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Physics 214 Lecture 11
Physics 214 Lecture 11

Document
Document

... 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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... E1344: Oscillations between a site and a ring Submitted by: Asaf Barak, Jeremy Gartner The problem: A given ring with length L = 1 has N sites, which have equal potential (V = 0). The hopping amplitude of a particle per time unit between neighbouring sites is c. Another site is added at the center o ...
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... • Particles, for example electrons, have wave and particle properties. • The thing that is waving in the case of a particle is probability. The square of the height of the wave (wave function) is a measure of the probability density. • All objects (atoms, molecules, etc.) exist in defined states of ...
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... examine principles of statistical physics, distribution functions and properties of electrons in metals and semiconductors. Prepare to answer the questions: What statistics can by applied to electrons in a metal? What statistics is applied to a non-degenerate system of microparticles? What statistic ...
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... concentrated in a small volume, which did not agree with the plum pudding model. Rutherford put forward another model which is called “planetary model”of atom. According to this model the electrons are revolving around a small positively charged nucleus similar to planets revolving around the Sun. B ...
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< 1 ... 905 906 907 908 909 910 911 912 913 ... 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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