By Michael D. Ciletti
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Additional resources for Advanced Digital Design with the Verilog HDL
In the standard application of the adiabatic approximation to (light) diatomic molecules one normally treats such terms as a small perturbation, and this is justified by the consideration that the spacing between the "environment" (here electronic) energy levels is very large compared to the characteristic energies of the "system" (here nuclear) motion; under these circumstances, no irreversible transfer of energy from the nuclear to the electronic degrees of freedom is possible, and the only effect of the perturbation is a renormalization of energy levels and matrix elements (which, moreover, turns out to be small, although this is not obvious without some calculation).
Indeed, probably the most striking feature of the q u a n t u m measurement paradox over the last fifty years has been that it has seemed totally impervious to any kind of experimental resolution. And it is indeed clear that, as long as we grant premise P, this will continue forever to be so. If, therefore, we have any hope at all that experiment may be able to provide some useful input to this problem (and, thereby, in the language of the average * As evidenced, inter alia, by the regularity with which it is rediscovered and republished as new in the literature.
59,347. , 1985, Phys. Today (April 1985) p. 38. E. Mutton, H. Prance, TD. Clark, A. Widom and G. Megaloudis, 1983, Helv. Phys. Acta 56, 789. , 1935, Naturwiss. 23,824. , 1990, Phys. Rev. Lett. 64,2358. CHAPTER 2 Quantum Tunneling Diffusion in Solids* Yu. V. P R O K O F E V Kurchatov institute of Atomic Energy Moscow, Russia * Translated from the Russian by Artavaz Beknazarov Quantum tunnelling in condensed media Edited by Yu. J. , 1992 37 Contents 1. Introduction 2. 1. 2. 3. 4. 5. The polaron operator 3.
Advanced Digital Design with the Verilog HDL by Michael D. Ciletti