NIRCam Short Wavelength Grism Time Series
JWST NIRCam's short wavelength grism time-series observing mode uses the Dispersed Hartmann Sensor (DHS) to perform rapid spectroscopic (R ~ 300) monitoring of bright, time-variable sources at 0.6–2.3 µm. It was added to the NIRCam grism time-series APT template for Cycle 4, but has its own calculation type in the JWST ETC.
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See also: NIRCam Grism Time-Series APT Template, NIRCam Short Wavelength Grism Time Series Observing Strategies and NIRCam Grism Time Series
The NIRCam DHS was designed to support phasing of the JWST mirror segments during commissioning, but is now available in the NIRCam Grism Time-Series APT Template to provide point source spectroscopy in the short wavelength (SW) channel. It can only be paired with the long wavelength (LW) grism, and in that combination provides wavelength coverage within the 0.6–5.0 µm range.
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More information about multistripe subarrays is available at NIRCam Multistripe Subarrays. The GDHS0 element, which disperses spectra along detector rows, is available for science. The GDHS60 element disperses at an oblique angle across the detectors, and is reserved for engineering purposes. Through the remainder of this article "DHS" implies the GDHS0 element in the NIRCam module A short wavelength channel. Science applications of the DHS for transit spectroscopy were described by Schlawin et al. (2017).
Due to the complexities of new detector readout operations and limited time to obtain on-sky calibration data prior to Cycle 4 observations, the accuracy of the JWST ETC for the short wavelength grism time-series calculations may not meet the 10% accuracy requirement. As a result, this capability is being offered on a shared-risk basis in Cycle 4. Calibration observations will be obtained and used to improve the accuracy of the ETC and the pipeline during and after Cycle-3.
Optical properties of the Dispersed Hartmann Sensor (DHS) pupil element and its grisms
The DHS pupil wheel element is composed of 10 separate grisms that occupy rectangular sub-apertures. Each grism includes a wedge in the cross-dispersion direction such that 10 spectra are produced, and are well separated in the cross-dispersion direction. The properties of the grisms and the spectra they produce are summarized below. A new detector readout mode, multistripe subarrays, has been implemented to optimally sample the individual spectra while skipping over portions of the detector devoid of spectral signal.
DHS pupil sub-aperture alignment to the primary mirror pupil
The alignment of the DHS sub-apertures has been adjusted such that the dispersion direction is parallel to detector rows of the NIRCam short wavelength detectors in module A, and is shown in Figure 1. This alignment allows narrow subarrays with short frame times to be used, which is desirable for observations of very bright host stars of transiting exoplanets. The location of the DHS sub-apertures relative to the JWST primary mirror pupil is shown below. Because the pupil wheel rotational position aligning spectra with rows is different from that used for commissioning of the primary mirror, overlap of some of the sub-apertures is less than optimal. Both the throughput and the quality of the PSF is degraded, particularly for sub-apertures 1 and 6. The highest throughput sub-apertures are 4 and 7, which also have the sharpest PSFs. Of the remaining sub-apertures, throughput and PSF quality don't vary greatly, with sub-aperture 9 being somewhat worse.
Table 1a. Fractional area of the DHS sub-apertures relative to the area of the primary mirror
DHS sub-aperture | 2 | 3 | 4 | 5 | 7 | 8 | 9 | 10 | Total |
Fractional Area (%) | 3.12 | 3.13 | 3.86 | 2.67 | 3.94 | 3.53 | 2.78 | 2.75 | 25.8 |
Sub-aperture (spectrum) combinations
Users can choose to simultaneously collect spectra from 2, 4 or 8 of the DHS sub-apertures (also simultaneously with the long-wavelength grism spectrum). The sub-apertures included in those combinations and the combined throughput is summarized in Table 1b.
Table 1b. DHS sub-apertures included in the 2-Spectra, 4-Spectra and 8-Spectra subarray
# of Spectra selected | 2 | 4 | 8 |
DHS sub-apertures included | 4, 7 | 2, 4, 7, 8 | 2, 3, 4, 5, 7, 8, 9, 10 |
\Sigma(Fractional aperture throughput) (%) | 7.8 | 14.5 | 25.8 |
Spectra produced by the DHS grisms
Example DHS spectra of a single point-source target are shown in Figure 2. The spectra fall on the lower (-V3) portions of detectors A2 and A4, and the upper (+V3) portions of detectors A1 and A3 (see NIRCam Field of View). Users have some flexibility to select which spectra to collect: the 2 brightest, the 4 brightest or the 8 brightest. Spectra from DHS sub-apertures 1 and 6 have very much lower throughput (see Figure 1, above), much broader point spread and line spread functions, and significantly lower resolving power than the other 8 sub-apertures, and data for them are not collected (and in fact fall in the SW detector gap, by design).
Long wavelength grism (left) and direct (right) images at two mosaic positions (1 & 2).
Short wavelength DHS spectra on the 4 SW detectors for mosaic position 1, and at the F444W along-dispersion field point.
Short wavelength DHS spectra on the 4 SW detectors for mosaic position 2, and at the F322W2 along-dispersion field point.
Click on the figures for a larger view.
Spectra and point source images from the long wavelength channel (top) from an observation taken to refine pointing for the short wavelength grism time-series mode. Two mosaic tiles are shown as a red/green overlay, and the data were used to accurately measure relative and absolute positions of spectra on the detectors. The middle and bottom panels show simultaneously-acquired DHS spectra through the F150W2 filter on the NIRCam module A short wavelength detectors for the lower (Tile 1) and the F444W along-dispersion position (middle panel) and the upper (Tile 2) position and the F322W2 along-dispersion position (bottom panel). Green rectangles in the middle and bottom panels indicate the approximate subarrays used to read out the spectra. The final pointing used for science places the DHS spectra for DHS subapertures 1 and 6 in the short wavelength SCA gap (indicated by the orange shading in the middle and bottom panels), and the long wavelength spectrum approximately half way between the locations shown in the top panel (see also Figure 8 below). Contamination spectra from another source are visible, particularly on the A1 and A3 detectors. Because the DHS produces 10 spectra for every source in the field, careful observation planning will be necessary to minimize contamination except for particularly well-isolated targets.
DHS point spread and line spread functions
Because the DHS sub-apertures are much smaller than the primary mirror aperture, and are oblong, the monochromatic PSFs from them are very different from the normal JWST PSFs. In particular they are very elongated in the dispersion direction. The width of the monochromatic PSF in the dispersion direction is the line spread function and determines the resolving power.
Dispersion and Resolving Power
The DHS grisms have constant dispersion over the wavelength range of interest (0.6–2.2 µm). The resolving power is entirely controlled by the line spread function at all wavelengths, and is also constant vs. wavelength. The values are given below for 1st and 2nd order. The grisms have significantly higher throughput below 0.9 µm in 2nd order than in 1st, so 2nd order spectra for the shortest filters (see Table 3) will be most useful for science. For the F150W2 filter, the 2nd order DHS spectra at wavelengths 1.01–1.15 µm overlap the 1st order spectrum starting at 2.02 µm. While that filter has good transmission out to 2.3 µm, observers should consider using the F200W filter if they are particularly interested in wavelengths 2.0–2.3 µm. Contamination by 2nd order spectra is only an issue for the F150W2 filter.
Table 2. DHS dispersion and resolving power
Dispersion (nm/pixel) | Resolving Power (\lambda / \delta \lambda) | ||
1st Order | 2nd Order | 1st Order | 2nd Order |
0.290 | 0.145 | 300 | 600 |
Throughput
The DHS grisms have an anti-reflection coating that has very high transmission beyond 1 µm, and a steeply declining transmission below that. The grism blaze function also results in lower throughput below about 1.2 µm, so the overall throughput in 1st order is low at the shortest NIRCam wavelengths. The grisms are more efficient in 2nd order below about 0.9 µm, as can be seen in Figure 4.
Allowed filters
The DHS can be paired with the filters given in Table 3. The F150W2 filter offers the largest grasp (1.01–2.38 μm), but is also more susceptible to contamination by nearby sources than the narrower filters. Moreover, longward of 2 μm the spectra are contaminated by 2nd order light from 1.01–1.19 μm, so observers should consider using F200W if they are interested in the 2–2.23 μm range. DHS throughput data at the wavelengths included in the F070W and F090W bandpasses is poorly characterized, but is significantly lower than for the longer filters, as shown in Figure 4.
Depending on the choice of LW filter, 2 possible field point locations along the spectral direction are possible, one corresponding to choosing long wavelength filters F277W/F356W/F322W2 and the other to choosing F444W (see NIRCam Grism Time Series). Selection of the long wavelength filter in APT controls the placement of the spectra in both the short and long wavelength channels: the location and spectral coverage in the short wavelength channel is entirely determined by the choice of long wavelength filter. Table 3 tabulates the spectral ranges on the SW detectors for each SW filter, spectral order, and choice of long wavelength filter. Cells marked in yellow correspond to low throughput combinations. The same ranges are visually displayed in Figure 5.
The exact wavelength ranges depend on the DHS sub-aperture. The values below are for the median dispersion solutions, but variations of ± ~0.01 µm occur due to slight differences in the location of the undeviated wavelength location on the detectors for the individual grisms. The undeviated wavelength is 1.36 μm.
Table 3. Wavelength coverage for the allowed SW grism spectroscopy blocking filters
DHS blocking filter | LW filter and spectral field point | Order | Wavelength range on A3/A4 (μm) | Wavelength range on A1/A2 (μm) |
---|---|---|---|---|
F070W | F277W/F356W/F322W2 | 2nd | 0.62–0.78 | - |
F444W | 1st | 0.63–0.78† | - | |
2nd | 0.64–0.78 | |||
F090W | F277W/F356W/F322W2 | 2nd | 0.8–0.83 | 0.86–1.00 |
F444W | 1st | 0.8–1.00† | - | |
2nd | 0.8–0.94 | |||
F115W | F277W/F356W/F322W2 | 1st | 1.07–1.28 | - |
2nd | - | 1.01–1.15†† | ||
F444W | 1st | 1.01–1.23 | ||
F150W2 | F277W/F356W/F322W2 | 1st | 1.07–1.66 | 1.71–2.01* |
F444W | 1st | 1.01–1.23 | 1.28–1.89 | |
F200W | F277W/F356W/F322W2 | 1st | - | 1.76–2.23 |
F444W | 1st | - | 1.76–1.89 |
† The DHS has low throughput below 1 μm for 1st order spectra
†† The DHS has low throughput above 1 μm for 2nd order spectra
* The 2.01 μm cutoff is due to 1st and 2nd order overlap, although nominally the spectra extend beyond it
Saturation and Sensitivity
Because the DHS sub-apertures sample such small fractions of the primary mirror (see Table 1), saturation limits are relatively high and sensitivity relatively low compared to the long wavelength grism time-series values.
Saturation limit varies by sub-aperture, with #7 having the highest throughput. Depending on how many sub-aperture spectra the user has chosen to collect (2, 4 or 8), saturation of the sub-aperture 7 spectrum may or may not be a particular concern. Figure 6 shows the saturation limit for sub-aperture 7, thus providing the most conservative estimate.
Subarrays for DHS time-series spectroscopy
The subarrays used to read out pixels associated with the individual DHS spectra (see Figure 1) are part of a new capability developed for Cycle 4, named multistripe. In summary, a multistripe subarray consists of multiple stripes (contiguous rows of pixels). These "substripes" need not be contiguous on the detector, and the placement of the substripes is configurable within certain limits. Users are referred to the article NIRCam Multistripe Subarrays for additional detail about the capability.
For DHS grism time-series observations, 4 sizes of multistripe subarrays are available, providing flexibility in terms of the frame time and the number of spectra read out. Each multistripe subarray includes 4 rows of reference pixels read out once per frame time (the same as for FULL frame readout, or normal subarrays at the -V3 or +V3 edges of the NIRCam detectors). Additional substripes are read out at the locations of the individual spectra from the DHS sub-apertures. The complete set of substripes, including the reference pixels, comprises a subarray frame.
When SW Channel Mode is set to GRISM in the NIRCam Grism Time Series APT template, the target is positioned such that 4 of the DHS spectra fall on detectors A1 and A3 while the other 4 spectra fall on A2 and A4. The same subarray size must be used in both the short and long wavelength channel of NIRCam. However, there is only one spectrum in the LW channel. The multistripe capability allows a single substripe to be read out repeatedly during the subarray frame time. That is done on the LW channel, providing multiple samples of the LW spectrum within the subarray frame time, while spatially separated stripes are being sampled on the SW detectors.
Figure 8 is a schematic showing the locations of the DHS spectra in the SW channel and the LW grism spectrum in the LW channel (see also Figure 2). While 2, 4 or 8 of the DHS spectra are being read, the corresponding LW grism substripe is read 1, 2 or 4 times more frequently. For targets where photon statistics dominate, the oversampling of the LW spectrum has a tiny effect on the SNR of that spectrum, but there are potential benefits in terms of the LW saturation limit. While the ETC does not currently capture those benefits, the level-1 and level-2a data products include the extra LW reads.
Table 4 summarizes the multistripe subarrays available for the SW DHS grism mode, and the corresponding oversampling that occurs in the LW channel.
Table 4. DHS time series multistripe subarray parameters
# Reads per spectrum per tFrame | ||||||||
Subarray | # Substripes per SCA | # Spectra | Rows per substripe | Frame time (tFrame) | Stripe time* | SW (DHS) | LW (Grism) | DHS spectra included |
SUB40S1_2-SPECTRA | 1 | 2 | 36 | 0.21485 | 0.18864 | 1 | 1 | 4, 7 |
SUB80S2_4-SPECTRA | 2 | 4 | 38 | 0.42445 | 0.19912 | 1 | 2 | 2, 4, 7, 8 |
SUB160S4_8-SPECTRA (SUB160STRIPE4_DHS) | 4 | 8 | 39 | 0.84365 | 0.20436 | 1 | 4 | 2, 3, 4, 5 7, 8, 9, 10 |
SUB256S4_8-SPECTRA (SUB256STRIPE4_DHS) | 4 | 8 | 63 | 1.34669 | 0.33012 | 1 | 4 |
* The time to read "Rows per substripe" rows of pixels. Prior to reading the first substripe, 4 rows of reference pixels are read in 0.02096 s. See also the "Multistripe timing equations" section in NIRCam Multistripe Subarrays
ETC Considerations
The JWST Exposure Time Calculator (ETC) includes a new calculation type: SW Grism Time Series. As with all ETC calculations for NIRCam, there are separate calculations for the short and long wavelength channels: the SW Grism Time Series calculation should only be paired with the LW Grism Time Series. Those two are represented in APT by the Grism Time Series observing template.
The DHS was never intended to provide accurate flux and wavelength calibration because neither was necessary for phasing of the JWST primary mirror. In particular, grism throughput below 1 µm is poorly characterized, and a new and somewhat approximate pupil mask had to be created to represent the DHS sub-apertures. Observations of calibration sources with the DHS began in Cycle 3, and improvements to the overall calibration may be possible prior to the start of Cycle 4 observations.
The primary selections that are distinct to the SW Grism Time Series calculation are the PSF Type (on the Instrument Setup tab) and Subarray (on the Detector Setup tab). In order to fully characterize their observing setup, users will need two separate calculations in the ETC: one for the SNR and one for saturation. Both will need to have the same detector configuration.
- Calculation of SNR for the 2- 4- and 8-spectra PSF types uses the sum of the corresponding sub-aperture areas (see Table 1a and 1b), and it uses the average PSF shape for those spectra at each wavelength.
- Calculation of saturation uses the spectrum from sub-aperture 7 which has the highest throughput and the sharpest PSF. The ETC PSF type called Brightest Spectrum (Saturation) provides a conservative estimate of saturation using just that sub-aperture. The spectrum from sub-aperture 7 is included in all DHS observations.
The PSF Type and the Subarray can't be selected independently because the subarray has to sample the individual DHS spectra correctly. For the 2 Spectra and 4 Spectra PSF Types only a single subarray selection is available; for the 8 Spectra PSF Type there are 2 available subarrays, SUB160STRIPE4_DHS and SUB256STRIPE4_DHS (with 160 or 256 total detector rows, respectively). These differ in frame time (see Table 4), and the SUB256 choice provides more sky and may be more useful if there are nearby sources that may contaminate the spectra of the science target. If the Brightest Spectrum (Saturation) PSF type is selected the user should select the subarray corresponding to their expected science exposure, and enter the same exposure parameters on the Detector Setup tab.
Data volume
When the DHS is selected as the SW optical element in APT, 5 detectors are read out as opposed to 3 detectors if SW imaging of any kind is paired w/ the LW grism. This results in data rates 67% higher than if SW imaging is selected. The larger data rate is easily handled on-board, but the corresponding increase in data volume per downlink may require observers to split their observations into multiple exposures or even multiple observations in order to stay within the data volume that can be downlinked each day. APT correctly reports data volume per observation and provides warnings or errors if observations exceed the downlink capability.
References
Schlawin et al. 2017, PASP, 129, 971
Two NIRCam Channels are Better than One: How JWST Can Do More Science with NIRCam’s Short-wavelength Dispersed Hartmann Sensor