EFFECT OF GAS ADSORPTION ON THE ABSORPTION SPECTRA OF CAROTENE CRYSTAL FILMS.
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Abstract
Thin films of all trans-$\beta$-carotene crystals at room temperature show three main absorption bands in the visible with $\lambda_{\max}$ at $502 m\mu, 468 m\mu$ and $442 m\mu$. The bands are broader in crystal films than in solution and the central one is most intense as in solution at room temperature. Cooling the film to $77^{\circ}K$ does not show any appreciable change except that the bands are slightly sharpened and red shifted with four bands now fairly resolved. The position of $\lambda_{\max}$ are at $505 m\mu, 471 m\mu$, $441 m\mu$ and $415 m\mu$. The average separation between bands is $1430 cm^{-1}$, the same as that observed in EPA glassy solution at $77^{\circ}K$. When the film of all-trans $\beta$-carotene crystals is exposed to vapors of toluene, pyridine, $CS_{2}$, 3-methyl pentane, methanol, ethanol, benzene, acetone, chloroform, hexane, or ether, a drastic change in the spectrum is observed. A new intense absorption band appears in the $535 m\mu$ region and the intensity of the main absorption region decreases as the intensity of the new band increases. The position of the new band depends on the adsorbed molecule, being $550 m\mu$ for $CS_{2}$ and $527 m\mu$ for hexane. This new band is separated from the main absorption band by about $1600 cm^{-1}$. With desorption of the foreign molecules, the intensity of the new band decreases and the spectrum tends to return to the original $\beta$-carotene crystal film absorption spectrum. All trans $\beta$-carotene when melted in the dark and in an inert atmosphere, cools into a deep red colored glass. Thin films of this glass, when exposed to different vapors do not show the new band in most cases---and when it does, the new band appears very weak compared to that in $\beta$-carotene crystals films. Similar results have been observed with $15,15^{1}$ cis $\beta$-carotene, isozeaxanthin, $\beta$-APO-8'-carotenal and astacene. Possible interpretations of these results will be discussed.
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This work is supported by Grant No. GM-10890 of the National Institute of General Medicine and the Public Health Service.
Author Institution: Department of Biophysics, Michigan State University