addition
发表于 2025-3-23 10:39:42
Introductory Overview and Heavy-Fermion Phenomenologyiparticles appear to have a very large effective mass, i.e., one which is hundreds of times larger than the free electron mass. Therefore these systems are often called heavy-fermion or heavy-electron systems. In the meantime research on those systems has developed into an own branch of metal physic
敲竹杠
发表于 2025-3-23 16:43:10
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分期付款
发表于 2025-3-23 18:53:39
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panorama
发表于 2025-3-24 00:35:08
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责难
发表于 2025-3-24 02:37:53
Effect of Disorder in the Periodic Anderson Modelnte Carlo techniques. We have examined for the first time the disorder both in hybridization between the local f-orbitals and the conduction electrons and in the local f=site energy, using a uniform distribution. We find that the disorder in hybridization has a dramatic effect on the low-temperature
开始没有
发表于 2025-3-24 09:58:29
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暖昧关系
发表于 2025-3-24 12:27:53
https://doi.org/10.1007/978-3-662-64593-2 of an R ion with a large magnetic moment does not significantly influence the superconductivity. In contrast, even the presence of small concentrations of magnetic impurity ions in a conventional superconductor inhibits superconductivity by interfering with the formation of Cooper pairs.
突袭
发表于 2025-3-24 17:24:42
https://doi.org/10.1007/978-1-4615-5989-4rrelations. Additional non-standard feature is the crucial role of relativistic phenomena. The last ingredient leads, for example, to a strong orbital polarization even in strongly itinerant systems, and to a strong coupling of the spin system to the crystal lattice, both being the consequence of strong spin-orbit interaction.
Interstellar
发表于 2025-3-24 22:47:46
The Role of Selected f Ions in the Suppression of High-Tc Superconductivity of an R ion with a large magnetic moment does not significantly influence the superconductivity. In contrast, even the presence of small concentrations of magnetic impurity ions in a conventional superconductor inhibits superconductivity by interfering with the formation of Cooper pairs.
florid
发表于 2025-3-25 02:36:40
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