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Titlebook: Advances in Nuclear Physics; Volume 7 Michel Baranger,Erich Vogt Book 1973 Springer Science+Business Media New York 1973 Cross section.Isos

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發(fā)表于 2025-3-21 16:52:30 | 只看該作者 |倒序?yàn)g覽 |閱讀模式
期刊全稱Advances in Nuclear Physics
期刊簡(jiǎn)稱Volume 7
影響因子2023Michel Baranger,Erich Vogt
視頻videohttp://file.papertrans.cn/150/149243/149243.mp4
圖書(shū)封面Titlebook: Advances in Nuclear Physics; Volume 7 Michel Baranger,Erich Vogt Book 1973 Springer Science+Business Media New York 1973 Cross section.Isos
影響因子As much by chance as by design, the present volume comes closer to having a single theme than any of our earlier volumes. That theme is the properties of nuclear strength functions or, alternatively, the problem of line spreading. The line spreading or strength function concepts are essential for the nucleus because of its many degrees of freedom. The description of the nucleus is approached by using model wave functions-for example, the shell model or the collective model-in which one has truncated the number of degrees of freedom. The question then is how closely do the model wave functions correspond to the actual nuclear wave functions which enjoy all the degrees of freedom of the nuclear Hamiltonian? More precisely, one views the model wave functions as vectors in a Hilbert space and one views the actual wave functions as vectors spanning another, larger Hilbert space. Then the question is: how is a single-model wave function (or vector) spread among the vectors corresponding to the actual wave functions? As an example we consider a model state which is a shell-model wave function with a single nucleon added to a closed shell. Such a model state is called a single-particle wav
Pindex Book 1973
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S. Michael Mauer,Blanche M. Chaversuse of the large number and density of final states it becomes expedient to deal with high-energy beta decay in the language of the statistical model [for general reviews, see Lynn (Lyn 68) and Vogt (Vog 68)], and to discuss the beta-decay rate in terms of a strength function.
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Book 1973tion is: how is a single-model wave function (or vector) spread among the vectors corresponding to the actual wave functions? As an example we consider a model state which is a shell-model wave function with a single nucleon added to a closed shell. Such a model state is called a single-particle wav
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n the question is: how is a single-model wave function (or vector) spread among the vectors corresponding to the actual wave functions? As an example we consider a model state which is a shell-model wave function with a single nucleon added to a closed shell. Such a model state is called a single-particle wav978-1-4615-9046-0978-1-4615-9044-6
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The Beta Strength Function,hmen mit individuellen Systemen und Praktiken müssen die GoB Aussagen darüber machen, . das Rechenwerk gestaltet werden kann, damit es als solches den Vorstellungen des Gesetzgebers entspricht. Eine Antwort auf das Wie w?re sehr einfach, wenn die GoB in Handels- und Steuerrecht umfassend geregelt w?
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