Fluorescence Enhancement of Phenanthro[9,10-d]imidazole Hosts
in all calculations. The final R indices [IϾ2σ(I)], R1 = 0.121,
wR(F2) = 0.273.
tion interaction), which includes the configuration with one elec-
tron excited from any occupied orbital to any unoccupied orbital,
where 225 configurations were considered [keyword CI (15 15)].
Crystal of 1·(CH3COOH)2: The transmission factors ranged from
0.97 to 1.00. The crystal structure was solved by direct methods by
using SAPI91.[19] The structures were expanded by using Fourier
techniques.[18] The non-hydrogen atoms were refined anisotropi-
cally. Some hydrogen atoms were refined isotropically; the rest were
fixed geometrically and not refined. Crystallographic data:
Acknowledgments
This work was partially supported by a Grant-in-Aid for Science
and Research from the Ministry of Education, Science, Sport and
Culture of Japan (Grant 21550181) and by a Special Research
Grant for Green Science from Kochi University.
C29H31N3O4,
M = 485.58, triclinic, a = 11.423(1) Å, b =
14.126(2) Å, c = 8.770(2) Å, α = 105.92(1)°, β = 105.44(1)°, γ =
83.68(1)°, U = 1310.7(4) Å3, ρcalcd. = 1.230 gcm–3, T = 296.2 K,
–1
¯
space group P1 (no.2), Z = 2, µ(Mo-Kα) = 0.83 cm , 4880 reflec-
tions measured, 4627 unique (Rint = 0.030), which were used in all
calculations. The final R indices [IϾ2σ(I)], R1 = 0.085, wR(F2) =
0.207.
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Crystal of 1·(CH3CH2COOH)2: The transmission factors ranged
from 0.99 to 1.00. The crystal structure was solved by direct meth-
ods by using SAPI91.[19] The structures were expanded by using
Fourier techniques.[18] The non-hydrogen atoms were refined aniso-
tropically. Some hydrogen atoms were refined isotropically; the rest
were fixed geometrically and not refined. Crystallographic data:
C31H35N3O4,
M = 513.64, triclinic, a = 11.712(2) Å, b =
13.955(2) Å, c = 9.611(2) Å, α = 107.03(1)°, β = 108.59(2)°, γ =
84.76(1)°, U = 1423.6(5) Å3, ρcalcd. = 1.198 gcm–3, T = 296.2 K,
–1
¯
space group P1 (no.2), Z = 2, µ(Mo-Kα) = 0.80 cm , 5272 reflec-
tions measured, 5007 unique (Rint = 0.012), which were used in all
calculations. The final R indices [IϾ2σ(I)], R1 = 0.073, wR(F2) =
0.193.
Crystal of 1·[CH3CH2C(CH2)2COOH]2: The transmission factors
ranged from 0.97 to 1.00. The crystal structure was solved by direct
methods by using SIR92.[17] The structures were expanded by using
Fourier techniques.[18] The non-hydrogen atoms were refined aniso-
tropically. Some hydrogen atoms were refined isotropically; the rest
were fixed geometrically and not refined. Crystallographic data:
C37H47N3O4, M = 597.80, orthorhombic, a = 22.296(5) Å, b =
27.49(1) Å, c = 11.342(4) Å, U = 6951(2) Å3, ρcalcd. = 1.141 gcm–3,
T = 296.2 K, space group Pbca (no.61), Z = 8, µ(Mo-Kα) =
0.74 cm–1, 6125 reflections measured, 6123 unique (Rint = 0.083),
which were used in all calculations. The final R indices [IϾ2σ(I)],
R1 = 0.097, wR(F2) = 0.252.
Crystal of 1·[HOOC(CH2)8COOH]2: The transmission factors
ranged from 0.96 to 1.00. The crystal structure was solved by direct
methods by using SIR92.[17] The structures were expanded by using
Fourier techniques.[18] The non-hydrogen atoms were refined aniso-
tropically. Some hydrogen atoms were refined isotropically; the rest
were fixed geometrically and not refined. Crystallographic data:
C30H32N3O2, M = 466.6, monoclinic, a = 10.819(4) Å, b =
18.650(3) Å, c = 13.063(3) Å, β = 102.89(2)°, U = 2569(1) Å3, ρcalcd.
= 1.206 gcm–3, T = 296.2 K, space group P21/c (no.14), Z = 4,
µ(Mo-Kα) = 0.76 cm–1, 4765 reflections measured, 4514 unique
(Rint = 0.049), which were used in all calculations. The final R in-
dices [IϾ2σ(I)], R1 = 0.075, wR(F2) = 0.219.
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1999, 64, 6566–6574.
Computational Methods: The semiempirical calculations were car-
ried out with the WinMOPAC Ver. 3.9 package (Fujitsu, Chiba,
Japan). Geometry calculations in the ground state were made by
using the AM1 method.[15] All geometries were completely opti-
mized (keyword PRECISE) by the eigenvector following routine
(keyword EF). Experimental absorption spectra of the eight com-
pounds were compared with their absorption data by the semiem-
pirical method CNDO/S (intermediate neglect of differential over-
lap/spectroscopic).[14] All CNDO/S calculations were performed by
using single excitation full SCF/CI (self-consistent field/configura-
[14] a) J. E. Ridley, M. C. Zerner, Theor. Chim. Acta 1973, 32, 111–
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Eur. J. Org. Chem. 2009, 5979–5990
© 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
www.eurjoc.org
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