高调 发表于 2025-3-28 14:34:49
http://reply.papertrans.cn/67/6653/665279/665279_41.pngAsseverate 发表于 2025-3-28 22:36:33
I. Katayama,S. Wakatsuki,I. Iino,M. Izuoon here is the effects of disorder, which is a separate topic in itself. Included in this talk will be spin-polarization as well as finite temperature effects, in both bulk and semi-infinite situations, and electron-hole plasmas. Interesting physical situations of two-dimensionality occuring in MosfMUTED 发表于 2025-3-29 01:33:21
http://reply.papertrans.cn/67/6653/665279/665279_43.pngTIGER 发表于 2025-3-29 05:04:58
http://reply.papertrans.cn/67/6653/665279/665279_44.pngcrumble 发表于 2025-3-29 10:32:00
J. A. Pinotti,R. C. B. de Pisani,L. C. Teixeira,S. Bastoswell as the short range repulsion between equally charged ions, since the Coulomb repulsion is sufficiently strong to keep them apart. The limiting situations of the potential (2) are: i) x-1, i.e. the pure metal, for which we recover the one component plasma (O.C.P.) model.; ii) x=0, i.e. the pure群岛 发表于 2025-3-29 11:30:50
M. G. Cattani,P. Gugliotta,M. P. Foschini,V. Eusebiwell as the short range repulsion between equally charged ions, since the Coulomb repulsion is sufficiently strong to keep them apart. The limiting situations of the potential (2) are: i) x-1, i.e. the pure metal, for which we recover the one component plasma (O.C.P.) model.; ii) x=0, i.e. the pure盘旋 发表于 2025-3-29 18:48:04
well as the short range repulsion between equally charged ions, since the Coulomb repulsion is sufficiently strong to keep them apart. The limiting situations of the potential (2) are: i) x-1, i.e. the pure metal, for which we recover the one component plasma (O.C.P.) model.; ii) x=0, i.e. the pure咆哮 发表于 2025-3-29 21:08:53
http://reply.papertrans.cn/67/6653/665279/665279_48.pngMigratory 发表于 2025-3-30 00:29:13
http://reply.papertrans.cn/67/6653/665279/665279_49.pngFavorable 发表于 2025-3-30 05:22:01
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