A BOSONIC OPERATOR REALIZATION OF THE KRICHEVER CONSTRUCTION AND bc SYSTEMS ON RIEMANN SURFACES

1988 ◽  
Vol 03 (17) ◽  
pp. 1689-1697 ◽  
Author(s):  
A.M. SEMIKHATOV

We propose an explicit operator construction for the algebro-geometric τ-function in terms of a bosonic conformal field theory on Riemann surfaces. As a consequence, the operator Bosonization formulae for fermionic bc systems on Riemann surfaces are deduced.

2001 ◽  
Vol 16 (05) ◽  
pp. 822-855 ◽  
Author(s):  
JUAN MALDACENA ◽  
CARLOS NUÑEZ

In the first part of this paper we find supergravity solutions corresponding to branes on worldvolumes of the form Rd×Σ where Σ is a Riemann surface. These theories arise when we wrap branes on holomorphic Riemann surfaces inside K3 or CY manifolds. In some cases the theory at low energies is a conformal field theory with two less dimensions. We find some non-singular supersymmetric compactifications of M-theory down to AdS5. We also propose a criterion for permissible singularities in supergravity solutions. In the second part of this paper, which can be read independently of the first, we show that there are no non-singular Randall-Sundrum or de-Sitter compactifications for large class of gravity theories.


1998 ◽  
Vol 13 (35) ◽  
pp. 2863-2871 ◽  
Author(s):  
VINCENZO MAROTTA ◽  
ANTONINO SCIARRINO

We consider a class of conformal field theories on Riemann surfaces represented as a Zk invariant covering of the sphere. The introduction of exchange interactions among couples of sheets generate effective parafermions. The outgoing theory can be seen as a fractional supersymmetry conformal field theory.


1989 ◽  
Vol 04 (17) ◽  
pp. 4437-4447
Author(s):  
NOUREDDINE CHAIR

The instanton sum in the partition function for D bosons on a Riemann surface of genus g, with values in a general D-dimensional torus, TD = RD/ΛD is given explicitly. When the rational metric Q of the lattice, ΛD, is the identity we get the bosonization formula of Alvarez-Gaumé et al. for SO( 2D ). If Q is orthogonal, in the bosonization formula, we get the theta function associated with the quadratic form Q, if Q is generic we get rational Conformal Field Theory. Also we look for conditions on a twisted spin bundle LE, which may ensure that our partition functions arise from some generalized bosonization formulas.


1988 ◽  
Vol 116 (2) ◽  
pp. 247-308 ◽  
Author(s):  
Noboru Kawamoto ◽  
Yukihiko Namikawa ◽  
Akihiro Tsuchiya ◽  
Yasuhiko Yamada

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