Titlebook: Part I: Physical Chemistry. Part II: Solid State Physics; Arthur S. Wightman Book 1997 Springer-Verlag Berlin Heidelberg 1997 Electronic S

削木头

书目名称Part I: Physical Chemistry. Part II: Solid State Physics影响因子(影响力)




书目名称Part I: Physical Chemistry. Part II: Solid State Physics影响因子(影响力)学科排名




书目名称Part I: Physical Chemistry. Part II: Solid State Physics网络公开度




书目名称Part I: Physical Chemistry. Part II: Solid State Physics网络公开度学科排名




书目名称Part I: Physical Chemistry. Part II: Solid State Physics被引频次




书目名称Part I: Physical Chemistry. Part II: Solid State Physics被引频次学科排名




书目名称Part I: Physical Chemistry. Part II: Solid State Physics年度引用




书目名称Part I: Physical Chemistry. Part II: Solid State Physics年度引用学科排名




书目名称Part I: Physical Chemistry. Part II: Solid State Physics读者反馈




书目名称Part I: Physical Chemistry. Part II: Solid State Physics读者反馈学科排名

bronchodilator

浮雕宝石

adipose-tissue

MAIZE

doxazosin

Calculation of the Rate of Elementary Association Reactionsr, the calculated values are somewhat too low, which cannot be explained by an inaccuracy of the method. Reasons for the discrepancy other than the possible nonadiabatic character of the reaction are discussed.

BILK

话

erry phases. Although few in number, Wigner‘s articles on solid-state physics laid the ground for the modern theory of the electronic structure of metals. W. Kohn writes about this in his annotation to Part 2 of the book and he also points out Wigner‘s great influence in the development of solid-state theory.978-3-642-63824-4978-3-642-59033-7

dainty

physics. In his annotation to the first part, N. Balazs clearly points out Wigner‘s role in early quantum chemistry and applied statistical mechanics. One corner stone was his introducing of what is now called the Wigner function, and his paper on adiabatic perturbations foreshadowed later work on B

Chipmunk

Bildung und Zerfall von Molekülen Gegenprozeß, nämlich der spontane Zerfall eines Moleküls, vor sich gehen kann. Als Begründung wird angeführt, daß es unendlich unwahrscheinlich ist, daß die Relativenergie der zusammenstoßenden Gebilde gerade einen quantenhaft zulässigen Energiewert des zu bildenden Moleküls beträgt.