Abstract
In the previous chapter we solved the Schrödinger equations for the potential barrier and the quantum well. These important and soluble systems, revealed fundamental properties present in the actual quantum systems. Some of the results obtained for these systems will reappear, in this and the coming chapters, and will enhance the insight into the quantum phenomena and their physical meaning. In this chapter we will study systems with slightly more complex structure, but still piecewise constant potentials. We will begin with the double quantum well with infinite walls, and we will continue with the double potential barrier and the double quantum well with finite lateral walls. In these systems a new phenomenon will appear: the splitting of the energy levels. We will conclude this chapter with a brief introduction to the finite periodic systems theory, applied to the Kronig–Penney model, taken as a finite sequence of rectangular wells and barriers. We will see that the energy levels splitting is responsible for the formation of energy bands, an essential property closely related to the quantum phase coherence, that makes it possible for us to see fundamental differences in the physical behavior of metals, semiconductors and insulators.
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- 1.
Usually the superposition of waves gives rise to constructive and destructive interferences. These interferences of well defined phases, are responsible of interesting effects like the energy levels splitting and the band structure in periodic systems.
- 2.
In the double barrier systems of the electronic devices, the potential function contains also the bias potential energy \(Fx\).
- 3.
Quite frequently one finds, in the scientific literature, approximate double well eigenfunctions. They are generally built with the eigenfunctions of the single wells and, when the barrier width is large, as single well eigenfunctions.
- 4.
Kronig, R. d. L. and Penney, W. G. Proc. Roy. Soc. A 130 499 (1931) .
- 5.
Notice that to simplify the calculations we are also assuming that the unit cell is invariant under time reversal.
- 6.
In 3D systems or systems with more than one propagating mode, \(\alpha \) and \(\beta \) are matrices. This kind of systems are beyond the purpose of this book.
- 7.
One can easily verify that \(p_{1}(\alpha _R) = -2\alpha _R\), \(p_{2}(\alpha _R) = 4\alpha _R^{2} - 1\), and so on.
- 8.
See P. Pereyra, Phys. Rev. Lett 80 (1998) 2677.
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© 2012 Springer-Verlag Berlin Heidelberg
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Pereyra Padilla, P. (2012). Quantum Coherence and Energy Levels Splitting . In: Fundamentals of Quantum Physics. Undergraduate Lecture Notes in Physics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-29378-8_5
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DOI: https://doi.org/10.1007/978-3-642-29378-8_5
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