The STIS aperture wheel has 65 positions, several of which correspond to multiple slits or masks. Only a small fraction of the full complement of spectroscopic apertures are currently supported. Table A.1 and
Table A.2 provide a complete list of STIS apertures for spectroscopy, together with comments regarding their characteristics or purposes. For most apertures, the aperture name gives the length in the spatial direction by the width in the dispersion direction in arcseconds. Schematics of three complex apertures are given in
Figure A.1,
Figure A.2, and
Figure A.3.
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0.2X0.06 and 0.2X0.2 are supported with E230M and E140M, while 0.2X0.09 and 0.2X0.2 are supported with E230H and E140H.
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The 6X0.2 long slit is supported with the echelles.
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Narrow-band filters. F25MGII is supported for E230H and E230M. Others are available with the NUV-MAMA only.
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These aperture positions put a target near the bottom edge of the FUV-MAMA and are intended for observation of very faint targets where it is necessary to minimize the contribution of the FUV-MAMA dark current. They are all supported with the G140L and G140M gratings. 52X0.05D1 and 52X0.1D1 are also supported for CCD peakups.
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As of Cycle 12, the 0.2X0.2 aperture is supported for use with all first-order gratings; it is available-but-unsupported with the PRISM. While not supported for first-order observations, the other echelle apertures can be used in first order as available-but-unsupported apertures. This includes the echelle neutral-density slits 0.2X0.05ND and 0.3X0.05ND with dex ND factors of 2.0 and 3.0, respectively.
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F25QTZ and F25SRF2 are supported for all MAMA gratings and PRISM, but are unavailable with the CCD .
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F25MGII is supported and these other filters are available -but-unsupported with the NUV-MAMA gratings and PRISM only.
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The F25LYA filter is available-but-unsupported with the G140L, G140M, E140H, and E140M gratings only.
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