MIRI Low Resolution Spectroscopy
Low-resolution spectroscopy is an observing mode for JWST’s Mid-Infrared Instrument (MIRI) that offers slit and slitless spectroscopy from 5 to 12 μm.
See also: MIRI LRS APT Template
MIRI's low-resolution spectrometer (LRS; Kendrew et al. 2015) offers both slit and slitless spectroscopy from 5 to 12 μm using a double prism mounted in the MIRI filter wheel. These optics provide a spectral resolving power (R = λ/Δλ) of ~100 at 7.5 µm, varying from R ~ 40 at 5 μm to R ~ 160 at 10 μm. The LRS forms part of the MIRI imager, and spectra are imaged onto the imager detector array.
The LRS can be operated to obtain spectra in the slit or in slitless mode. Slitless spectroscopy is only available for time-series observations of time variable phenomena, such as transiting exoplanets or eclipsing binaries.
When preparing observations, the observer has control of 3 primary variables: (1) choice of slit vs. slitless, (2) dithering requirements (for slit only), and (3) detector readout mode and exposure settings.
Slit vs. slitless spectroscopy
The spectral dispersion for LRS is achieved with a double prism mounted in the imager filter wheel. The same disperser is used for both slit and slitless modes.
Words in bold italics are buttons
or parameters in GUI tools. Bold
style represents GUI menus/
panels & data software packages.
The slit and slitless modes have some operational differences.
The LRS slit mode is suited to a broad range of spectroscopic observations and therefore supports a wider range of operational choices.
The single slit is 4.7" long (3.18 mm; 42.7 pixels) and 0.51" wide (0.33 mm; 4.6 pixels). The projected location of the slit on the focal plane array lies between the imager field of view and the coronagraphy regions on the imager detector; its location is fixed. There is no subarray choice for LRS slit: for these observations, the entire imager array is read out (APT Subarray parameter set to FULL). The structure containing the slit blocks a large portion of the background close to the source from the detector, providing better sensitivity than the slitless mode.
Slitless LRS is a mode dedicated to time-series observations (TSOs), and operation is optimized for high precision spectrophotometry over long observations, e.g. of exoplanet transits.
This mode uses a dedicated subarray region on the detector (APT Subarray parameter set to SLITLESSPRISM); its location is shown in Figure 1. The use of a smaller subarray provides faster read times and thus a greater dynamical range. The saturation limit is several magnitudes brighter than for LRS slit. The absence of the slit, however, allows more background radiation to be dispersed over the science spectrum, reducing the sensitivity by around an order of magnitude. Whilst LRS slitless is ideal for high-precision spectrophotometric observations of bright point-source targets, the slit is expected to give better performance for faint targets.
As both modes use the same dispersing element, the dispersion profile is, in principle, the same for both. The nominal spectral range of 5–12 µm is dispersed over approximately ~370 pixels. The dispersion profile however folds over below 4.5 µm (where the prism throughput is very low), superimposing two parts of the spectrum onto each other. A dedicated filter is mounted over the slit to block radiation shortward of 4.5 µm to avoid this contamination in the slit. This effect is not mitigated for LRS in slitless mode, causing some spectral contamination at the shortest wavelengths.
Table 1 below shows the main differences between the slit and slitless modes of LRS.
Table 1. Comparison between LRS slit and slitless modes
|Not available for Time Series Observations||Time Series Observation setting mandatory|
|FULL array||SLITLESSPRISM subarray|
|Better sensitivity, fainter saturation limit||Worse sensitivity, brighter saturation limit|
|Exposures limited to 10,000 s||Allows > 10,000 s exposures|
|Dithering possible||No dithering allowed|
|No spectral foldover below ~4.5 µm||Affected by spectral foldover < 4.5 µm|
|Sensitive to pointing uncertainty, drift||No slit losses|
|Time Series Observation special requirement not permitted||Time Series Observation special requirement mandatory|
Sources in the imager field of view when performing LRS slit spectroscopy
There is no shutter or other way to block light from entering the imager field of view (see Figure 1) when taking a low-resolution spectrum in the slit. Point sources in the imaging field will therefore appear as slitless spectra on the imager portion of the field of view (FOV). The broad bandpass of the LRS double prism can easily cause the detector to saturate if bright and extended sources are present in the imager portion of the array. Very bright or saturated sources can cause detector artifacts along rows and columns around the bright source, which could in principle create artifacts in the spectrum of the source in the LRS slit. If possible, observers should avoid having very bright sources in the imager portion of the detector field of view whilst exposing with the LRS (they can check using the Aladin visualization option in APT). The full detector read out will be available to observers, allowing any such sources, if present, to be identified, which can help with data analysis.
The spectra of sources coincidentally located in the imager field cannot be processed or calibrated.
Dithering is available and mandatory for observations in the LRS slit. Dithering mitigates for the effects of bad pixels, provides subpixel sampling, and provides observations of the background for background subtraction purposes.
Three dither options are offered in the MIRI LRS Template in APT:
- ALONG SLIT NOD
The ALONG SLIT NOD option places the target alternately at 30% and 70% along the slit length, i.e. a separation of approximately 1.9". This should be the default choice for slit spectroscopy of point or compact sources.
The MAPPING option can be chosen to map a wider field. Selecting this option then asks the user to define the number of steps in the spatial and spectral directions, and the step size in each direction (in arcseconds). Although the maximum dither size is set by avoiding the need to acquire new guide stars, a useful guideline is that dithers larger than 20" will be much slower than ones smaller than this limit. When choosing the Mapping option, the user does not control the order in which the exposures will be executed.
In LRS slitless mode, dithering is disabled. This mode is optimized for high-precision spectrophotometry in time-series observations; for such observations, dithering is not scientifically useful and therefore not supported.
LRS exposure specifications
MIRI LRS slit spectroscopy supports two different detector readout patterns:
The maximum exposure duration for a single exposure with the LRS slit is 10,000 s. This limit applies to all JWST instruments and modes that are not time-series observations. However, LRS slitless observations are always marked as time-series observations. Therefore, the 10,000 second limit is waived to allow for lengthy observations of time-variable phenomena.
A few additional items should be considered:
- for extended targets, a dedicated observation may be required to measure the sky background.
- to cover the full extent of extended targets, observers can specify mosaics for slit spectroscopy.
- for both slit and slitless observations, target acquisition is highly recommended (mandatory for slitless TSOs).
Further advice for preparing observations with MIRI LRS can be found on the following pages: