Selective excitation of atomic-scale dynamics by coherent exciton motion in the non-born–Oppenheimer regime
Time-domain investigations of the nonadiabatic coupling between electronic and vibrational degrees of freedom have focused primarily on the formation of electronic superpositions induced by atomic motion. The effect of electronic nonstationary-state dynamics on atomic motion remains unexplored. H...
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Main Authors: | , , , , , |
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Other Authors: | |
Format: | Article |
Language: | English |
Published: |
2014
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Subjects: | |
Online Access: | https://hdl.handle.net/10356/101655 http://hdl.handle.net/10220/18680 |
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Institution: | Nanyang Technological University |
Language: | English |
Summary: | Time-domain investigations of the nonadiabatic coupling between
electronic and vibrational degrees of freedom have focused primarily on the formation
of electronic superpositions induced by atomic motion. The effect of electronic
nonstationary-state dynamics on atomic motion remains unexplored. Here, phasecoherent
excitation of the two lowest electronic transitions in semiconducting singlewalled
carbon nanotubes by broadband <5-fs pulses directly triggers coherent exciton
motion along the axis of the nanotubes. Optical pump−probe spectroscopy with sub-10-fs
time resolution reveals that exciton motion selectively excites the high-frequency G mode
coherent phonon, in good agreement with results obtained from time-domain ab initio
simulations. This observed phenomenon arises from the direct modulation of the C−C
interatomic potential by coherent exciton motion on a time scale that is commensurate
with atomic motion. Our results suggest the possibility of employing light-field
manipulation of electron densities in the non-Born−Oppenheimer regime to initiate
selective atomic motion. |
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