Tech Briefs

Compact f/2.4 design efficiently handles large numbers of optical fibers at the entrance aperture.

Headwall Photonics, Fitchburg, Massachusetts

Raman spectroscopy has risen to the top of a short list of technologies for identifying substances with high specificity. As a result, Raman spectrometers with high spectral resolution, high spatial resolution, high throughput, and small footprints are in high demand. Utilizing holographic diffraction gratings technology, Headwall Photonics has developed an imaging spectrometer that satisfies these performance demands through a retro-reflective concentric design utilizing the optimized properties of an advanced, highly efficient convex grating (see Figure 1).

Figure 1. Raman Explorer’s Concentric Optical Design enables multiple high-resolution spectra on one array detector.
Headwall Photonics’ Raman Explorer is an imaging spectrometer that is optimized to detect Raman signals that are shifted up to 4000 cm-1 by a 785-nm laser. A multi-channel, multi-spectrum imaging spectrometer with improved photometric and spectral resolution accuracy has several unique features, including the ability to place “dual spectra” onto the detector plane by using two separate entrance apertures. Each entrance aperture is located at a separate off-axis position and offset from one another in the spectral domain. This configuration allows each input aperture to direct its radiation at a unique input angle of incidence to the grating.

Figure 2. This 3-mm tall ray trace shows the Spatial Imaging Performance of a 532-nm excitation Raman Explorer configuration at 603 nm, using a 50-μm fiber core diameter.
Both inputs are then dispersed and re-imaged as two separate wavelength ranges on the detector, one directly above the other. Therefore, when using a 26.6-mm long CCD, roughly 0 to 2000 cm-1 is dispersed across the top half of the detector, and roughly 2,000 to 4,000 cm-1 is dispersed across the bottom. Spectral resolution performance of 0.4-nm FWHM, or approximately 4 cm-1, based on the Raleigh criterion, was measured at 912 nm using a 50-μm slit and a 1024 × 256-element detector with 26-μm pixels.

Spatial resolution in a spectrometer design refers to the instrument’s ability to faithfully reproduce an image positioned at the entrance aperture, or front focal plane, onto a multi-element detector array, or back focal plane. High spatial resolution is important for an application that requires collecting a signal with a bundle of fibers because the fibers have to be aligned in a linear array at the entrance aperture to maintain spectral resolution. Many spectrometers are capable of reproducing a one-point image, such as a single optical fiber onto a detector array, but they are unable to discriminate features or fibers stacked above or below a single point because of astigmatism and aberrations. This results in an unacceptable compromise of both spatial and spectral resolution performance.

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