2009
DOI: 10.1143/jpsj.78.074719
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Continuous-Time Quantum Monte Carlo Approach to Singlet–Triplet Kondo Systems

Abstract: Dynamical properties are studied numerically for a variant of the Kondo model with singlet and triplet crystalline electric field (CEF) levels where Kondo and CEF singlets compete for the ground state. Using the continuous-time quantum Monte Carlo method, we derive the t-matrix of conduction electrons and dynamical susceptibilities of local electrons without encountering the negative sign problem. When the CEF splitting is comparable to the Kondo temperature, the dynamical response has only a quasi-elastic pea… Show more

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Cited by 6 publications
(11 citation statements)
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“…In the DMFT, the vertices in eqs. (9) and (12) are the same. Hence, we can obtain χ λλ ′ by solving these equations simultaneously.…”
Section: Susceptibilities With Two-sublatticesmentioning
confidence: 99%
See 1 more Smart Citation
“…In the DMFT, the vertices in eqs. (9) and (12) are the same. Hence, we can obtain χ λλ ′ by solving these equations simultaneously.…”
Section: Susceptibilities With Two-sublatticesmentioning
confidence: 99%
“…The parameter α γ is chosen as 0 for ferromagnetic interaction (J γ < 0) and 1 for antiferromagnetic coupling (J γ > 0) in order to avoid the minus sign problem as noted in ref. 9. The constant term may be neglected in the simulation.…”
Section: Ct-qmc Algorithmmentioning
confidence: 99%
“…In interacting electron systems with two f -electrons per site as in some Pr and U compounds, the distinction between itinerant and localized characters of electrons is not as explicit as in Ce or Yb compounds with f 1 or f 13 configuration, respectively. The difference comes from the Kramers degeneracy; the ground state of each non-Kramers ion such as Pr 3+ or U 4+ can be a singlet even without Kondo effect provided the CEF favors the non-degenerate ground state.…”
Section: Introductionmentioning
confidence: 99%
“…The difference comes from the Kramers degeneracy; the ground state of each non-Kramers ion such as Pr 3+ or U 4+ can be a singlet even without Kondo effect provided the CEF favors the non-degenerate ground state. On the contrary, the Kramers degeneracy in f 1 or f 13 can only be removed by exchange (Kondo) interaction with conduction electrons. The dichotomy between itinerant and localized characters of f -electrons leads to intriguing phenomena in heavy fermion systems.…”
Section: Introductionmentioning
confidence: 99%
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