quantum algorithms:
A parameterized quantum system is a quantum system depending on “external” or “classical” parameters.
In typical examples arising in quantum mechanics, this simply means that the Hamiltonian is not just one fixed linear operator on a given Hilbert space of quantum states , but a continuous (or suitably smooth) map
of such, from some topological “parameter space” .
More abstractly, where a single quantum system is described by linear type theory (see also at quantum logic), a parameterized quantum system is described by dependent linear type theory.
The quantum adiabatic theorem says that/how the evolution of a parameterized quantum system under sufficiently slow movement of the external parameters remains in an eigenstate for a given system of commuting quantum observables. The remaining transformations on these eigenspaces are known as (non-abelian) Berry phases. These are used as quantum gates in adiabatic quantum computation.
For example, time-dependent Hamiltonians/quantum systems are described this way for interpreted as the space of time-parameters.
See also at Dyson formula.
In some models of braid group statistics (see there for more) the anyons are defects/solitons whose positions serve as external parameters of the system, so that the (non-abelian) Berry phases under their adibatic moverment constitutes a braid group representation on the quantum system‘s ground states.
Discussion of classically-parameterized quantum circuits:
(…)
Discussion of quantumly-parameterized quantum circuits:
following
Guillaume Verdon, Jason Pye, Michael Broughton, A Universal Training Algorithm for Quantum Deep Learning [arXiv:1806.09729]
Prasanth Shyamsundar, Non-Boolean Quantum Amplitude Amplification and Quantum Mean Estimation [arXiv:2102.04975]
Last revised on March 29, 2023 at 16:52:40. See the history of this page for a list of all contributions to it.