Page 62 - Vibrational Spectroscopic Imaging for Biomedical Applications
P. 62

38    Cha pte r  T w o




             60
           100
           80
             40
           60
              μm
           40
             20
           20
           0
              0
               0      20     40     60
                          μm                         (b)
                           (a)

        FIGURE 2.6  Unprocessed IR (a) and visible (b) grey-scale images of an
        agglomeration of 6- μm polystyrene beads. The IR image is generated from
                            –1
        the absorption at 3025 cm  and 100 on the grey scale that corresponds to
        0.125 absorption units. This was measured in transmission at IRENI.
         0.90









         0.00
                  (a)          (b)           (c)          (d)
         FIGURE 2.7  IR images of a benign prostate gland using (a) Spotlight FTIR
         point mapping (10 μm × 10 μm), (b) Spotlight FTIR imaging using a linear
         array detector (6.25 μm × 6.25 μm), (c) Varian FTIR with focal plane array
         (5.5 μm × 5.5 μm) and (d) the IRENI beam line with a focal plane array
         (0.54 μm × 0.54 μm). (Printed with permission from Ref. 19.)

        aberrations due to thick-flow chamber windows has hampered high
                                                     6
        resolution in vivo IR studies. In phycology, Heraud et al.  have pioneered
        measurements on living algal cells using a custom flow-through cham-
        ber with several millimeter thick-halide windows. They acquired the
        data at the IR beamline 11.1 at the Synchrotron Radiation Source in Dares-
        bury (UK). The use of synchrotron radiation as an IR light source allows
        researchers in principle to push the effective resolution to the diffraction
        limit with very good signal-to-noise ratios 21,22  but only if optical/(SNR)
        aberrations are negligible. This resolution is necessary to distinguish
        subcellular structures, e.g., the nucleus from the chloroplast.
            In this section we describe a new flow chamber that accommo-
        dates high-magnification objectives and features very low-optical
        aberrations. It thus permits the achievement of high-resolution data
   57   58   59   60   61   62   63   64   65   66   67