메뉴 건너뛰기




Volumn 112, Issue 22, 2008, Pages 8408-8418

Nature of charge carriers in long doped oligothiophenes: The effect of counterions

Author keywords

[No Author keywords available]

Indexed keywords

COUNTER-IONS; DICATIONS; OLIGO-THIOPHENE; OLIGOTHIOPHENES;

EID: 53549096243     PISSN: 19327447     EISSN: 19327455     Source Type: Journal    
DOI: 10.1021/jp7111582     Document Type: Article
Times cited : (53)

References (92)
  • 1
    • 0004139257 scopus 로고    scopus 로고
    • Müllen, K, Wegner, G, Eds, Wiley-VCH: Weinheim, Germany
    • (a) Electronic Materials: The Oligomer Approach; Müllen, K., Wegner, G., Eds.; Wiley-VCH: Weinheim, Germany, 1998.
    • (1998) Electronic Materials: The Oligomer Approach
  • 2
    • 0003471459 scopus 로고    scopus 로고
    • Fichou, D, Ed, Wiley-VCH: Weinheim, Germany
    • (b) Handbook of Oligo- and Polythiophenes; Fichou, D., Ed.; Wiley-VCH: Weinheim, Germany, 1999.
    • (1999) Handbook of Oligo- and Polythiophenes
  • 3
    • 0003714767 scopus 로고    scopus 로고
    • 2nd ed, Skotheim, T. A, Elsenbaumer, R. L, Reynolds, J. R, Eds, Marcel Dekker: New York
    • (c) Handbook of Conducting Polymers, 2nd ed.; Skotheim, T. A., Elsenbaumer, R. L., Reynolds, J. R., Eds.; Marcel Dekker: New York, 1998.
    • (1998) Handbook of Conducting Polymers
  • 7
  • 27
    • 53549108123 scopus 로고    scopus 로고
    • Mozer, A. J.; Sariciftci, N. S. In Handbook of Conducting Polymers. Conjugated Polymers: processing and applications, 3nd ed.; Skotheim, T. A., Reynolds, J. R., Eds.; CRC Press: Boca Raton, FL, 2007; Chapter 10, p 10-1.
    • Mozer, A. J.; Sariciftci, N. S. In Handbook of Conducting Polymers. Conjugated Polymers: processing and applications, 3nd ed.; Skotheim, T. A., Reynolds, J. R., Eds.; CRC Press: Boca Raton, FL, 2007; Chapter 10, p 10-1.
  • 62
    • 53549102571 scopus 로고    scopus 로고
    • Frisch, M. J, Trucks, G. W, Schlegel, H. B, Scuseria, G. E, Robb, M. A, Cheeseman, J. R, Montgomery, J. A, Jr, Vreven, T, Kudin, K. N, Burant, J. C, Millam, J. M, Iyengar, S. S, Tomasi, J, Barone, V, Mennucci, B, Cossi, M, Scalmani, G, Rega, N, Petersson, G. A, Nakatsuji, H, Hada, M, Ehara, M, Toyota, K, Fukuda, R, Hasegawa, J, Ishida, M, Nakajima, T, Honda, Y, Kitao, O, Nakai, H, Klene, M, Li, X, Knox, J. E, Hratchian, H. P, Cross, J. B, Adamo, C, Jaramillo, J, Gomperts, R, Stratmann, R. E, Yazyev, O, Austin, A. J, Cammi, R, Pomelli, C, Ochterski, J. W, Ayala, P. Y, Morokuma, K, Voth, G. A, Salvador, P, Dannenberg, J. J, Zakrzewski, V. G, Dapprich, S, Daniels, A. D, Strain, M. C, Farkas, O, Malick, D. K, Rabuck, A. D, Raghavachari, K, Foresman, J. B, Ortiz, J. V, Cui, Q, Baboul, A. G, Clifford, S, Cioslowski, J, Stefanov, B. B, Liu, G, Liashenko, A, Piskorz, P, Komaromi, I, Martin, R. L, Fox, D. J, Keith, T, Al-L
    • Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M. A.; Cheeseman, J. R.; Montgomery, J. A., Jr.; Vreven, T.; Kudin, K. N.; Burant, J. C.; Millam, J. M.; Iyengar, S. S.; Tomasi, J.; Barone, V.; Mennucci, B.; Cossi, M.; Scalmani, G.; Rega, N.; Petersson, G. A.; Nakatsuji, H.; Hada, M.; Ehara, M.; Toyota, K.; Fukuda, R.; Hasegawa, J.; Ishida, M.; Nakajima, T.; Honda, Y.; Kitao, O.; Nakai, H.; Klene, M.; Li, X.; Knox, J. E.; Hratchian, H. P.; Cross, J. B.; Adamo, C.; Jaramillo, J.; Gomperts, R.; Stratmann, R. E.; Yazyev, O.; Austin, A. J.; Cammi, R.; Pomelli, C.; Ochterski, J. W.; Ayala, P. Y.; Morokuma, K.; Voth, G. A.; Salvador, P.; Dannenberg, J. J.; Zakrzewski, V. G.; Dapprich, S.; Daniels, A. D.; Strain, M. C.; Farkas,. O.; Malick, D. K.; Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Ortiz, J. V.; Cui, Q.; Baboul, A. G.; Clifford, S.; Cioslowski, J.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz, P.; Komaromi, I.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.; Peng, C. Y.; Nanayakkara, A.; Challacombe, M.; Gill, P. M. W.; Johnson, B.; Chen, W.; Wong, M. W.; Gonzalez, C.; Pople, J. A. Gaussian 03, Revision C.02; Gaussian, Inc.: Wallingford, CT, 2004.
  • 67
    • 53549120292 scopus 로고    scopus 로고
    • 2 values that differ from 0 (pure singlet) or 2 (pure triplet).
    • 2 values that differ from 0 (pure singlet) or 2 (pure triplet).
  • 69
    • 53549086219 scopus 로고    scopus 로고
    • Correlated ab initio methods can not be used in this study because they can be applied only to relatively small molecules, and polaron- bipolaron equilibrium is not observed for small systems (such as 8T2, The DFT and HF levels of theory are the only practical options available for studying doped oligothiophenes of sufficient length to enable the transition from bipolaron to polaron-pair to be observed. The HF level is inapplicable to the study of oligothiophene dications (as well as other charged conjugated systems) due to the huge spin contamination obtained if a pure HF wave function is used.19
    • 19
  • 75
    • 53549087044 scopus 로고    scopus 로고
    • We have tested the applicability of the broken-symmetry B3LYP/6-31G(d) level to appropriately describe oligothiophene dications by comparing it to CASSCF results.21 Both methods agreed qualitatively on the relative energies of singlet and triplet oligothiophene dications and on the electronic structure (bipolaron versus polaron pair) of the dications
    • 21 Both methods agreed qualitatively on the relative energies of singlet and triplet oligothiophene dications and on the electronic structure (bipolaron versus polaron pair) of the dications.
  • 78
    • 53549083868 scopus 로고    scopus 로고
    • The position of counterion in-plane with the oligothiophene chains was found to be true minima according to frequency analysis of 8T+Cl 3, see Supporting Information
    • - (see Supporting Information).
  • 79
    • 53549106438 scopus 로고    scopus 로고
    • -.
    • -.
  • 80
    • 2942656823 scopus 로고    scopus 로고
    • Wave function instability can be expected for low HOMO-LUMO gap systems as the number of conjugated double bonds increases. Wave function instability has been observed previously for bare oligothíophene dications. 18,21 Similarly, RHF-UHF wave function instability has been predicted for other types of long conjugated systems, such as oligoacenes starting from hexacene at B3LYP/6-31Gd, see Bendikov, M, Duong, H. M, Starkey, K, Houk, K. N, Carter, E. A, Wudl, F. J. Am. Chem. Soc. 2004, 126, 7416
    • 18,21 Similarly, RHF-UHF wave function instability has been predicted for other types of long conjugated systems, such as oligoacenes starting from hexacene at B3LYP/6-31G(d); see Bendikov, M.; Duong, H. M.; Starkey, K.; Houk, K. N.; Carter, E. A.; Wudl, F. J. Am. Chem. Soc. 2004, 126, 7416.
  • 81
    • 53549100272 scopus 로고    scopus 로고
    • When the C1-C2 and C3-C4 bonds of a thiophene ring (Scheme 1) are shorter than the C2-C 3 bond (so producing a A-shaped pattern in the sets of three linked data points shown in Figure 3, the ring is considered aromatic. By contrast, when the C1-C2 and C3-C4 bonds of a thiophene ring are longer than the C2-C3 bond (thus, producing a V-shaped pattern in the sets of three linked data points shown the Figure 3, the ring is considered quinoid Scheme 1
    • 3 bond (thus, producing a V-shaped pattern in the sets of three linked data points shown the Figure 3), the ring is considered quinoid (Scheme 1).
  • 82
    • 53549085507 scopus 로고    scopus 로고
    • BLA patterns for other isomers are available in Supporting Information
    • BLA patterns for other isomers are available in Supporting Information.
  • 83
    • 53549132889 scopus 로고    scopus 로고
    • 2 are presented in Supporting Information.
    • 2 are presented in Supporting Information.
  • 84
    • 53549102007 scopus 로고    scopus 로고
    • The fact that α and β orbitals are mirror images of each other resembles frontier orbital picture of long oligoacenes that correspond to disjoint diradicals; see ref 43 and references therein
    • The fact that α and β orbitals are mirror images of each other resembles frontier orbital picture of long oligoacenes that correspond to disjoint diradicals; see ref 43 and references therein.
  • 88
    • 53849132691 scopus 로고    scopus 로고
    • in press DOI: 10.1002/chem.200701182
    • Zade, S. S.; Bendikov, M. Chem. Eur. J. 2008, 14, in press (DOI: 10.1002/chem.200701182).
    • (2008) Chem. Eur. J , vol.14
    • Zade, S.S.1    Bendikov, M.2
  • 89
    • 53549131610 scopus 로고    scopus 로고
    • (51 ) The shortest oligothiophene length at which a bipolaron will become unstable and dissociate into two polarons (a polaron-pair) will depend (and might even strongly depend) on the level of theory used (see Theoretical Methods and the discussion about charge distribution). However, it is clear that the bipolaron will be unstable and will dissociate into two polarons at some oligothiophene length.
    • (51 ) The shortest oligothiophene length at which a bipolaron will become unstable and dissociate into two polarons (a polaron-pair) will depend (and might even strongly depend) on the level of theory used (see Theoretical Methods and the discussion about charge distribution). However, it is clear that the bipolaron will be unstable and will dissociate into two polarons at some oligothiophene length.
  • 90
    • 53549092833 scopus 로고    scopus 로고
    • We note that the charge distribution pattern in oligothiophene cation radicals is significantly dependent on the amount of HF exchange used. Localization of charges is proportional to the amount of HF exchange with charge distribution very localized at the HF level and practically completely delocalized at pure DFT levels (Zade, S. S, Bendikov, M, unpublished. Similar conclusions were also drawn for oligo(phenylene vinylene) cation radicals; see Geskin, V. M, Grozema, F. C, Siebbeles, L. D. A, Bejonne, D, Brédas, J. L, Cornil, J. J. Phys. Chem. B 2005,109,20237, Although presently it is unclear which theoretical method reproduces the charge distribution partem correctly, it was also observed that for polyacetylene chains in the presence of counterions different levels of theory such as HF, MP2, and B3LYP provide similar bond length alternation and charge distribution patterns.25
    • 25
  • 91
    • 53549101742 scopus 로고    scopus 로고
    • Unsurprisingly, extrapolation of eqs. 1 and 5 to infinite chain lengths results in an energetic degeneracy between the dication vs. two monocations and between divalent vs. two monovalent salts (Figure 5a).
    • Unsurprisingly, extrapolation of eqs. 1 and 5 to infinite chain lengths results in an energetic degeneracy between the dication vs. two monocations and between divalent vs. two monovalent salts (Figure 5a).
  • 92
    • 53549130514 scopus 로고    scopus 로고
    • Preliminary estimation of solvent effect on the electronic structure of divalent oligothiophene salts was performed using PCM approximation. Inclusion of solvent favor the polaron pair state over the bipolaron state even more strongly compared to gas phase calculations of divalent oligothiophene salts (Zamoshchik, N.; Salzner, U.; Bendikov, M., unpublished).
    • Preliminary estimation of solvent effect on the electronic structure of divalent oligothiophene salts was performed using PCM approximation. Inclusion of solvent favor the polaron pair state over the bipolaron state even more strongly compared to gas phase calculations of divalent oligothiophene salts (Zamoshchik, N.; Salzner, U.; Bendikov, M., unpublished).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.