Time-dependent view of an isotope effect in electron-nuclear nonequilibrium dynamics with applications to N2
Time-dependent view of an isotope effect in electron-nuclear nonequilibrium dynamics with applications to N2
复制标题
DOI:
10.1073/pnas.1804455115
复制
发表时间:
2018-05
期刊:
影响因子:
--
通讯作者:
J. Ajay;K. Komarova;F. Remacle;F. Remacle;R. Levine;R. Levine
中科院分区:
文献类型:
--
作者:
J. Ajay;K. Komarova;F. Remacle;F. Remacle;R. Levine;R. Levine
Significance Wide-range isotopic anomalies found in extraterrestrial sources suggest that we seek better mechanistic insights on photochemical processes induced by far UV radiation. To be able to follow the process, we simulate the progress in time of an N2 molecule excited by an ultrafast pulse in the vacuum UV (VUV). Such a short pulse necessarily initiates a nonstationary state of the molecule that we follow in silico. In the VUV, N2 is pumped to a valence excited and Rydberg states. The ultrashort pulse creates a coherent combination of these electronic states, localized in the Franck–Condon region, leading to a dynamical isotope effect. Isotopic fractionation in the photodissociation of N2 could explain the considerable variation in the 14N/15N ratio in different regions of our galaxy. We previously proposed that such an isotope effect is due to coupling of photoexcited bound valence and Rydberg electronic states in the frequency range where there is strong state mixing. We here identify features of the role of the mass in the dynamics through a time-dependent quantum-mechanical simulation. The photoexcitation of N2 is by an ultrashort pulse so that the process has a sharply defined origin in time and so that we can monitor the isolated molecule dynamics in time. An ultrafast pulse is necessarily broad in frequency and spans several excited electronic states. Each excited molecule is therefore not in a given electronic state but in a superposition state. A short time after excitation, there is a fairly sharp onset of a mass-dependent large population transfer when wave packets on two different electronic states in the same molecule overlap. This coherent overlap of the wave packets on different electronic states in the region of strong coupling allows an effective transfer of population that is very mass dependent. The extent of the transfer depends on the product of the populations on the two different electronic states and on their relative phase. It is as if two molecules collide but the process occurs within one molecule, a molecule that is simultaneously in both states. An analytical toy model recovers the (strong) mass and energy dependence.