SPIRE Design Description - Research Services
SPIRE Design Description - Research Services
SPIRE Design Description - Research Services
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Draft <strong>SPIRE</strong> <strong>Design</strong> <strong>Description</strong> Document<br />
The main disadvantages are that the observing modes are complicated (jiggling or scanning) and that the<br />
efficiency for mapping is a less than the ideal (Griffin, 2000). This means that the full collecting area of the<br />
telescope is not used with maximum efficiency.<br />
In order to collect the radiation from a point source with good efficiency, the detector through put must be of<br />
the order of λ 2 . The diffraction-limited beamsize of a telescope of diameter D is approximately θ ≈ 1.2λ/D.<br />
The corresponding solid angle on the sky is Ωsky = π(θ/2) 2 . The throughput (the product of area and solid<br />
angle, which is conserved in an ideal optical system) is therefore<br />
AtelΩsky ≈ [πD 2 /4][π(1.2λ/2D) 2 ] ≈ λ 2 .<br />
The <strong>SPIRE</strong> photometer uses smooth wall, single-mode feedhorns - the circular waveguide section allows<br />
propagation of only one mode (TE11). The corresponding throughput (defined as the area-solid angle<br />
product) is exactly λ 2 . The spectrometer uses multi-mode feedhorns that pass both TE and TM modes.<br />
4.4.6 Bolometer array thermal-mechanical design<br />
The design of the <strong>SPIRE</strong> array units (called Bolometer Detector Arrays, BDA's) is illustrated in<br />
Optical<br />
entrance<br />
Kevlar<br />
supports<br />
76<br />
300 mK strap<br />
attachment<br />
2 K<br />
mounting<br />
flange<br />
Readout<br />
cable<br />
attachment<br />
Figure 4-21. Each BDA unit is split into a 2-K and a 300-mK section. The 300-mK section contains the<br />
feedhorns, waveguides, bolometer array wafer and the supporting structure. The 2-K detector structure<br />
forms the mechanical interface between the 300-mK structure and the photometer or spectrometer 2-K<br />
enclosures. The enclosures are connected via thermal straps to the 1.7-K stage of the Herschel cryostat. The<br />
heat load from the 2-K structure to the 300-mK structure of the BDA is minimised by suspending the 300mK<br />
section from the 2-K structure with two pre-tensioned 3000-denier Kevlar cords. Kevlar has high<br />
mechanical strength in tension and a very low thermal conductivity at this temperature, and forms gives<br />
good thermal isolation between the assemblies. The estimated heat load is less than 1.6 µW per array. The<br />
high mechanical rigidity of the Kevlar cord yields a high resonant frequency (> 200Hz).