2018
DOI: 10.1039/c7sc04221c
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Dynamics of recombination via conical intersection in a semiconductor nanocrystal

Abstract: The ultrafast dynamics of nonradiative recombination at dangling bond defects is elucidated by nanoscale multireference ab initio molecular dynamics simulations.

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Cited by 28 publications
(45 citation statements)
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“…It is well established that the ultrafast nonradiative relaxation of molecules often occurs at conical intersections (CIs), points of degeneracy between potential energy surfaces (PES). , Upon passage through such CIs, electronic energy is converted into vibrational energy along specific branching modes, which lift the degeneracy between PESs. These modes promote the progress of a photochemical reaction toward a particular product following nonradiative decay. , CIs associated with surface defect sites have been implicated in the nonradiative recombination of semiconductor nanocrystals, and the role of branching modes in driving the nonradiative recombination dynamics in silicon dangling bond defects has been explored …”
mentioning
confidence: 99%
“…It is well established that the ultrafast nonradiative relaxation of molecules often occurs at conical intersections (CIs), points of degeneracy between potential energy surfaces (PES). , Upon passage through such CIs, electronic energy is converted into vibrational energy along specific branching modes, which lift the degeneracy between PESs. These modes promote the progress of a photochemical reaction toward a particular product following nonradiative decay. , CIs associated with surface defect sites have been implicated in the nonradiative recombination of semiconductor nanocrystals, and the role of branching modes in driving the nonradiative recombination dynamics in silicon dangling bond defects has been explored …”
mentioning
confidence: 99%
“…where and denote the electronic and nuclear equation of motion from κSE, as given in eqs 12 and 21, and where the additional terms are decay-of-mixing (DM) terms, which are explained in detail elsewhere. 48,53 In tCSDM decoherence contribution to the change in the nuclear momentum is 53 (24) in which is the decoherence time, K is the pointer state, and is the decoherence vector for states I and K given by (25) where is the internal vibrational momentum, and a0 ≡ 1 bohr.…”
Section: Theorymentioning
confidence: 99%
“…1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19 Recent advances on these topics have enabled quantitative accurate simulations for medium-size molecules and qualitatively accurate simulations for nano-sized molecules or clusters. 20,21,22,23,24,25,26,27,28,29,30,31 The electronic structure must be treated quantum mechanically, and for simulating all but the smallest systems, one uses a semiclassical treatment of nuclear motion. The present article is concerned with direct dynamics, where, instead of requiring parametrized analytic functions for the energies and couplings, all required energies, forces, and couplings for each geometry that is important for evaluating dynamical properties are obtained directly from electronic structure calculations when they are needed in the dynamics calculation.…”
Section: Introductionmentioning
confidence: 99%
“…[41][42][43][44] For the truly multiconfigurational approaches, the computational cost is enormous and these techniques are not readily used to study interfacial electronic structure (though see recent work of Levine et al for an interesting CAS calculation of dangling bonds on a silicon cluster). 56 At this point, it should be clear to the reader that strong approximations will be necessary in order to practically and robustly solve for the electronic structure of a molecule reacting on a metal surface, while capturing enough correlation energy for even qualitative (and ideally quantitative) accuracy. In order to achieve such a goal, in this paper, we will follow a three-pronged approach.…”
Section: Introductionmentioning
confidence: 99%