Matrix Models and Superintegrability: Deformations and Integrals

superintegrability w operators and matrix n.w
1 / 11
Embed
Share

Explore the concepts of superintegrability, W-operators, and matrix integrals in mathematical physics through deformations and generalizations. Learn about matrix models, Hermitian Gaussian model, W-representations, and more. Discover the significance of deformation of integration space, combining W-operators, and partition functions in this insightful study.

  • Matrix Models
  • Superintegrability
  • Deformations
  • Integrals
  • Mathematical Physics

Uploaded on | 1 Views


Download Presentation

Please find below an Image/Link to download the presentation.

The content on the website is provided AS IS for your information and personal use only. It may not be sold, licensed, or shared on other websites without obtaining consent from the author. If you encounter any issues during the download, it is possible that the publisher has removed the file from their server.

You are allowed to download the files provided on this website for personal or commercial use, subject to the condition that they are used lawfully. All files are the property of their respective owners.

The content on the website is provided AS IS for your information and personal use only. It may not be sold, licensed, or shared on other websites without obtaining consent from the author.

E N D

Presentation Transcript


  1. SUPERINTEGRABILITY, W-OPERATORS AND MATRIX INTEGRALS THREE SIDES OF A COIN THROUGH THE DEFORMATIONS A.A. Oreshina ITEP, MIPT Problems of the Modern Mathematical Physics February, 2024

  2. Plan Short review on matrix models Simple example: Hermitian Gaussian model Deformations and generalizations Central object of report: -WLZZ Helpful functions: Izikson-Zuber integral and Dunkle operator The main result: -WLZZ integral representation

  3. Matrix models Matrix models special kind of matrix integrals ? = ?? ??? ?(?) Historically, they arose in the statistical physics and have found further application in string theory, combinatory, topological gravity. Three types of representation: Integral W-representation Polynomial representation (superintegrability)

  4. Simple example: Hermitian Gaussian model ? = ?????[ 1 2?? ?2+ ??????] Integral representation ? 1 2 ? = ??? 2(?)? ?? ?? 2 ?? ? ? 1 2 ?+1 2(?)? ?? ?? 2 ?? 0 = ??? ?? ??? ? 1 2 ?) 2(?)? ?? ?? 2 ?? 0 = ??? ?( ?? ? ?= ? ?? ?? ?? ? ?? ?? ?? ??? ? 1 ?2 2= ??? = 0 ? ? ???+2) ??? 2(?)? ?? ?? 2 ?? ( ? ?? ???+?+ ?????? ? ???? 2? = ?0 ?2? = 0 ? = ??2 1 W-representation

  5. Hermitian Gaussian model ?2SRpk = ??,? ?? (??) ? =?+ + 1 ?!(?2)?? pk ? = ??2 1 = ? ?(??) = ??????,2??(??) = ????(??) ? ? Superintegrability: ??? ????,1 ????,2 = ?? ??? ????,1 ??= = (? ? + ?) (?,?) ?

  6. Deformations and generalizations 1) Deformation of integration space: ? 1 2 -deformation: ? = ??? 2?(?)? ?? ?? ( =1, , 2 for hermitian, orthogonal and simplectic models) q,t-deformation 2 ?? 2) Combining different W-operators (and respective models) to a class of models (WLZZ class) Object of our interest -WLZZ class

  7. -WLZZ ??= ? ??/? 1, ?0= ??0 ???1 ??= ???/? ? ????, ? < 0 Partition function of positive, negative and zero branches: ? > 0 ?2= [?0,[?0,?1]] 1 ?![?2,? ?],? 2 Negative branch ? ? 1= ?2 ? +(1 ?) ? Zero branch ?0= ? (? + ?)???? + ? ? ??+? ? ? 1 ?? ???+? ?????? 2 ??? ? ?2= [?0,[?0, ??1]] Positive branch ??+1= 1 ?![?2,??],? 2

  8. Auxillary objects Izikson-Zuber integral original definition angular matrix integral ?(?,?) = ?? exp[???+?] Harish-Chandra form: ? 1 ? ?,? =detexp[????] ?! (?) (?) ?=1 IZ integral as eigenfunction of Calogero-Mozer hamiltonian ? ??? Polynomial form: 2 1 (? ??? ? 2???,? ??????,? = ( + 2? ???))???,? = ?? ?? ?? ? ?<? ??(??,1) ??(?) ??? ??(?) ||??||2 1??? ??(?) ???,? = ? 1 = ?? ? ? Dunkle operator 1 ??,? ?? ?? ??= ??+ ? ? ?

  9. -WLZZ integral representation Motivation: Ambiguity in the defining W-representation Integral representation lets study dividing into phases, that appears in the Kontsevich model and Brezin-Gross-Witten model Convenient for making further generalizations and deformations, that could bound the model with other knowing models. For this purpose in the integral representation one could add a potential or change the integrating space Virasoro constraints can not be restored from the W- representation, but there are some methods that produced it from the integral representation Some symmetries could be found only in the integral representation

  10. -WLZZ integral representation ????,??, = ??? ??? 2 x 2 y exp ?? ?+ ?? ?? ?,? ? (?, ) ? ?? ? ?? Sketch of proof: Starting with =0. Notice, that for ? ? = ??? 2 x exp ?? ?+??+1 ? + 1 ?? ?+1? ?,? ? ?? ?+??)? ? = 0 for all j ??? 2 y exp ?? It is true that (?? ? ?? ?(?? ?+??)? ? = 0 ? ?? Leads to the Virasoro equation ?? (?)? = ?? ?+1 ???+1 (?)reproduces partition function of -WLZZ And the operator ?? ?+1

  11. -WLZZ integral representation Use polynomial representation of the partition function ? = ??? ??? 2 x 2 y exp ?? ?+ ?? ?? ?,? ? ?? ? ?? ??? ????,1 = ??(??)??(??) ? Orthogonallity relation: ???? = ??,? |R| ????,??, = ??? ??? 2 x 2 y exp ?? ?+ ?? ?? ?,? ? ?, = ? ?? ? ?? ??? ????,1 ??? ????,1 ????,1 ??? = ??? ??? 2 x 2 y ? ?,? ??(??)??(?) ??(?)??(??) ?? ??? = ? ? ? ????,1 ??? ??? ????,1 ?|?| = ?,? ??????/????? ????,1 ??? ??? ????,1 ?|?|= ????,??, = ??????/????? ?,? = ??? ??? 2 x 2 y exp ?? ?+ ?? ?? ?,? ? (?, ) ? ?? ? ??

Related


More Related Content