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Volumn 112, Issue 51, 2008, Pages 13282-13286

EDOT-type materials: Planar but not rigid

Author keywords

[No Author keywords available]

Indexed keywords

CHEMICAL PROPERTIES; MATERIALS PROPERTIES; OPTICAL PROPERTIES; ORGANIC POLYMERS; QUANTUM CHEMISTRY; THIOPHENE;

EID: 58149171795     PISSN: 10895639     EISSN: None     Source Type: Journal    
DOI: 10.1021/jp809632z     Document Type: Article
Times cited : (40)

References (38)
  • 10
    • 33645678475 scopus 로고    scopus 로고
    • Perepichka, I. P.; Roquet, S.; Leriche. P.; Raimundo, J.-M.; Frère, P.; Roncali, J. Chem. Eur. J. 2006, 12, 2960.
    • Perepichka, I. P.; Roquet, S.; Leriche. P.; Raimundo, J.-M.; Frère, P.; Roncali, J. Chem. Eur. J. 2006, 12, 2960.
  • 19
    • 58149158814 scopus 로고    scopus 로고
    • 2 have been recorded in frozen MeTHF at 80 K and in dichloromethane at room T, and have been taken from ref 6. The absorption and emission spectra of 4T have been recorded in tetradecane at 12 and 290 K.
    • 2 have been recorded in frozen MeTHF at 80 K and in dichloromethane at room T, and have been taken from ref 6. The absorption and emission spectra of 4T have been recorded in tetradecane at 12 and 290 K.
  • 20
    • 4243539377 scopus 로고    scopus 로고
    • TURBOMOLE 5.7.1 quantum-chemical package: Electronic Structure Calculations on Workstation Computers: The Program System TUR- BOMOLE. Ahlrichs, R.; Bär, M.; Häser, M.; Horn, H.; Kölmel. C. Chem. Phys. Lett. 1989, 162, 165.
    • TURBOMOLE 5.7.1 quantum-chemical package: Electronic Structure Calculations on Workstation Computers: The Program System TUR- BOMOLE. Ahlrichs, R.; Bär, M.; Häser, M.; Horn, H.; Kölmel. C. Chem. Phys. Lett. 1989, 162, 165.
  • 29
    • 58149152090 scopus 로고    scopus 로고
    • The general recursion formula for displaced distorted harmonic oscillators reads as given in: Henry, B. R.; Siebrand, W. In Organic Molecular Photophxsics; Bilks, J. B., Ed.; John Wiley & Sons Ltd.: Bristol, U.K., 1973; p 218.
    • The general recursion formula for displaced distorted harmonic oscillators reads as given in: Henry, B. R.; Siebrand, W. In Organic Molecular Photophxsics; Bilks, J. B., Ed.; John Wiley & Sons Ltd.: Bristol, U.K., 1973; p 218.
  • 30
    • 0001024508 scopus 로고
    • Acta Physicochem
    • Duschinsky, F. Acta Physicochem. URSS 1937, 7, 551.
    • (1937) URSS , vol.7 , pp. 551
    • Duschinsky, F.1
  • 31
    • 58149148900 scopus 로고    scopus 로고
    • In the case of 4T, the torsional frequencies of the ground state were taken from a non-planar C2 equilibrium geometry because the torsional frequencies of the planar structure were found to be non-real as a result of performing the calculations in vacuo. The suitability of the frequencies of the C2 conformer arises from the almost identical geometries of both structures, and the small dihedral angles between the thiophene rings in the C2 conformer 15-20°
    • 2 conformer (15-20°).
  • 33
    • 58149171072 scopus 로고    scopus 로고
    • The MOshavebeen depicted using the MOLEKEL4.3 program: Flükiger, P.; Lüthi, H. P.; Portmann, S.; Weber, J. Swiss Center for Scientific Computing, Manno, Switzerland, 2000-2002. Portmann, Stefan; Lüthi, Hans Peter. MOLEKEL: An Interactive Molecular Graphics Tool. CHIMIA 2000, 54, 766.
    • The MOshavebeen depicted using the MOLEKEL4.3 program: Flükiger, P.; Lüthi, H. P.; Portmann, S.; Weber, J. Swiss Center for Scientific Computing, Manno, Switzerland, 2000-2002. Portmann, Stefan; Lüthi, Hans Peter. MOLEKEL: An Interactive Molecular Graphics Tool. CHIMIA 2000, 54, 766.
  • 34
    • 58149150616 scopus 로고    scopus 로고
    • 3b'4 with an average of 2.96 Å. The somewhat longer S• O distances (ca. 3.06 Å) in mixed thiophene-EDOT compounds (ref 3b) arise mainly from the fact that the structures are not planar but show torsional dihedral angles of about 14°.
    • 3b'4 with an average of 2.96 Å. The somewhat longer S• O distances (ca. 3.06 Å) in mixed thiophene-EDOT compounds (ref 3b) arise mainly from the fact that the structures are not planar but show torsional dihedral angles of about 14°.
  • 36
    • 58149157117 scopus 로고    scopus 로고
    • For 2EDOT model calculation at the BHLYP/cc-pVTZ level gives α, 124.02°. β, 121.93° for TP and α, 124.00°. β, 121.94° for 90°. Δ, 0.03. For 2T. α, 123.15°, β, 123.36° for TP and α, 122.53. β, 124.11° for 90°, Δ, 1.37 is obtained
    • For 2EDOT model calculation at the BHLYP/cc-pVTZ level gives α = 124.02°. β = 121.93° for TP and α = 124.00°. β = 121.94° for 90°. Δ =-0.03. For 2T. α = 123.15°, β = 123.36° for TP and α = 122.53. β = 124.11° for 90°, Δ =-1.37 is obtained.
  • 37
    • 58149165892 scopus 로고    scopus 로고
    • This attractive force can vary significantly; e.g, Raos et al. 29 calculated A, 0.60 for dimethoxy-substituted 2T
    • 29 calculated A = +0.60 for dimethoxy-substituted 2T.
  • 38
    • 58149168010 scopus 로고    scopus 로고
    • 2h) yields 2.92 Å, not much smaller than the van der Waals distance (3.05 Å).
    • 2h) yields 2.92 Å, not much smaller than the van der Waals distance (3.05 Å).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.