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We then intro- duce the effective single-particle Hamiltonian near the QPT atε= 0 and use it to construct the many-body Hamiltonian

Effective Hamiltonian close to the QPT Since an ISC generally breaks spin-rotation invariance forB x ̸= 0, we introduce ˆUYSR = exp(−iγn· ˆσ/2) with n=g×z/|g×z|, wheregdenotes the

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Yu-Shiba-Rusinov States in Ising Superconductors

cond-mat.supr-con · 2026-05-12 · unverdicted · novelty 5.0

Magnetic impurities produce distinct spectral features in Yu-Shiba-Rusinov states that encode and differentiate Ising superconductivity from conventional pairing.

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  • Yu-Shiba-Rusinov States in Ising Superconductors cond-mat.supr-con · 2026-05-12 · unverdicted · none · ref 7

    Magnetic impurities produce distinct spectral features in Yu-Shiba-Rusinov states that encode and differentiate Ising superconductivity from conventional pairing.