Classical and Quantum Dynamics pp 295-300 | Cite as
Maslov Anomaly and the Morse Index Theorem
Chapter
Abstract
Our starting point is again the phase space integral with periodic boundary conditions X (0) = X (T) and
$$ {e^{{\rm{i}}\mathord{\buildrel{\lower3pt\hbox{$\scriptscriptstyle\frown$}}\over \Gamma } \left[ {\tilde M} \right]}} = \int {{D_{{X^a}}}{e^{iSn\left[ {x,\tilde M} \right]}}} $$
(27.1)
$$ {S_{{\rm{fl}}}}\left[ {x,\tilde M} \right] = {1 \over 2}\int_0^T {dt{{\bar x}_a}\left( t \right){{\left[ {{\partial \over {\partial t}} - \tilde M\left( t \right)} \right]}^a}_b{x^b}\left( t \right)} . $$
(27.2)
Preview
Unable to display preview. Download preview PDF.
Copyright information
© Springer-Verlag Berlin Heidelberg 1994