Last Updated Mar 24, 2017
Introduction
The JWST Near Infrared Imager and Slitless Spectrograph (NIRISS) provides observing modes for grism spectroscopy, high-contrast interferometric imaging, and imaging, over wavelengths between 0.6 and 5.0 μm. Although NIRISS is packaged with the Fine Guidance Sensor (FGS), the two instruments are functionally independent of each other.
Observational capabilities
When used in specific combinations, optical elements in the NIRISS pupil and filter wheel enable 4 observing modes:
Wide field slitless spectroscopy (WFSS) over the entire field of view, using one or both of a pair of identical grisms and a selection of blocking filters to isolate specific wavelength intervals between 0.8 and 2.2 μm. The grisms are mounted to disperse light in orthogonal directions on the detector.
- Single object slitless spectroscopy (SOSS) with a cross-dispersed grism designed to deliver broad wavelength coverage and spectrophotometric stability.
- Aperture masking interferometry (AMI) through specific filters that is enabled by a mask with 7 sub-apertures.
- Imaging in 7 wide- and 5 medium-band filters that are closely matched to the NIRCam filter set between 0.9 and 5.0 μm.
Table 1. Specific properties of NIRISS observing modes
Observing | Wavelength | Field of | Pixel scale | Resolving power | FWHM | Comment |
---|---|---|---|---|---|---|
0.8–2.2 | 133 × 133 | 0.065 | 150 @ 1.4 μm | ... | Orthogonal dispersion | |
0.6–2.8 | ... | 0.065 | 700 @ 1.4 μm | ... | Subarrays are standard; full-frame allowed | |
Aperture masking interferometry (AMI) | 2.8–4.8 | 5.2 × 5.2 | 0.065 | ... | ... | Subarray is standard; full-frame allowed |
Imaging | 0.8–5.0 | 133 × 133 | 0.065 | 4–10 | 2 pix @3.4 μm | Full-frame standard; only used in parallel mode
|
Optical elements
The optical path of NIRISS is illustrated schematically in Figure 2a. A solid-body representation of the instrument is shown in Figure 2b.
Light from the Optical Telescope Element of JWST is processed sequentially by
- a pick-off mirror
- a collimator (three reflections)
- a user-selected element in the pupil wheel
- a user-selected element in the filter wheel
- a camera (three reflections)
- a detector in the focal plane assembly
Table 2. Allowed combinations of optical elements for 4 observing modes
Observing mode | Allowed pupil | Allowed filter |
---|---|---|
F090W F115W F150W F200W F140M F158M | GR150C GR150R | |
Single object slitless spectroscopy (SOSS) | GR700XD | CLEAR |
NRM | F277W F380M F430M F480M | |
Imaging (0.9 μm to 2.0 μm) Imaging (2.7 μm to 4.8 μm) | F090W F115W F150W F200W F140M F158M CLEARP | CLEAR F277W F356W F444W F380M F430M F480M |
NIRISS has a single Teledyne H2RG detector with 2040 × 2040 pixels sensitive to light. The pixels, measuring 18 μm on a side, are made of HgCdTe with a composition tuned to provide a long-wavelength cutoff near 5.2 μm. In its full-frame format, the detector is read out non-destructively every 10.74 s through 4 readout channels. Subarray formats are available for most modes to decrease the readout time. The smallest subarray (64 × 64 pixels) can be read out in 45.5 ms.
Sensitivity and performance
Please consult the JWST Exposure Time Calculator for definitive estimates of performance in each observing mode.
Wide field slitless spectroscopy
Single object slitless spectroscopy
Table 3 lists the J-band magnitude for which saturation first occurs in the specified order, with the specified number of samples up-the-ramp (NGROUPS) for the subarrays available for use with SOSS.
Table 3. SOSS saturation limits for a G2 V spectrum
Subarray | Order | NGROUPS | J magnitude |
---|---|---|---|
256 × 2048 | 1 | 2 | 8.05 |
256 × 2048 | 2 | 2 | 6.75 |
96 × 2048 | 1 | 2 | 7.05 |
96 × 2048 | 1 | 1 | 6.35 |
Aperture masking interferometry (AMI)
The saturation limit for AMI corresponds to a magnitude of M ~ 4 with NGROUPS = 2.
Imaging
Table 4 lists the estimated point-source sensitivity for Imaging through broad-band filters. The limits are expressed as the limiting flux achieved with S/N = 10 in an integration of 10 ks.
Table 4. Estimated point-source sensitivities in broad-band filters
Filter | nJy |
---|---|
F090W | 14.3 |
F115W | 12.6 |
F150W | 11.1 |
F200W | 9.7 |
F277W | 10.7 |
F356W | 10.0 |
F444W | 15.0 |
Data calibration and analysis
coming soon...
Acknowledgements
NIRISS is a contribution of the Canadian Space Agency to the JWST Project. The Principal Investigator of NIRISS is Professor René Doyon of the Université de Montréal. Honeywell International designed and built the instrument, with additional technical support from the National Research Council of Canada.
Related links
Near Infrared Imager and Slitless Spectrograph, NIRISS
Exposure Time Calculator (ETC)
References
Doyon, R., et al. 2012, SPIE, 8442, 2RD
The JWST Fine Guidance Sensor (FGS) and Near-Infrared Imager and Slitless Spectrograph (NIRISS)
Doyon, R. JWST Community Webinar Series (2016 April 19)
NIRISS Overview
On this page
JWST Observatory and Instrumentation