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Chapter 4 Section 2
Chapter 4 Section 2

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Chapter 11

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1st Semester Exam Review2

LEP 5.1.03 -15 Franck-Hertz experiment with Ne-tube
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... 1913: An isolated atom consists of a positively charged nucleus about which electrons are distributed in successive orbits. He also postulated that only those orbits occur for which the angular momentum of the electron is an integral multiple of h/2p, i.e. n*h/2p, where n is an integer and h is Plan ...
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... Notes on E(K) • The extrema for the conduction and valence bands are at different values of K for silicon and germanium – these are called indirect bandgap semiconductors ...
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Chapter 7 Quantum Theory and the Electronic Structure of Atoms

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... on the surface of the sphere – it is parametrized by a single amplitude and a single relative phase. This is the same as the description of a classical spin, or the polarisation (Stokes parameters) of a classical light field. Of course, only one basis yields a definite result, so a better descriptio ...
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... Chapter 9. Classical and quantum dynamics of density matrices Statistical mechanics makes the connection between macroscopic dynamics and equilibriums states based on microscopic dynamics. For example, while thermodynamics can manipulate equations of state and fundamental relations, it cannot be use ...
< 1 ... 927 928 929 930 931 932 933 934 935 ... 1073 >

Theoretical and experimental justification for the Schrödinger equation

The theoretical and experimental justification for the Schrödinger equation motivates the discovery of the Schrödinger equation, the equation that describes the dynamics of nonrelativistic particles. The motivation uses photons, which are relativistic particles with dynamics determined by Maxwell's equations, as an analogue for all types of particles.This article is at a postgraduate level. For a more general introduction to the topic see Introduction to quantum mechanics.
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