REVIEW 3 major objections 4 minor 120 references
Herschel map of Saturn's stratospheric water, delivered by the plumes of Enceladus
T0 review · 3 major / 4 minor · reviewed 2026-08-14 · deepseek-v4-flash
Pith's one-line read Saturn's stratospheric water is concentrated in an equatorial band, pointing to Enceladus's plumes as its main source.
desk verdict First disk-resolved H2O map robustly kills the uniform-IDP picture, but the Enceladus attribution is more interpretive than the abstract lets on. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is the disk-resolved line-area map of the 66.44-micrometer water transition, interpreted with a line-by-line radiative-transfer calculation on a densely sampled three-dimensional grid. The tested water distributions take the form $y_{\mathrm{H_2O}}(\phi)=y_{\mathrm{eq}}\exp(-\phi^2/2\sigma^2)$ above the local condensation level, where $\phi$ is planetocentric latitude, $y_{\mathrm{eq}}$ the equatorial mole fraction, and $\sigma$ the Gaussian half-width; a meridionally uniform profile is the competing interplanetary-dust model. The argument works by convolving synthetic line maps with the instrument beam and comparing them with the 225 observed spectra, first with a storm-free thermal field and then with a three-dimensional field that inserts +10 K and +5 K patches over the two Great Storm beacons so the equatorial excess can be isolated. The same setup produces the disk-averaged 1097 GHz HIFI line, which probes slightly higher altitudes and exposes the residual vertical-profile incompatibility.
What would settle it
Recompute the fits using beacon temperature profiles retrieved directly from contemporaneous Composite Infrared Spectrometer data instead of the four tested uniform increments; if the best-fit Gaussian moves away from $y_{\mathrm{eq}}=1.1$ ppb and $\sigma=25^\circ$, or if a uniform profile becomes acceptable, the central claim is undermined. An independent check is a water map taken at a time without storm beacons, which should show the same equatorial Gaussian without inserted temperature patches.
Extended reading notes
Core claim
The paper's central claim is that Enceladus, through its plume-fed neutral torus, is the main source of Saturn's stratospheric water. The evidence is the 66.44-micrometer water line map: with the two warm storm beacons added to the thermal field, the observed map is best reproduced by a Gaussian meridional abundance profile centered on the equator, with equatorial mole fraction 1.1 ppb and half-width at half-maximum 25 degrees, giving a normalized chi-squared of 1.1. A meridionally uniform profile, representing interplanetary dust, fails with a normalized chi-squared of 16.2, and a uniform background component is limited to about 0.06 ppb at the 2-sigma level. The water falling from the rings that spacecraft instruments measured in 2017 cannot explain the 2010-2011 observations because that infall appeared later. The paper also reports that adding a vertical gradient above the condensation level reduces, but does not fully remove, the factor-of-five abundance gap between the disk-averaged HIFI line and the disk-resolved PACS map.
Load-bearing premise
The result depends on the assumed temperature and size of the two warm storm vortices: if their actual temperatures, vertical structure, or latitude range differ from the +10 K and +5 K patches used here, the fitted equatorial abundance and width would shift.
Editorial extensions
If this is right
- Enceladus's plume-fed neutral torus, not interplanetary dust or the rings, supplied the stratospheric water seen in 2010-2011.
- A meridionally uniform dust-like contribution is at most about an order of magnitude fainter than the equatorial source, around 0.06 ppb.
- The ring-infall water measured in 2017 cannot be the source of the Herschel-era water; it must have intensified after 2010-2011.
- If the input flux from Enceladus has the predicted 15-degree width, the observed 25-degree width implies meridional eddy mixing of roughly $2\times10^8\ \mathrm{cm^2\,s^{-1}}$ over the downward transport time.
- The next step is two-dimensional photochemical transport modeling, since no simple empirical vertical profile fully reconciles the disk-averaged and disk-resolved water abundances.
Reading between the lines
- The paper does not test this, but the storm-beacon correction could be validated by analyzing a PACS map taken when no storm beacons are present; the same equatorial Gaussian should emerge without inserted temperature patches.
- One could extract a cleaner transport measurement by replacing the paper's rough eddy-mixing estimate with a 2D model that fits the full observed width as a function of altitude, rather than assuming a single diffusion timescale.
- Because the HIFI/PACS abundance gap narrows when a vertical gradient is added, part of the quoted 1.1 ppb may depend on the assumed phosphine continuum and sideband calibration; a re-analysis with those parameters varied would show how robust the equatorial abundance is.
- If the ring source seen in 2017 is still active, future observations should see a narrower equatorial water band superimposed on the Enceladus Gaussian; detecting such a component would confirm the paper's temporal separation of the two sources.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents the first disk-resolved Herschel/PACS map of H2O emission at 66.44 um from Saturn's stratosphere, together with a disk-averaged Herschel/HIFI spectrum of the 1097 GHz H2O line. Several empirical meridional H2O distributions are tested with a 3D radiative-transfer model. A meridionally uniform distribution, representing an IDP source, is robustly rejected: its chi2/N is 18.9 without and 16.2 with the Great Storm beacon temperature adjustments. A Gaussian distribution centered on the equator, with equatorial mole fraction yeq=1.1 ppb and HWHM sigma=25 deg, gives chi2/N=1.1 after adding uniform +10 K/+5 K temperature increases in the two storm beacons. A meridionally uniform background component is constrained to be below 0.06 ppb. A vertical gradient in the H2O profile reduces the HIFI/PACS abundance discrepancy from a factor of about 5 to about 2.4, but does not fully reconcile the two datasets. The paper concludes that Enceladus is the main source of Saturn's stratospheric water.
Significance. If the source attribution holds, the paper resolves a long-standing question about the origin of Saturn's stratospheric water and provides the first direct spatial constraint on its meridional distribution. The robust rejection of a meridionally uniform H2O layer, the derived upper limit on the IDP background, and the rough eddy-mixing estimate are valuable and falsifiable results. The paper's strengths include the careful handling of the PACS raster geometry, the use of a time-dependent CIRS thermal field, explicit chi2/N comparisons among models, and an unusually candid discussion of the remaining HIFI/PACS inconsistency. The central qualitative result, that stratospheric H2O peaks at the equator, is strongly supported. However, the identification of Enceladus as the unique main source is not uniquely determined by the map, because the ring source is also equator-centered and approximately Gaussian, and the quantitative fit depends heavily on an ad hoc beacon thermal model.
major comments (3)
- [Section 5 and Section 4.1] The conclusion that Enceladus is the main source does not follow uniquely from the PACS map. As Section 3.2 acknowledges, the ring source is also centered on the equator and has, to first order, a Gaussian shape; with a PACS beam of 9.42 arcsec HPBW against a planetary diameter of 17.26 arcsec, a compact equatorial source and a 25-degree Gaussian cannot be easily separated. Section 4.1 excludes the rings using the 2017 Cassini INMS/CDA flux measurements and the appearance of D68 clumps in 2015, but this only shows that the 2017 ring influx was too large and too recent; it does not constrain an older, smaller ring influx of order 8 kg/s that could have been present at the Herschel epoch. The abstract's 'demonstrates' therefore overstates what the data alone establish: the map constrains the meridional shape of the H2O column, not the identity of the source.
- [Section 4.3] The beacon thermal model is ad hoc and load-bearing. The paper assumes B1 and B2 span 30N-50N, applies a uniform temperature increase above 10 mbar, and selects the +10 K/+5 K combination from a four-element grid that minimizes chi2. The pre-beacon Gaussian fit has chi2/N=6.3, while the post-beacon fit has chi2/N=1.1, so the reported yeq=1.1 ppb and sigma=25 deg depend strongly on this assumption. The paper itself notes that CIRS had observed only the northern edges of the beacons and that the actual vertical structure was more complex, with a peak at 0.5 mbar. A sensitivity analysis varying the beacon latitude range, cut-off pressure, and vertical profile shape, with uncertainties propagated into yeq and sigma, is needed before these parameters can be reported as the best-fit values.
- [Sections 4.4 and 4.5] The HIFI and PACS data remain mutually inconsistent in abundance. Even after introducing a vertical gradient with n=2 and pgradient=0.1 mbar, the HIFI best fit requires yeq=2.2e-7 while the PACS best fit requires yeq=9e-8, a factor of 2.4, and Section 4.5 states that 'we find no H2O distribution that enables us to fully reconcile the HIFI and PACS data.' This indicates that the empirical model and/or the error budget is incomplete. The qualitative rejection of a uniform distribution is robust, but the quantitative best-fit model and the implied mass flux should be presented with this caveat explicitly stated, and the potential PH3 and thermal-field systematics should be quantified rather than only listed as possible explanations.
minor comments (4)
- [Section 2.1] There is a typo in the sentence describing the line-area map: 'the line-line-area maparea map can be safely analyzed' should read 'the line-area map can be safely analyzed.'
- [Figure 1 caption] The caption contains the typo 'poitings' for 'pointings.'
- [Abstract] The word 'demonstrates' is used twice for conclusions that, given the remaining HIFI/PACS discrepancy and the ring-source degeneracy discussed in Section 4.5 and Section 5, would be more accurately worded as 'indicates' or 'supports.'
- [Section 4.2 and Figure 6] The phrase 'marginally acceptable solutions (chi2/N<9)' is misleading: with roughly 225 PACS pixels, chi2/N=6.3 is formally a very poor fit unless the noise is correlated. The text should either justify the effective number of independent pixels or describe these models as 'best among the tested families' rather than 'acceptable.'
Circularity Check
No significant circularity: the PACS map fit is an empirical result, and the Enceladus attribution rests on external prior evidence and a temporal exclusion of the ring source, not on a self-referential reduction.
full rationale
The derivation chain is not circular. The paper's genuinely new map result is the rejection of a meridionally uniform H2O distribution (chi2/N = 16.2-18.9) in favor of an equator-centered Gaussian (best fit chi2/N = 1.1 after including the storm beacons). That is a data fit, not a prediction drawn from the Enceladus hypothesis. The Enceladus attribution is an interpretation layered on top of the fit, supported by independent prior evidence: the Hartogh et al. (2011) detection of an Enceladus-fed water torus and the Cassidy & Johnson (2010) prediction of an equator-centered Gaussian influx. The fitted width (25 deg) actually disagrees with the prior prediction (15 deg), which the paper explicitly treats as a discrepancy and uses to estimate eddy mixing; hence the fit does not reduce to the prior prediction by construction. The most serious scientific caveat is source degeneracy: the paper itself notes in Section 3.2 that the ring source 'shares common properties with the Enceladus source' and is 'centered on the equator and has, to the first order, a Gaussian shape.' The ring source is excluded by a temporal/flux argument (2017 Cassini influx cannot explain 2010-2011 Herschel water), which is external to the map. That exclusion may be debatable, but it is not a self-referential reduction of the kind required for circularity. The ad hoc beacon temperature increases in Section 4.3 are fitted nuisance parameters; they affect the best-fit yeq and sigma values but are not presented as independent predictions. Section 4.5 candidly reports that no H2O distribution fully reconciles the HIFI and PACS data, further showing that the model is not being forced to match a predetermined conclusion. Overall, no load-bearing step equates a fitted quantity with a predicted quantity or imports a conclusion from an unverified self-citation.
Assumptions & free parameters
free parameters (5)
- yeq (equatorial H2O mole fraction) =
1.1 ppb (PACS best fit); 7.2 ppb (HIFI, simple model); 9e-8 / 2.2e-7 (with vertical gradient)
- sigma (Gaussian HWHM) =
25 deg
- ymin (uniform background component) =
<0.06 ppb (2-sigma upper limit)
- Beacon temperature increases (deltaT_B1, deltaT_B2) =
+10 K / +5 K
- Vertical gradient parameters (n, p_gradient) =
n=2, p_gradient=0.1 mbar
assumptions (6)
- standard math LTE and non-scattering radiative transfer for the H2O lines
- domain assumption Thermal field from Cassini/CIRS (Fletcher et al. 2017) interpolated to the observation dates is accurate; isothermal extrapolation above 0.2 mbar
- domain assumption The 1097 GHz H2O line is unaffected by the Enceladus torus because its lower-state energy (136.76 cm-1) is high
- domain assumption A Gaussian meridional distribution centered on the equator represents the Enceladus source
- domain assumption The ring atmosphere is not a significant neutral H2O source because of low densities and charge-exchange losses
- ad hoc to paper Beacon thermal perturbation is uniform above 10 mbar over 30N-50N with the chosen deltaT values
Cite this review
Pith. "Pith review of Herschel map of Saturn's stratospheric water, delivered by the plumes of Enceladus." pith.science (2026). https://pith.science/paper/XDBUAVPB
@misc{pith2026190807399,
author = {Pith},
title = {Pith review of: Herschel map of Saturn's stratospheric water, delivered by the plumes of Enceladus},
year = {2026},
howpublished = {\url{https://pith.science/paper/XDBUAVPB}},
note = {Machine review of arXiv:1908.07399}
}
read the original abstract
Context. The origin of water in the stratospheres of Giant Planets has been an outstanding question ever since its first detection by ISO some 20 years ago. Water can originate from interplanetary dust particles, icy rings and satellites and large comet impacts. Analysis of Herschel Space Observatory observations have proven that the bulk of Jupiter's stratospheric water was delivered by the Shoemaker-Levy 9 impacts in 1994. In 2006, the Cassini mission detected water plumes at the South Pole of Enceladus, placing the moon as a serious candidate for Saturn's stratospheric water. Further evidence was found in 2011, when Herschel demonstrated the presence of a water torus at the orbital distance of Enceladus, fed by the moon's plumes. Finally, water falling from the rings onto Saturn's uppermost atmospheric layers at low latitudes was detected during the final orbits of Cassini's end-of-mission plunge into the atmosphere. Aims. In this paper, we use Herschel mapping observations of water in Saturn's stratosphere to identify its source. Methods. Several empirical models are tested against the Herschel-HIFI and -PACS observations, which were collected on December 30, 2010, and January 2nd, 2011 (respectively). Results. We demonstrate that Saturn's stratospheric water is not uniformly mixed as a function of latitude, but peaking at the equator and decreasing poleward with a Gaussian distribution. We obtain our best fit with an equatorial mole fraction 1.1 ppb and a half-width at half-maximum of 25{\deg}, when accounting for a temperature increase in the two warm stratospheric vortices produced by Saturn's Great Storm of 2010-2011. Conclusions. This work demonstrates that Enceladus is the main source of Saturn's stratospheric water.
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Works this paper leans on
-
[1]
, " * write output.state after.block = add.period write newline
ENTRY address archiveprefix author booktitle chapter edition editor howpublished institution eprint journal key month note number organization pages publisher school series title type volume year label extra.label sort.label short.list INTEGERS output.state before.all mid.sentence after.sentence after.block FUNCTION init.state.consts #0 'before.all := #1 ...
-
[2]
write newline
" write newline "" before.all 'output.state := FUNCTION n.dashify 't := "" t empty not t #1 #1 substring "-" = t #1 #2 substring "--" = not "--" * t #2 global.max substring 't := t #1 #1 substring "-" = "-" * t #2 global.max substring 't := while if t #1 #1 substring * t #2 global.max substring 't := if while FUNCTION word.in bbl.in " " * FUNCTION format....
-
[3]
2014, , 238, 205
Altobelli , N., Lopez-Paz , D., Pilorz , S., et al. 2014, , 238, 205
2014
-
[4]
A., Lellouch , E., Harwit , M., et al
Bergin , E. A., Lellouch , E., Harwit , M., et al. 2000, , 539, L147
2000
-
[5]
2002, , 159, 95
B \'e zard , B., Lellouch , E., Strobel , D., Maillard , J.-P., & Drossart , P. 2002, , 159, 95
2002
-
[6]
1985, , 296, 644
Borysow , J., Trafton , L., Frommhold , L., & Birnbaum , G. 1985, , 296, 644
1985
-
[7]
& Frommhold , L
Borysow , A. & Frommhold , L. 1986, , 304, 849
1986
-
[8]
1988, , 326, 509
Borysow , J., Frommhold , L., & Birnbaum , G. 1988, , 326, 509
1988
Show all 120 references
-
[9]
Brown , L. R. & Plymate , C. 1996, , 56, 263
1996
-
[10]
2006, , 184, 634
Burgdorf , M., Orton , G., van Cleve , J., Meadows , V., & Houck , J. 2006, , 184, 634
2006
-
[11]
Cassidy , T. A. & Johnson , R. E. 2010, , 209, 696
2010
-
[12]
2008 a , , 56, 1573
Cavali \'e , T., Billebaud , F., Biver , N., et al. 2008 a , , 56, 1573
2008
-
[13]
2008 b , , 484, 555
Cavali \'e , T., Billebaud , F., Fouchet , T., et al. 2008 b , , 484, 555
2008
-
[14]
2009, , 203, 531
Cavali \'e , T., Billebaud , F., Dobrijevic , M., et al. 2009, , 203, 531
2009
-
[15]
2010, , 510, A88
Cavali \'e , T., Hartogh , P., Billebaud , F., et al. 2010, , 510, A88
2010
-
[16]
2012, , 61, 3
Cavali \'e , T., Biver , N., Hartogh , P., et al. 2012, , 61, 3
2012
-
[17]
2013, , 553, A21
Cavali \'e , T., Feuchtgruber , H., Lellouch , E., et al. 2013, , 553, A21
2013
-
[18]
2014, , 562, A33
Cavali \'e , T., Moreno , R., Lellouch , E., et al. 2014, , 562, A33
2014
-
[19]
2017, , 291, 1
Cavali \'e , T., Venot , O., Selsis , F., et al. 2017, , 291, 1
2017
-
[20]
Connerney , J. E. P. & Waite , J. H. 1984, , 312, 136
1984
-
[21]
Connerney , J. E. P. 1986, , 13, 773
1986
-
[22]
Conrath , B. J. & Gautier , D. 2000, , 144, 124
2000
-
[23]
1998, , 336, L85
Coustenis , A., Salama , A., Lellouch , E., et al. 1998, , 336, L85
1998
-
[24]
R., Griffin , M
Davis , G. R., Griffin , M. J., Naylor , D. A., et al. 1996, , 315, L393
1996
-
[25]
1997, , 321, L13
de Graauw , T., Feuchtgruber , H., Bezard , B., et al. 1997, , 321, L13
1997
-
[26]
P., Phillips , T
de Graauw , T., Helmich , F. P., Phillips , T. G., et al. 2010, , 518, L6
2010
-
[27]
J., Drouin , B
Dick , M. J., Drouin , B. J., & Pearson , J. C. 2009, , 110, 619
2009
-
[28]
C., & Hickson , K
Dobrijevic , M., H \'e brard , E., Loison , J. C., & Hickson , K. M. 2014, , 228, 324
2014
-
[29]
E., de Pater , I., Wright , M., Hogerheijde , M
Dunn , D. E., de Pater , I., Wright , M., Hogerheijde , M. R., & Molnar , L. A. 2005, , 129, 1109
2005
-
[30]
1997, , 389, 159
Feuchtgruber , H., Lellouch , E., de Graauw , T., et al. 1997, , 389, 159
1997
-
[31]
S., Gurnett , D
Fischer , G., Kurth , W. S., Gurnett , D. A., et al. 2011, , 475, 75
2011
-
[32]
2010, , 58, 1758
Flandes , A., Spilker , L., Morishima , R., et al. 2010, , 58, 1758
2010
-
[33]
N., Irwin , P
Fletcher , L. N., Irwin , P. G. J., Teanby , N. A., et al. 2007, , 188, 72
2007
-
[34]
N., Orton , G
Fletcher , L. N., Orton , G. S., Teanby , N. A., & Irwin , P. G. J. 2009 a , , 202, 543
2009
-
[35]
N., Orton , G
Fletcher , L. N., Orton , G. S., Teanby , N. A., Irwin , P. G. J., & Bjoraker , G. L. 2009 b , , 199, 351
2009
-
[36]
N., Hesman , B
Fletcher , L. N., Hesman , B. E., Irwin , P. G. J., et al. 2011, Science, 332, 1413
2011
-
[37]
N., Swinyard , B., Salji , C., et al
Fletcher , L. N., Swinyard , B., Salji , C., et al. 2012, , 539, A44
2012
-
[38]
N., Guerlet , S., Orton , G
Fletcher , L. N., Guerlet , S., Orton , G. S., et al. 2017, Nature Astronomy, 1, 765
2017
-
[39]
N., Gustafsson , M., & Orton , G
Fletcher , L. N., Gustafsson , M., & Orton , G. S. 2018 a , , 235, 24
2018
-
[40]
N., Orton , G
Fletcher , L. N., Orton , G. S., Sinclair , J. A., et al. 2018 b , Nature Communications, 9, 3564
2018
-
[41]
F., et al
Fouchet , T., Guerlet , S., Strobel , D. F., et al. 2008, , 453, 200
2008
-
[42]
& Schmitt , B
Fray , N. & Schmitt , B. 2009, , 57, 2053
2009
-
[43]
Friedson , A. J. & Moses , J. I. 2011, AGU Fall Meeting Abstracts, P13C
2011
-
[44]
Gautier , D., Hersant , F., Mousis , O., & Lunine , J. I. 2001, , 550, L227
2001
-
[45]
A., & Michael Flasar , F
Guerlet , S., Fouchet , T., B \'e zard , B., Simon-Miller , A. A., & Michael Flasar , F. 2009, , 203, 214
2009
-
[46]
2010, , 209, 682
Guerlet , S., Fouchet , T., B \'e zard , B., et al. 2010, , 209, 682
2010
-
[47]
M., & Simon-Miller , A
Guerlet , S., Fouchet , T., B \'e zard , B., Flasar , F. M., & Simon-Miller , A. A. 2011, , 38, L09201
2011
-
[48]
2014, , 238, 110
Guerlet , S., Spiga , A., Sylvestre , M., et al. 2014, , 238, 110
2014
-
[49]
J., Esposito , L., Stewart , A
Hansen , C. J., Esposito , L., Stewart , A. I. F., et al. 2006, Science, 311, 1422
2006
-
[50]
2009, , 57, 1596
Hartogh , P., Lellouch , E., Crovisier , J., et al. 2009, , 57, 1596
2009
-
[51]
2011, , 532, L2
Hartogh , P., Lellouch , E., Moreno , R., et al. 2011, , 532, L2
2011
-
[52]
Hedman , M. M. & Showalter , M. R. 2016, , 279, 155
2016
-
[53]
Hersant , F., Gautier , D., & Lunine , J. I. 2004, , 52, 623
2004
-
[54]
M., Loison , J
Hickson , K. M., Loison , J. C., Cavali \'e , T., H \'e brard , E., & Dobrijevic , M. 2014, , 572, A58
2014
-
[55]
2014, Experimental Astronomy, 37, 433
Higgins , R., Teyssier , D., Borys , C., et al. 2014, Experimental Astronomy, 37, 433
2014
-
[56]
2018, Science, 362, aat3185
Hsu , H.-W., Schmidt , J., Kempf , S., et al. 2018, Science, 362, aat3185
2018
-
[57]
Hue , V., Cavali \'e , T., Dobrijevic , M., Hersant , F., & Greathouse , T. K. 2015, , 257, 163
2015
-
[58]
K., Cavali \'e , T., Dobrijevic , M., & Hersant , F
Hue , V., Greathouse , T. K., Cavali \'e , T., Dobrijevic , M., & Hersant , F. 2016, , 267, 334
2016
-
[59]
Hue , V., Hersant , F., Cavali \'e , T., Dobrijevic , M., & Sinclair , J. A. 2018, , 307, 106
2018
-
[60]
E., Luhmann , J
Johnson , R. E., Luhmann , J. G., Tokar , R. L., et al. 2006, , 180, 393
2006
-
[61]
& Richardson , J
Jurac , S. & Richardson , J. D. 2007, , 34, L08102
2007
-
[62]
A., & Gr \"u n , E
Landgraf , M., Liou , J.-C., Zook , H. A., & Gr \"u n , E. 2002, , 123, 2857
2002
-
[63]
M., Lellouch , E., Gonz \'a lez , M., Moreno , R., & Rengel , M
Lara , L. M., Lellouch , E., Gonz \'a lez , M., Moreno , R., & Rengel , M. 2014, , 566, A143
2014
-
[64]
P., Fink , U., Treffers , R., & Gautier , III, T
Larson , H. P., Fink , U., Treffers , R., & Gautier , III, T. N. 1975, , 197, L137
1975
-
[65]
1995, , 373, 592
Lellouch , E., Paubert , G., Moreno , R., et al. 1995, , 373, 592
1995
-
[66]
I., et al
Lellouch , E., B \'e zard , B., Moses , J. I., et al. 2002, , 159, 112
2002
-
[67]
2005, , 430, L37
Lellouch , E., Moreno , R., & Paubert , G. 2005, , 430, L37
2005
-
[68]
F., et al
Lellouch , E., B \'e zard , B., Strobel , D. F., et al. 2006, , 184, 478
2006
-
[69]
2008, , 313, 175
Lellouch , E. 2008, , 313, 175
2008
-
[70]
2010, , 518, L152
Lellouch , E., Hartogh , P., Feuchtgruber , H., et al. 2010, , 518, L152
2010
-
[71]
1993, Journal of Molecular Spectroscopy, 157, 172
Levy , A., Lacome , N., & Tarrago , G. 1993, Journal of Molecular Spectroscopy, 157, 172
1993
-
[72]
1994, Journal of Molecular Spectroscopy, 166, 20
Levy , A., Lacome , N., & Tarrago , G. 1994, Journal of Molecular Spectroscopy, 166, 20
1994
-
[73]
F., Sweetnam , D
Lindal , G. F., Sweetnam , D. N., & Eshleman , V. R. 1985, , 90, 1136
1985
-
[74]
& Fegley , Jr., B
Lodders , K. & Fegley , Jr., B. 1994, , 112, 368
1994
-
[75]
Lomb , N. R. 1976, , 39, 447
1976
-
[76]
Luszcz-Cook , S. H. & de Pater , I. 2013, , 222, 379
2013
-
[77]
E., Mousis , O., Marty , B., et al
Mandt , K. E., Mousis , O., Marty , B., et al. 2015, , 197, 297
2015
-
[78]
1993, , 406, 285
Marten , A., Gautier , D., Owen , T., et al. 1993, , 406, 285
1993
-
[79]
E., Owen , T., et al
Marten , A., Matthews , H. E., Owen , T., et al. 2005, , 429, 1097
2005
-
[80]
G., Perry , M
Mitchell , D. G., Perry , M. E., Hamilton , D. C., et al. 2018, Science, 362, aat2236
2018
-
[81]
2010, Journal of Geophysical Research (Space Physics), 115, A11317
Moore , L., Mueller-Wodarg , I., Galand , M., Kliore , A., & Mendillo , M. 2010, Journal of Geophysical Research (Space Physics), 115, A11317
2010
-
[82]
E., & Biraud , Y
Moreno , R., Marten , A., Matthews , H. E., & Biraud , Y. 2003, , 51, 591
2003
-
[83]
M., et al
Moreno , R., Lellouch , E., Lara , L. M., et al. 2012, , 221, 753
2012
-
[84]
2015, , 245, 355
Moore , L., O'Donoghue , J., M \"u ller-Wodarg , I., Galand , M., & Mendillo , M. 2015, , 245, 355
2015
-
[85]
2017, , 608, L5
Moreno , R., Lellouch , E., Cavali \'e , T., & Moullet , A. 2017, , 608, L5
2017
-
[86]
I., Lellouch , E., B \'e zard , B., et al
Moses , J. I., Lellouch , E., B \'e zard , B., et al. 2000, , 145, 166
2000
-
[87]
I., Fouchet , T., B \'e zard , B., et al
Moses , J. I., Fouchet , T., B \'e zard , B., et al. 2005, Journal of Geophysical Research (Planets), 110, E08001
2005
-
[88]
Moses , J. I. & Poppe , A. R. 2017, , 297, 33
2017
-
[89]
N., Lebreton , J.-P., et al
Mousis , O., Fletcher , L. N., Lebreton , J.-P., et al. 2014, , 104, 29
2014
-
[90]
H., Spilker , T., et al
Mousis , O., Atkinson , D. H., Spilker , T., et al. 2016, , 130, 80
2016
-
[91]
H., Cavali \'e , T., et al
Mousis , O., Atkinson , D. H., Cavali \'e , T., et al. 2018, , 155, 12
2018
-
[92]
S., Knacke , R
Noll , K. S., Knacke , R. F., Geballe , T. R., & Tokunaga , A. T. 1986, , 309, L91
1986
-
[93]
N., et al
Norwood , J., Moses , J., Fletcher , L. N., et al. 2016, , 128, 018005
2016
-
[94]
O'Donoghue , J., Moore , L., Connerney , J. E. P., et al. 2017, , 44, 11
2017
-
[95]
L., Dobrij \'e vic , M., & Parisot , J
Ollivier , J. L., Dobrij \'e vic , M., & Parisot , J. P. 2000, , 48, 699
2000
-
[96]
S., Gustafsson , M., Burgdorf , M., & Meadows , V
Orton , G. S., Gustafsson , M., Burgdorf , M., & Meadows , V. 2007, , 189, 544
2007
-
[97]
S., Yanamandra-Fisher , P
Orton , G. S., Yanamandra-Fisher , P. A., Fisher , B. M., et al. 2008, , 453, 196
2008
-
[98]
2010, in , Vol
Ott , S. 2010, in , Vol. 434, Astronomical Data Analysis Software and Systems XIX, ed. Y. Mizumoto , K.-I. Morita , & M. Ohishi , 139
2010
-
[99]
& Encrenaz , T
Owen , T. & Encrenaz , T. 2003, , 106, 121
2003
-
[100]
E., Waite Jr., J
Perry, M. E., Waite Jr., J. H., Mitchell, D. G., et al. 2018, , 45, 10,093
2018
-
[101]
M., Poynter , R
Pickett , H. M., Poynter , R. L., Cohen , E. A., et al. 1998, , 60, 883
1998
-
[102]
L., Riedinger , J
Pilbratt , G. L., Riedinger , J. R., Passvogel , T., et al. 2010, , 518, L1
2010
-
[103]
2010, , 518, L2
Poglitsch , A., Waelkens , C., Geis , N., et al. 2010, , 518, L2
2010
-
[104]
Poppe , A. R. 2016, , 264, 369
2016
-
[105]
C., Helfenstein , P., Thomas , P
Porco , C. C., Helfenstein , P., Thomas , P. C., et al. 2006, Science, 311, 1393
2006
-
[106]
Prang \'e , R., Fouchet , T., Courtin , R., Connerney , J. E. P., & McConnell , J. C. 2006, , 180, 379
2006
-
[107]
2014, , 561, A4
Rengel , M., Sagawa , H., Hartogh , P., et al. 2014, , 561, A4
2014
-
[108]
2014, , 563, A4
Rezac , L., de Val-Borro , M., Hartogh , P., et al. 2014, , 563, A4
2014
-
[109]
R., Helmich , F
Roelfsema , P. R., Helmich , F. P., Teyssier , D., et al. 2012, , 537, A17
2012
-
[110]
E., Maguire , W
Samuelson , R. E., Maguire , W. C., Hanel , R. A., et al. 1983, , 88, 8709
1983
-
[111]
2011, , 475, 71
S \'a nchez-Lavega , A., del R \' o-Gaztelurrutia , T., Hueso , R., et al. 2011, , 475, 71
2011
-
[112]
A., Irwin , P
Sinclair , J. A., Irwin , P. G. J., Fletcher , L. N., et al. 2013, , 225, 257
2013
-
[113]
N., et al
Spilker , L., Ferrari , C., Cuzzi , J. N., et al. 2003, , 51, 929
2003
-
[114]
J., Pilorz , S
Spilker , L. J., Pilorz , S. H., Edgington , S. G., et al. 2005, Earth Moon and Planets, 96, 149
2005
-
[115]
Strobel , D. F. & Yung , Y. L. 1979, , 37, 256
1979
-
[116]
1999, , 142, 125
van der Tak , F., de Pater , I., Silva , A., & Millan , R. 1999, , 142, 125
1999
-
[117]
H., Combi , M
Waite , J. H., Combi , M. R., Ip , W.-H., et al. 2006, Science, 311, 1419
2006
-
[118]
H., Perryman , R
Waite , J. H., Perryman , R. S., Perry , M. E., et al. 2018, , 362, 51
2018
-
[119]
J., Lunine , J
Wang , D., Gierasch , P. J., Lunine , J. I., & Mousis , O. 2015, , 250, 154
2015
-
[120]
Weisstein , E. W. & Serabyn , E. 1996, , 123, 23
1996
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