Two-Dimensional-Gauge-Theoriesand-Quantum-Integrable-Sys:两维规范理论量子可积系统课件.ppt
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1、,Two Dimensional Gauge Theoriesand Quantum Integrable Systems,Nikita Nekrasov IHESImperial College April 10,2008,Based on,NN,S.Shatashvili,to appearPrior work:E.Witten,1992;A.Gorsky,NN;J.Minahan,A.Polychronakos;M.Douglas;1993-1994;A.Gerasimov 1993;G.Moore,NN,S.Shatashvili 1997-1998;A.Losev,NN,S.Shat
2、ashvili 1997-1998;A.Gerasimov,S.Shatashvili 2006-2007,We are going to relate 2,3,and 4 dimensional susy gauge theorieswith four supersymmetries N=1 d=4,And quantum integrable systemssoluble by Bethe Ansatz techniques.,Mathematically speaking,the cohomology,K-theory and elliptic cohomology of various
3、 gauge theory moduli spaces,like moduli of flat connections and instantons,And quantum integrable systemssoluble by Bethe Ansatz techniques.,For example,we shall relate the XXX Heisenberg magnet and 2d N=2 SYM theory with some matter,(pre-)History,In 1992 E.Witten studied two dimensional Yang-Mills
4、theory with the goal to understand the relation between the physical and topological gravities in 2d.,(pre-)History,There are two interesting kinds of Two dimensional Yang-Mills theories,Yang-Mills theories in 2d,(1)Cohomological YM=twisted N=2 super-Yang-Mills theory,with gauge group G,whose BPS(or
5、 TFT)sector is related to the intersection theory on the moduli space MG of flat G-connections on a Riemann surface,Yang-Mills theories in 2d,N=2 super-Yang-Mills theory,Field content:,Yang-Mills theories in 2d,(2)Physical YM=N=0 Yang-Mills theory,with gauge group G;The moduli space MG of flat G-con
6、nections=minima of the action;The theory is exactly soluble(A.Migdal)with the help of the Polyakov lattice YM action,Yang-Mills theories in 2d,Physical YM,Field content:,Yang-Mills theories in 2d,Witten found a way to map the BPS sector of the N=2 theory to the N=0 theory.The result is:,Yang-Mills t
7、heories in 2d,Two dimensional Yang-Mills partition function is given by the explicit sum,Yang-Mills theories in 2d,In the limit the partition function computes the volume of MG,Yang-Mills theories in 2d,Wittens approach:add twisted superpotential and its conjugate,Yang-Mills theories in 2d,Take a li
8、mit,In the limit the fields are infinitely massive and can be integrated out:one is left with the field content of the physical YM theory,Yang-Mills theories in 2d,Both physical and cohomological Yang-Millstheories define topological field theories(TFT),Yang-Mills theories in 2d,Both physical and co
9、homological Yang-Millstheories define topological field theories(TFT),Vacuum states+deformations=quantum mechanics,YM in 2d and particles on a circle,Physical YM is explicitly equivalent to a quantum mechanical model:free fermions on a circle,Can be checked by a partition function on a two-torus,Gro
10、ssDouglas,YM in 2d and particles on a circle,Physical YM is explicitly equivalent to a quantum mechanical model:free fermions on a circle,States are labelled by the partitions,for G=U(N),YM in 2d and particles on a circle,For N=2 YM these free fermions on a circle,Label the vacua of the theory defor
11、med by twisted superpotential W,YM in 2d and particles on a circle,The fermions can be made interacting by adding a localized matter:for example a time-like Wilson loopin some representation V of the gauge group:,YM in 2d and particles on a circle,One gets Calogero-Sutherland(spin)particles on a cir
12、cle(1993-94)A.Gorsky,NN;J.Minahan,A.Polychronakos;,History,In 1997 G.Moore,NN and S.Shatashvili studied integrals over various hyperkahler quotients,with the aim to understand instanton integrals in four dimensional gauge theories,History,In 1997 G.Moore,NN and S.Shatashvili studied integrals over v
13、arious hyperkahler quotients,with the aim to understand instanton integrals in four dimensional gauge theoriesThis eventually led to the derivation in 2002 of the Seiberg-Witten solution of N=2 d=4 theory,Inspired by the work of H.Nakajima,Yang-Mills-Higgs theory,Among various examples,MNS studied H
14、itchins moduli space MH,Yang-Mills-Higgs theory,Unlike the case of two-dimensionalYang-Mills theory where the moduli space MG is compact,Hitchins moduli space is non-compact(it is roughly T*MG modulo subtleties)and the volume is infinite.,Yang-Mills-Higgs theory,In order to cure this infnity in a re
15、asonable way MNS used the U(1)symmetry of MH,The volume becomes a DH-type expression:,Where H is the Hamiltonian,Yang-Mills-Higgs theory,Using the supersymmetry and localization the regularized volume of MH was computed with the result,Yang-Mills-Higgs theory,Where the eigenvalues solve the equation
16、s:,YMH and NLS,The experts would immediately recognise theBethe ansatz(BA)equations for the non-linear Schroedinger theory(NLS),NLS=large spin limit of the SU(2)XXX spin chain,YMH and NLS,Moreover the NLS Hamiltoniansare the 0-observables of the theory,like,The VEV of the observable=The eigenvalue o
17、f the Hamiltonian,YMH and NLS,Since 1997 nothing came out of this result.It could have been simply a coincidence.,In 2006 A.Gerasimov and S.Shatashvili have revived the subject,History,YMH and interacting particles,GS noticed that YMH theory viewed as TFT is equivalent to the quantum Yang system:N p
18、articles on a circle with delta-interaction:,YMH and interacting particles,Thus:YM with the matter-fermions with pair-wise interaction,History,More importantly,GS suggested that TFT/QIS equivalence is much more universal,Today,We shall rederive the result of MNS from a modern perspectiveGeneralize t
19、o cover virtually all BA soluble systems both with finite and infinite spinSuggest natural extensions of the BA equations,Hitchin equations,Solutions can be viewed as the susy field configurations for the N=2 gauged linear sigma model,For adjoint-valued linear fields,Hitchin equations,The moduli spa
20、ce MH of solutions is a hyperkahler manifoldThe integrals over MH are computed by the correlation functions of an N=2 d=2 susy gauge theory,Hitchin equations,The kahler form on MH comes fromtwisted tree level superpotentialThe epsilon-term comes from a twisted mass of the matter multiplet,Generaliza
21、tion,Take an N=2 d=2 gauge theory with matter,In some representation R of the gauge group G,Generalization,Integrate out the matter fields,compute the effective(twisted)super-potentialon the Coulomb branch,Mathematically speaking,Consider the moduli space MR of R-Higgs pairswith gauge group G,Up to
22、the action of the complexified gauge group GC,Mathematically speaking,Stability conditions:,Up to the action of the compact gauge group G,Mathematically speaking,Pushforward the unit class down to the moduli space MG of GC-bundlesEquivariantly with respect to the actionof the global symmetry group K
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