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= ∫ ( ) = ∫ ( )
= ∫ ( ) = ∫ ( )

1 Derivation of Schrödinger`s equation Mikhail Batanov, Associate
1 Derivation of Schrödinger`s equation Mikhail Batanov, Associate

The Uncertainty Principle and Covalent Bonding
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... closely related problem – that of the “wave-particle duality”. When trying to interpret the behavior of both light and matter at the atomic scale, it seemed that two different modes of communication were necessary to accommodate the full range of known phenomena. Some experiments, such as the diffra ...
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... While lights are the fastest and the most robust carriers of information, it is difficult to localize and store them. Recently, a novel scheme to store the photonic information in an atomic ensemble was proposed [1], which is based on the phenomenon of ultraslow light propagation [2]. Ultraslow ligh ...
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... Einstein suggested in the context of special relativity that energy and mass are equivalent, and related through the famous E = mc2. De Broglie realized that, if all matter was quantized, this implied a general relation between the momentum of a particle and its energy as expressed in terms of frequ ...
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... The fractional quantum Hall effect: Laughlin wave function The fractional QHE is evidently prima facie impossible to obtain within an independentelectron picture, since it would appear to require that the extended states be only partially occupied and this would immediately lead to a nonzero value o ...
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... Without being bounded by R, we would get an infinite degeneracy for positive m’s. For ν = 0 only positive m’s will result in the ground state energy. Being bounded by a disc of radius R, m will be limited and so the degeneracy will be finite. The effective radial potential is a function of m (m) ...
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... pattern is observed when x-rays of many wavelengths are incident on a crystal and diffraction can therefore occur from many planes simultaneously. …pretty ...
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Matter wave

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