Dynamical spin structure factor of one-dimensional interacting fermions

We revisit the dynamic spin susceptibility, $χ(q,ω)$, of one-dimensional interacting fermions. To second order in the interaction, backscattering results in a logarithmic correction to $χ(q,ω)$ at $q\ll k_F$, even if the single-particle spectrum is linearized near the Fermi points. Consequently, the dynamic spin structure factor, $\mathrm{Im}χ(q,ω)$, is non-zero at frequencies above the single-particle continuum. In the boson language, this effect results from the marginally irrelevant backscattering operator of the sine-Gordon model. Away from the threshold, the high-frequency tail of $\mathrm{Im}χ(q,ω)$ due to backscattering is larger than that due to finite mass by a factor of $k_F/q$. We derive the renormalization group equations for the coupling constants of the $g$-ology model at finite $ω$ and $q$ and find the corresponding expression for $χ(q,ω)$, valid to all orders in the interaction but not in the immediate vicinity of the continuum boundary, where the finite-mass effects become dominant.

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