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... • For reasons that will become apparent shortly, operators like the translation operator are often called “symmetry operators.” ...
Hamiltonian Equations
Hamiltonian Equations

... Constraints are time-independent „ This makes T = L2 ( q, t ) q j qk See Lecture 4, or Forces are conservative Goldstein Section 2.7 „ This makes V = − L0 ( q ) ...
An Invitation to Quantum Complexity Theory
An Invitation to Quantum Complexity Theory

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Document
Document

... Thus, putting of a system into the thermostat is equivalent to an effective doubling of freedom degrees number. It results in cutting of a peculiar degeneration of state. Therefore we transfer from initial vacuum for particles |0> to a new vacuum for quasi-particles |0>>, which is dependent from tem ...
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Quantum Theory

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Quantum Mechanics Basics

Similarity between quantum mechanics and thermodynamics
Similarity between quantum mechanics and thermodynamics

Prezentacja programu PowerPoint
Prezentacja programu PowerPoint

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(normal) Zeeman Effect with Spin Spin

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... This motivates us to interpret the state |~pi as the momentum eigenstate of a single particle of mass m. To stress this, from now on we will write Ep~ everywhere instead of ωp~ . Let’s check this particle interpretation by studying the other quantum numbers of |~pi. We may take the classical total m ...
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Quantum Gravity - General overview and recent developments

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... an exact quantum collective coordinate with frequency ~1!, independent of g and N, where N is the number of electrons. The collective coordinate V may also be separated into a center-of-mass and relative-coordinate part, V5V c.m.1V rel . For a 52, it can be shown that each component separately satis ...
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Mean field theory and Hartree
Mean field theory and Hartree

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Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
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