Spectral Networks - a Story of Wall-Crossing in Geometry and Physics
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TWAS Fellowships Worldwide
CDC Round Table, ICTP April 2016 With science and engineering, countries can address challenges in agriculture, climate, health TWAS’s and energy. guiding principles 2 Food security Challenges Water quality for a Energy security new era Biodiversity loss Infectious diseases Climate change 3 A Globally, 81 nations fall troubling into the category of S&T- gap lagging countries. 48 are classified as Least Developed Countries. 4 The role of TWAS The day-to-day work of TWAS is focused in two critical areas: •Improving research infrastructure •Building a corps of PhD scholars 5 TWAS Research Grants 2,202 grants awarded to individuals and research groups (1986-2015) 6 TWAS’ AIM: to train 1000 PhD students by 2017 Training PhD-level scientists: •Researchers and university-level educators •Future leaders for science policy, business and international cooperation Rapidly growing opportunities P BRAZIL A K I N D I CA I RI A S AF TH T SOU A N M KENYA EX ICO C H I MALAYSIA N A IRAN THAILAND TWAS Fellowships Worldwide NRF, South Africa - newly on board 650+ fellowships per year PhD fellowships +460 Postdoctoral fellowships +150 Visiting researchers/professors + 45 17 Programme Partners BRAZIL: CNPq - National Council MALAYSIA: UPM – Universiti for Scientific and Technological Putra Malaysia WorldwideDevelopment CHINA: CAS - Chinese Academy of KENYA: icipe – International Sciences Centre for Insect Physiology and Ecology INDIA: CSIR - Council of Scientific MEXICO: CONACYT– National & Industrial Research Council on Science and Technology PAKISTAN: CEMB – National INDIA: DBT - Department of Centre of Excellence in Molecular Biotechnology Biology PAKISTAN: ICCBS – International Centre for Chemical and INDIA: IACS - Indian Association Biological Sciences for the Cultivation of Science PAKISTAN: CIIT – COMSATS Institute of Information INDIA: S.N. -
Mirror Symmetry for Honeycombs
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 373, Number 1, January 2020, Pages 71–107 https://doi.org/10.1090/tran/7909 Article electronically published on September 10, 2019 MIRROR SYMMETRY FOR HONEYCOMBS BENJAMIN GAMMAGE AND DAVID NADLER Abstract. We prove a homological mirror symmetry equivalence between the A-brane category of the pair of pants, computed as a wrapped microlocal sheaf category, and the B-brane category of its mirror LG model, understood as a category of matrix factorizations. The equivalence improves upon prior results in two ways: it intertwines evident affine Weyl group symmetries on both sides, and it exhibits the relation of wrapped microlocal sheaves along different types of Lagrangian skeleta for the same hypersurface. The equivalence proceeds through the construction of a combinatorial realization of the A-model via arboreal singularities. The constructions here represent the start of a program to generalize to higher dimensions many of the structures which have appeared in topological approaches to Fukaya categories of surfaces. Contents 1. Introduction 71 2. Combinatorial A-model 78 3. Mirror symmetry 95 4. Symplectic geometry 100 Acknowledgments 106 References 106 1. Introduction This paper fits into the framework of homological mirror symmetry, as introduced in [23] and expanded in [19, 20, 22]. The formulation of interest to us relates the A-model of a hypersurface X in a toric variety to the mirror Landau-Ginzburg B- model of a toric variety X∨ equipped with superpotential W ∨ ∈O(X∨). Following Mikhalkin [27], a distinguished “atomic” case is when the hypersurface is the pair of pants ∗ n ∼ ∗ 1 n Pn−1 = {z1 + ···+ zn +1=0}⊂(C ) = T (S ) n+1 with mirror Landau-Ginzburg model (A ,z1 ···zn+1). -
SUPERSYMMETRY 1. Introduction the Purpose
SUPERSYMMETRY JOSH KANTOR 1. Introduction The purpose of these notes is to give a short and (overly?)simple description of supersymmetry for Mathematicians. Our description is far from complete and should be thought of as a first pass at the ideas that arise from supersymmetry. Fundamental to supersymmetry is the mathematics of Clifford algebras and spin groups. We will describe the mathematical results we are using but we refer the reader to the references for proofs. In particular [4], [1], and [5] all cover spinors nicely. 2. Spin and Clifford Algebras We will first review the definition of spin, spinors, and Clifford algebras. Let V be a vector space over R or C with some nondegenerate quadratic form. The clifford algebra of V , l(V ), is the algebra generated by V and 1, subject to the relations v v = v, vC 1, or equivalently v w + w v = 2 v, w . Note that elements of· l(V ) !can"b·e written as polynomials· in V · and this! giv"es a splitting l(V ) = l(VC )0 l(V )1. Here l(V )0 is the set of elements of l(V ) which can bCe writtenC as a linear⊕ C combinationC of products of even numbers ofCvectors from V , and l(V )1 is the set of elements which can be written as a linear combination of productsC of odd numbers of vectors from V . Note that more succinctly l(V ) is just the quotient of the tensor algebra of V by the ideal generated by v vC v, v 1. -
Proofs JHEP 092P 1215 Xxxxxxx ???, 2016 Springer : Doi: March 1, 2016 : Y February 25, 2016 December 11, 2015 : : Setting
Published for SISSA by Springer Received: December 11, 2015 Revised: February 25, 2016 Accepted: March 1, 2016 Published: ???, 2016 proofs JHEP_092P_1215 Notes on super Killing tensors P.S. Howea and U. Lindstr¨omb,c aDepartment of Mathematics, King’s College London, The Strand, London WC2R 2LS, U.K. bDepartment of Physics and Astronomy, Theoretical Physics, Uppsala University, SE-751 20 Uppsala, Sweden cTheoretical Physics, Imperial College London, Prince Consort Road, London SW7 2AZ, U.K. E-mail: [email protected], [email protected] Abstract: The notion of a Killing tensor is generalised to a superspace setting. Conserved quantities associated with these are defined for superparticles and Poisson brackets are used to define a supersymmetric version of the even Schouten-Nijenhuis bracket. Superconformal Killing tensors in flat superspaces are studied for spacetime dimensions 3,4,5,6 and 10. These tensors are also presented in analytic superspaces and super-twistor spaces for 3,4 and 6 dimensions. Algebraic structures associated with superconformal Killing tensors are also briefly discussed. Keywords: Extended Supersymmetry, Superspaces, Higher Spin Symmetry ArXiv ePrint: 1511.04575 Open Access, c The Authors. doi:xxxxxxx Article funded by SCOAP3. Contents 1 Introduction 1 2 Killing tensors in superspace 3 3 Superparticles 6 4 SCKTs in flat superspaces 10 proofs JHEP_092P_1215 5 Analytic superspace 18 6 Components of superconformal Killing tensors 24 6.1 D = 3 25 6.2 D = 4 26 6.3 D = 6 27 6.4 Algebras 28 7 Comments on higher spin 29 8 Concluding remarks 30 A Supersymmetric SN bracket 31 1 Introduction In ordinary Lorentzian spacetime a Killing vector, K, is a symmetry of the metric, i.e. -
Supersymmetric Lagrangians
1 Section 1 Setup Supersymmetric Lagrangians Chris Elliott February 6, 2013 1 Setup Let's recall some notions from classical Lagrangian field theory. Let M be an oriented supermanifold: our spacetime, of dimension njd. For our purposes, we will most often think about the case where M is either Minkowski space Mˇ n = R1;n−1, or Super Minkowski space M = Mˇ n × ΠS where S is a representation of Spin(1; n − 1). Definition 1.1. Let E ! M be a smooth (super) fibre bundle. The associated space of fields is the space of smooth sections φM ! E.A Lagrangian density on F is a function L: F! Dens(M) { where Dens(M) denotes the bundle of densities on M { that satisfies a locality condition. Precisely, we form the pullback bundle Dens(M)F / Dens(M) M × F / M π1 and require L to be a section of this bundle such that, for some k, for all m 2 M, L(m; φ) only depends on the first k derivatives of φ. We can phrase this in terms of factoring through the kth jet bundle of E. As usual, we define the action functional to be the integral Z S(φ) = L(φ): M A Lagrangian system generally includes additional information, namely a choice of variational 1-form γ. In general I won't use this data, but I should mention when it might play a role. 1.1 Symmetries In this talk, we will be discussing Lagrangian systems with certain kinds of symmetry called supersymmetry. As such, it'll be important to understand what it actually means to be a symmetry of such a system. -
[Math.RA] 14 Jun 2007 the Minkowski and Conformal Superspaces
IFIC/06-28 FTUV-05/0928 The Minkowski and conformal superspaces R. Fioresi 1 Dipartimento di Matematica, Universit`adi Bologna Piazza di Porta S. Donato, 5. 40126 Bologna. Italy. e-mail: fi[email protected] M. A. Lled´o Departament de F´ısica Te`orica, Universitat de Val`encia and IFIC C/Dr. Moliner, 50, E-46100 Burjassot (Val`encia), Spain. e-mail: Maria.Lledo@ific.uv.es and V. S. Varadarajan Department of Mathematics, UCLA. Los Angeles, CA, 90095-1555, USA e-mail: [email protected] Abstract We define complex Minkowski superspace in 4 dimensions as the big cell inside a complex flag supermanifold. The complex conformal supergroup acts naturally on this super flag, allowing us to interpret it arXiv:math/0609813v2 [math.RA] 14 Jun 2007 as the conformal compactification of complex Minkowski superspace. We then consider real Minkowski superspace as a suitable real form of the complex version. Our methods are group theoretic, based on the real conformal supergroup and its Lie superalgebra. 1Investigation supported by the University of Bologna, funds for selected research top- ics. 1 Contents 1 Introduction 3 2 The complex Minkowski space time and the Grassmannian G(2,4) 6 2.1 The Pl¨ucker embedding and the Klein quadric . 7 2.2 Therealform ........................... 10 3 Homogeneous spaces for Lie supergroups 11 3.1 The supermanifold structure on X = G/H ........... 12 3.2 The action of G on X ...................... 15 3.3 The functor of points of X = G/H ............... 16 4 The super Poincar´eand the translation superalgebras 17 4.1 Thetranslationsuperalgebra. -
Lectures on Supersymmetry and Superstrings 1 General Superalgebra
Lectures on supersymmetry and superstrings Thomas Mohaupt Abstract: These are informal notes on some mathematical aspects of su- persymmetry, based on two ‘Mathematics and Theoretical Physics Meetings’ in the Autumn Term 2009.1 First super vector spaces, Lie superalgebras and su- percommutative associative superalgebras are briefly introduced together with superfunctions and superspaces. After a review of the Poincar´eLie algebra we discuss Poincar´eLie superalgebras and introduce Minkowski superspaces. As a minimal example of a supersymmetric model we discuss the free scalar superfield in two-dimensional N = (1, 1) supersymmetry (this is more or less copied from [1]). We briefly discuss the concept of chiral supersymmetry in two dimensions. None of the material is original. We give references for further reading. Some ‘bonus material’ on (super-)conformal field theories, (super-)string theories and symmetric spaces is included. These are topics which will play a role in future meetings, or which came up briefly during discussions. 1 General superalgebra Definition: A super vector space V is a vector space with a decomposition V = V V 0 ⊕ 1 and a map (parity map) ˜ : (V V ) 0 Z · 0 ∪ 1 −{ } → 2 which assigns even or odd parity to every homogeneous element. Notation: a V a˜ =0 , ‘even’ , b V ˜b = 1 ‘odd’ . ∈ 0 → ∈ 1 → Definition: A Lie superalgebra g (also called super Lie algebra) is a super vector space g = g g 0 ⊕ 1 together with a bracket respecting the grading: [gi , gj] gi j ⊂ + (addition of index mod 2), which is required to be Z2 graded anti-symmetric: ˜ [a,b]= ( 1)a˜b[b,a] − − (multiplication of parity mod 2), and to satisfy a Z2 graded Jacobi identity: ˜ [a, [b,c]] = [[a,b],c] + ( 1)a˜b[b, [a,c]] . -
Relative Quantum Field Theory 3
RELATIVE QUANTUM FIELD THEORY DANIEL S. FREED AND CONSTANTIN TELEMAN Abstract. We highlight the general notion of a relative quantum field theory, which occurs in several contexts. One is in gauge theory based on a compact Lie algebra, rather than a compact Lie group. This is relevant to the maximal superconformal theory in six dimensions. 1. Introduction The (0, 2)-superconformal field theory in six dimensions, which we term Theory X for brevity, was discovered as a limit of superstring theories [W1, S]. It is thought not to have a lagrangian description, so is difficult to access directly, yet some expectations can be deduced from the string theory description [W2, GMN]. Two features are particularly relevant: (i) it is not an ordinary quantum field theory, and (ii) the theory depends on a Lie algebra, not on a Lie group. A puzzle, emphasized by Greg Moore, is that the dimensional reduction of Theory X to five dimensions is usually understood to be an ordinary quantum field theory—contrary to (i)—and it is a supersym- metric gauge theory so depends on a particular choice of Lie group—contrary to (ii). In this paper we spell out the modified notion indicated in (i), which we call a relative quantum field theory, and use it to resolve this puzzle about Theory X by pointing out that the dimensional reduction is also a relative theory. Relative gauge theories are not particular to dimension five. In fact, the possibility of studying four-dimensional gauge theory as a relative theory was exploited in [VW] and [W3]. -
Breakthrough Prize in Mathematics Awarded to Terry Tao
156 Breakthrough Prize in Mathematics awarded to Terry Tao Our congratulations to Australian Mathematician Terry Tao, one of five inaugu- ral winners of the Breakthrough Prizes in Mathematics, announced on 23 June. Terry is based at the University of California, Los Angeles, and has been awarded the prize for numerous breakthrough contributions to harmonic analysis, combi- natorics, partial differential equations and analytic number theory. The Breakthrough Prize in Mathematics was launched by Mark Zuckerberg and Yuri Milner at the Breakthrough Prize ceremony in December 2013. The other winners are Simon Donaldson, Maxim Kontsevich, Jacob Lurie and Richard Tay- lor. All five recipients of the Prize have agreed to serve on the Selection Committee, responsible for choosing subsequent winners from a pool of candidates nominated in an online process which is open to the public. From 2015 onwards, one Break- through Prize in Mathematics will be awarded every year. The Breakthrough Prizes honor important, primarily recent, achievements in the categories of Fundamental Physics, Life Sciences and Mathematics. The prizes were founded by Sergey Brin and Anne Wojcicki, Mark Zuckerberg and Priscilla Chan, and Yuri and Julia Milner, and aim to celebrate scientists and generate excitement about the pursuit of science as a career. Laureates will receive their trophies and $3 million each in prize money at a televised award ceremony in November, designed to celebrate their achievements and inspire the next genera- tion of scientists. As part of the ceremony schedule, they also engage in a program of lectures and discussions. See https://breakthroughprize.org and http://www.nytimes.com/2014/06/23/us/ the-multimillion-dollar-minds-of-5-mathematical-masters.html? r=1 for further in- formation.. -
NEWSLETTER No
NEWSLETTER No. 458 May 2016 NEXT DIRECTOR OF THE ISAAC NEWTON INSTITUTE In October 2016 David Abrahams will succeed John Toland as Director of the Isaac Newton Institute for Mathematical Sciences and NM Rothschild and Sons Professor of Mathematics in Cambridge. David, who is a Royal Society Wolfson Research Merit Award holder, has been Beyer Professor of Applied Mathematics at the University of Man- chester since 1998. From 2014-16 he was Scientific Director of the International Centre for Math- ematical Sciences in Edinburgh and was President of the Institute of Mathematics and its Applica- tions from 2007-2009. David’s research has been in the broad area of applied mathematics, mainly focused on the theoretical understanding of wave processes including scattering, diffraction, localisation and homogenisation. In recent years his research has broadened somewhat, to now cover topics as diverse as mathematical finance, nonlinear vis- He has also been involved in a range of public coelasticity and glaciology. He has close links with engagement activities over the years. He a number of industrial partners. regularly offers mathematics talks of interest David plays an active role within the internation- to school students and the general public, al mathematics community, having served on over and ran the annual Meet the Mathematicians 30 national and international working parties, outreach events for sixth form students with panels and committees over the past decade. Chris Howls (Southampton). With Chris Budd This has included as a Member of the Applied (Bath) he has organised a training conference Mathematics sub-panel for the 2008 Research As- in 2010 on How to Talk Maths in Public, and in sessment Exercise and Deputy Chair for the Math- 2014 co-chaired the inaugural Festival of Math- ematics sub-panel in the 2014 Research Excellence ematics and its Applications. -
M-Theory from the Superpoint
M-Theory from the Superpoint John Huerta∗, Urs Schreibery March 21, 2017 Abstract The \brane scan" classifies consistent Green{Schwarz strings and membranes in terms of the invariant cocycles on super-Minkowski spacetimes. The \brane bouquet" generalizes this by consecutively forming the invariant higher central extensions induced by these cocycles, which yields the complete brane content of string/M-theory, including the D-branes and the M5- brane, as well as the various duality relations between these. This raises the question whether the super-Minkowski spacetimes themselves arise as maximal invariant central extensions. Here we prove that they do. Starting from the simplest possible super-Minkowski spacetime, the superpoint, which has no Lorentz structure and no spinorial structure, we give a systematic process of consecutive maximal invariant central extensions, and show that it discovers the super- Minkowski spacetimes that contain superstrings, culminating in the 10- and 11-dimensional super-Minkowski spacetimes of string/M-theory and leading directly to the brane bouquet. Contents 1 Introduction 2 2 Automorphisms of super-Minkowski spacetimes9 3 The consecutive maximal invariant central extensions of the superpoint 12 4 Outlook 17 A Background 17 A.1 Super Lie algebra cohomology............................... 17 A.2 Super Minkowski spacetimes................................ 20 ∗CAMGSD, Instituto Superior T´ecnico,Av. Ravisco Pais, 1049-001 Lisboa, Portugal yMathematics Institute of the Academy, Zitnaˇ 25, 115 67 Praha 1, Czech Republic, on leave at Bonn 1 1 Introduction In his \vision talk" at the annual string theory conference in 2014, Greg Moore highlighted the following open question in string theory [41, section 9]: Perhaps we need to understand the nature of time itself better. -
On The\'Etale Homotopy Type of Higher Stacks
ON THE ETALE´ HOMOTOPY TYPE OF HIGHER STACKS DAVID CARCHEDI Abstract. A new approach to ´etale homotopy theory is presented which applies to a much broader class of objects than previously existing approaches, namely it applies not only to all schemes (without any local Noetherian hypothesis), but also to arbitrary higher stacks on the ´etale site of such schemes, and in particular to all algebraic stacks. This approach also produces a more refined invariant, namely a pro-object in the infinity category of spaces, rather than in the homotopy category. We prove a profinite comparison theorem at this level of generality, which states that if X is an arbitrary higher stack on the ´etale site of affine schemes of finite type over C, then the ´etale homotopy type of X agrees with the homotopy type of the underlying stack Xtop on the topological site, after profinite completion. In particular, if X is an Artin stack locally of finite type over C, our definition of the ´etale homotopy type of X agrees up to profinite completion with the homotopy type of the underlying topological stack Xtop of X in the sense of Noohi [30]. In order to prove our comparison theorem, we provide a modern reformulation of the theory of local systems and their cohomology using the language of -categories which we believe to be of independent interest. ∞ 1. Introduction Given a complex variety V, one can associate topological invariants to this variety by computing invariants of its underlying topological space Van, equipped with the complex analytic topology. However, for a variety over an arbitrary base ring, there is no good notion of underlying topological space which plays the same role.