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Information in statistical physics
Information in statistical physics

Conf. Ser. 724 (2016) 012029 1 - The Racah Institute of Physics
Conf. Ser. 724 (2016) 012029 1 - The Racah Institute of Physics

Design of Strongly Modulating Pulses to Implement Precise Effective
Design of Strongly Modulating Pulses to Implement Precise Effective

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hep-th/0302002 PDF - at www.arxiv.org.

Spacetime physics with geometric algebra
Spacetime physics with geometric algebra

General - Pillar Connections/Cross Ties connection
General - Pillar Connections/Cross Ties connection

Bound states in inhomogeneous magnetic field in graphene
Bound states in inhomogeneous magnetic field in graphene

Real-time evolution for weak interaction quenches in quantum systems
Real-time evolution for weak interaction quenches in quantum systems

Stochastic dominance-constrained Markov decision processes
Stochastic dominance-constrained Markov decision processes

here
here

The Membrane Vacuum State
The Membrane Vacuum State

black hole statistical physics: entropy
black hole statistical physics: entropy

Preparing topologically ordered states by Hamiltonian
Preparing topologically ordered states by Hamiltonian

Third-order optical response of intermediate
Third-order optical response of intermediate

Optimal consumption and portfolio choice with borrowing constraints
Optimal consumption and portfolio choice with borrowing constraints

The polygon representation of three dimensional gravitation and its
The polygon representation of three dimensional gravitation and its

Round Robin Scheduling - A Survey
Round Robin Scheduling - A Survey

2 + 1 dimensional gravity as an exactly soluble system
2 + 1 dimensional gravity as an exactly soluble system

Nonequilibrium Fermi Golden Rule for electronic transitions
Nonequilibrium Fermi Golden Rule for electronic transitions

Quantum Mechanics
Quantum Mechanics

Chirality quantum phase transition in the Dirac oscillator - E
Chirality quantum phase transition in the Dirac oscillator - E

Chapter 6 Groups and Representations in Quantum Mechanics
Chapter 6 Groups and Representations in Quantum Mechanics

arXiv:1504.04012v1 [cond-mat.quant
arXiv:1504.04012v1 [cond-mat.quant

Floquet topological insulators Phys. Stat. Sol. Rap
Floquet topological insulators Phys. Stat. Sol. Rap

Spin-Orbit Interactions in Topological Insulators
Spin-Orbit Interactions in Topological Insulators

... This is followed by a chapter in which it is shown how the spin-orbit interaction, or Thomas term, arises in the non-relativistic limit of the Dirac equation. One reason that the spin orbit interaction is derived here is that it is this term that is responsible for the band structure in the spin orb ...
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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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