SCUBA-2 with FTS and 80K blackbody source
SCUBA-2 with FTS and 80K blackbody source
SCUBA-2 with FTS and 80K blackbody source
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2. Define the optical system of <strong>SCUBA</strong>-2 (include the telescope <strong>and</strong> sky)<br />
Assume cosine weighting of beam which illuminates optics <strong>and</strong> telescope (see definition later)<br />
Insert extra optics in the Tel_optics matrix below:<br />
Tel_optics :=<br />
⎢<br />
⎡<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎣<br />
Det_optics :=<br />
"Surface"<br />
⎡<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎢<br />
⎣<br />
"Sky"<br />
"Primary-sec"<br />
"Cabin optics"<br />
2 6<br />
<strong>FTS</strong>trans := 2⋅TrBS ⋅TrM<br />
"Feed optics"<br />
"Window"<br />
"Blocker"<br />
"optic"<br />
"optic"<br />
"CS-filter"<br />
"CS aperture"<br />
"dichroic"<br />
"field mirror"<br />
"edge filter"<br />
"b<strong>and</strong>pass"<br />
"detector"<br />
"Temperature"<br />
280<br />
280<br />
150<br />
4<br />
4<br />
1<br />
1<br />
1<br />
1<br />
0.1<br />
0.1<br />
0.1<br />
270<br />
280<br />
280<br />
1 ( 0.995⋅Ruze) 3<br />
−<br />
0.02<br />
0.05<br />
1 − 0.995⋅Ruze 1 − 0.995⋅Ruze 1 − 0.95<br />
1<br />
0.05<br />
1 − 0.995⋅Ruze 0.1<br />
0.1<br />
0.2<br />
"emissivity"<br />
( )<br />
1 − Trans A, pwv,<br />
ν , Δν<br />
1 − 0.95⋅0.92 1 ( 0.995⋅Ruze) 4<br />
−<br />
net transmission of telescope beam through <strong>FTS</strong><br />
<strong>FTS</strong>trans = 0.437<br />
( )<br />
Spectrometer := "<strong>FTS</strong>" 280 0 <strong>FTS</strong>trans 0 AΩsys⋅I( n)<br />
0 0<br />
( 0.995⋅Ruze) 3<br />
0.98<br />
0.95<br />
0.995⋅Ruze 0.995⋅Ruze 0.95<br />
1<br />
0.95<br />
0.995⋅Ruze 0.9<br />
0.9<br />
0.8<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
1.0<br />
n ≡ 1<br />
"trans"<br />
( )<br />
Trans A, pwv,<br />
ν , Δν<br />
0.95⋅0.92 ( 0.995⋅Ruze) 4<br />
AΩsys⋅I( n)<br />
AΩsys⋅I( n)<br />
AΩsys⋅I( n)<br />
AΩsys⋅I( n)<br />
AΩsys⋅I( n)<br />
AΩsys⋅I( n)<br />
AΩpixel<br />
AΩpixel<br />
AΩpixel<br />
AΩpixel<br />
AΩpixel<br />
AΩpixel<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
I( n)<br />
= 0.901<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
0<br />
⎤<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎥<br />
⎦<br />
"net trans"<br />
1.0<br />
0<br />
0<br />
"AOmega"<br />
AΩsys⋅I( n)<br />
AΩsys⋅I( n)<br />
AΩsys⋅I( n)<br />
εM := 1 − 0.995⋅Ruze εBS := 0.025<br />
TrM := 0.995⋅Ruze TrBS := 0.475<br />
The factor of I(n) is to account for the fact that the beam<br />
which illuminates the telescope is not flat (assume a<br />
circularly symmetric cosine^n weighted field <strong>with</strong><br />
intensity of 0.5 (3db's) at the edge of the primary.<br />
"Pback (pW)"<br />