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| Format: | Preprint |
| Published: |
2022
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| Subjects: | |
| Online Access: | https://arxiv.org/abs/2211.00333 |
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Table of Contents:
- We present a microscopic derivation from a nonequilibrium spin-boson model to a $\PT$-symmetric non-Hermitian sine-Gordon (SG) effective theory, via the Keldysh functional-integral formalism, a Lang-Firsov polaron transformation, bosonization, and a Grassmann coherent-state spin trace.The spin trace yields the generic reduced vertex $g_r\cos(λΦ_1)+ig_i\sin(λΦ_1)$, where the imaginary part originates from the nonequilibrium Keldysh distribution asymmetry $δn(ω)=n_+(ω)-n_-(ω)$. We provide an explicit dictionary between the spin-boson microscopic parameters and the NH-SG couplings: $K=v_f/\tilde{J}_\parallel^2$ (Luttinger parameter from $J_\parallel$), $g_r\propto J_\perp^2/Γ$ (from the transverse coupling and impurity width), and $\mathcal{I}=g_i/g_r\proptoμ/v_f$ (bias ratio, an exact RG invariant).One-loop Wilson momentum-shell RG on the NH-SG action gives the closed equations $\diff K/\diff l=-g_r^2(1-\mathcal{I}^2)K^2$ and $\diff g_r/\diff l=(2-K)g_r$, identical to those of Ashida \textit{et al.}\ for the $\PT$-symmetric SG; the present work supplies the microscopic initial conditions from the spin-boson Keldysh reduction. The BKT separatrix $K=2$ (Toulouse line), the EP fixed manifold $\mathcal{I}=1$ ($μ=μ_c$), and the mass gap $m\simΛe^{-c/\sqrt{K_0-2}}$ all follow from this closed system.In the non-relativistic soliton sector near the EP, the effective coupling $\tilde{g}=g_r\sqrt{1-\mathcal{I}^2}$ reduces the S-matrix to the Lieb-Liniger rational form and the Bethe ansatz becomes exact for that auxiliary gas.Within this sector we derive $n$-string bound states with$E_n^{\rm bind}=-n(n^2-1)\tilde{g}^2/12$, identify the EP as the many-body bound-state threshold, and construct the Jordan-partner state from the $ε$-regularised dimer.