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Optofluidic Micr oscope    261


               with a thin metal layer and that has a line of small apertures that are
               etched onto the metal layer. Each aperture should be situated at the
               center of each sensor pixel. The sensor pixel will then be sensitive
               only to light transmitted through the aperture. By placing a target
               object on top of the grid, we can then obtain a sparsely sampled image
               of the object (Fig. 11-1a). We can “fill in” the image by raster-scanning
               the object over the grid (or equivalently, raster-scanning the grid
               under the object) and compositing the time-varying transmissions
               through the apertures appropriately (Fig. 11-1b). We can see that in
               this case, the resolution is fundamentally determined by the aperture
               size and not the pixel size. Therefore, by choosing the appropriate
               aperture size, we can achieve high resolution.
                  This imaging strategy can be simplified by tilting the aperture
               grid slightly and replacing the raster-scan pattern with a single linear


                                                                  Image
                              Scheme

          (a)





          (b)
                                      Raster scan

                   y
          (c)
                        x             Translation
                          θ

                                 Flow
              y
          (d)
                  x                       θ

          FIGURE 11-1  Comparison of direct projection imaging strategies. (a) By placing the
          specimen on a grid of apertures, we can obtain a sparsely sampled image of the
          object. (b) We can “fi ll in” the image by raster-scanning the object over the grid (or
          equivalently, raster-scanning the grid under the object) and compositing the time-
          varying transmissions through the apertures appropriately. (c) This imaging strategy
          can be simplifi ed by tilting the aperture grid slightly and replacing the raster-scan
          pattern with a single linear translation of the object across the grid. (d) This design
          can be further simplifi ed by replacing the tilted 2D aperture grid with a long tilted
          1D aperture array. This scheme is the basis for the optofl uidic microscopy method.
          (X. Cui, L. M. Lee, X. Heng, W. Zhong, P. W. Sternberg, D. Psaltis, and C. Yang,
          “Lensless high-resolution on-chip optofl uidic microscopes for Caenorhabditis
          elegans and cell imaging,” Proceedings of the National Academy of Sciences of the
          United States of America, vol. 105 (31), pp. 10670–10675, 2008. Copyright (2008)
          National Academy of Sciences, USA.)
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