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This preprint presents a rigorous theoretical analysis of the spin-boson model's critical dynamics using Schwinger--Keldysh techniques and Majorana spinors. The study identifies specific fixed points governing transitions between delocalized and localized states, offering new insights into quantum phase boundaries relevant to decoherence in open systems. While foundational for condensed matter physics, these results are primarily of interest to researchers developing error-corrected qubits rather than immediate applications in general AI or classical computing infrastructure.
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Critical Dynamics of Spin Boson Model

arXiv2 min read

arXiv:2501.12457v3 Announce Type: replace-cross Abstract: In this work, we study the low-energy properties of the spin-boson model (SBM), which describes the dynamics of a spin-1/2 coupled to a bosonic environment characterized by a power-law spectral density $f(\omega)\propto \omega^s$. The theoretical description is based on the Schwinger--Keldysh technique combined with a Majorana spinor representation of the spin. This approach enables a renormalization group analysis of the model's critical dynamics without relying on quantum-classical mapping. We show that the transition from a delocalized to a localized state arises due to a Wilson--Fisher fixed point in both the ohmic ($s=1$) and sub-ohmic ($s<1$) cases. Our analysis recovers key results of Leggett's theory and identifies $s=1/2$ as the upper critical dimension, marking the boundary where critical exponents become mean-field. The findings are in good agreement with the predictions of quantum-classical mapping and state-of-the-art numerical data.

Abstract:In this work, we study the low-energy properties of the spin-boson model (SBM), which describes the dynamics of a spin-1/2 coupled to a bosonic environment characterized by a power-law spectral density $f(\omega)\propto \omega^s$. The theoretical description is based on the Schwinger--Keldysh technique combined with a Majorana spinor representation of the spin. This approach enables a renormalization group analysis of the model's critical dynamics without relying on quantum-classical mapping. We show that the transition from a delocalized to a localized state arises due to a Wilson--Fisher fixed point in both the ohmic ($s=1$) and sub-ohmic ($s<1$) cases. Our analysis recovers key results of Leggett's theory and identifies $s=1/2$ as the upper critical dimension, marking the boundary where critical exponents become mean-field. The findings are in good agreement with the predictions of quantum-classical mapping and state-of-the-art numerical data.

Statistical Mechanics (cond-mat.stat-mech); Quantum Physics (quant-ph)

arXiv:2501.12457 [cond-mat.stat-mech]

(or arXiv:2501.12457v3 [cond-mat.stat-mech] for this version)

Full text under the publisher's open licence · 150 words

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