Optical arrangements[Project home page] With increasing sample depth, there will almost certainly be an increase
in signal contamination from the sea water that the cells are suspended
within, which may prove difficult to correct for. This will be particularly
true with estuarine samples, which are likely to contain significant amounts
of organic matter. C shows an optical arrangement that will maximise the
fraction of laser energy reaching the cell. Here, the laser and fibreoptic
are both positioned at 55° to the x, y plane, forming an angle of 70°
between the laser and the fibreoptic. Inevitably, this arrangement will
result in the poly-L-lysine immediately below the sample being turned into
plasma and contaminating the signal. We shall assess the need to correct for
the poly-L-lysine signal by sampling within a cell-free region. The optical
arrangement in D employs a mirror to steer the beam of the laser, so that it
hits the sample at 90° to the x, y plane. As with the arrangements in parts
B and C, the fibreoptic is at 55° to the x, y plane. The main disadvantage
with this arrangement is that the mirror will have to be moved in and out of
the path between the sample and microscope with each LIBS measurement. It
may also prove difficult to concentrate the beam (using a short focal length
lens) whilst remaining below the damage threshold of the mirror. |