NIRSpec spectra
Here you can find various ways to access uniformly-reduced public NIRSpec datasets:
- nirspec_graded_v3.html: Searchable table of all public spectra reduced so far
- For pannable images with various possible layers, including HST and JWST filters as well as spectral observations, see the Map View pages. To see individual spectra, pan over a source with the different Spectra overlays enabled.
- See the nirspec-data-products post for examples on working directly with the catalog and individual extracted spectra
More documentation coming soon. The spectroscopy reduction process is described in de Graaff et al. (2024) and Heintz et al. (2023) and those should be cited if you use the DJA NIRSpec data products, along with any relevant citations to the separate surveys and program IDs for specific spectra. The msaexp software used to process the spectra is freely available.
Public NIRSpec datasets (v3)
These are the public datasets in the nirspec_graded_v3.html compilation:
JWST program | Survey | root |
Grating-Filter (t) | N total | N grade=3 |
---|---|---|---|---|---|
1180 | JADES D’Eugenio et al. (2024) |
jades-gds-wide-v3 jades-gds-wide2-v3 jades-gds-wide3-v3 |
G140M-F070LP ( 1.7) G235M-F170LP ( 1.7) G395M-F290LP ( 1.7) PRISM-CLEAR ( 1.0) |
1255 | 669 |
1181 | JADES | jades-gdn-v3 jades-gdn09-v3 jades-gdn10-v3 jades-gdn11-v3 jades-gdn2-blue-v3 jades-gdn2-v3 |
G140M-F070LP ( 1.7) G140M-F100LP ( 1.7) G235M-F170LP ( 1.7) G395H-F290LP ( 1.7) G395M-F290LP ( 1.7) PRISM-CLEAR ( 1.7) |
1717 | 1154 |
1199 | GTO Stiavelli et al. (2023) | macs1149-stiavelli-v3 | G235M-F170LP ( 6.2) G395M-F290LP ( 6.9) |
294 | 77 |
1207 | GTO (G. Rieke) | gds-rieke-v3 | G140M-F100LP ( 1.9) G235M-F170LP ( 1.9) |
168 | 137 |
1210 | JADES | gds-deep-v3 | G140M-F070LP ( 4.6) G235M-F170LP ( 4.6) G395H-F290LP ( 4.6) G395M-F290LP ( 4.6) PRISM-CLEAR (18.5) |
217 | 166 |
1211 | GTO WIDE Maseda et al. (2024) |
goodsn-wide-v3 goodsn-wide0-v3 goodsn-wide1-v3 goodsn-wide2-v3 goodsn-wide3-v3 goodsn-wide6-v3 goodsn-wide7-v3 goodsn-wide8-v3 |
G235H-F170LP ( 0.9) G395H-F290LP ( 1.0) PRISM-CLEAR ( 0.7) |
1115 | 753 |
1212 | GTO WIDE | jades-gds-w03-v3 jades-gds-w05-v3 jades-gds-w06-v3 jades-gds-w07-v3 jades-gds-w08-v3 jades-gds-w09-v3 |
G140M-F100LP ( 0.7) G235H-F170LP ( 0.9) G395H-F290LP ( 1.0) PRISM-CLEAR ( 0.7) |
1119 | 514 |
1213 | GTO WIDE | gto-wide-egs1-v3 gto-wide-egs2-v3 |
G235H-F170LP ( 0.9) G395H-F290LP ( 1.0) PRISM-CLEAR ( 0.7) |
739 | 434 |
1214 | GTO WIDE | gto-wide-cos01-v3 gto-wide-cos02-v3 gto-wide-cos03-v3 gto-wide-cos05-v3 |
G235H-F170LP ( 0.9) G395H-F290LP ( 1.0) PRISM-CLEAR ( 0.7) |
479 | 343 |
1215 | GTO WIDE | gto-wide-uds10-v3 gto-wide-uds11-v3 gto-wide-uds12-v3 gto-wide-uds13-v3 gto-wide-uds14-v3 |
G235H-F170LP ( 0.9) G395H-F290LP ( 1.0) PRISM-CLEAR ( 0.7) |
645 | 431 |
1286 | JADES | jades-gds02-v3 jades-gds03-v3 jades-gds04-v3 jades-gds05-v3 jades-gds06-v3 jades-gds07-v3 jades-gds08-v3 jades-gds1-v3 |
G140M-F070LP ( 2.4) G235M-F170LP ( 2.4) G395H-F290LP ( 2.4) G395M-F290LP ( 2.4) PRISM-CLEAR ( 1.6) |
2092 | 897 |
1324 | GLASS-ERS Mascia et al. (2024) |
abell2744-glass-v3 | G140H-F100LP ( 9.7) G235H-F170LP ( 9.7) G395H-F290LP ( 9.7) |
182 | 79 |
1345 | CEERS-ERS Finkelstein et al. (2023) |
ceers-v3 | G140M-F100LP ( 1.7) G235M-F170LP ( 0.9) G395M-F290LP ( 0.9) PRISM-CLEAR ( 0.9) |
1184 | 747 |
1433 | MACS-J0647 Hsiao et al. (2024) |
macsj0647-single-v3 macsj0647-v3 |
PRISM-CLEAR ( 1.8) | 226 | 90 |
1747 | BoRG (G. Roberts-Borsani) | borg-0037m3337-v3 borg-0314m6712-v3 borg-0409m5317-v3 borg-0440m5244-v3 borg-0859p4114-v3 borg-0955p4528-v3 borg-1033p5051-v3 borg-1437p5044-v3 borg-2203p1851-v3 |
PRISM-CLEAR ( 0.7) | 404 | 199 |
1810 | Bluejay Belli et al. (2024) |
bluejay-north-v3 bluejay-south-v3 |
G140M-F100LP (25.9) G235M-F170LP ( 6.5) G395M-F290LP ( 1.6) |
140 | 132 |
1869 | LyC-22 (D. Schaerer) |
lyc22-schaerer-03-v3 lyc22-schaerer-12-v3 |
G140M-F100LP (18.2) G235M-F170LP (14.6) |
92 | 76 |
1871 | (J. Chisholm) | gdn-chisholm-v3 | G235H-F170LP (29.2) G395H-F290LP ( 5.3) |
22 | 12 |
1879 | (M. Curti) | cosmos-curti-v3 | G140M-F100LP (30.8) G235H-F170LP ( 5.8) G235M-F170LP ( 7.3) |
75 | 69 |
1914 | AURORA Shapely et al. (2024) |
aurora-gdn01-v3 aurora-gdn02-v3 |
G140M-F100LP (12.2) G235M-F170LP ( 7.9) G395M-F290LP ( 4.1) |
106 | 86 |
2028 | Wang et al. (2024) | j0910-wang-v3 | G395M-F290LP ( 3.6) PRISM-CLEAR ( 1.1) |
264 | 114 |
2073 | (J. Hennawi) | j0252m0503-hennawi-07-v3 j1007p2115-hennawi-v3 |
PRISM-CLEAR ( 1.3) | 434 | 161 |
2110 | SUSPENSE Slob et al. (2024) |
suspense-kriek-v3 | G140M-F100LP (16.2) | 43 | 39 |
2198 | Barrufet et al. (2024) | gds-barrufet-s156-v3 gds-barrufet-s67-v3 |
PRISM-CLEAR ( 0.7) | 139 | 130 |
2282 | Bradley et al. (2023) | whl0137-v3 | PRISM-CLEAR ( 1.0) | 214 | 59 |
2478 | (D. Stark) | stark-a1703-v3 stark-rxcj2248-v3 |
G140M-F100LP ( 3.4) G235M-F170LP ( 0.9) G395M-F290LP ( 0.9) |
94 | 18 |
2561 | UNCOVER Bezanson et al. (2024) |
uncover-61-v3 uncover-62-v3 uncover-v3 |
PRISM-CLEAR ( 4.4) | 858 | 569 |
2565 | Nanayakkara et al. (2024) | glazebrook-cos-obs1-v3 glazebrook-cos-obs2-v3 glazebrook-cos-obs3-v3 glazebrook-egs-v3 glazebrook-v3 |
PRISM-CLEAR ( 0.5) | 631 | 443 |
2593 | CECILIA Strom et al. (2023) |
cecilia-v3 | G235M-F170LP (38.9) G395M-F290LP ( 1.2) |
51 | 30 |
2674 | (P. Arrabal Haro) | gdn-pah123-v3 gdn-pah4-v3 |
G395M-F290LP ( 2.9) | 204 | 105 |
2736 | SMACS-0723 ERO Pontoppidan et al. (2022) |
smacs0723-ero-v3 | G235M-F170LP ( 9.7) G395M-F290LP ( 9.7) |
62 | 26 |
2750 | Arrabal Haro et al. (2023) | ceers-ddt-v3 | PRISM-CLEAR ( 5.1) | 154 | 125 |
2756 | (W. Chen) | abell2744-ddt-v3 | PRISM-CLEAR ( 0.6) | 123 | 68 |
2767 | Williams et al. (2023) | rxj2129-ddt-v3 | G140M-F070LP ( 3.3) PRISM-CLEAR ( 1.2) |
145 | 50 |
3073 | Castellano et al. (2024) | abell2744-castellano1-v3 | PRISM-CLEAR ( 1.8) | 281 | 132 |
3215 | JADES Ultra-Deep Eisenstein et al. (2023) |
gds-udeep-v3 | G140M-F070LP ( 6.9) G395M-F290LP (37.0) PRISM-CLEAR (27.7) |
226 | 145 |
3543 | EXCELS Carnall et al. (2024) |
excels-uds01-v3 excels-uds02-v3 |
G140M-F100LP ( 8.0) G235M-F170LP (10.9) G395M-F290LP ( 8.0) |
292 | 135 |
4106 | (E. Nelson) | egs-nelsonx-v3 | G395M-F290LP ( 2.2) PRISM-CLEAR ( 3.6) |
136 | 102 |
4233 | RUBIES de Graaff et al. (2024) |
rubies-egs51-v3 rubies-egs52-v3 rubies-egs53-v3 rubies-egs61-v3 rubies-egs62-v3 rubies-egs63-v3 rubies-uds1-v3 rubies-uds2-v3 rubies-uds21-v3 rubies-uds22-v3 rubies-uds23-v3 rubies-uds3-v3 rubies-uds31-v3 rubies-uds32-v3 rubies-uds33-v3 rubies-uds41-v3 rubies-uds42-v3 rubies-uds43-v3 |
G395M-F290LP ( 0.8) PRISM-CLEAR ( 0.8) |
5054 | 2387 |
4246 | (A. Abdurro’uf) | macsj0647-hr-v3 | G395H-F290LP ( 1.9) | 134 | 44 |
4446 | Frye et al. (2023) | snh0pe-v3 | G140M-F100LP ( 2.4) G235M-F170LP ( 3.6) PRISM-CLEAR ( 0.2) |
42 | 24 |
4557 | (H. Yan) | pearls-transients-v3 | PRISM-CLEAR ( 7.8) | 214 | 25 |
6541 | (E. Egami) | gds-egami-ddt-v3 | PRISM-CLEAR ( 2.3) | 339 | 132 |
6585 | (D. Coulter) | cosmos-transients-v3 | PRISM-CLEAR ( 3.3) | 300 | 181 |
- The
root
column is a general rootname simply indicating spectra that were reduced together. For many programs that corresponds to individual MSA mask plans (e.g., RUBIES), but for some programs a singleroot
name can correspond to multiple masks. For those roots that contain multiple mask plans, all spectra of a particular source from potentially multiple plans were co-added. This inconsistency of the co-addition treatment is due to the rolling nature of the processing of archival datasets as they became public and may be standardized in future reductions. - The
root
values are linked to individual tables summarizing the sources in that mask. Those tables have slightly different columns than the grade summary as they are generated before the redshifts are estimated from the spectra. - As below, exposure time per spectrum t (in hours) computed from
median(exptime)
in the spectra files, which isn’t quite correct and double-counts exposure times for spectral extractions that overlap both NRS1 and NRS2 detectors - “N total” is the total number of estimated unique sources in that complation.
Public NIRSpec datasets (v1)
These are the public datasets in the nirspec_graded.html compilation:
root |
JWST program | Grating-Filter | t, hours | N total | N grade=3 |
---|---|---|---|---|---|
abell2744-ddt-v1 | 2756 | PRISM-CLEAR | 0.6 | 111 | 51 |
abell2744-glass-v1 | 1324 | G140H-F100LP | 6.5 | 179 | 27 |
abell2744-glass-v1 | 1324 | G235H-F170LP | 6.5 | 176 | 35 |
abell2744-glass-v1 | 1324 | G395H-F290LP | 6.5 | 177 | 31 |
ceers-ddt-v1 | 2750 | PRISM-CLEAR | 5.1 | 266 | 109 |
ceers-lr-v1 | 1345 | PRISM-CLEAR | 0.9 | 1058 | 539 |
ceers-mr-v1 | 1345 | G140M-F100LP | 1.7 | 302 | 77 |
ceers-mr-v1 | 1345 | G235M-F170LP | 1.7 | 302 | 115 |
ceers-mr-v1 | 1345 | G395M-F290LP | 1.7 | 302 | 126 |
gds-deep-hr-v1 | 1210 | G395H-F290LP | 4.6 | 154 | 57 |
gds-deep-lr-v1 | 1210 | PRISM-CLEAR | 9.2 | 294 | 159 |
gds-deep-mr-v1 | 1210 | G140M-F070LP | 4.6 | 217 | 18 |
gds-deep-mr-v1 | 1210 | G235M-F170LP | 4.6 | 216 | 59 |
gds-deep-mr-v1 | 1210 | G395M-F290LP | 4.6 | 221 | 68 |
goodsn-wide-v1 | 1211 | PRISM-CLEAR | 0.7 | 182 | 80 |
macsj0647-single-v1 | 1433 | PRISM-CLEAR | 1.8 | 69 | 19 |
macsj0647-v1 | 1433 | PRISM-CLEAR | 1.8 | 132 | 46 |
rxj2129-ddt-v1 | 2767 | G140M-F070LP | 2.2 | 20 | 0 |
rxj2129-ddt-v1 | 2767 | G140M-F100LP | 2.2 | 20 | 3 |
rxj2129-ddt-v1 | 2767 | PRISM-CLEAR | 1.2 | 103 | 34 |
smacs0723-ero-v1 | 2736 | G235M-F170LP | 9.7 | 50 | 12 |
smacs0723-ero-v1 | 2736 | G395M-F290LP | 9.7 | 51 | 16 |
snH0pe-v1 | 4446 | G140M-F100LP | 2.4 | 39 | 17 |
snH0pe-v1 | 4446 | G235M-F170LP | 3.6 | 39 | 15 |
snH0pe-v1 | 4446 | PRISM-CLEAR | 0.2 | 39 | 17 |
whl0137-v1 | 2282 | PRISM-CLEAR | 1.0 | 405 | 80 |
Total | 5124 | 1810 |
- Exposure time per spectrum t computed from
median(effexptm)
in the spectra files, which isn’t quite correct and double-counts exposure times for spectral extractions that overlap both NRS1 and NRS2 detectors
Full visualization
Spectral coverage comparison
One aspect of the unique power of the NIRSpec PRISM mode is the broad wavelength coverage from 0.7 < λ < 5.3 µm. The comparisons below show the wavelength coverage from WFC3 G141 slitless spectroscopy or from a ground-based near-infrared spectrograph such as Keck/MOSFIRE with its attendant atmospheric windows. Note that the comparison just shows the wavelength coverage, not differences in sensitivity and spectral resolution, which are significant between these observing modes.