A laser-microprobe fluorescence/Raman spectrometer with a 700-channel detector has been constructed and applied to the collection of data on the distribution of a green fluorophor throughout the exposed area ofa human lens sectioned along the visual axis. The area ("'6.5 X 9.5 mm) covering the lens section was scanned automatically by the microprobe programmed to measure the fluorescence intensity at 1200 data points. The spectrometer output was accumulated in a microcomputer and displayed as a three-dimensional perspective view showing the fluorescence intensity at each point on the grid. The method permits the precise and detailed mapping at high resolution of the spatial distribution of a fluorophor or Ramanemissive constituent in a plane ofthe frozen lens to give results not obtainable by any other feasible procedure. The green fluorophor (441.6 nm, excitation wavelength; 520 nm, peak emission wavelength) has a distribution indicating a metabolic rather than a photochemical mode of production. Moreover, the lower level of fluorophor in the anterior segment suggests the existence of mechanisms in the anterior cortex (including the epithelium) that reduce significantly the accumulation of fluorophor. Such distribution studies are invaluable in clarifying metabolic interrelationships among the different zones of the lens, including especially photochemical reactions postulated to involve the effect of daylight on the lens in human subjects.The application of fluorescence and Raman spectroscopy to human and animal lenses has yielded information on the intact living lens that is hardly obtainable by other means (1, 2). We herein describe a greatly modified system that presents several advantages over our previous procedure that required the excitation beam to penetrate the lens at least to the zone where the emission originated. The system scans the surface of a frozen lens section and is, therefore, not affected by opaque regions in the body of the lens; this is a great advantage for cataract research.Our fluorescence/Raman imaging system has a number of important capabilities: (i) multichannel detection of "position-defined" fluorescence/Raman spectra from gridded points (1-8 ,um); (it) scanning of micro (10 ,um x 10 ,um) and macro (2.5 cm x 2.5 cm) samples; (iii) automated simultaneous acquisition of intensity data of up to six spectral lines (either peak or integrated intensities) from each point; (iv) excellent stray-light rejection to allow detection of weak Raman lines from solid samples; (v) normalization of fluorescence intensity with Raman signals (fluorescence/Raman intensity ratio); and (vi) presentation of the x-y data set in three-dimensional perspective, three-dimensional perspective with cursor-sectioning, six-color map representing regions of various intensity intervals, and topographic contour map with lines intersecting the intensity data with constant height intensity planes.We here describe how it has been employed to make fluorescence intensity measurements from a human lens section ...