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Titlebook: Oscillator Representation in Quantum Physics; M. Dineykhan,G. V. Efimov,S. N. Nedelko Book 1995 Springer-Verlag Berlin Heidelberg 1995 Pha

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發(fā)表于 2025-3-21 16:43:29 | 只看該作者 |倒序瀏覽 |閱讀模式
書目名稱Oscillator Representation in Quantum Physics
編輯M. Dineykhan,G. V. Efimov,S. N. Nedelko
視頻videohttp://file.papertrans.cn/705/704853/704853.mp4
叢書名稱Lecture Notes in Physics Monographs
圖書封面Titlebook: Oscillator Representation in Quantum Physics;  M. Dineykhan,G. V. Efimov,S. N. Nedelko Book 1995 Springer-Verlag Berlin Heidelberg 1995 Pha
描述The investigation ofmost problems of quantum physics leads to the solution of the Schrodinger equation with an appropriate interaction Hamiltonian or potential. However, the exact solutions are known for rather a restricted set of potentials, so that the standard eternal problem that faces us is to find the best effective approximation to the exact solution of the Schrodinger equation under consideration. In the most general form, this problem can be formulated as follows. Let a total Hamiltonian H describing a relativistic (quantum field theory) or a nonrelativistic (quantum mechanics) system be given. Our problem is to solve the Schrodinger equation Hlft = Enlftn, n i. e. , to find the energy spectrum {En} and the proper wave functions {lft } n including the‘ground state or vacuum lft = 10). The main idea of any ap- o proximation technique is to find a decomposition in such a way that Ha describes our physical system in the "closest to H" manner, and the Schrodinger equation HolJt. (O) = E(O)lJt. (O) n n n can be solved exactly. The interaction Hamiltonian HI is supposed to give small corrections to the zero approximation which can be calculated. In this book, we shall consider t
出版日期Book 1995
關(guān)鍵詞Phase structure; canoncial transformation; oscillator representation; quantum field theory; quantum mech
版次1
doihttps://doi.org/10.1007/978-3-540-49186-6
isbn_softcover978-3-662-14063-5
isbn_ebook978-3-540-49186-6Series ISSN 0940-7677
issn_series 0940-7677
copyrightSpringer-Verlag Berlin Heidelberg 1995
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沙發(fā)
發(fā)表于 2025-3-21 23:40:30 | 只看該作者
in zweckentsprechender Weise hintereinander schaltet. In Fig. 107 ist eine Wechselstrommaschine mit feststehendem Magnetgestell und rotierendem Anker dargestellt, Fig. 108 zeight eine Maschine mit feststehendem Anker und rotierendem Magnetrad. Gestshieht die Erregung der Magnete in beiden F?llen mit
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Introductionystem in the “closest to .” manner, and the Schr?dinger equation . can be solved exactly. The interaction Hamiltonian .. is supposed to give small corrections to the zero approximation which can be calculated.
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as Feld eines beliebigen Magnetgestelles ausführt. Man braucht demnach nur die Enden einer solchen Windung an zwei auf der Achse des Ankers sitzende isolierte Schleifringe anzuschlie?en und kann dann den Wechselstrom aus zwei auf diesen Ringen schleifenden feststehenden Bürsten direkt abnehmen. Da n
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Introduction potential. However, the exact solutions are known for rather a restricted set of potentials, so that the standard eternal problem that faces us is to find the best effective approximation to the exact solution of the Schr?dinger equation under consideration. In the most general form, this problem c
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發(fā)表于 2025-3-23 09:28:07 | 只看該作者
Formulation of the Methodlems of a strong coupling regime and phase transitions in various quantum field models. Many readers might think that this is an unusual manner in which to describe some new calculational techniques taking as an example the most difficult part of quantum physics. However, we hope that astonishment w
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