2015
DOI: 10.1016/j.orgel.2015.06.050
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Electromodulation and magnetomodulation of exciton dissociation in electron donor (starburst amine) : electron acceptor (bathocuproine) system

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Cited by 10 publications
(10 citation statements)
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“…4 ) has been obtained for NP-B1 solar devices with the HWHM equal to B LFE = 55 mT and B HFE = 600 mT while for NP-SQ2 devices B LFE = 17 mT and B HFE = 400 mT. Note that the HWHM of the low field component is much broader than hyperfine field in the EHP model, which is typically ~3 mT in organic compounds 9 10 21 23 . Furthermore, the strong spin-orbit coupling in N719 and B1 dyes induced by the high orbital magnetic field of ruthenium atom switches off the hyperfine field-scale effects 18 23 , therefore, HFM spin-mixing mechanism is rather not appropriate here.…”
Section: Resultsmentioning
confidence: 92%
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“…4 ) has been obtained for NP-B1 solar devices with the HWHM equal to B LFE = 55 mT and B HFE = 600 mT while for NP-SQ2 devices B LFE = 17 mT and B HFE = 400 mT. Note that the HWHM of the low field component is much broader than hyperfine field in the EHP model, which is typically ~3 mT in organic compounds 9 10 21 23 . Furthermore, the strong spin-orbit coupling in N719 and B1 dyes induced by the high orbital magnetic field of ruthenium atom switches off the hyperfine field-scale effects 18 23 , therefore, HFM spin-mixing mechanism is rather not appropriate here.…”
Section: Resultsmentioning
confidence: 92%
“…In the relevant components of the formula (2) representing the low-field (LFE) and high-field (HFE) effects A LFE and A HFE parameters denote the MPC signal magnitudes for , whereas B LFE and B HFE determine the half width (B 1/2 ) at half signal maximum (HWHM) 10 . The relatively good fitting based on double-Lorentzian function (solid lines in Fig.…”
Section: Resultsmentioning
confidence: 99%
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