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The equations of motion
The equations of motion

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document

... Reinterpret Feynman diagram for e- moving through space. Direction and l → momentum vector, f → energy Absolute  cannot be measured, only D s are observable. Probably  universe is symmetric under global phase changes but special relativity doecn’t allow application of global symmetries. Our e- sh ...
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Third Quarter 2011 (Volume 6, Number 2)
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Frustrated Quantum Magnetism with Laser-Dressed Rydberg Atoms

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The mystery of square root of minus one in quantum mechanics, and

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Commun. math. Phys. 52, 239—254

Linköping University Post Print New quantum limits in plasmonic devices
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Unit 3 Matter Energy Interface Suggested Time: 24 Hours

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Quantum Algorithms - University of Sydney

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Chapter 2: Quantum Mechanics and Symmetry

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... by major developments in the sciences. It is true that, historically, most of those scientific developments have involved revolutionary changes at the level of fundamental theory (especially, of course, the revolutionary changes in physics at the beginning of the 20th Century.) It’s also true that ...
Physics 610: Quantum Optics
Physics 610: Quantum Optics

... lectures will cover material on the fully-quantum mechanical description of the radiation field and its interaction with matter, as treated in the later chapters. We begin at chapter 10, in which Maxwell’s equations are quantized, and we then proceed to consider various properties, measurements, and ...
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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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