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Time independent Schrödinger Equation
Time independent Schrödinger Equation

... • Consider 2 identical particles: particle 1 in state 1 particle 2 in state  2 • The state could just as well be: particle 1 in state 2 particle 2 in state  1 • Thus the two particle wavefunction is ...
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... linear: if Y is a solution, so too is A Y , where A is any (complex) constant. What we must do, then, is pick this undetermined multiplicative factor so that The integral of |Y (x, t)|2 over space must be 1 This process is called normalizing the wave function. • Physically realizable states correspo ...
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... The quasi-separability of the charges allows the use of this simple functional model. In general, why can we consider the possibility of describing many-electron atoms based on a hydrogen-like atom model, e.g., electronic distribution? This is possible since the interaction among electrons, in gener ...
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... described by points – but, rather as two-dimensional rings that have been expanding since the origin of space and time? ...
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Why Quantum Theory? Lucien Hardy November 13, 2001 Centre for Quantum Computation,

... measurement apparatus set to distinguish a set of N distinguishable states, the only outcomes observed (apart from the null outcome) are those associated with a subset of M of these distinguishable states. In both classical and quantum theory the system will behave like one of dimension M in such ca ...
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On Gauge Invariance and Covariant Derivatives in Metric Spaces

... derivatives and connection coefficients. Covariant derivatives have three general properties which are related to the corresponding properties of ordinary derivatives [2]. They are also assumed to possess two additional properties [2,3]. We will mention these properties in Sec.II. In this article, w ...
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... The Stark effect measures the interaction of a molecular dipole moment with an electric field, while the Zeeman effect measures the interaction of a molecular magnetic moment with a magnetic field. While both electric and magnetic dipoles are rank one tensor quantities, they have quite different sym ...
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... dynamics of quantum many-body systems. Today’s talk: strong manifestations of enhanced fluctuations in dynamics of low dimensional condensates Thanks to: ...
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Quantum typicality: what is it and what can be done... Jochen Gemmer LMU Muenchen, May, Friday 13th, 2014 University of Osnabrück,

... Why it exists: We see it in system we assume to be closed. Why it does not exist: There are issues with the underlying theory: Quantum Mechanics (Non-eq.) Thermodynamics autonomous dynamics of a few macrovariables attractive fixed point, equilibrium often describable by master equations, Fokker-Plan ...
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Renormalization group



In theoretical physics, the renormalization group (RG) refers to a mathematical apparatus that allows systematic investigation of the changes of a physical system as viewed at different distance scales. In particle physics, it reflects the changes in the underlying force laws (codified in a quantum field theory) as the energy scale at which physical processes occur varies, energy/momentum and resolution distance scales being effectively conjugate under the uncertainty principle (cf. Compton wavelength).A change in scale is called a ""scale transformation"". The renormalization group is intimately related to ""scale invariance"" and ""conformal invariance"", symmetries in which a system appears the same at all scales (so-called self-similarity). (However, note that scale transformations are included in conformal transformations, in general: the latter including additional symmetry generators associated with special conformal transformations.)As the scale varies, it is as if one is changing the magnifying power of a notional microscope viewing the system. In so-called renormalizable theories, the system at one scale will generally be seen to consist of self-similar copies of itself when viewed at a smaller scale, with different parameters describing the components of the system. The components, or fundamental variables, may relate to atoms, elementary particles, atomic spins, etc. The parameters of the theory typically describe the interactions of the components. These may be variable ""couplings"" which measure the strength of various forces, or mass parameters themselves. The components themselves may appear to be composed of more of the self-same components as one goes to shorter distances.For example, in quantum electrodynamics (QED), an electron appears to be composed of electrons, positrons (anti-electrons) and photons, as one views it at higher resolution, at very short distances. The electron at such short distances has a slightly different electric charge than does the ""dressed electron"" seen at large distances, and this change, or ""running,"" in the value of the electric charge is determined by the renormalization group equation.
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