2016
DOI: 10.1063/1.4959962
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The adiabatic limit of the exact factorization of the electron-nuclear wave function

Abstract: Exact solutions of a particle in a box with a delta function potential: The factorization method Am. J. Phys. 78, 839 (2010) We propose a procedure to analyze the relation between the exact factorization of the electron-nuclear wave function and the Born-Oppenheimer approximation. We define the adiabatic limit as the limit of infinite nuclear mass. To this end, we introduce a unit system that singles out the dependence on the electron-nuclear mass ratio of each term appearing in the equations of the exact fact… Show more

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Cited by 57 publications
(66 citation statements)
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“…25,26 The discussed methods can be still improved, e.g. along the lines of a more accurate factorization method such as the exact factorization 5456 known for electron–nuclear problems, or trajectory based methods 50,57 can be applied to simulate such systems dynamically. This work has direct implications on more complex correlated matter-photon problems that can be approximately solved employing the cavity Born–Oppenheimer approximation to better understand complex correlated light-matter coupled systems.…”
Section: Summary and Outlookmentioning
confidence: 99%
“…25,26 The discussed methods can be still improved, e.g. along the lines of a more accurate factorization method such as the exact factorization 5456 known for electron–nuclear problems, or trajectory based methods 50,57 can be applied to simulate such systems dynamically. This work has direct implications on more complex correlated matter-photon problems that can be approximately solved employing the cavity Born–Oppenheimer approximation to better understand complex correlated light-matter coupled systems.…”
Section: Summary and Outlookmentioning
confidence: 99%
“…6 This limitation is only due to numerical reasons, as the TDPEC is defined everywhere in space. 7 The interested reader can consult for example References 36,41,85-87 for discussions on the importance of adequately selecting initial conditions for nonadiabatic dynamics. 8 Methods employing coupled trajectories, as those described in Section 5.1.1 for example, or methods based on TBFs would naturally include such decoherence effects.…”
Section: Applications Of Nonadiabatic Molecular Dynamicsmentioning
confidence: 99%
“…We call both (24) and (26) the clock-dependent Schrödinger equation (CDSE) in analogy to the TDSE, because they become TDSEs if the classical limit for the clock is taken. How to take this classical limit is discussed in [15], and we only sketch here the steps that need to be done, using some results of an analysis of the adiabatic limit in the Exact Factorization [37]. First, we introduce a parameter µ := m/M which is the ratio of the mass of the system to that of the clock.…”
Section: Of the Vector Potential A Such Thatmentioning
confidence: 99%
“…the change of the scalar potential (R) when the classical limit is taken or how to perform the classical limit in a gauge invariant way, i.e., including the vector potential A(R). While some of those details are explained in [15,37], some are still open problems and may be rewarding topics for future research. We need not be concerned with them here, however, because we keep the clock fully quantum mechanical and derive the continuity equation for such a quantum clock.…”
Section: Of the Vector Potential A Such Thatmentioning
confidence: 99%
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