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Titlebook: Density Matrix Theory and Applications; Karl Blum Book 1981 Springer Science+Business Media New York 1981 Matrix.Matrix Theory.density.fie

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書目名稱Density Matrix Theory and Applications
編輯Karl Blum
視頻videohttp://file.papertrans.cn/266/265638/265638.mp4
圖書封面Titlebook: Density Matrix Theory and Applications;  Karl Blum Book 1981 Springer Science+Business Media New York 1981 Matrix.Matrix Theory.density.fie
描述Quantum mechanics has been mostly concerned with those states of systems that are represented by state vectors. In many cases, however, the system of interest is incompletely determined; for example, it may have no more than a certain probability of being in the precisely defined dynamical state characterized by a state vector. Because of this incomplete knowledge, a need for statistical averaging arises in the same sense as in classical physics. The density matrix was introduced by J. von Neumann in 1927 to describe statistical concepts in quantum mechanics. The main virtue of the density matrix is its analytical power in the construction of general formulas and in the proof of general theorems. The evaluation of averages and probabilities of the physical quantities characterizing a given system is extremely cumbersome without the use of density matrix techniques. The representation of quantum mechanical states by density matrices enables the maximum information available on the system to be expressed in a compact manner and hence avoids the introduction of unnecessary vari- ables. The use of density matrix methods also has the advantage of providing a uniform treatment of all qua
出版日期Book 1981
關鍵詞Matrix; Matrix Theory; density; fields; information; mechanics; physics; quantum mechanics; quantum theory; s
版次1
doihttps://doi.org/10.1007/978-1-4615-6808-7
isbn_ebook978-1-4615-6808-7
copyrightSpringer Science+Business Media New York 1981
The information of publication is updating

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Jetzt abspringen: Augen zu und durch!In this chapter the concepts introduced in Chapter 1 will be generalized to systems with more than two degrees of freedom. The examples discussed in the preceding sections will provide the physical background for the general treatment in this chapter. We will begin with a further discussion of pure and mixed states.
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Some Applications,nstructive examples of their utility. As the first example, we will show how . can be obtained from a determination of the Stokes parameters. In particular, we will consider the case of excitation of atoms by electron impact under the conditions described in Sections 3.5 and 4.6.
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Das Gehirn ist das Epizentrum aller Drogenons between a quantum system and an external . field. In this chapter we will consider the problem of describing the state of a quantum system which is interacting with other (detected or undetected) . systems. This is an important topic and is of central importance to the following discussions in t
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