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E5668: Spin precession due to spin-orbit interaction
E5668: Spin precession due to spin-orbit interaction

... An electron, with mass M , charge e and gyromagnetic constant g, launched with energy E in a one dimensional conductor, in the direction of the X axis. The conductor passes through capacitor plates of length L. The capacitor creates an electric field E in the Y direction. Likewise, there’s a magneti ...
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Fall 2011 CHEM 760: Introductory Quantum Chemistry Homework 9

... this hypothetical universe. The spin portion of your wave function should be in terms of the spin functions (ms = 1),  (ms = 1), and  (ms = -1). b) For each of the trial functions you wrote down above, what is the value of the projection of the total spin angular momentum vector onto the z-axis, ...
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Ising model

The Ising model (/ˈaɪsɪŋ/; German: [ˈiːzɪŋ]), named after the physicist Ernst Ising, is a mathematical model of ferromagnetism in statistical mechanics. The model consists of discrete variables that represent magnetic dipole moments of atomic spins that can be in one of two states (+1 or −1). The spins are arranged in a graph, usually a lattice, allowing each spin to interact with its neighbors. The model allows the identification of phase transitions, as a simplified model of reality. The two-dimensional square-lattice Ising model is one of the simplest statistical models to show a phase transition.The Ising model was invented by the physicist Wilhelm Lenz (1920), who gave it as a problem to his student Ernst Ising. The one-dimensional Ising model has no phase transition and was solved by Ising (1925) himself in his 1924 thesis. The two-dimensional square lattice Ising model is much harder, and was given an analytic description much later, by Lars Onsager (1944). It is usually solved by a transfer-matrix method, although there exist different approaches, more related to quantum field theory.In dimensions greater than four, the phase transition of the Ising model is described by mean field theory.
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