2022
DOI: 10.1098/rsta.2022.0301
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Dynamical invariant formalism of shortcuts to adiabaticity

Abstract: We give a pedagogical introduction to dynamical invariant formalism of shortcuts to adiabaticity. For a given operator form of the Hamiltonian with undetermined coefficients, the dynamical invariant is introduced to design the coefficients. We discuss how the method allows us to mimic adiabatic dynamics and describe a relation to the counterdiabatic formalism. The equation for the dynamical invariant takes a familiar form and is often used in various fields of physics. We introduce examples of Lax pair, quantu… Show more

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Cited by 2 publications
(4 citation statements)
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“…It is also notable that the left-hand side of equation (6) in the classical limit can be regarded as the total derivative of a classical quantity (see, e.g. [58]). It was shown that the solution of the Schrödinger equation (1) can be expressed as…”
Section: Lewis-riesenfeld Theorymentioning
confidence: 99%
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“…It is also notable that the left-hand side of equation (6) in the classical limit can be regarded as the total derivative of a classical quantity (see, e.g. [58]). It was shown that the solution of the Schrödinger equation (1) can be expressed as…”
Section: Lewis-riesenfeld Theorymentioning
confidence: 99%
“…The integer K is known as the Krylov dimension and it satisfies K ⩽ D 2 − D + 1. By using the Krylov basis, fictitious time evolution of the operator Ô0 = ∂ t Ĥ(t)/b 0 in the Heisenberg picture, Ô(s) = Û † fic (s) Ô0 Ûfic (s), which appears in equation (58), can be expanded as…”
Section: Then We Can Express a Trial Counterdiabatic Hamiltonian Asmentioning
confidence: 99%
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