Physics of Organic Semiconductors 2012
DOI: 10.1002/9783527654949.ch9
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Organic Magnetoresistance and Spin Diffusion in Organic Semiconductor Thin‐Film Devices

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Cited by 4 publications
(5 citation statements)
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“…The OMAR response of the Au/BDTT thin film/Au device showed a distinct non-Lorentzian behavior with a relatively larger MR ratio and much wider line width compared to that of the single-crystal one for a wide range of current and temperature (Figure 4b,c). Unlike conventional non-Lorentz fitted OMAR curves, which show a clear down-curving trend when the magnetic field increases (those shapes generally remain the same with various current and temperature, from a few K up to room temperature), 4 the behavior of the thin-filmbased OMAR exhibited a strong dependence on the measurement conditions. We speculate that this abnormal phenomenon is related to the trap-state-induced regulation mechanism in the pure bipolaron model.…”
Section: Resultsmentioning
confidence: 75%
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“…The OMAR response of the Au/BDTT thin film/Au device showed a distinct non-Lorentzian behavior with a relatively larger MR ratio and much wider line width compared to that of the single-crystal one for a wide range of current and temperature (Figure 4b,c). Unlike conventional non-Lorentz fitted OMAR curves, which show a clear down-curving trend when the magnetic field increases (those shapes generally remain the same with various current and temperature, from a few K up to room temperature), 4 the behavior of the thin-filmbased OMAR exhibited a strong dependence on the measurement conditions. We speculate that this abnormal phenomenon is related to the trap-state-induced regulation mechanism in the pure bipolaron model.…”
Section: Resultsmentioning
confidence: 75%
“…The singlecrystal devices show a small B sat of ∼10 mT, and MR curves are in agreement with the saturated Lorentz model (Figure 3b), which are much different from noncrystal materials reported with a saturation magnetic field B sat generally above 50 mT and even with an unsaturated line shape. 4 Considering the non-Lorentzian model is the most commonly used, OMAR curves are also fitted with the non-Lorentz model for comparison (Figure 3c, Table S1). The MR of BDTT single-crystal device decreases slightly as the current increases at a constant temperature (Figure 3b), while as the temperature increases, the MR curves are slightly broadened and the value of MR declines (Figure 3c).…”
Section: Resultsmentioning
confidence: 99%
“…Molecular spintronics, which combines the potential of spintronics and organic electronics is a promising alternative to conventional spintronics with inorganic materials [193]. The mixing of the triplet and singlet states as a result of the hyperfine field (of the hydrogen atoms) in organic semiconductors manifests itself as a large magnetoresistance effect [194,195]. Presumably, if electrical leads could be easily attached to conjugated polymers and molecules in a DAC for magneto-electric measurements, high pressure could serve as a powerful tuning parameter to study spin transport in organic spintronics.…”
Section: Discussionmentioning
confidence: 99%
“…As a result, the electron spin becomes a robust quantity within the OS (namely, it has long spin diffusion length and coherence time). Electron spin diffusion lengths in the range of 5-100 nm have been demonstrated (depending on the experiment, film morphology, temperature); [10][11][12][13] moreover, even longer ~1 μm spin diffusion length have been measured in doped OS. [14] Electron spin coherence times last as long as ~1 μsec.…”
Section: General Overviewmentioning
confidence: 98%