NIRSpec BOTS Wavelength Ranges and Gaps
A physical gap between the JWST NIRSpec detectors affects the S1600A1 slit used for BOTS observations at high resolutions. Wavelength coverage is also affected by subarrays. Wavelength ranges and gaps are given here for all grating-filter and subarray combinations.
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Table 1. NIRSpec BOTS wavelength coverage for each disperser-filter and subarray combination (in μm)
|Disperser-filter||SUB2048||SUB1024A||SUB1024B||SUB512 or SUB512S|
|G140H/F100LP||0.97–1.31, 1.35–1.83||0.97–1.07, 1.59–1.83||1.07–1.31, 1.35–1.59||1.07–1.19, 1.47–1.59|
|G235H/F170LP||1.66–2.20, 2.27–3.07||1.66–1.79, 2.67–3.07||1.79–2.20, 2.27–2.67||1.79–2.00, 2.47–2.67|
|G395H/F290LP||2.87–3.72, 3.82–5.18||2.87–3.03, 4.51–5.18||3.03–3.72, 3.82–4.51||3.03–3.38, 4.17–4.51|
† PRISM spectra do not map to an area of the detector covered by the SUB1024A subarray for the S1600A1 aperture used for BOTS observing mode.
The full spectral range sampled by the disperser-filter combination (except for gaps mentioned above) is measured by the SUB2048 subarray options in BOTS mode. The SUB1024A and SUB1024B subarrays read out only half of the detector pixels in the dispersion direction. SUB1024A reads out both the red and blue ends of the waveband, and SUB1024B reads out the inner region of the waveband with a small separation between due to the detector gap. The smaller SUB512 and SUB512S options were designed to cover the full wavelength range for the PRISM. They span only a sub-range of the high-resolution grating data and could also be used for high-resolution spectra on very bright sources.
Figure 1 depicts the nominal spectral coverage of the S1600A1 aperture for the nine available disperser-filter combinations when SUB2048 is used. The limits are expressed in units of μm. The gaps in the spectra are shown in yellow. The exact position of the wavelength gap depends on the grating wheel assembly (GWA) tilt angle and will vary slightly from observation to observation, typically on a scale less than 0.025 μm for the PRISM and 0.01 μm for the gratings. Spectra at wavelengths that fall in the detector gaps are not recoverable when using the S1600A1 slit. Spectra obtained with the medium-resolution gratings or the PRISM do not have a wavelength gap because the complete spectrum will fall onto one detector, NRS1.