Topological Quiver Matrix Models and Quantum Foam
Topological quiver matrix models and quantum foam Daniel L. Jafferis ∗ Jefferson Physical Laboratory Harvard University Cambridge, MA 02138 May 15, 2007 Abstract We study the matrix models that describe the BPS bound states of branes arising from the quiver picture of the derived category. These theories have a topological partition function that localizes to the Euler character of the anti-ghost bundle over the classical BPS moduli space. We examine the effective internal geometry of D6/D2 bound states in the local vertex geometry, using BPS 0-brane probes. The Kahler blowups of the Calabi-Yau that we find utilizing these quiver theories are a realization of A-model quantum foam in the full IIA theory. ∗E-mail: jaff[email protected] arXiv:0705.2250v1 [hep-th] 16 May 2007 1 1 Introduction The idea that the topological A-model involves quantized fluctuations of the Kahler geometry of a Calabi-Yau was introduced in [23]. They argued that the topological string partition function could be reproduced by summing over non-Calabi-Yau blow ups along collections of curves and points. The equivalent Donaldson-Thomas theory, given by a topologically twisted =2 U(1) gauge theory on the Calabi-Yau, involves a sum over singular instantons, which canN be blown up to obtain the fluctuations of the geometry. The connection between this theory of BPS bound states of D2 and D0 branes to a 6-brane was further explained in [13] by lifting to M-theory. The D6-brane lifts to a Taub-NUT geometry in 11 dimensions, and the Donaldson-Thomas theory results in precisely that repackaging of the Gopakumar-Vafa invariants counting bound states of D2/D0 at the center of the Taub-NUT which is required to reproduce the A-model. -
Lectures on D-Branes, Gauge Theories and Calabi-Yau
UPR-1086-T Lectures on D-branes, Gauge Theories and Calabi-Yau Singularities Yang-Hui He Department of Physics and Math/Physics RG University of Pennsylvania Philadelphia, PA 19104–6396, USA Abstract These lectures, given at the Chinese Academy of Sciences for the BeiJing/HangZhou International Summer School in Mathematical Physics, are intended to introduce, to the beginning student in string theory and mathematical physics, aspects of the rich and beautiful subject of D-brane gauge theories constructed from local Calabi-Yau spaces. arXiv:hep-th/0408142v1 18 Aug 2004 Topics such as orbifolds, toric singularities, del Pezzo surfaces as well as chaotic duality will be covered. ∗[email protected] Contents 1 Introduction 2 2 Minute Waltz on the String 5 2.1 The D3-brane in R1,9 ............................... 6 2.2 D3-branesonCalabi-Yauthreefolds . ...... 7 3 The Simplest Case: S = C3 8 4 Orbifolds and Quivers 10 4.1 ProjectiontoDaughterTheories. ..... 10 4.2 Quivers ...................................... 12 4.3 TheMcKayCorrespondence . 12 4.4 McKay, Dimension 2 and N =2......................... 15 4.5 N = 1 Theories and C3 Orbifolds ........................ 15 4.6 Quivers, Modular Invariants, Path Algebras? . ......... 17 4.7 MoreGames.................................... 17 5 Gauge Theories, Moduli Spaces andSymplectic Quotients 19 5.1 QuiverGaugeTheory............................... 20 5.2 An Illustrative Example: The Conifold . ...... 21 5.3 ToricSingularities.. .. .. ... 22 5.3.1 A Lightning Review on Toric Varieties . ... 23 5.3.2 Witten’s Gauged Linear Sigma Model (GLSM) . .. 23 5.4 TheForwardAlgorithm ............................. 24 5.4.1 Forward Algorithm for Abelian Orbifolds . ..... 25 5.5 TheInverseAlgorithm ............................. 28 5.6 Applications of Inverse Algorithm . ...... 29 5.6.1 delPezzoSurfaces ........................... -
1.3 Self-Dual/Chiral Gauge Theories 23 1.3.1 PST Approach 27
Durham E-Theses Chiral gauge theories and their applications Berman, David Simon How to cite: Berman, David Simon (1998) Chiral gauge theories and their applications, Durham theses, Durham University. Available at Durham E-Theses Online: http://etheses.dur.ac.uk/5041/ Use policy The full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-prot purposes provided that: • a full bibliographic reference is made to the original source • a link is made to the metadata record in Durham E-Theses • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders. Please consult the full Durham E-Theses policy for further details. Academic Support Oce, Durham University, University Oce, Old Elvet, Durham DH1 3HP e-mail: [email protected] Tel: +44 0191 334 6107 http://etheses.dur.ac.uk Chiral gauge theories and their applications by David Simon Berman A thesis submitted for the degree of Doctor of Philosophy Department of Mathematics University of Durham South Road Durham DHl 3LE England June 1998 The copyright of this tliesis rests with tlie author. No quotation from it should be published without the written consent of the author and information derived from it should be acknowledged. 3 0 SEP 1998 Preface This thesis summarises work done by the author between October 1994 and April 1998 at the Department of Mathematical Sciences of the University of Durham and at CERN theory division under the supervision of David FairUe. -
Localization and Dualities in Three-Dimensional Superconformal Field Theories
Localization and Dualities in Three-dimensional Superconformal Field Theories Thesis by Brian Willett In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 2012 (Defended May 15, 2012) ii c 2012 Brian Willett All Rights Reserved iii Abstract In this thesis we apply the technique of localization to three-dimensional N = 2 superconformal field theories. We consider both theories which are exactly superconformal, and those which are believed to flow to nontrivial superconformal fixed points, for which we consider implicitly these fixed points. We find that in such theories, the partition function and certain supersymmetric observables, such as Wilson loops, can be computed exactly by a matrix model. This matrix model consists of an integral over g, the Lie algebra of the gauge group of the theory, of a certain product of 1-loop factors and classical contributions. One can also consider a space of supersymmetric deformations of the partition function corresponding to the set of abelian global symmetries. In the second part of the thesis we apply these results to test dualities. We start with the case of 7 ABJM theory, which is dual to M-theory on an asymptotically AdS4 × S background. We extract strong coupling results in the field theory, which can be compared to semiclassical, weak coupling results in the gravity theory, and a nontrivial agreement is found. We also consider several classes of dualities between two three-dimensional field theories, namely, 3D mirror symmetry, Aharony duality, and Giveon-Kutasov duality. Here the dualities are typically between the IR limits of two Yang-Mills theories, which are strongly coupled in three dimensions since Yang-Mills theory is asymptotically free here. -
T Hooft Operators in Four-Dimensional Gauge Theories and S-Duality
PHYSICAL REVIEW D 74, 025005 (2006) Wilson-’t Hooft operators in four-dimensional gauge theories and S-duality Anton Kapustin* California Institute of Technology, Pasadena California 91125 USA (Received 14 May 2006; published 7 July 2006) We study operators in four-dimensional gauge theories which are localized on a straight line, create electric and magnetic flux, and in the UV limit break the conformal invariance in the minimal possible way. We call them Wilson-’t Hooft operators, since in the purely electric case they reduce to the well- known Wilson loops, while in general they may carry ’t Hooft magnetic flux. We show that to any such 2 2 operator one can associate a maximally symmetric boundary condition for gauge fields on AdSE S .We show that Wilson-’t Hooft operators are classified by a pair of weights (electric and magnetic) for the gauge group and its magnetic dual, modulo the action of the Weyl group. If the magnetic weight does not belong to the coroot lattice of the gauge group, the corresponding operator is topologically nontrivial (carries nonvanishing ’t Hooft magnetic flux). We explain how the spectrum of Wilson-’t Hooft operators transforms under the shift of the -angle by 2. We show that, depending on the gauge group, either SL 2; Z or one of its congruence subgroups acts in a natural way on the set of Wilson-’t Hooft operators. This can be regarded as evidence for the S-duality of N 4 super-Yang-Mills theory. We also compute the one-point function of the stress-energy tensor in the presence of a Wilson-’t Hooft operator at weak coupling.