NIRSpec spectra

example spectrum JADES-DEEP Prism spectrum of GOODS-South #58975

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 single root 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

1000 NIRSpec prism spectra in one plot!

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.

spetrum comparison