The systems are sketched in Figs. 4.10 and 4.11.
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The measurements described in Chapters
7 and
8 cover the wavevector range
about
.
By using Eqs. (4.1) and
(4.4), we obtain
and
.
A
beam diameter, obtained with
lenses with
diameter, as shown in
Fig. 4.2, is enough to ensure
that the intensity is constant over the length
. For the
measurements described in Chapters 7 and
8, we used larger lenses with
diameter, with a larger beam diameter, in order to
ensure a better uniformity, and
was increased acordingly.
Following Eq. (4.3), we obtain the
magnification:
. We used a 20X microscope objective and
numerical aperture of 0.45.
The whole optical system for ENFS is shown in Fig. 4.2.
For ONFS, we insert a beam stop through a hole inside the lens mount. The beam stop and its adjustable mount is shown in Fig. 4.7.