Optical properties of free and substituted porphyrins (PP) doped borate glass matrix are reported for the first time. Absorption spectral !l5urernents of H2 TPP, CdTPP, MgTPP and ZnTPP doped borate glass matrix have been made in the 200-1100 nm region and the :l:traobtained are analyzed to obtain the optical bandgap (Eg) and other important spectral parameters viz. oscillator strength (f), molar :Iinction coefficient (e), electric dipole strength (l), absorption cross-section (a.) and molecular concentration (N). Intense fluorescence ~observed in the region 668-685 nm for CdTPP, ZnTPP and MgTPP doped matrices, whereas no such fluorescence was observed in ~TPP doped matrix. Fluorescence intensity was observed to be almost similar in all the metallated porphyrine matrices. Fluorescence mdwidth (~)..), decay time (r), stimulated emission cross-section (a) and optical gain (G) of the principal fluorescence transitions iUesponding to the Q-band excitation were also evaluated and discussed. © 2002 Elsevier Science B.V. All rights reserved. [·mail address: spapforum@vsnl.com (N.v. Unnikrishnan).systems in realizing intense fluorescence and optical amplification is enhanced by the above mentioned factors; (iv) the present systems studied possess such properties and may have significant applications in energy storage devices. The aim of the present work is, in general, to elucidate the optical absorption and emission spectral properties of H2 TPP, CdTPP, ZnTPP and MgTPP molecules in borate glassy matrix and to investigate the effect of the metal ions on these properties. A quantitative analysis of the spectral and radiative properties of the investigated samples have also been reported and discussed.
ExperimentalAll the glass samples were prepared by the well-known rapid quenching technique [3]. Reagent grade boric acid (H3B03) and doubly sublimed PP have been used as the starting materials for the preparation of the glass samples. The weighed quantities of the starting materials for 18 gm of glass are mixed homogeneously using an agate mortar. The batch was then placed in a silica crucible and heated in an electric muffle furnace. A slow heating was initially maintained until the temperature reaches 80°C and decomposition of H3B03 to B203 is complete. The temperature was then rapidly increased to 120°C so as to obtain a greenish melt. The melt was retained for about 10 min and then 0254'()584/02/$ -see front matter