2020
DOI: 10.1134/s1063783420010266
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Spin Fluctuations and Concentration Magnetic Transitions in Chiral Helical Ferromagnets Fe1 – xCoxSi

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Cited by 5 publications
(5 citation statements)
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“…A possible reason for this discrepancy might root in the failure of DFT to capture the effect of electronic correlations which can dramatically change the overall behavior of the system, as was recently demonstrated using dynamical mean-field theory [49]. On the other hand, since the difference in total energy for q DFT min and q exp min due to the twist is small, E(q DFT min , Ω) − E(q exp min , Ω) = 8µeV, we speculate that it can be overtaken by higher order magnetic interactions [35] or by quantum fluctuations [50] shifting q DFT min towards q exp min .…”
Section: Discussionsupporting
confidence: 54%
“…A possible reason for this discrepancy might root in the failure of DFT to capture the effect of electronic correlations which can dramatically change the overall behavior of the system, as was recently demonstrated using dynamical mean-field theory [49]. On the other hand, since the difference in total energy for q DFT min and q exp min due to the twist is small, E(q DFT min , Ω) − E(q exp min , Ω) = 8µeV, we speculate that it can be overtaken by higher order magnetic interactions [35] or by quantum fluctuations [50] shifting q DFT min towards q exp min .…”
Section: Discussionsupporting
confidence: 54%
“…Let us consider a strongly correlated electronic system of chiral ferromagnets Fe 1−x Co x Si with Hamiltonian taking into account the zone motion energy, intra-atomic Coulomb spin and charge correlations, differing in nodes occupied by Fe atoms on Co. At the same time we will keep in mind that use of spin-dependent energy spectrum from first-principles LSDA + U + SO, causes concentration dependences and values of local magnetizations Fe 1−x Co x Si, not matching with the experimental data [7]. Satisfactory agreement with the experiment is obtained at self-consistent calculation of local magnetization within fluctuation theory of zone magnetism, where the results of the first-principles LDA + U + SO are used only to model electronic structure [5].…”
Section: Modelmentioning
confidence: 97%
“…In particular, such transition in the narrow range of temperatures (T s − T c ) ≪ T c occurs in MnSi, where it is accompanied by sharp change of volume and occurrence of lambdalike anomaly of VCTE [4]. A transition extended by temperature related to change of mode-mode parameter sign change in Fe 1−x Co x Si [5], as a result of fluctuations of intra-atomic potentials of electronelectron repulsion in nodes occupied by iron and cobalt atoms [5], is implemented in a wider range of temperatures (T s − T c ) ∼ T c , and in the experiment instead of lambdaanomaly of negative VCTEs, a wide temperature minimum occurs [6].…”
Section: Introductionmentioning
confidence: 94%
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