Path integral and moduli space of Riemann surfaces

introduction

\(Z=\sum_{g=0}^{\infty} g_{s}^{-\chi(\Sigma_{g})}Z_{g}=\sum_{g=0}^{\infty} g_{s}^{2g-2}Z_{g}=\frac{1}{g_{s}^2}Z_{0}+g_{s}^{0}Z_{1}+g_{s}^2Z_{2}+\cdots\)

classical

\(\frac{1}{g_{s}^2}Z_{0}\)

other terms : loop (=quantum ) corrections

 

 

 

Scattering amplitude

\(Z(V_1,\cdots, V_{s},V_{s+1},\cdots, V_{s+p})=\sum_{g=0}^{\infty} g_{s}^{-\chi(\Sigma_{g})}Z_{g}(V_1,\cdots, V_{s},V_{s+1},\cdots, V_{s+p})\)

 

Polchinski I,5

 

 

 

related items

• Moduli spaces of Riemann surfaces
• 0 modular invariance in math and physics