Abstract:A simplification of the symmetric single‐impurity Kondo model is introduced and studied. In the Ising–Kondo model, host electrons scatter off a single magnetic impurity at the origin whose spin orientation is dynamically conserved. This reduces the problem to potential scattering of spinless fermions that can be solved exactly using the equation‐of‐motion technique. The Ising–Kondo model provides an example for static screening. At low temperatures, the thermodynamics at finite magnetic fields resembles that o… Show more
“…Note that V z 2 is the second-order Ising-Kondo contribution to the single-impurity Kondo model, see [13]. In section SM I of the supplemental material, we explicitly calculate the exact result of the free energy of the Ising-Kondo model for a constant density of states, see equation (13). In this way, we can compare the results from perturbation theory of appendix A with those from the Taylor series of the exact result.…”
Section: J Stat Mech (2024) 043102mentioning
confidence: 99%
“…To make progress, we define Following Bauerbach et al [13], we derive the free energy of the Ising-Kondo model for a constant density of states using the equation-of-motion method. Since we have explicitly performed the second-order perturbation theory for the Ising-Kondo model, see appendix A.1, we can directly compare the Taylor series of the exact result with perturbation theory.…”
Section: B62 Numerical Check For X Amentioning
confidence: 99%
“…(2024) 043102 variational wave functions, and numerical approaches such as the density-matrix renormalization group (DMRG) and the NRG methods. Also in the year 2020, Bauerbach et al [13] introduced a simplification of the Kondo model, the so-called Ising-Kondo model, in which the spin-exchange term of the full Kondo Hamiltonian is neglected. Thereby, the complexity of the Kondo model is reduced to that of potential scattering of spinless fermions, which can be solved analytically using the equation of motion method.…”
We determine the impurity-induced free energy and the impurity-induced zero-field susceptibility of the symmetric single-impurity Kondo model from weak-coupling perturbation theory up to third order in the Kondo coupling at low temperatures and small magnetic fields. We reproduce the analytical structure of the zero-field magnetic susceptibility as obtained from Wilson’s renormalization group method. This permits us to obtain analytically the first two Wilson numbers.
“…Note that V z 2 is the second-order Ising-Kondo contribution to the single-impurity Kondo model, see [13]. In section SM I of the supplemental material, we explicitly calculate the exact result of the free energy of the Ising-Kondo model for a constant density of states, see equation (13). In this way, we can compare the results from perturbation theory of appendix A with those from the Taylor series of the exact result.…”
Section: J Stat Mech (2024) 043102mentioning
confidence: 99%
“…To make progress, we define Following Bauerbach et al [13], we derive the free energy of the Ising-Kondo model for a constant density of states using the equation-of-motion method. Since we have explicitly performed the second-order perturbation theory for the Ising-Kondo model, see appendix A.1, we can directly compare the Taylor series of the exact result with perturbation theory.…”
Section: B62 Numerical Check For X Amentioning
confidence: 99%
“…(2024) 043102 variational wave functions, and numerical approaches such as the density-matrix renormalization group (DMRG) and the NRG methods. Also in the year 2020, Bauerbach et al [13] introduced a simplification of the Kondo model, the so-called Ising-Kondo model, in which the spin-exchange term of the full Kondo Hamiltonian is neglected. Thereby, the complexity of the Kondo model is reduced to that of potential scattering of spinless fermions, which can be solved analytically using the equation of motion method.…”
We determine the impurity-induced free energy and the impurity-induced zero-field susceptibility of the symmetric single-impurity Kondo model from weak-coupling perturbation theory up to third order in the Kondo coupling at low temperatures and small magnetic fields. We reproduce the analytical structure of the zero-field magnetic susceptibility as obtained from Wilson’s renormalization group method. This permits us to obtain analytically the first two Wilson numbers.
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