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The Mean-Field Limit for the Dynamics of Large Particle Systems
The Mean-Field Limit for the Dynamics of Large Particle Systems

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The averaged dynamics of the hydrogen atom in crossed electric

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Second-order coupling between excited atoms and surface polaritons

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Topological insulators and superconductors

... We now try to understand how one can put the above manipulations that lead to the Z2 index for TRI topological insulators into a bigger context. Let us review what (topological) classification schemes we already encountered. The first example was the characterization of a spin-1/2 in a magnetic fiel ...
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Supersymmetric Quantum Mechanics - Uwe

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Quantization as Selection Rather than Eigenvalue Problem

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Gravity in Curved Phase-Spaces, Finsler Geometry and Two

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The Hierarchy of Hamiltonians for a Restricted Class of Natanzon

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Regents Pathways - Think Through Math

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Algebraic spin liquid in an exactly solvable spin model

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Today Iterative improvement algorithms Example: Travelling

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An introduction to analytical mechanics

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Evolving Graph Databases under Description Logic - CEUR
Evolving Graph Databases under Description Logic - CEUR

... where β is a basic action and K is an arbitrary ALCHOIQbr–formula. The special symbol  denotes the empty action. An action α is ground if it has no variables. An action α0 is called a ground instance of an action α if α0 is ground and it can be obtained from α by replacing each variable by an indiv ...
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Chapter 2 Atomic Motion in an Optical Standing Wave

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Universal edge information from wavefunction deformation

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Page 1 Lecture: Quantum Optics Derivation of the Master Equation

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A Rough Guide to Quantum Chaos

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2001. (with Gordon Belot) Pre-Socratic Quantum Gravity. In Physics

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Dirac bracket

The Dirac bracket is a generalization of the Poisson bracket developed by Paul Dirac to treat classical systems with second class constraints in Hamiltonian mechanics, and to thus allow them to undergo canonical quantization. It is an important part of Dirac's development of Hamiltonian mechanics to elegantly handle more general Lagrangians, when constraints and thus more apparent than dynamical variables are at hand. More abstractly, the two-form implied from the Dirac bracket is the restriction of the symplectic form to the constraint surface in phase space.This article assumes familiarity with the standard Lagrangian and Hamiltonian formalisms, and their connection to canonical quantization. Details of Dirac's modified Hamiltonian formalism are also summarized to put the Dirac bracket in context.
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