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LECTURE NOTES ON STATISTICAL MECHANICS Scott Pratt Department of Physics and Astronomy
LECTURE NOTES ON STATISTICAL MECHANICS Scott Pratt Department of Physics and Astronomy

... to understand why all states are equally populated from the perspective of dynamics. The Ergodic theorem is built on the symmetry of time-reversal, i.e., the rate at which one changes from state i to state j is the same as the rate at which one changes from state j to state i. Here, we can consider ...
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... and the book [22] of Holevo. Although both the classical Cramér-Rao inequality and its quantum analog are mathematically as trivial as the Schwarz inequality, the subject takes a lot of attention because it is located on the boundary of statistics, information and quantum theory. As a starting poin ...
Causal Sets: Discrete Gravity (Notes for the Valdivia Summer School)
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... provide a close connection between solid-state systems and atomic physics [1]. The models used to describe these systems generally assume that each lattice site’s wave function is easily built up from single-particle states [2]. Here we argue that this approximation is inappropriate for quantitative ...
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... continuous atomic time scale based on TAI with simultaneous broadcasting these two reference timescales (current UTC and continuous atomic time scale) on equal basis. However, practical implementation of Methods A and B seems difficult due to: - in case of Method A the problems related to disseminat ...
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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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