珍珠无
发表于 2025-3-21 19:16:59
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Slit-Lamp
发表于 2025-3-21 22:07:23
W. G. Schmidt,P. H. Hahn,F. Bechstedt main tools to be employed here are the first- and second-order density matrices (see Section 2.2), including the important observable electron density ρ(.) for the analytical development presented. Closely related tools, e.g., the Greens function, are used in discussing quantum computer simulations.
POLYP
发表于 2025-3-22 02:08:11
Peter Schmitteckert,Günter Schneidery quantitative examination of the problem. In contrast, as already mentioned, one has qualitative consequences in multicenter problems that are worthy of full consideration. Let us start by reviewing the situation in the H. molecule, going back to the pioneering work on the theory of the chemical bond by Heitler and London (1927).
gregarious
发表于 2025-3-22 06:13:45
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异端邪说下
发表于 2025-3-22 10:39:49
Outline, main tools to be employed here are the first- and second-order density matrices (see Section 2.2), including the important observable electron density ρ(.) for the analytical development presented. Closely related tools, e.g., the Greens function, are used in discussing quantum computer simulations.
Pillory
发表于 2025-3-22 12:56:33
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Pillory
发表于 2025-3-22 18:48:21
,Metal—Insulator Transitions and the Chemical Bond,l of Chapter 3 as the background neutralizing density is lowered, the type of transition from delocalized wave functions, belonging to the molecule or solid as a whole, to localized wave functions has been clearly identified.
saturated-fat
发表于 2025-3-23 00:14:29
Martin Karrenbach,Petra Knopf,Matthias JacobThe methods of the preceding chapter are very powerful for calculating the correlation energy of many-electron systems. In the present chapter, as well as the next, attention will be focused primarily on the interpreation of specific physical phenomena that arise solely from electron—electron interactions.
NAVEN
发表于 2025-3-23 05:11:27
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偶然
发表于 2025-3-23 07:33:13
Quasiparticles and Collective Excitations (Especially Plasmons),The methods of the preceding chapter are very powerful for calculating the correlation energy of many-electron systems. In the present chapter, as well as the next, attention will be focused primarily on the interpreation of specific physical phenomena that arise solely from electron—electron interactions.