Abstract
It is demonstrated that all known results for the conformation properties of semiflexible polymers can be exactly reproduced with the help of the Euclidean version of Dirac's propagator. The obtained single chain results are further generalized to the case on monodisperse solutions of semiflexible polymers. Flory's results for this case are reproduced exactly at the mean field saddle point level approximation to the functional integral which is a direct extension of the one proposed earlier for the fully flexible chains.
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