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Grisms Michael Sholl Space Sciences Laboratory 29 March 2003 Practical implementation for SNAP.

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Presentation on theme: "Grisms Michael Sholl Space Sciences Laboratory 29 March 2003 Practical implementation for SNAP."— Presentation transcript:

1 Grisms Michael Sholl Space Sciences Laboratory 29 March 2003 Practical implementation for SNAP

2 Dispersive Elements

3 NICMOS Grisms Resolving power: 200 Central wavelengths: 0.967, 1.414, 2.067μm Bandpass: 0.8-1.2, 1.1-1.9, 1.4-2.5μm Interference filters made by OCA Spacing: 44.82, 30.66, 20.97 lines/mm Wedge angles: 5.8, 5.8, 5.9 Image taken through wide-band filter for calibration (slitless) No collimating optics (f/45 beam) Materials: fused silica and CaF (high-λ throughput) 1cm size

4 GRISM Design Parameters Interference filters are used to prevent order overlap Resolving power: 100-200 (λ/Δλ)  easy to achieve --Increases with wedge angle --Increased by more rulings (larger grism, or smaller spacing) Overall bandpass: 0.35-1.7μm --fused silica acceptable for throughput Beyond 2.5μm, would use CaF, ZnSe or sapphire --Individual grism bandpass limited by order overlap Use interference filter on grism front surface Must use several grisms to span bandpass Practical constraints --Desire one interference filter design for all grisms (performance degraded off-axis  constrains wedge angle) --Replica gratings produced in discrete line spacings  vary wedge angle slightly to achieve desired R ~f/22 beam: collimating optics required for spatial resolution? 5cm x 5cm field of view?

5 Potential GRISM Designs Goal: ~200 resolving power (easy to go down to 100) Span 0.35-1.7 μm bandpass Grating lengths: 1cm (size of collimated beam) (tertiary-focal plane: ~ f/11) Materal: fused silica Pixel Size: 10.5um Prism/focal plane angle: 3deg λ (μm)Wedge (°)d (μm)/ (lines/mm) RGFD1 (cm) GFD1. 5 (cm) GFD2 (cm) 0.44 (0.35-0.55)2.422.8/43.82011116.522 0.64 (0.5-0.8)3.522.8/43.82017.611.315.1 0.88 (0.7-1.1)4.822.8/43.82015.58.211.0 1.36 (1.0-1.7)7.422.8/43.82033.65.37.1

6 GRISM Configuration 02 In front of focal plane Lens axes normal to slant ray Out of plane dispersion

7 GRISM Configuration 03 In front of focal plane No collimating optics Out of plane dispersion

8 GRISM Configuration 11 Behind Focal Plane Good stray light Images focal plane Out of plane dispersion

9 Large field of view: 5cm x 5cm Back side of focal plane: requires large lenses to collimate and refocus Front side of focal plane --stray light worse (need to quantify) --can we do without collimating optics? --quantify spot size and shift with grism Grating lengths: size of f/11 beam at grism Prism/focal plane angle: 3deg

10 Grism in front of focal plane 5cm by 5cm grism Distance from focal plane: 11cm 2.4° wedge angle Line spacing: 22.8µm Design central wavelength: 0.44 µm Inplane dispersion

11 Image degradation/shift Configuration1-σ X (μm)1-σ Y (μm)Shift X(μm)Shift Y(μm) Standard1.312.3000 Prism only12.528.121480 Grism1.312.3000

12 Conclusions: Grisms may be added to SNAP focal plane Decision on R TBD Decision on # of pixels/Δλ TBD Stray light analysis TBD


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