Titlebook: Quantum Mechanics; An Introduction Walter Greiner Textbook 2001Latest edition Springer-Verlag Berlin Heidelberg 2001 curvilinear coordinate

ANNOY

書(shū)目名稱Quantum Mechanics影響因子(影響力)




書(shū)目名稱Quantum Mechanics影響因子(影響力)學(xué)科排名




書(shū)目名稱Quantum Mechanics網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱Quantum Mechanics網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱Quantum Mechanics被引頻次




書(shū)目名稱Quantum Mechanics被引頻次學(xué)科排名




書(shū)目名稱Quantum Mechanics年度引用




書(shū)目名稱Quantum Mechanics年度引用學(xué)科排名




書(shū)目名稱Quantum Mechanics讀者反饋




書(shū)目名稱Quantum Mechanics讀者反饋學(xué)科排名

flamboyant

糾纏

Wave Aspects of Matter,ctly in the photoelectric effect. So for light, the relations describing waveparticle duality are already known. But what about material particles? Their particulate nature is rather obvious; do they also possess a wave aspect?

FISC

LEERY

比賽用背帶

Conceptual and Philosophical Problems of Quantum Mechanics,ion made by quantum mechanics has been disproved experimentally. In spite of this success, conceptual problems with the theory exist; in fact, there have been many attempts to interpret quantum mechanics in a new way or even to replace it by another theory based on a more obvious conceptual and philosophical foundation.

頑固

lays the foundations for the rest of the course on quantum mechanics, advanced quantum mechanics, and field theory. Starting from black-body radiation, the photoelectric effect, and wave-particle duality, Greiner goes on to discuss the uncertainty relations, spin, and many-body systems; he includes

Urgency

Mathematical Supplement, the functions ψ(., .) are not orthogonal, but the eigendifferentials △ψ(., .) are. Furthermore, because the △ψ(., .) have finite spatial extension, they can be normalized. Then in the limit △. → 0, a meaningful normalization of the functions ψ(., .) themselves follows: the normalization on δ functions.

強(qiáng)壯

,The Schr?dinger Equation,ch an equation, not derived but guessed at intuitively, would then be a postulate of the new theory, and its validity would have to be checked by experiment. This equation for the calculation of quantum-mechanical states is called the ..; let us now “derive” it.

清楚說(shuō)話

Identical Particles,s we will not be able to establish later on whether particle no. 1 or no. 2 or another particle can be found at the point in space r. Because of the possible interaction (momentum exchange etc.), dynamical properties cannot be used to distinguish between them, either.