Fixed point annihilation for a spin in a fluctuating field
arXiv:2202.08431 · doi:10.1103/PhysRevB.106.L081109
Abstract
A quantum spin impurity coupled to a critical free field (the Bose-Kondo model) can be represented as a 0+1D field theory with long-range-in-time interactions that decay as . This theory is a simpler analogue of nonlinear sigma models with topological Wess-Zumino-Witten terms in higher dimensions. In this note we show that the RG flows for the impurity problem exhibit an annihilation between two nontrivial RG fixed points at a critical value of the interaction exponent. The calculation is controlled at large spin . This clarifies the phase diagram of the Bose-Kondo model and shows that it serves as a toy model for phenomena involving fixed-point annihilation and "quasiuniversality" in higher dimensions.
4 pages, 1 figure
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- Reclaiming the Lost Conformality in a non-Hermitian Quantum 5-state Potts Model
- SU(2)-Symmetric Spin-Boson Model: Quantum Criticality, Fixed-Point Annihilation, and Duality
- Complex entanglement entropy for complex conformal field theory
- Critical phase induced by Berry phase and dissipation in a spin chain
- The Aubry-Andre Anderson model: Magnetic impurities coupled to a fractal spectrum
- Persistent Corner Spin Mode at the Quantum Critical Point of a Plaquette Heisenberg Model
- Continuous order-to-order quantum phase transitions from fixed-point annihilation
- Tunable phase transition in a dissipative two-spin system: A renormalization group study
- Tunable quantum criticality and pseudocriticality across the fixed-point annihilation in the anisotropic spin-boson model