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Titlebook: Electronic States in Crystals of Finite Size; Quantum confinement Shang Yuan Ren Book 20061st edition Springer-Verlag New York 2006 Finite

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發(fā)表于 2025-3-23 13:46:37 | 只看該作者
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發(fā)表于 2025-3-23 13:54:50 | 只看該作者
,Ebene der Schülerinnen und Schüler,ntial period and . is a positive integer.. On the basis of the theory of differential equations in Chapter 2, exact and general results on the electronic states in such an ideal finite crystal can be analytically obtained. We will see that in obtaining the results in this chapter, it is the understa
13#
發(fā)表于 2025-3-23 19:02:01 | 只看該作者
https://doi.org/10.1007/978-3-658-34021-6 this part and in Part II is that the corresponding Schr?dinger equation for the electronic states in a three-dimensional crystal is a . differential equation; therefore, now the problem is a more difficult one. This is due to the fact that relative to the solutions of ordinary differential equation
14#
發(fā)表于 2025-3-24 01:01:21 | 只看該作者
15#
發(fā)表于 2025-3-24 04:28:06 | 只看該作者
https://doi.org/10.1007/978-3-322-80900-1n one more direction. In this chapter, we are interested in the electronic states in an orthorhombic finite crystal or quantum dot that can be considered as the onedimensional Bloch waves in a rectangular quantum wire discussed in Chapter 6 further confined by two boundary surfaces perpendicularly i
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發(fā)表于 2025-3-24 07:25:07 | 只看該作者
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發(fā)表于 2025-3-24 14:08:49 | 只看該作者
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發(fā)表于 2025-3-24 18:22:52 | 只看該作者
Concluding Remarkss, based on a theory of differential equations approach. By ideal, it is assumed that (i) the potential . inside the low-dimensional system or the finite crystal is the same as in a crystal with translational invariance and (ii) the electronic states are completely confined in the limited size of the low-dimensional system or the finite crystal.
19#
發(fā)表于 2025-3-24 20:37:25 | 只看該作者
978-1-4419-2087-4Springer-Verlag New York 2006
20#
發(fā)表于 2025-3-25 00:43:02 | 只看該作者
Electronic States in Crystals of Finite Size978-0-387-26304-5Series ISSN 0081-3869 Series E-ISSN 1615-0430
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