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The speed of quantum information and the preferred frame
The speed of quantum information and the preferred frame

Full Text - International Press of Boston
Full Text - International Press of Boston

the heisenberg uncertainty relation derived by multiplying matter
the heisenberg uncertainty relation derived by multiplying matter

An Introduction to Quantum Spin Systems Notes for MA5020 (John
An Introduction to Quantum Spin Systems Notes for MA5020 (John

Identical Quantum Particles and Weak Discernibility - Philsci
Identical Quantum Particles and Weak Discernibility - Philsci

Thermal equilibrium states for quantum fields on
Thermal equilibrium states for quantum fields on

slides
slides

Quantum Optics - University of Arizona
Quantum Optics - University of Arizona

Dissipative decoherence in the Grover algorithm
Dissipative decoherence in the Grover algorithm

Lecture 34: The `Density Operator
Lecture 34: The `Density Operator

Ohmic vs Markovian heat bath — two-page
Ohmic vs Markovian heat bath — two-page

... Ornstein-Uhlenbeck stochastic process which is nonMarkovian itself. Fortunately, the pair of phase space coordinates satisfy Markovian equations (let’s go back to the quantum case): q̂˙ = p̂/M p̂˙ = −V 0 (q̂) − η p̂/M + X. Hence the Ohmic (or high-T ) dynamics is often called Markovian. The classica ...
Relativistic quantum field theory Nobel Lecture, December 11, 1965
Relativistic quantum field theory Nobel Lecture, December 11, 1965

The non-equilibrium Green`s function method
The non-equilibrium Green`s function method

Quantum Tunneling - GK-12 Program at the University of Houston
Quantum Tunneling - GK-12 Program at the University of Houston

Kitaev Honeycomb Model [1]
Kitaev Honeycomb Model [1]

... operator Wp = σ1x σ2y σ3z σ4x σ5y σ6z which commutes with the Remember the operators Wp did the same. Using a theorem Hamiltonian and itself. Thus, the Hamiltonian can be called ”Lieb’s Theorem”, we know that the groundstate solved individually for the eigenspaces of Wp . The original of the system ...
Mathematical Research Letters 8, 331–345 (2001) VERTEX
Mathematical Research Letters 8, 331–345 (2001) VERTEX

SCHRODINGER`S CAT-IN-THE-BOX WITH THE COPENHAGEN
SCHRODINGER`S CAT-IN-THE-BOX WITH THE COPENHAGEN

... are necessary if the ‘quantum character of the phenomenon shall be made visible. The contradictions disappear when the limitation in the concepts are taken properly into account”(Heisenberg,1977:6). The method of complementarity, according to Heisenberg, i represented as a tendency in the methods of ...
Chapter 12: Symmetries in Physics: Isospin and the Eightfold Way
Chapter 12: Symmetries in Physics: Isospin and the Eightfold Way

... The mass of the up and down quarks are not identical but they are both of the order of a few M eV /c2 ’s which is minuscule compared to the typical energy scale of hadrons (i.e. strongly interacting particles) which is about a GeV /c2 . This is why isospin is such a good symmetry and why isomultiple ...
Quantum Psychoanalysis
Quantum Psychoanalysis

... Gargiulo proposes that the collapse of the wave function is analogous to creating the dynamically repressed unconscious in psychoanalysis through the vehicle of interpretation. Mind you, interpretation creates the unconscious; it does not discover an already existing uncons ...
Introduction to Quantum Monte Carlo
Introduction to Quantum Monte Carlo

demartini
demartini

A Rough Guide to Quantum Chaos
A Rough Guide to Quantum Chaos

Space and Time in Computation and Discrete Physics
Space and Time in Computation and Discrete Physics

... taking such an elementary consideration as our theme, we are able to bring together a very wide range of ideas and techniques under one roof and make connections among them. The present paper is an expanded version of [27]. The second section is a brief discussion of Step, written in non-technical l ...
Deterministic Bell State Discrimination
Deterministic Bell State Discrimination

Relation Between Schrödinger and Polymer Quantum Mechanics
Relation Between Schrödinger and Polymer Quantum Mechanics

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Quantum group

In mathematics and theoretical physics, the term quantum group denotes various kinds of noncommutative algebra with additional structure. In general, a quantum group is some kind of Hopf algebra. There is no single, all-encompassing definition, but instead a family of broadly similar objects.The term ""quantum group"" first appeared in the theory of quantum integrable systems, which was then formalized by Vladimir Drinfeld and Michio Jimbo as a particular class of Hopf algebra. The same term is also used for other Hopf algebras that deform or are close to classical Lie groups or Lie algebras, such as a `bicrossproduct' class of quantum groups introduced by Shahn Majid a little after the work of Drinfeld and Jimbo.In Drinfeld's approach, quantum groups arise as Hopf algebras depending on an auxiliary parameter q or h, which become universal enveloping algebras of a certain Lie algebra, frequently semisimple or affine, when q = 1 or h = 0. Closely related are certain dual objects, also Hopf algebras and also called quantum groups, deforming the algebra of functions on the corresponding semisimple algebraic group or a compact Lie group.Just as groups often appear as symmetries, quantum groups act on many other mathematical objects and it has become fashionable to introduce the adjective quantum in such cases; for example there are quantum planes and quantum Grassmannians.
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