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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 />

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