Effect of TiO2 particles on normal and resonance Raman spectra of coumarin 343: a theoretical investigation
It is well known that interfacial structures and charge transfer in dye-sensitized solar cells are extremely important for the enhancement of cell efficiency. Here, the normal Raman spectra (NRS) and resonance Raman spectra (RRS) of a C343-sensitized TiO 2 cluster (Ti 9 O 18 ) are theoretically pred...
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Veröffentlicht in: | Physical chemistry chemical physics : PCCP 2015-04, Vol.17 (16), p.191-1918 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | It is well known that interfacial structures and charge transfer in dye-sensitized solar cells are extremely important for the enhancement of cell efficiency. Here, the normal Raman spectra (NRS) and resonance Raman spectra (RRS) of a C343-sensitized TiO
2
cluster (Ti
9
O
18
) are theoretically predicted from combined electronic structure calculations and a vibrationally-resolved spectral method to reveal the relationship between interfacial geometries and excited-state dynamics. The results show that although the NRS of free C343 and the C343-TiO
2
cluster correspond to the vibrational motions of C343 in a high frequency domain, their mode frequencies show obvious differences due to the interaction of the TiO
2
cluster on C343, and several new Raman active fingerprint modes, such as bidentate chelating bonding modes, can be used to determine interfacial geometries. However, the resonance Raman activities of low-frequency modes are significantly enhanced and several modes from the TiO
2
cluster can be observed, consistent with experimental measurements. Furthermore, the RRS from a locally excited state and a charge transfer state of C343-TiO
2
are dramatically different, for instance, new Raman active modes with 1212 cm
−1
, 1560 cm
−1
and 1602 cm
−1
, corresponding to the motions of CH
2
rocking, C&z.dbd;C/C-N/C&z.dbd;O stretching and C&z.dbd;O/C&z.dbd;C stretching, appear from the charge transfer state. The obtained information on mode-specific reorganization energies from these excited states is greatly helpful to understand and control interfacial electron transfer.
Both the normal Raman spectra (NRS) and resonance Raman spectra (RRS) can be used to figure out the isomers and their interfacial structures. Furthermore, the differences in RRS between the locally excited state and the charge transfer state of C343-TiO
2
are helpful to understand and control the electron transfer at the interface. |
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ISSN: | 1463-9076 1463-9084 |
DOI: | 10.1039/c4cp05794e |