The ballistic regime of vibrational energy transport in oligomeric molecular chains occurs with a constant, often high, transport speed and high efficiency. Such a transport regime can be initiated by exciting a chain end group with a mid-infrared (IR) photon. To better understand the wavepacket formation process, two chemically identical end groups, azido groups with normal, N-, and isotopically substituted, N-, nitrogen atoms, were tested for wavepacket initiation in compounds with alkyl chains of = 5, 10, and 15 methylene units terminated with a carboxylic acid (-a) group, denoted as NC-a and NC-a. The transport was initiated by exciting the azido moiety stretching mode, the ν tag, at 2100 cm (NC-a) or 2031 cm (NC-a). Opposite to the expectation, the ballistic transport speed was found to decrease upon N → N isotope editing. Three mechanisms of the transport initiation of a vibrational wavepacket are described and analyzed. The first mechanism involves the direct formation of a wavepacket via excitation with IR photons of several strong Fermi resonances of the tag mode with the ν + ν combination state while each of the combination state components is mixed with delocalized chain states. The second mechanism relies on the vibrational relaxation of an end-group-localized tag into a mostly localized end-group state that is strongly coupled to multiple delocalized states of a chain band. Harmonic mixing of ν of the azido group with CH wagging states of the chain permits a wavepacket formation within a portion of the wagging band, suggesting a fast transport speed. The third mechanism involves the vibrational relaxation of an end-group-localized mode into chain states. Two such pathways were found for the ν initiation: The ν mode relaxes efficiently into the twisting band states and low-frequency acoustic modes, and the ν mode relaxes into the rocking band states and low-frequency acoustic modes. The contributions of the three initiation mechanisms in the ballistic energy transport initiated by ν tag are quantitatively evaluated and related to the experiment. We conclude that the third mechanism dominates the transport in alkane chains of 5-15 methylene units initiated with the ν tag and the wavepacket generated predominantly at the CH twisting band. The isotope effect of the transport speed is attributed to a larger contribution of the faster wavepackets for NC-a or to the different breadth of the wavepacket within the twisting band. The study offers a systematic description of different transport initiation mechanisms and discusses the requirements and features of each mechanism. Such analysis will be useful for designing novel materials for energy management.
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http://dx.doi.org/10.1021/acs.jpcb.1c03986 | DOI Listing |
PLoS One
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Graduate Institute of Injury Prevention and Control, College of Public Health, Taipei Medical University, Taipei City, Taiwan.
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ISME J
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View Article and Find Full Text PDFSci Rep
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