Abstract:In principle, we should not need the time-dependent extension of
density-functional theory (TDDFT) for excitations, and in particular not for
Molecular Dynamics (MD) studies: the theorem by Hohenberg and Kohn teaches us
that for any observable that we wish to look at (including dynamical properties
or observables dependent on excited states) there is a corresponding functional
of the ground-state density. Yet the unavailability of such magic functionals
in many cases (the theorem is a non-constructive existenc… Show more
“…Overall, our findings open the door to include a multitude of quantum chemical concepts and methods into the polaritonic chemistry context, which were successfully developed and applied over the past decades. For example, one can give up our initial dilute system assumptions and start to investigate more realistic and complex chemical setups by including, for example temperature, electron overlap, different orientations, solvent effects, driving laser fields, and much more. , This paves the way to many novel discoveries and applications based on ab initio polaritonic chemistry methods, all of which nurture the hope that by collective strong coupling, unprecedented local control of chemical processes may become within reach.…”
A fundamental question
in the field of polaritonic chemistry is
whether collective coupling implies local modifications of chemical
properties scaling with the ensemble size. Here we demonstrate from
first-principles that an impurity present in a collectively coupled
chemical ensemble features such locally scaling modifications. In
particular, we find the formation of a novel dark state for a nitrogen
dimer chain of variable size, whose local chemical properties are
altered considerably at the impurity due to its embedding in the collectively
coupled environment. Our simulations unify theoretical predictions
from quantum optical models (e.g., collective dark states and bright
polaritonic branches) with the single molecule quantum chemical perspective,
which relies on the (quantized) redistribution of charges leading
to a local hybridization of light and matter. Moreover, our findings
suggest that recently developed
ab initio
methods
for strong light-matter coupling are suitable to access these local
polaritonic effects and provide a detailed understanding of photon-modified
chemistry.
“…Overall, our findings open the door to include a multitude of quantum chemical concepts and methods into the polaritonic chemistry context, which were successfully developed and applied over the past decades. For example, one can give up our initial dilute system assumptions and start to investigate more realistic and complex chemical setups by including, for example temperature, electron overlap, different orientations, solvent effects, driving laser fields, and much more. , This paves the way to many novel discoveries and applications based on ab initio polaritonic chemistry methods, all of which nurture the hope that by collective strong coupling, unprecedented local control of chemical processes may become within reach.…”
A fundamental question
in the field of polaritonic chemistry is
whether collective coupling implies local modifications of chemical
properties scaling with the ensemble size. Here we demonstrate from
first-principles that an impurity present in a collectively coupled
chemical ensemble features such locally scaling modifications. In
particular, we find the formation of a novel dark state for a nitrogen
dimer chain of variable size, whose local chemical properties are
altered considerably at the impurity due to its embedding in the collectively
coupled environment. Our simulations unify theoretical predictions
from quantum optical models (e.g., collective dark states and bright
polaritonic branches) with the single molecule quantum chemical perspective,
which relies on the (quantized) redistribution of charges leading
to a local hybridization of light and matter. Moreover, our findings
suggest that recently developed
ab initio
methods
for strong light-matter coupling are suitable to access these local
polaritonic effects and provide a detailed understanding of photon-modified
chemistry.
“…Most methods which can describe the electron dynamics are often modified versions of their well-known quantumchemical counter parts and neglect the influence of the nuclear motion [19][20][21][22][23] or treat it classically [24][25][26][27]. One of the possibilities to treat both the nuclear and the electron dynamics in a molecular systems is the quantum-mechanical NEMol ansatz [28][29][30][31][32].…”
Photo-initiated processes in molecules often involve complex situations where the induced dynamics is characterized by the interplay of nuclear and electronic degrees of freedom. The interaction of the molecule with an ultrashort laser pulse or the coupling at a conical intersection (CoIn) induces coherent electron dynamics which is subsequently modified by the nuclear motion. The nuclear dynamics typically leads to a fast electronic decoherence but also, depending on the system, enables the reappearance of the coherent electron dynamics. We study this situation for the photo-induced nuclear and electron dynamics in the nucleobase uracil. The simulations are performed with our ansatz for the coupled description of the nuclear and electron dynamics in molecular systems (NEMol). After photo-excitation uracil exhibits an ultrafast relaxation mechanism mediated by CoIn's. Both processes, the excitation by a laser pulse and the non-adiabatic relaxation, are explicitly simulated and the coherent electron dynamics is monitored using our quantum mechanical NEMol approach. The electronic coherence induced by the CoIn is observable for a long time scale due to the delocalized nature of the nuclear wavepacket.
“…Further techniques are based on the coupled propagation of the nuclear and electronic wavefunction on a single time-dependent potential energy surface [30][31][32][33] . But for larger molecular systems the main techniques used are mixed quantum classical representations [34][35][36][37] . For example, the electron dynamics is described using TD-DFT and the nuclear motion is considered using an Ehrenfest approach 34,35 .…”
Section: Introductionmentioning
confidence: 99%
“…But for larger molecular systems the main techniques used are mixed quantum classical representations [34][35][36][37] . For example, the electron dynamics is described using TD-DFT and the nuclear motion is considered using an Ehrenfest approach 34,35 . But these methods do not reflect the quantum nature of the nuclei which, however, becomes important for ultrashort pulse excitation and nonadiabatic transitions.…”
Ultrafast optical techniques allow to study ultrafast molecular dynamics involving both nuclear and electronic motion. To support interpretation, theoretical approaches are needed that can describe both the nuclear and electron dynamics. Hence, we revisit and expand our ansatz for the coupled description of the nuclear and electron dynamics in molecular systems (NEMol). In this purely quantum mechanical ansatz the quantum-dynamical description of the nuclear motion is combined with the calculation of the electron dynamics in the eigenfunction basis. The NEMol ansatz is applied to simulate the coupled dynamics of the molecule NO 2 in the vicinity of a conical intersection (CoIn) with a special focus on the coherent electron dynamics induced by the non-adiabatic coupling. Furthermore, we aim to control the dynamics of the system when passing the CoIn. The control scheme relies on the carrier envelope phase (CEP) of a few-cycle IR pulse. The laser pulse influences both the movement of the nuclei and the electrons during the population transfer through the CoIn.
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