The effect of H-bonding solvents on the
electronically exited states properties of 7-dimethylamino-4-methyl-coumarin and
psoralens
L.A. Brueva, N.E. Voropaeva, I.V. Sokolova, J.P. Morozova.
One of the most important problems of optics and spectroscopy of poly
atomic molecules is the determination of how the spectral-luminescent properties are
connected with the features of the electronic structure of the molecule. Knowing of such
regularities is that allows one to create compounds with the efficient radiating rate. In
the case of fluorescent probes or biological labels the sensitive reaction of the
fluorophore on the smaller changing of the environment properties is the dominant. The
derivatives of coumarin are those satisfying such requirements. A particularity of the
structure of the coumarins is the high polarizability of such molecules and their high
charge transition rate and high dipole moment values. Representatives of this class take
one of the first places among the most efficient green-blue spectral region laser dyes.
Almost all photochemical and chemical reactions elapse
in the liquid medium. Hence, a complete analysis of the mechanism, kinetics and
thermodynamics of the reaction should include medium influence consideration, i.e.
consideration of the solvatation effects. It is necessary to have a look on the solvent
influence into parameters being measured. A location intensity and shape of the absorption
and emission bands use to depend on the solvent. This dependence is the result of the
molecular interaction forces leading to changing of energy difference between the ground
and the first exited states.
The goal of this investigation is to begin building of the solvation
shells of the 7-dimethylamino-4-methyl-coumarin (coumarin 1) molecule and psoralen
molecule being relative to the coumarin 1 molecule. Psoralens are widely used in medicine.
being combined with the UV-radiation they are successfully used for the cure of skin
maladies.
We regard interaction of these molecules the hydroxil-containing
solvent - the methanol molecule for studying of the solvatation process give a possibility
of prognosis of the molecular spectral properties in the solvent mixtures. Together with
the experimental investigation a quantum-chemical calculation of the 1:1 complexes of
coumarin 1 + methanol and psoralen + methanol, i.e. the first stage of the specific
solvatation was investigates by the means of super molecules method. The theoretical
consideration of electronic structure and spectral properties of aminocoumarin molecules
where carried out by INDO method using the special spectroscopic parametrization
[1]. The result of the quantum-chemical calculations are the level scheme given in Table
1.
Table 1.
State |
Wavelength, nm |
E, eV |
Oscillator strength |
Polarization |
PSORALEN |
S1 pp* |
314.4 |
3.94 |
0.103 |
xy |
S2 np* |
306.9 |
4.04 |
0.007 |
z |
S3 pp* |
284.5 |
4.36 |
0.448 |
xy |
S4 pp* |
250.3 |
4.95 |
0.352 |
xy |
S5 ps* |
250.3 |
4.95 |
0.002 |
z |
S6 ps* |
239.8 |
5.17 |
0.0015 |
z |
COMPLEX |
S1 pp* |
316.5 |
3.92 |
0.109 |
xy |
S2 np* |
304.9 |
4.07 |
0.0004 |
z |
S3 pp* |
289.1 |
4.29 |
0.461 |
xy |
S4 ps* |
253.1 |
4.90 |
0.00006 |
z |
S5 pp* |
253.1 |
4.90 |
0.357 |
z |
COUMARIN 1 |
S1 pp* |
361.5 |
3.43 |
0.708 |
xy |
S2 pp* |
351.3 |
3.53 |
0.266 |
xy |
S3 ps* |
318.6 |
3.89 |
0.008 |
z |
S4 ps* |
307.8 |
4.03 |
0.0001 |
z |
S5 ps*+np* |
300.6 |
4.12 |
0.0003 |
z |
S6 pp* |
265.1 |
4.68 |
0.006 |
z |
COMPLEX |
S1 pp* |
354.1 |
3.50 |
0.605 |
xy |
S2 pp* |
345.0 |
3.59 |
0.409 |
xy |
S3 ps* |
312.8 |
3.96 |
0.0074 |
z |
S4 ps* |
305.7 |
4.06 |
0.00003 |
z |
S5 np* |
269.3 |
4.60 |
0.0004 |
z |
S6 ps* |
267.1 |
4.64 |
0.015 |
z |
From the data of these tables one can see, that the blue shift of the pp*-levels and of the np*-levels
occur when approaching of methanol molecule. But in experiment the red shift of the pp*-levels occur. Also the inversion of 4 and 5 levels is
observed in the case of psoralen and that of 5 and 6 - in the case of coumarin 1. Dipole
moment increases relative to one of the isolated molecule. However, the shifts in spectra
are not large and wrong direction of shift for pp* band,
allowing to conclude that a more complicated complex than of the 1:1 , really arises
consequently, it is necessary to increase an amount of molecules of methanol and to
consider the interaction of nitrogen of diethylamino-group with methanol. The results of
experimental investigation are presented in the graph of the absorption and emission band
shift dependence on the alcohol concentration in the solvent. One sees from the
experimental data that a shift to the lager wave length region when increasing the alcohol
concentration. It seems also, that the shift does occur by the addition of alcohol. It
leads to conclusion that the structure of solvation shell does not fit the structure of
the solvent.
The experiment showed that the absorption band had a complicated form.
Two singlet pp* and one np*
transition were observed.
The capability for intermolecular interaction and the most probable
paths for the approach of the proton or proton-donor solvent are determined with the help
of the method of molecular electrostatic potential (MESP) using wave function obtained by
INDO method [2,3]. the results of this work are present in Table 2 and Table 3.
Table 2 Values of MESP minimums.
State |
MESP minimums,
ccal/mol |
z=0 |
x |
y |
COUMARIN 1 |
S0 |
-129.06 |
5.0 |
3.6 |
6.93 |
-1.9 |
-1.5 |
S1 pp* |
-140.94 |
5.0 C=O |
3.6 |
2.94 |
-1.4 |
-1.6 |
S5 np* |
-24.43 |
-1.4 |
-1.0 |
-12.88 |
1.1 |
-0.9 |
-9.58 |
2.1 |
4.1 |
-3.99 |
5.1 |
-1.8 |
T1 pp* |
-141.06 |
5.0 C=O |
3.6 |
-121.04 |
5.6 |
2.4 |
-20.50 |
5.1 |
-1.3 |
-17.41 |
4.1 |
-0.9 |
COMPLEX |
S0 |
-105.04 |
4.7 C=O |
3.7 |
-86.82 |
5.5 |
2.1 |
-86.80 |
5.6 |
2.3 |
-73.52 |
8.1 |
3.9 |
S1 pp* |
-120.53 |
4.7 C=O |
3.7 |
-105.29 |
5.5 |
2.1 |
-79.28 |
8.1 |
3.8 |
-14.22 |
4.1 |
0.9 |
S5 np* |
-36.12 |
8.1 |
3.9 |
-28.17 |
-1.4 |
-1.0 |
-9.71 |
1.1 |
-0.9 |
-6.28 |
1.8 |
4.1 |
T1 pp* |
-116.56 |
4.7 C=O |
3.7 |
-101.92 |
5.5 |
2.1 |
-78.33 |
8.1 |
3.9 |
|
Table 3 Values of MESP minimums.
State |
MESP minimums,
ccal/mol |
z=0 |
x |
y |
PSORALEN |
S0 |
-117.8 |
5.0 |
3.6 |
-0.27 |
-2.6 |
3.7 |
S1 pp* |
-126.63 |
5.0 C=O |
3.6 |
-1.74 |
4.4 |
-1.5 |
S2 np* |
-28.22 |
-2.4 |
3.6 |
-26.44 |
-1.3 |
-0.9 |
-15.53 |
1.2 |
-1.0 |
-12.69 |
1.0 |
-2.0 |
T1 pp* |
-120.19 |
5.0 C=O |
3.6 |
T2 pp* |
-122.36 |
5.0 |
3.6 |
6.65 |
-2.6 |
3.8 |
COMPLEX |
S0 |
-94.55 |
4.7 C=O |
3.7 |
-74.43 |
8.1 |
2.3 |
-73.99 |
5.6 |
2.3 |
-3.52 |
6.0 |
9.1 |
S1 pp* |
-105.56 |
4.7 C=O |
3.7 |
-87.30 |
5.5 |
2.1 |
-78.61 |
8.1 |
3.9 |
-5.38 |
4.5 |
8.4 |
S2 np* |
-41.89 |
8.1 |
4.0 |
-25.95 |
-2.4 |
3.6 |
-23.78 |
-1.3 |
-0.9 |
-12.38 |
1.2 |
-1.0 |
T1 pp* |
-116.56 |
4.7 C=O |
3.7 |
-101.92 |
5.5 |
2.1 |
-78.33 |
8.1 |
3.9 |
-4.42 |
4.5 |
8.4 |
T2 pp* |
-99.74 |
4.7 C=O |
3.7 |
-80.60 |
5.5 |
2.1 |
-80.54 |
5.6 |
2.3 |
-76.33 |
8.1 |
3.9 |
|
From the data of Table 2 and Table 3 one can see that proton-accepting ability of
the carbonyl group increases in these compounds in Spp*, Tpp* states and decreases in Spp*, Tpp* states.
Also, the excitation of the coumarin 1 and psoralen to the pp* state of any multiplication leads to increasing of the
probability of proton-transfer reaction and solvation at the C=O group, and the exitation
to the np* state leads to decreasing of this channel.
References.
- V.Ya. Artykhov and A.I. Galeeva, Izv. Vyssh Uchebn. Zaved., Ser. Fizika, No. 11,
96(1986).
- G.N. Jones, W.R.Jackson, Choi Chol-yao, W.R.Bergmark, J. Phys. Chem., 89(1985).
- K.M.Degtyarenko, T.N. Kopylova, R.T. Kuznetsova, G.V. Mayer, E.N. Tel'minov, Atmos.
Oceanic Opt., 6(1993)421.
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