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(1)Notizen 509 The Relaxation Time of the Orientation Polarization and its Influence on the Luminescence Intensity Distribution * A

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Notizen 509 The Relaxation Time of the Orientation Polarization

and its Influence on the Luminescence Intensity Distribution *

A. Kawski

Luminescence Research Group, Institute of Experimental Physics, University of Gdansk, Gdansk, Poland

Z. Naturforsch. 39a, 509-510 (1984);

received December 21, 1983

The characteristic relaxation time rR of the orientation polarization of polar solvent molecules around polar luminescent molecules influences the spectral emission distribution depending on rf > tr or tf ^ tr . This is shown on the luminescence of the polar molecules 4-iso- cyanate-4'-dimethylamino-transstilbene (CDS), 4-isocya- nate-4'-methoxy-trans-stilbene (CMS) and 4-isocyanate- 3',4'-dimethoxy-trans-stilbene (CDMS) (having a very short lifetime tf < 10 ps) in chlorobenzene.

As known from the experiments and theoretical considerations of Galley and Purkey [1], the inten­

sity distribution 7(v) within the fluorescence band and the band position of polar fluorescing mole­

cules in frozen polar liquids are strongly influenced by the orientation polarization of the solvent mole­

cules around the solute molecules. In this case the dependence of /(v) on the excitation frequency vexc is due to the spectral heterogeneity of the medium.

Such effects on stilbene derivatives in frozen and liquid mixed solutions have been observed previous­

ly [2], An asymmetrical broadening of the fluores­

cence bands of indol and dimethylindol in mixed liquid solutions described in the papers [3, 4] can be interpreted in the same way.

Strongly polar solute molecules in different liquid polar solvents have different surroundings, and every surrounding fluctuates with a characteristic relaxation time t R [5]. If the lifetime t f of the solute molecule in the excited state is much longer than t r , the surroundings of all excited centres relaxe to a new statistical equilibrium before the emission.

The solution appears to be homogeneous; the emis­

sion bands are homogeneously broadened. In this case, one expects a fluorescence emission band, the intensity distribution of which is independent of the excitation frequency vexc.

* Carried out under Research Project M.R.I.5.

Reprint requests to Prof. Dr. Alfons Kawski, ul. Gen. Wb Sikorskiego 11, 84200 Wejherowo, Poland.

If, however, t f is comparable or shorter from t r , than the emission is expected to start partly before the relaxation, the emission bands should be broad­

ened inhomogeneously and therefore the spectral emission intensity distribution should depend on vexc. Using short time pulse excitation, the spectral intensity distribution should be time dependent too.

Of special interest is the fluorescence of a class of substances (4-isocyanate-4'-dimethylamino-trans- stilbene (CDS), 4-isocyanate-4'-methoxy-trans-stil- bene (CMS) and 4-isocyanate-3',4'-dimethoxy-trans- stilbene (CDMS)), the mean lifetimes of which are very short. The lifetimes tf of these substances are less then 10 ps in chlorobenzene [6]. The relaxation time tr of chlorobenzene in dilute benzene solutions has been measured with cm waves to be 7.5 ps at 292 K [7] and 10.8 ps at 291.5 K [8], and using meter waves one gets 10.6 ps at 296 K [9]. Thus, for the polar CDS, CMS and CDMS molecules [10] in chlorobenzene, the condition t f % t r is held.

V [kK]

Fig. 1. Fluorescence spectra of CDS in chlorobenzene at 295 K: vexc = 28600 cm-1 (•); vexc = 27000 cm"1 (x); vexc = 24400 cm"1 (o).

0340-4811 / 84 / 0500-0507 $ 01.3 0/0. - Please order a reprint rather than making your own copy.

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510 Notizen In the unpolar benzene and cyclohexane the fluorescence intensity distribution 7(v) of CDS, CMS and CDMS was found to be independent of vexc. However, in chlorobenzene we observed for the three substances a marked dependence of / (v) on

vexc. As an example, the fluorescence spectra of CDS in chlorobenzene for three excitation wave numbers can be seen in Figure 1. They show clearly the excitation and emission of distinguishable centres by different excitation wave numbers.

[1] W. C. Galley and R. M. Purkey, Nat. Acad. Sei. USA 67,1116 (1970).

[2] A Kawski, M. Ston, and I. Janic, Z. Naturforsch. 39 a, 322 (1983).

[3] A Kawski and J. Czajko, Z. Naturforsch. 29 a, 84 (1974).

[4] A Kawski, Chimia 28, 715 (1974).

[5] W. Liptay and G. Walz, Z. Naturforsch. 26 a, 2007 (1971).

[6] A Kawski and M. Alicka, Z. Naturforsch. 35 a, 775 (1980).

[7] D. H. Whiffen and H. W. Thompson, Trans. Faraday Soc. 42 A, 114, 122(1946).

[8] F. J. Cripwell and G. B. B. M. Sutherland, Trans.

Faraday Soc. 42 A, 149 (1946).

[9] E. Fischer, Z. Naturforsch. 4 a, 707 (1949).

[10] I. Gryczynski, A. Kawski, Ch. Jung, and I. Janic, Z. Naturforsch. 37 a, 259 (1982).

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