Light path through WEAVE/LIFU
Light from an astronomical source passes through the following
en route to a WEAVE detector (click on some of the
figures to see full-size):
There is no second-order blocking filter in the red arm. Any second-order blue light passing into this arm will be strongly defocused.
The figure below, provided by Remko Stuik (NOVA, Univ. Leiden),
shows the spectrograph in high-resolution mode, i.e. with the
blue and red cameras positioned at the ends of the 'bananas' (shown in red)
closest to the slit-exchange unit. The footprint of the spectrograph on
the optical bench is ~ 2.1 m x 1.9 m in low-res mode,
and 1.7 m x 1.7 m in high-res mode. The maximum height of the components above the
bench is ~ 1.8 m.
For an enlarged view, click on the figure.
The light path is shown from injection at the pseudo-slit (upper centre),
via the dichroic (transmitting red, reflecting blue) to the blue camera (left)
and the red camera (right). The shutter box in each arm includes both the
fast shutter used to limit exposure times and the Hartmann shutters
used for focusing. A set of internal (flat-field) calibration lamps is
positioned between the camera and VPH on each arm.
Switching the spectrograph between
low-resolution mode (first figure below) and high-resolution mode
(second figure, same configuration as above)
involves rotating the camera arms in
the horizontal plane:
(these figures are taken from WEAVE internal document WEAVE-SYS-007).
In both low-res and high-res configurations, the spectrograph
operates in Littrow mode, i.e. the angles of incidence and dffraction at the grating are equal:
20 deg in low-res mode, and 51.6 deg in high-res mode.
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