Page 190 - Vibrational Spectroscopic Imaging for Biomedical Applications
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166    Cha pte r  S i x


        longer experiments. Because of this trade-off between fluorescence and
        SNR, the laser excitation wavelength chosen should be based on the
        specific application and goal.

        6.4.2  Correction for Dark Current
        Cameras containing a CCD sensor are often used as detectors in
        chemical imaging. Because Raman scattering is a weak phenomenon,
        a highly sensitive camera containing an electron-multiplying CCD
        (EMCCD) has become a preference for widefield Raman imaging. For
        all types of CCDs, the dark current attributed to the sensor must be
        corrected and thus eliminated from the background.
            In the absence of radiation, a constant charge accumulates within
        the camera wells and on the chip that is the result of the random gen-
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        eration of electrons.  This constant response, or dark current, adds to
        the signal produced. To remove this response, a background image is
        collected without any source of radiation. This image is then subtracted
        from each image frame during acquisition. Alternatively, it may also be
        subtracted from the image stack after data acquisition is complete.
        6.4.3 Cosmic Filtering
        One important step that is applied to widefield Raman images before
        other preprocessing steps is a cosmic filter. Random cosmic events
        often occur while collecting Raman data. These events are seen as
        bright pixels while scrolling through the wavelength dimension of a
        widefield Raman image. Applying a cosmic filter eliminates these
        cosmic spikes. The cosmic filter is a median filter that considers each
        pixel in the image and checks the nearby neighboring pixels to deter-
        mine if it is representative of its surroundings. A standard deviation
        and a window size are set to determine the range and acceptable pixel
        intensity. An alternative method is to perform a threshold filter to the
        data. Using this method, upper and lower threshold values are set.
        Any pixels outside of this threshold value are replaced by the average
        intensity of the moving window of a selected size of neighboring pixels.
        This intensity is filtered at the center.

        6.4.4  Instrument Response Correction
        A major source of background interference in widefield Raman
        images is signal contributed by the instrument, known as instrument
        response. Every Raman imaging instrument contains complex optical
        components. The signal attributed to these components is present in
        the background and should be removed to reveal the subtle differences
        in the Raman signal of biological samples. A sample with a known
        spectral profile, such as calibrated light sources, blackbody radiators,
        and white light, may be used to  correct for  instrument response.
        Recently, the National Institute of Standards and Technology (NIST)
        has tested and developed standard reference materials (SRM) with
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