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2h constrained geometries.
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We note that it was recently reported that the reorganization energy of oligothiophenes scales linearly with the square root of n for n, 2-12 at the same level of theory.[26a] It was also noted that the reorganization energy beyond the localization length of the polaron will remain constant and the square root trend will cut off.[26a
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[26a]
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We note, however, that achievement of an "ideally ordered" polymer is currently not a practical possibility, although synthetic methods for synthesis of conjugated polymers with a high degree of order were reported. H. Meng, D. F. Perepichka, M. Bendikov, F. Wudl, G. Z. Pan, W. Yu, W. Dong, S. Brown, J. Am. Chem. Soc. 2003, 125, 15151-15162.
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In experimentally studied doped conducting polymers the polaron length should be shorter than in calculations on gas-phase oligomers, which are performed without the presence of counterion or dopant, For effect of dopant see: N. Zamoshchik, U. Salzner, M. Bendikov, J. Phys. Chem. C. 2007, 112, 8408-8418. However, in the case of active semiconductors in OFETs the polaron length should be similar to that from calculations, since counterions are not present in both calculations and OFET
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In experimentally studied doped conducting polymers the polaron length should be shorter than in calculations on gas-phase oligomers, which are performed without the presence of counterion or dopant, For effect of dopant see: N. Zamoshchik, U. Salzner, M. Bendikov, J. Phys. Chem. C. 2007, 112, 8408-8418. However, in the case of active semiconductors in OFETs the polaron length should be similar to that from calculations, since counterions are not present in both calculations and OFET.
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However, for such a system, the charge density might also be low
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However, for such a system, the charge density might also be low.
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84
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[48] so that oligomers larger than 20-mers might exhibit a linear correlation for reorganization energy versus 1/n.
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[48] so that oligomers larger than 20-mers might exhibit a linear correlation for reorganization energy versus 1/n.
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-
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90
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53849095729
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N→x δL/δN = 0.
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N→x δL/δN = 0.
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-
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91
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0033881239
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Similar results were reported for short oligothiophenes: G. Moro, G. Scalmani, U. Cosentino, D. Pitea, Synth. Met. 2000, 108, 165-172.
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Similar results were reported for short oligothiophenes: G. Moro, G. Scalmani, U. Cosentino, D. Pitea, Synth. Met. 2000, 108, 165-172.
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92
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S. S. Zade, M. Bendikov, unpublished results. For similar studies on oligo(phenylene vinylene) cation radicals, see V. M. Geskin, F. C. Grozema, L. D. A. Siebbeles, D. Beljonne, J. L. Brédas, J. Cornil, J. Phys. Chem. B 2005, 109, 20237-20243.
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S. S. Zade, M. Bendikov, unpublished results. For similar studies on oligo(phenylene vinylene) cation radicals, see V. M. Geskin, F. C. Grozema, L. D. A. Siebbeles, D. Beljonne, J. L. Brédas, J. Cornil, J. Phys. Chem. B 2005, 109, 20237-20243.
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93
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See also ref, 26a
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See also ref. [26a]
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94
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The most detailed theoretical study addressing the dependence of theoretical levels on delocalization in conjugated systems is that of T. Bally, D. A. Hrovat, W. T. Borden, Phys Chem. Chem. Phys. 2000, 2, 3363-3371, who studied the spin distribution in polyenyl radicals. Unfortunately, DFT and HF-based methods are the only practical options to study long oligothiophenes and oligoseleno-phenes
-
The most detailed theoretical study addressing the dependence of theoretical levels on delocalization in conjugated systems is that of T. Bally, D. A. Hrovat, W. T. Borden, Phys Chem. Chem. Phys. 2000, 2, 3363-3371, who studied the spin distribution in polyenyl radicals. Unfortunately, DFT and HF-based methods are the only practical options to study long oligothiophenes and oligoseleno-phenes.
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95
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53849099362
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Note that the second, rough, assumption is solely to simplify the mathematical equations. Our conclusions are also valid for the more realistic situation in which charge is not equally distributed inside the rings, but is equally distributed between all rings
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Note that the second, rough, assumption is solely to simplify the mathematical equations. Our conclusions are also valid for the more realistic situation in which charge is not equally distributed inside the rings, but is equally distributed between all rings.
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96
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