Search results for "Quantum evolution"

showing 3 items of 3 documents

Quantum evolution of near-extremal Reissner-Nordstrom black holes

2000

We study the near-horizon AdS_2\timesS^2 geometry of evaporating near-extremal Reissner-Nordstrom black holes interacting with null matter. The non-local (boundary) terms t_{\pm}, coming from the effective theory corrected with the quantum Polyakov-Liouville action, are treated as dynamical variables. We describe analytically the evaporation process which turns out to be compatible with the third law of thermodynamics, i.e., an infinite amount of time is required for the black hole to decay to extremality. Finally we comment briefly on the implications of our results for the information loss problem.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsNull (mathematics)FOS: Physical sciencesBoundary (topology)General Relativity and Quantum Cosmology (gr-qc)Information lossAction (physics)Quantum evolutionGeneral Relativity and Quantum CosmologyPartícules (Física nuclear)General Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)Effective field theoryCamps Teoria quàntica deQuantumThird law of thermodynamicsMathematical physics
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Coherent quantum evolution via reservoir driven holonomies.

2006

We show that in the limit of a strongly interacting environment a system initially prepared in a decoherence-free subspace (DFS) coherently evolves in time, adiabatically following the changes of the DFS. If the reservoir cyclicly evolves in time, the DFS states acquire a holonomy.

PhysicsQuantum decoherenceHolonomyGeneral Physics and AstronomyComputer Science::Software EngineeringQuantum evolutionComputer Science::PerformanceQuantum mechanicsHolonomieLimit (mathematics)Decoherence-free subspace (DFS)Quantum evolutionComputer Science::Data Structures and AlgorithmsSubspace topologyPhysical review letters
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A Noncommutative Approach to Ordinary Differential Equations

2005

We adapt ideas coming from Quantum Mechanics to develop a non-commutative strategy for the analysis of some systems of ordinary differential equations. We show that the solution of such a system can be described by an unbounded, self-adjoint and densely defined operator H which we call, in analogy with Quantum Mechanics, the Hamiltonian of the system. We discuss the role of H in the analysis of the integrals of motion of the system. Finally, we apply this approach to several examples.

Pure mathematicsPhysics and Astronomy (miscellaneous)General MathematicsIntegrating factorExamples of differential equationsStochastic partial differential equationMethod of quantum characteristicsQuantum evolutionQuantum statistical mechanicsC0-semigroupDifferential algebraic equationSettore MAT/07 - Fisica MatematicaOrdinary differential equationSeparable partial differential equationMathematicsInternational Journal of Theoretical Physics
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