Abstract
A spin-fermion model relevant for the description of cuprates ladders is studied in a path integral formalism, where, after integrating out the fermions, an effective action for the spins in term of a Fermi-determinant results. The determinant can be evaluated in the long-wavelength, low-frequency limit to all orders in the coupling constant, leading to a non-linear $\ensuremath{\sigma}$ model with doping dependent coupling constants. An explicit evaluation shows that the magnon gap diminishes upon doping, as opposed to previous mean-field treatments.
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