PhysLean Documentation

PhysLean.QuantumMechanics.FiniteTarget.Basic

Finite target quantum mechanics #

The phrase 'finite target' is used to describe quantum mechanical systems where the Hilbert space is finite.

Physical examples of such systems include:

A FiniteTarget structure that is basis independent, i.e. use a linear map for the hamiltonian instead of a matrix."

  • hdim : Module.finrank H = n

    the Hilbert space has the provided (finite) dimension.

  • Ham : H →L[] H

    The Hamiltonian, written now as a continuous linear map.

  • Ham_selfAdjoint : IsSelfAdjoint self.Ham

    The Hamiltonian is self-adjoint.

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    Given a finite target QM system A, the time evolution operator for a t : ℝ, A.timeEvolution t is defined as exp(- I t /ℏ * A.Ham). Still a map.

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      The matrix representation of the time evolution operator in a given basis. Given a Planck constant , the matrix is a self-adjoint n × n matrix describing the timeEvolution.

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        An instance of timeEvolutionmatrix over the standard basis.

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