1994
DOI: 10.1002/cpa.3160470403
|View full text |Cite
|
Sign up to set email alerts
|

The τ‐function of the universal whitham hierarchy, matrix models and topological field theories

Abstract: The universal Whitham hierarchy is considered from the viewpoint of topological field theories. The r-function is defined for this hierarchy. It is proved that the algebraic orbits of Whitham hierarchy can be identified with various topological matter models coupled with topological gravity.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
500
0
51

Year Published

1995
1995
2016
2016

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 399 publications
(553 citation statements)
references
References 36 publications
2
500
0
51
Order By: Relevance
“…We thus recover the well known result: the two-points function is equal to the Bergmann kernel on the Riemann surface corresponding to the algebraic equation E(x, y) = 0 (cf [5,20,27,30] (y(r) − y(q))U 1 (q, y(r); p 1 ) dx(q) = − W 2 (q; p 1 )U 0 (q, y(r)) dx(q) 2 − P 1 (x(q), y(r); p 1 ) +d p 1 U 0 (p 1 , y(r)) (x(q) − x(p 1 )) dx(p 1 ) (B.7)…”
Section: Riemann Bilinear Identitysupporting
confidence: 81%
See 1 more Smart Citation
“…We thus recover the well known result: the two-points function is equal to the Bergmann kernel on the Riemann surface corresponding to the algebraic equation E(x, y) = 0 (cf [5,20,27,30] (y(r) − y(q))U 1 (q, y(r); p 1 ) dx(q) = − W 2 (q; p 1 )U 0 (q, y(r)) dx(q) 2 − P 1 (x(q), y(r); p 1 ) +d p 1 U 0 (p 1 , y(r)) (x(q) − x(p 1 )) dx(p 1 ) (B.7)…”
Section: Riemann Bilinear Identitysupporting
confidence: 81%
“…, x k ) are obtained by derivation of w 1 with respect to the potential In what follows, we assume that the leading resolvent, i.e. the function Y (x) is known, and we refer the reader to the existing literature on that topic, for instance [5,20,27,30].…”
Section: Fixed Filling Fractionsmentioning
confidence: 99%
“…In the A 1 case, for example, the qq-character modifies to In this way we get the realization of the W -algebra and its qq-deformation in gauge theory. We also get a new perspective on the rôle of Whitham hierarchies [46,63] and their quantum and qq-deformations in gauge theory. See also [13] for more applications of qq-characters in the U(1) case.…”
Section: Jhep03(2016)181mentioning
confidence: 98%
“…(The at coordinates t 1 , ..., t n can be expressed via Casimirs of the original Poisson bracket and action variables and wave n umbers along the invariant tori -see details in [53,54].) To de ne a tensor c (t) o n M (or, equivalently, the \primary free energy" F(t)) we need to use a semiclassical limit of the -function of the original hierarchy [87,88,44,45,133]. For the dispersionless limit the de nition of the semiclassical -function reads log semiclassical (T 0 ; T 1 ; : : : ) = lim !0 2 log ( t 0 ; t 1 ; : : : ) : (6:20) Then F = log semiclassical (6:21) for a particular -function of the hierarchy.…”
Section: Appendix Hmentioning
confidence: 99%