Abstract
The global phase structure for heterotic string theory is studied. Three different types of representations for thermo-partition functions are provided. We show how modular invariance arises and analyze finite-temperature divergences. A three-phase structure, involving a new nonperturbative high-temperature phase, for the heterotic string is found. The transition into this new phase takes place at \ensuremath{\beta}=\ensuremath{\pi}/${\ensuremath{\beta}}_{h}$T, where ${\ensuremath{\beta}}_{h}$ is the conventional ``Hagedorn temperature'' for the heterotic string.
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