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Algal Cells, Cartilage, and IRENI    39


        (provided by a synchrotron light source) of aqueous samples such as
        living specimen. Furthermore, the recent advent of multielement
        mid-IR detectors such as line detectors or FPAs reduces the acqui-
        sition times by several orders of magnitude. In combination with the
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        high brightness of a synchrotron light source,  it opens the possibil-
        ity for the in vivo acquisition of kinetic microspectroscopic maps of
        biological samples.
            For this publication we demonstrate the performance of the flow
        chamber using an algal specimen (Micrasterias sp.), but the chamber
        can in principle be used with any aqueous/biological, nonaqueous or
        even gaseous samples.


        2.3.1  Flow Chamber Design
        One challenge in the design of a flow chamber is the choice of an
        appropriate window material: many commonly used crystals are
        water soluble (e.g., KBr, NaCl) or toxic (e.g., CdTe, KRS-5), absorb
        portions of the bandwidth of interest (e.g., Si, Al O ), or exhibit dis-
                                                  2  3
        persion (e.g., ZnS, CaF , BaF ) leading to optical aberrations. The lat-
                           2    2
        ter effect is made worse by the fact that the halide materials cannot be
        made into windows with a thickness of less than several millimeters
        due to their brittleness. This prevents the use of high numerical aper-
        ture microscope objectives with their short working distance.
        Furthermore, some of these substances are tinted (e.g., ZnSe) or
        opaque (e.g., Si, AMTIR) in the visible, which renders comparisons
        and co-localization of features in the visible (e.g., stained sections or parts
        labeled with fluorescent markers) and the IR difficult or impossible.
            To circumvent the problems mentioned above, we chose diamond
        as a material for our windows. This material has several considerable
        advantages: it is water insoluble, nontoxic, transparent, and colorless
        in the visible as well as in the entire mid-IR spectrum of interest.
        Additionally, it exhibits a very low dispersion in the mid-IR region.
        This is illustrated by its relatively constant refractive index over the
        full mid-IR spectral range compared to other commonly used win-
        dow materials (ZnS, BaF , and CaF ) as shown in Fig. 2.8.
                             2        2
            Multiple internal reflections inside the window materials of the
        order of micrometers thick can pose a serious problem because they
        lead to fringes on the IR spectra. This is worst when the fringe fre-
        quency is comparable to typical spectral peak widths. We overcome
        this by using sub-micrometer (less than one micron) thin diamond
        films such that the fringe frequency is comparable to the entire spec-
        tral range. The fringe(s) can then essentially be treated as an addi-
        tional baseline and subtracted from the interesting spectral features.
        Diamond can be grown very thin by chemical vapor deposition
        (CVD) techniques. Thin films also help to keep the flow chamber
        design slim so that it can accommodate high numerical aperture
        objectives with short working distances.
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