2019
DOI: 10.1007/978-3-319-95987-0_17
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Conducting Polymers and Composites

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Cited by 6 publications
(9 citation statements)
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“…The effect of g -strain is very small at the X-band EPR used; however, it was taken into account when calculating the spectra. Besides, polarons forming in adjacent polymer chains, starting with some critical concentration, can, in principle, collapse into interchain mobile diamagnetic P mob +• P mob +• or intrachain localized paramagnetic P loc –• P loc +• bipolarons with equal g -factors. , The transition polaron ↔ bipolaron can change the experimental LEPR spectra as well. To separate the contributions of different charge carriers into the sum LEPR spectra and to analyze their changes at different experimental conditions, such spectra should be deconvoluted according to the procedure described earlier. , In Figure , the dashed lines represent the effective LEPR spectra and their spectral contributions due to polarons P PANI +• and P +• stabilized in the PANI and photoinitiated in copolymer matrices, respectively, as well as mobile pairs of polarons and methanofullerene radical anions P mob +• mF mob –• photoinitiated in the copolymer backbone of the samples by white light with T c = 3300 K. This allowed one to obtain separately the main magnetic resonance, electron relaxation, and dynamic parameters for all spins at a wide variation of experimental conditions.…”
Section: Resultsmentioning
confidence: 99%
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“…The effect of g -strain is very small at the X-band EPR used; however, it was taken into account when calculating the spectra. Besides, polarons forming in adjacent polymer chains, starting with some critical concentration, can, in principle, collapse into interchain mobile diamagnetic P mob +• P mob +• or intrachain localized paramagnetic P loc –• P loc +• bipolarons with equal g -factors. , The transition polaron ↔ bipolaron can change the experimental LEPR spectra as well. To separate the contributions of different charge carriers into the sum LEPR spectra and to analyze their changes at different experimental conditions, such spectra should be deconvoluted according to the procedure described earlier. , In Figure , the dashed lines represent the effective LEPR spectra and their spectral contributions due to polarons P PANI +• and P +• stabilized in the PANI and photoinitiated in copolymer matrices, respectively, as well as mobile pairs of polarons and methanofullerene radical anions P mob +• mF mob –• photoinitiated in the copolymer backbone of the samples by white light with T c = 3300 K. This allowed one to obtain separately the main magnetic resonance, electron relaxation, and dynamic parameters for all spins at a wide variation of experimental conditions.…”
Section: Resultsmentioning
confidence: 99%
“…Besides, polarons forming in adjacent polymer chains, starting with some critical concentration, can, in principle, collapse into interchain mobile diamagnetic P mob +• ↔ P mob +• or intrachain localized paramagnetic P loc −• ↔ P loc +• bipolarons with equal g-factors. 67,68 The transition polaron ↔ bipolaron can change the experimental LEPR spectra as well. To separate the contributions of different charge carriers into the sum LEPR spectra and to analyze their changes at different experimental conditions, such spectra should be deconvoluted according to the procedure described earlier.…”
Section: Resultsmentioning
confidence: 99%
“…60 To confirm this supposition, it would be important to obtain also respective correlations of magnetic resonant, spin and dynamic parameters of mobile and localized charge carriers with molecular and structural properties of the initial and doped composites, as well as with the exciting photon energy. It should also to analyze a possible formation of localized polaron pairs P loc +• ↔ P loc −• with equal energetic and magnetic resonant parameters 61 as well as diamagnetic bipolarons each potentially dissociating into spin polaron couples, BP 2+ ↔ 2P +• in polymer composite matrices, 62,63 including P3DDT. 64 Some charge carriers captured by spin traps can also be released from the latter when interacting with light photons of a certain energy.…”
Section: Resultsmentioning
confidence: 99%
“…This allows the conclusion in this and analogous systems of spin tunneling within the framework of the Miller–Abrahams model in parallel with their intrachain hopping, which depends on spin traps and also on their exchange interaction with the nearest spin ensembles. One should, however, take into account a possible initial formation in the composites of pairs of localized oppositely charged polarons P loc +• ↔ P loc –• with equal energy and g -factors and diamagnetic bipolarons which are able to dissociate into spin polaron couples, BP 2+ ↔2 P +• . The combination of these processes could also initiate the appearance of the above-mentioned term in the temperature dependences obtained.…”
Section: Resultsmentioning
confidence: 99%
“…It should be noted that the appearance occurred only after some time in the dependencies shown in Figure of the bell-like component as in the case of other polymer:fullerene composites. , Assuming the presumption of formation of an equal quantity of positively and negatively charged carriers upon excitons’ dissociation, some reasons for such effect can be proposed. Dissociation of some diamagnetic bipolarons into polaron pairs and/or formation in composites of pairs of localized oppositely charged polarons P loc +• ↔ P loc –• with equal energy and g -factors are possible . Spin-dependent and trap-controlled reversible transition P loc +• ↔ P mob +• can also provoke such dependence .…”
Section: Resultsmentioning
confidence: 99%