REVIEW 3 major objections 5 minor 89 references
Excess Ultraviolet Emission at High Galactic Latitudes: A New Horizons View
T0 review · 3 major / 5 minor · reviewed 2026-08-10 · deepseek-v4-flash
Pith's one-line read New Horizons measurements from 57 AU give the first firm measurement of the cosmic ultraviolet background in the 912–1100 Å band and find that roughly half of the high-latitude UV background is unidentified.
desk verdict The 1500 Å result is solid; the 1000 Å 'first detection' needs an LSF systematics estimate before I'd trust the quoted uncertainty. 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 carrier of the argument is the data-processing sequence that turns Alice raw counts into a clean background spectrum, built around two foreground subtractions. Dark counts from the spacecraft's radioisotope thermoelectric generator are measured with door-closed exposures interleaved with the sky exposures. The dominant contaminant, scattering of the intense interplanetary Lyman-alpha line across the detector, is removed with a template formed by differencing Alice observations of the same sky region made in 2007 at about 8 AU and in 2023 at about 57 AU, scaled by the Lyman-alpha line counts; the solar Lyman-alpha signal fell by a factor of 3.5 over that interval, so the difference isolates the scattering function. Because aperture-filling diffuse calibration is difficult, the 1400–1700 Å Alice band is cross-calibrated against GALEX diffuse observations, and a single scale factor is applied to the whole Alice spectrum. The residual after these subtractions, plotted against the mean Planck $E(B-V)$ in each aperture, yields the linear fits and zero-reddening offsets.
What would settle it
To test the first-detection claim, one could observe a hot white dwarf or B star with a model-atmosphere spectrum through Alice's short-wavelength (KBr) and long-wavelength (CsI) channels and compare the 912–1100 Å count rate with the model prediction; if the single GALEX-derived scale factor is wrong for the short-wavelength channel by more than the quoted errors, the $221 \pm 11$ photon units offset at 1000 Å would shift and the firm detection would be called into question.
Extended reading notes
Core claim
The paper's central claim is that the cosmic ultraviolet background at high Galactic latitudes has a substantial component not explained by any known source, and that this component can now be measured in the previously inaccessible 912–1100 Å band. From 25 fields observed with the Alice spectrograph at 57 AU, after subtracting dark counts and a scattering template for interplanetary Lyman-$\alpha$, the CUVB surface brightness is linear in the Planck $E(B-V)$: at 1000 Å the best fit is $2994 \pm 446$ photon units per magnitude of $E(B-V)$ plus an offset of $221 \pm 11$ photon units; at 1500 Å it is $6723 \pm 909$ photon units per magnitude plus $264 \pm 24$ photon units, where photon units are photons cm$^{-2}$ s$^{-1}$ sr$^{-1}$ Å$^{-1}$. The 1000 Å offset is the first firm measurement of the zero-reddening offset between 912 and 1100 Å; the only earlier measurement, from the Voyager ultraviolet spectrometers, was an upper limit near 200 photon units. Adding the integrated light of unresolved galaxies, faint stars, O VI and C IV line emission, and two-photon emission accounts for roughly half the offsets, leaving $133 \pm 17$ photon units at 1000 Å and $103 \pm 31$ photon units at 1500 Å with no identified source. In the 600–800 Å band the measured surface brightness is $3.2 \pm 3.0$ photon units, so no background is detected below the Lyman limit.
Load-bearing premise
The load-bearing assumption is that a single scale factor, derived from a 1400–1700 Å comparison with GALEX, applies unchanged across the entire Alice spectrum, including the 912–1100 Å band that uses a different detector coating.
Editorial extensions
If this is right
- The 912–1100 Å zero-reddening offset becomes a measured number, $221 \pm 11$ photon units, rather than an upper limit, so models of the extragalactic UV background must now reproduce it.
- After accounting for galaxies, stars, line emission, and two-photon emission, an excess of $133 \pm 17$ photon units at 1000 Å and $103 \pm 31$ photon units at 1500 Å remains, indicating an unidentified isotropic component of the high-latitude UV sky.
- The null detection below the Lyman limit, $3.2 \pm 3.0$ photon units in the 600–800 Å band, constrains the metagalactic ionizing background and implies that the local EUV field seen by earlier missions is dominated by a few nearby stars.
- Because the 1400–1800 Å Alice and GALEX offsets agree to $-23 \pm 24$ photon units, the paper concludes that 1300–1800 Å background measurements are feasible from low Earth orbit, whereas the 912–1100 Å band requires an outer-solar-system vantage point where Lyman-alpha scattering is weak.
Reading between the lines
- A natural next test, not performed in the paper, is to replace the single GALEX-derived scale factor with a wavelength-dependent calibration anchored to stellar model atmospheres; if the 1000 Å offset moves by more than its stated error, the first-detection claim would rest on a calibration artifact.
- If the residual excess is a real astrophysical component, cross-correlating the 1000 Å residual map with galaxy redshift surveys, X-ray maps, and far-infrared dust maps would show whether it is Galactic halo emission or genuinely extragalactic; the paper already cites a clustering analysis that argues against an extragalactic origin for a comparable 1500 Å monopole.
- The combination of a substantial 912–1100 Å offset with a null below 912 Å implies that the unknown emitter produces photons just longward of the Lyman limit but not ionizing photons; warm partially ionized gas or a decaying-particle source would make concrete predictions that future short-wavelength UV observations could test.
- If a future deep-space platform observes the same 912–1100 Å window with an independently calibrated spectrograph, the comparison would be a clean check of whether the 221 photon units offset is a property of the sky or of Alice's calibration.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper presents new observations of the cosmic ultraviolet background (CUVB) with the Alice spectrograph on New Horizons at ~57 AU from the Sun, targeting high-latitude fields with |b| > 40°. The authors subtract detector dark counts (measured with the door closed and interleaved with sky exposures) and a Lyα scattering template built by differencing 2007 and 2023 blank-sky observations. They then correlate Alice surface brightness in two bands (912–1100 Å and 1400–1700 Å) with Planck E(B−V), finding zero-reddening offsets of 221 ± 11 photon units at 1000 Å and 264 ± 24 photon units at 1500 Å. The former is claimed as the first firm detection of the offset in the 912–1100 Å range. Comparing with known contributors (unresolved galaxies, stars, O VI/C IV line emission, two-photon emission) leaves an unexplained excess of about 133 and 103 photon units in the two bands. An upper limit of 3.2 ± 3.0 photon units is reported for 600–800 Å emission below the Lyman limit.
Significance. If correct, this is a landmark measurement: it would be the first firm detection of the diffuse ultraviolet background in the 912–1100 Å band from outside the solar system, and the agreement with earlier GALEX-based offsets at 1500 Å would validate the method. The paper is careful in its dark subtraction, uses interleaved dark exposures, constructs a Lyα template from the 2007–2023 orbital baseline, and makes electronic data available. The high-latitude, outer-solar-system vantage point removes geocoronal and zodiacal foregrounds that have plagued earlier measurements. These strengths make the paper valuable regardless of the final verdict. However, the central first-detection claim depends on two assumptions that need explicit support: that the Box spectrum in the 912–1100 Å band is not dominated by red-wing leakage from longer wavelengths, and that a single GALEX-based scale factor, calibrated at 1400–1700 Å, applies across the entire Alice spectrum including the KBr-coated short-wavelength region.
major comments (3)
- [§4.4 / §2.1] The first-firm-detection claim at 912–1100 Å is not yet supported because the analysis does not address the spectral purity of the Box measurement. The Box has a FWHM of 172 Å (§2.1), nearly the full 188 Å width of the claimed band, and §4.4 states that the detector region was integrated down to 850 Å to capture the short-wavelength signal. Without a line-spread-function deconvolution or an explicit leakage estimate, the 912–1100 Å band will include red-wing counts from the 1100–1350 Å region (blanked in Fig. 15) and potentially from 1400–1800 Å, where the measured offset is 264 ± 24 photon units. The paper itself cautions that the decrease in offsets from 1100 to 912 Å 'may be an artifact of the Box line width.' The quoted 221 ± 11 photon units includes only the statistical errors from the fit and template subtraction, not an LSF modeling error. The Stem measurement in the same band, 172 ± 48 photon units, is far less precise and cannot by itself establish a firm detection. Please quantify the red-wing contribution using the measured LSF and the observed spectrum at λ > 1100 Å, or deconvolve the spectrum; unless this is done, the first-detection claim is not load-bearing.
- [§4.2] The absolute calibration of the 912–1100 Å band rests on an assumption that is stated but not validated. Section 4.2 derives a single scale factor from the correlation between Alice 1400–1700 Å counts and GALEX FUV background, and then 'rescaled the Alice spectra by these factors, assuming that a single scale factor applies over the entire Alice spectrum.' The Alice detector has a split coating of KBr (520–1180 Å) and CsI (1250–1870 Å) (§2.1). If the relative sensitivity of the two coatings has drifted since ground calibration, or if the diffuse-source calibration differs between the two coatings, the 1000 Å offset of 221 ± 11 photon units would shift by an amount not captured by the quoted uncertainty. Please provide evidence that the short-wavelength response tracks the 1400–1700 Å response, for example from stellar observations at 912–1100 Å or from a stability analysis of the KBr/CsI boundary region, or propagate a conservative systematic uncertainty into the 1000 Å offset.
- [§4.3] The reported EUV limit of 3.2 ± 3.0 photon units at 600–800 Å is presented as an absolute surface brightness, but it is converted using the same GALEX-derived calibration that is only established for 1400–1700 Å. The text does not describe any calibration check for the 520–912 Å KBr-coated region, which is the part of the detector most likely to have a different sensitivity history. Either provide a validation for the short-wavelength calibration or present the EUV result as an upper limit in count-space rather than in photon units, with the calibration uncertainty included.
minor comments (5)
- [§4.2] Please clarify the direction of the rescaling: the fit gives Alice = 0.71 × GALEX for the Box, so the correction factor to apply to Alice spectra should be 1/0.71, yet the text says 'rescaled the Alice spectra by these factors' without specifying whether 'factors' means the slope or its inverse.
- [§3.3 / Fig. 8] The caption of Fig. 8 writes the subtracted component as D2023 + T × L2007, while Eq. (3) defines CUVB = (S − D) − L ∗ T; please reconcile the notation for the template scaling so that L and T are not confused with each other.
- [Table 7] The 912–1100 Å STEM row reports a slope of 2214 ± 1694 photon units mag−1, a relative uncertainty of ~76%; please state explicitly that the Stem is too noisy to constrain the slope and that all quantitative conclusions rely on the Box.
- [§4.4] The text says the offsets are 'close to flat between 1400 – 1800 ˚A at a level of about 290 photon units,' but Table 7 quotes 264 ± 24 photon units for 1400–1700 Å; please specify whether the 290 value refers to a different wavelength range or a different estimate.
- [§3.3.1] The error propagation description adds dark, sky, and template errors in quadrature, but it does not state how the template normalization uncertainty (the scaling by the Lyα line ratio L2007/L2023) is incorporated into the template error; please add one sentence describing the scaling uncertainty.
Circularity Check
Main 912–1100 Å derivation is not circular, but the 1500 Å 'confirmation' and the 'near-zero atmospheric offset' restate the GALEX cross-calibration fit rather than independent measurements.
-
fitted input called prediction
[Section 4.2 (GALEX cross-calibration) and Section 6 (Summary)]
"We have, therefore, rescaled the Alice spectra by these factors, assuming that a single scale factor applies over the entire Alice spectrum. There is evidence for a small offset (≈ 23 photon units at 1 σ) between GALEX and Alice, perhaps due to two-photon emission arising in the Earth’s atmosphere (Kulkarni 2022). ... Importantly, we have found that there is, at most, an offset of −23 ± 24 photon units between the Alice observations and GALEX data at 1500 Å."
The Alice 1400–1700 Å data are cross-calibrated by a least-squares fit to GALEX diffuse data (slope 0.71, intercept −23.2 for the Box). After rescaling, the reported 'offset between Alice and GALEX at 1500 Å' is exactly the fitted intercept of that calibration fit, not an independently measured quantity. The 1500 Å zero-reddening offset of 264 ± 24 photon units is likewise a deterministic transform of the GALEX offset that was used to set the Alice scale. Therefore the abstract's statement that 'the latter result confirms previous results from GALEX' overstates the independence: it is a re-derivation of the calibration input. The 912–1100 Å offset is not circular because no GALEX data exist at those wavelengths, but it inherits the single-scale-factor assumption.
full rationale
The central new claim—the 912–1100 Å zero-reddening offset of 221 ± 11 photon units—is derived from Alice sky counts after dark subtraction and Lyα-template removal, regressed against external Planck E(B−V) values. That offset is not fitted to the claimed excess; it is the intercept of an independent linear regression against an external reddening map, and the excess over known sources is computed by subtracting external literature estimates (galaxy counts, stellar models, O VI/C IV, two-photon emission). This portion of the derivation chain is self-contained and not circular. The one circular element is at 1400–1800 Å: the Alice data are calibrated using GALEX diffuse maps, and then the same comparison is reported as a 'finding' of near-zero atmospheric contribution and as a 'confirmation' of GALEX offsets. That is a fitted calibration parameter presented as a measurement, warranting a small deduction (score 2). Self-citations of earlier CUVB measurements (Akshaya et al., Henry et al., Murthy et al.) are present, but they are used for context and comparison, not as load-bearing justification for the new 1000 Å detection. The paper explicitly flags a spectral-resolution caveat: the Box line width is 172 Å, and the authors caution that the apparent decline from 1100 to 912 Å 'may be an artifact of the Box line width.' That is a measurement limitation, not circularity, but it should temper the 'first firm detection' headline. Overall, no significant circularity in the primary derivation chain; the 912–1100 Å result is an extrapolated measurement with unverified cross-coating calibration, not a conclusion forced by the inputs.
Assumptions & free parameters
free parameters (2)
- Box GALEX scale factor =
0.71 ± 0.05
- Stem GALEX scale factor =
0.82 ± 0.14
assumptions (3)
- domain assumption The CUVB surface brightness in the template field was identical in 2007 and 2023, so that (S2007-D2007)-(S2023-D2023) isolates the solar Ly-alpha scattering.
- domain assumption A single Alice-to-GALEX calibration scale factor applies over the entire Alice spectrum, including 912-1100 Å where no direct cross-calibration exists.
- domain assumption At high Galactic latitudes, the dust-scattered ultraviolet intensity is linearly proportional to E(B-V) with no additional color dependence over the sampled range.
Cite this review
Pith. "Pith review of Excess Ultraviolet Emission at High Galactic Latitudes: A New Horizons View." pith.science (2026). https://pith.science/paper/NM6DXB6K
@misc{pith2026250100787,
author = {Pith},
title = {Pith review of: Excess Ultraviolet Emission at High Galactic Latitudes: A New Horizons View},
year = {2026},
howpublished = {\url{https://pith.science/paper/NM6DXB6K}},
note = {Machine review of arXiv:2501.00787}
}
abstract
We present new observations of the cosmic ultraviolet background (CUVB) at high Galactic latitudes ($|b| > 40^{\circ}$), made using the Alice UV spectrograph on board the New Horizons spacecraft. These observations were taken at about 57 AU from the Sun, outside much of the foreground emission affecting previous missions, and allowed a new determination of the spectrum of the CUVB between 912 -- 1100~\AA\ and 1400 -- 1800~\AA. We found a linear correlation between the CUVB and the Planck E(B~-~V) with offsets at zero-reddening of $221 \pm 11$ photon units at 1000~\AA\ and $264 \pm 24$ \photu\ at 1500~\AA\ ($4.4 \pm 0.2$ nW m$^{-2}$ sr$^{-1}$ at 1000~\AA\ and $5.3 \pm 0.5$ nW m$^{-2}$ sr$^{-1}$ at 1500~\AA). The former is the first firm detection of the offset in the range 912 -- 1100 \AA\ while the latter result confirms previous results from \galex, showing that there is little emission from the Solar System from 1400 -- 1800 \AA. About half of the offset may be explained by known sources (the integrated light of unresolved galaxies, unresolved stars, emission from ionized gas, and two-photon emission from warm hydrogen in the halo) with the source of the remaining emission as yet unidentified. There is no detectable emission below the Lyman limit with an upper limit of $3.2 \pm 3.0$ photon units.
Figures
Figures from the paper (11 more)
Reference graph
Works this paper leans on
-
[1]
S., Murthy, J., Ravichandran, S., Henry, R
Akshaya, M. S., Murthy, J., Ravichandran, S., Henry, R. C., & Overduin, J. 2018, ApJ, 858, 101, doi: 10.3847/1538-4357/aabcb9 —. 2019, MNRAS, 489, 1120, doi: 10.1093/mnras/stz2186
-
[2]
Anderson, R. C., Henry, R. C., Brune, W. H., Feldman, P. D., & Fastie, W. G. 1979, ApJ, 234, 415, doi: 10.1086/157510
doi:10.1086/157510 1979
-
[3]
Barcons, X., & Fabian, A. C. 1992, The X-Ray Background (Cambridge University Press)
1992
-
[4]
L., Halpern, M., Hinshaw, G., et al
Bennett, C. L., Halpern, M., Hinshaw, G., et al. 2003, ApJS, 148, 1, doi: 10.1086/377253
doi:10.1086/377253 2003
-
[5]
2018, Ap&SS, 363, 56, doi: 10.1007/s10509-018-3277-2
Bianchi, L., de la Vega, A., Shiao, B., & Bohlin, R. 2018, Ap&SS, 363, 56, doi: 10.1007/s10509-018-3277-2
-
[6]
1991, ARA&A, 29, 59, doi: 10.1146/annurev.aa.29.090191.000423
Bowyer, S. 1991, ARA&A, 29, 59, doi: 10.1146/annurev.aa.29.090191.000423
arXiv 1991
-
[7]
Carleton, T., Windhorst, R. A., O’Brien, R., et al. 2022, The Astronomical Journal, 164, 170, doi: 10.3847/1538-3881/ac8d02
-
[8]
F., Weaver, H
Cheng, A. F., Weaver, H. A., Conard, S. J., et al. 2008, SSRv, 140, 189
2008
Show all 89 references
-
[9]
2019, ApJ, 877, 150, doi: 10.3847/1538-4357/ab1b35
Chiang, Y.-K., M´ enard, B., & Schiminovich, D. 2019, ApJ, 877, 150, doi: 10.3847/1538-4357/ab1b35
2019 doi
-
[10]
2010, in Astronomical Society of the Pacific Conference Series, Vol
Coulais, A., Schellens, M., Gales, J., et al. 2010, in Astronomical Society of the Pacific Conference Series, Vol. 434, Astronomical Data Analysis Software and Systems XIX, ed. Y. Mizumoto, K.-I. Morita, & M. Ohishi, 187
2010
-
[11]
2011, arXiv preprint arXiv:1101.0679
Coulais, A., Schellens, M., Gales, J., et al. 2011, arXiv preprint arXiv:1101.0679
2011 arXiv
-
[12]
Cravens, T. E. 2000, ApJL, 532, L153, doi: 10.1086/312574
2000 doi
-
[13]
H., Peebles, P
Dicke, R. H., Peebles, P. J. E., Roll, P. J., & Wilkinson, D. T. 1965, ApJ, 142, 414
1965
-
[14]
Dixon, W. V. D., Sallmen, S., Hurwitz, M., & Lieu, R. 2001, ApJL, 552, L69, doi: 10.1086/320265
2001 doi
-
[15]
P., Andrews, S
Driver, S. P., Andrews, S. K., Davies, L. J., et al. 2016, ApJ, 827, 108, doi: 10.3847/0004-637X/827/2/108
2016 doi
-
[16]
1995, ApJ, 455, 574
Thejll, P. 1995, ApJ, 455, 574
1995
-
[17]
D., Brune, W
Feldman, P. D., Brune, W. H., & Henry, R. C. 1981, ApJL, 249, L51, doi: 10.1086/183657
1981 doi
-
[18]
C., Redfield, S., & Slavin, J
Frisch, P. C., Redfield, S., & Slavin, J. D. 2011, ARA&A, 49, 237
2011
-
[19]
R., et al
Galeazzi, M., Chiao, M., Collier, M. R., et al. 2014, Nature, 512, 171, doi: 10.1038/nature13525
2014 doi
-
[20]
P., Brown, T
Gardner, J. P., Brown, T. M., & Ferguson, H. C. 2000, ApJL, 542, L79, doi: 10.1086/312930
2000 doi
-
[21]
R., & Rossi, B
Giacconi, R., Gursky, H., Paolini, F. R., & Rossi, B. B. 1962, PhRvL, 9, 439, doi: 10.1103/PhysRevLett.9.439
1962 doi
-
[22]
Gillmon, K., & Shull, J. M. 2006, ApJ, 636, 908, doi: 10.1086/498055
2006 doi
-
[23]
M., Brasseur, C
Ginsburg, A., Sip˝ ocz, B. M., Brasseur, C. E., et al. 2019, AJ, 157, 98, doi: 10.3847/1538-3881/aafc33
2019 doi
-
[24]
Girardi, L., Groenewegen, M. A. T., Hatziminaoglou, E., & da Costa, L. 2005, A&A, 436, 895, doi: 10.1051/0004-6361:20042352 18
2005 doi
-
[25]
R., Pryor, W
Gladstone, G. R., Pryor, W. R., Stern, S. A., et al. 2018, Geophys. Res. Lett., 45, 8022, doi: 10.1029/2018GL078808
2018 doi
-
[26]
T., Schiminovich, D., & Seibert, M
Hamden, E. T., Schiminovich, D., & Seibert, M. 2013, ApJ, 779, 180, doi: 10.1088/0004-637X/779/2/180
2013 doi
-
[27]
1969, Ap&SS, 5, 493, doi: 10.1007/BF00652397
Hayakawa, S., Yamashita, K., & Yoshioka, S. 1969, Ap&SS, 5, 493, doi: 10.1007/BF00652397
1969 doi
-
[28]
Henry, R. C. 1991, ARA&A, 29, 89, doi: 10.1146/annurev.aa.29.090191.000513
1991
-
[29]
C., Feldman, P
Henry, R. C., Feldman, P. D., Fastie, W. G., & Weinstein, A. 1978, ApJ, 223, 437, doi: 10.1086/156278
1978 doi
- [30]
-
[31]
C., Murthy, J., Overduin, J., & Tyler, J
Henry, R. C., Murthy, J., Overduin, J., & Tyler, J. 2015, ApJ, 798, 14, doi: 10.1088/0004-637X/798/1/14
2015 doi
-
[32]
C., Swandic, J
Henry, R. C., Swandic, J. R., Shulman, S. D., & Fritz, G. 1977, ApJ, 212, 707, doi: 10.1086/155095
1977 doi
-
[33]
Holberg, J. B. 1986, ApJ, 311, 969, doi: 10.1086/164834
1986 doi
-
[34]
1984, A&A, 139, 481
Jakobsen, P., Bowyer, S., Kimble, R., et al. 1984, A&A, 139, 481
1984
-
[35]
2017, The Astrophysical Journal Supplement Series, 231, 21, doi: 10.3847/1538-4365/aa8091
Jo, Y.-S., Seon, K.-I., Min, K.-W., Edelstein, J., & Han, W. 2017, The Astrophysical Journal Supplement Series, 231, 21, doi: 10.3847/1538-4365/aa8091
2017 doi
-
[36]
2019, ApJS, 243, 9, doi: 10.3847/1538-4365/ab22ae
Jo, Y.-S., Seon, K.-i., Min, K.-W., et al. 2019, ApJS, 243, 9, doi: 10.3847/1538-4365/ab22ae
2019 doi
-
[37]
M., Cruvellier, P., Masnou, J
Joubert, M., Deharveng, J. M., Cruvellier, P., Masnou, J. L., & Lequeux, J. 1983, A&A, 128, 114
1983
- [38]
-
[39]
A., Weinberg, D
Kollmeier, J. A., Weinberg, D. H., Oppenheimer, B. D., et al. 2014, ApJ, 789, L32
2014
-
[40]
M., Kim, M
Korngut, P. M., Kim, M. G., Arai, T., et al. 2022, The Astrophysical Journal, 926, 133, doi: 10.3847/1538-4357/ac44ff
2022 doi
-
[41]
P., Bellstedt, S., et al
Koushan, S., Driver, S. P., Bellstedt, S., et al. 2021, MNRAS, 503, 2033, doi: 10.1093/mnras/stab540
2021 doi
-
[42]
Kulkarni, S, R., & Shull, J. M. 2023, PASP, 135, 124301
2023
-
[43]
Kulkarni, S. R. 2022, PASP, 134, 084302, doi: 10.1088/1538-3873/ac689e
2022 doi
-
[44]
2004, A&A, 422, 391, doi: 10.1051/0004-6361:20035625
Lallement, R. 2004, A&A, 422, 391, doi: 10.1051/0004-6361:20035625
2004 doi
-
[45]
L., Crifo, F., & Sfeir, D
Lallement, R., Welsh, B., Vergely, J. L., Crifo, F., & Sfeir, D. 2003, A&A, 411, 447
2003
-
[46]
R., Postman, M., Weaver, H
Lauer, T. R., Postman, M., Weaver, H. A., et al. 2021, ApJ, 906, 77, doi: 10.3847/1538-4357/abc881
2021 doi
-
[47]
R., Postman, M., Spencer, J
Lauer, T. R., Postman, M., Spencer, J. R., et al. 2022, ApJL, 927, L8, doi: 10.3847/2041-8213/ac573d
2022 doi
- [48]
-
[49]
1990, ApJ, 350, 242, doi: 10.1086/168376
Martin, C., & Bowyer, S. 1990, ApJ, 350, 242, doi: 10.1086/168376
1990 doi
-
[50]
1990, ApJ, 354, 220, doi: 10.1086/168681
Martin, C., Hurwitz, M., & Bowyer, S. 1990, ApJ, 354, 220, doi: 10.1086/168681
1990 doi
-
[51]
2011, The Astrophysical Journal, 737, 2, doi: 10.1088/0004-637x/737/1/2
Matsuura, S., Shirahata, M., Kawada, M., et al. 2011, The Astrophysical Journal, 737, 2, doi: 10.1088/0004-637x/737/1/2
2011 doi
-
[52]
2019, Contemporary Physics, 60, 23, doi: 10.1080/00107514.2019.1586130
Mattila, K., & V¨ ais¨ anen, P. 2019, Contemporary Physics, 60, 23, doi: 10.1080/00107514.2019.1586130
2019
-
[53]
2017, Monthly Notices of the Royal Astronomical Society, 470, 2152, doi: 10.1093/mnras/stx1296 Miville-Deschˆ enes, M.-A., & Lagache, G
Mattila, K., V¨ ais¨ anen, P., Lehtinen, K., von Appen-Schnur, G., & Leinert, C. 2017, Monthly Notices of the Royal Astronomical Society, 470, 2152, doi: 10.1093/mnras/stx1296 Miville-Deschˆ enes, M.-A., & Lagache, G. 2005, ApJS, 157, 302, doi: 10.1086/427938
2017 doi
-
[54]
2009, Ap&SS, 320, 21, doi: 10.1007/s10509-008-9855-y —
Murthy, J. 2009, Ap&SS, 320, 21, doi: 10.1007/s10509-008-9855-y —. 2014, ApJS, 213, 32, doi: 10.1088/0067-0049/213/2/32 —. 2016, MNRAS, 459, 1710, doi: 10.1093/mnras/stw755
2009 doi
-
[55]
Murthy, J., Conn Henry, R., & Holberg, J. B. 2012, ApJS, 199, 11, doi: 10.1088/0067-0049/199/1/11
2012 doi
-
[56]
C., & Holberg, J
Murthy, J., Hall, D., Earl, M., Henry, R. C., & Holberg, J. B. 1999, ApJ, 522, 904, doi: 10.1086/307652
1999 doi
-
[57]
C., & Sujatha, N
Murthy, J., Henry, R. C., & Sujatha, N. V. 2010, ApJ, 724, 1389, doi: 10.1088/0004-637X/724/2/1389
2010 doi
-
[58]
Murthy, J., & Sahnow, D. J. 2004, ApJ, 615, 315, doi: 10.1086/424441
2004 doi
-
[59]
1991, ApJ, 379, 532, doi: 10.1086/170526
Onaka, T., & Kodaira, K. 1991, ApJ, 379, 532, doi: 10.1086/170526
1991 doi
-
[60]
F., & Bowyer, S
Paresce, F., McKee, C. F., & Bowyer, S. 1980, ApJ, 240, 387, doi: 10.1086/158244
1980 doi
-
[61]
2022, Journal of Open Source Software, 7, 4633, doi: 10.21105/joss.04633
Park, J., Duvert, G., Coulais, A., et al. 2022, Journal of Open Source Software, 7, 4633, doi: 10.21105/joss.04633
2022 doi
-
[62]
Peebles, P. J. E. 2020, Principles of Physical Cosmology (Princeton University Press)
2020
-
[63]
2010, A&A, 524, A42, doi: 10.1051/0004-6361/201015362
Stobie, E. 2010, A&A, 524, A42, doi: 10.1051/0004-6361/201015362
2010 doi
-
[64]
A., & Wilson, R
Penzias, A. A., & Wilson, R. W. 1965, ApJ, 142, 419, doi: 10.1086/148307 Planck Collaboration, Abergel, A., Ade, P. A. R., et al. 2014, A&A, 571, A11, doi: 10.1051/0004-6361/201323195 Planck Collaboration, Ade, P. A. R., Aghanim, N., et al. 2016, A&A, 586, A132, doi: 10.1051/0...
1965 doi
- [65]
-
[66]
Reynolds, R. J. 1992, ApJL, 392, L35, doi: 10.1086/186419 19
1992 doi
-
[67]
G., et al
Saldana-Lopez, A., Dom ´ ınguez, A., P´ erez-Gonz´ alez, P. G., et al. 2021, MNRAS, 507, 5144, doi: 10.1093/mnras/stab2393
2021 doi
-
[68]
G., Martin, C., & Morrissey, P
Schiminovich, D., Friedman, P. G., Martin, C., & Morrissey, P. F. 2001, ApJL, 563, L161, doi: 10.1086/338656
2001 doi
-
[69]
J., Finkbeiner, D
Schlegel, D. J., Finkbeiner, D. P., & Davis, M. 1998, ApJ, 500, 525, doi: 10.1086/305772
1998 doi
-
[70]
Sciama, D. W. 1990, ApJ, 364, 549
1990
-
[71]
L., Kruk, J
Shelton, R. L., Kruk, J. W., Murphy, E. M., et al. 2001, ApJ, 560, 730, doi: 10.1086/322478
2001 doi
-
[72]
Fardal, M. A. 1999, AJ, 118, 1450
1999
-
[73]
L., Cox, D
Snowden, C. L., Cox, D. P., McCammon, D., & Sanders, W. T. 1990, ApJ, 354, 211
1990
-
[74]
N., Verde, L., Peiris, H
Spergel, D. N., Verde, L., Peiris, H. V., et al. 2003, ApJS, 148, 175
2003
-
[75]
Stern, S. A. 2008, SSRv, 140, 3, doi: 10.1007/s11214-007-9295-y
2008 doi
-
[76]
A., Becker, T
Stern, S. A., Becker, T. M., Parker, J. W., et al. 2025, New Horizons Alice Kuiper Belt Extended Mission 2 Raw Data Collection, URN:nasa:pds:nh alice:kem2 raw::1.0, NASA Planetary Data System, doi: 10.26007/03vn-5336
2025 doi
-
[77]
A., Slater, D
Stern, S. A., Slater, D. C., Scherrer, J., et al. 2008, SSRv, 140, 155, doi: 10.1007/s11214-008-9407-3
2008 doi
-
[78]
A., Bagenal, F., Ennico, K., et al
Stern, S. A., Bagenal, F., Ennico, K., et al. 2015, Science, 350, doi: 10.1126/science.aad1815
2015 doi
-
[79]
A., Weaver, H
Stern, S. A., Weaver, H. A., Spencer, J. R., et al. 2019, Science, 364, eaaw9771, doi: 10.1126/science.aaw9771
2019 doi
-
[80]
Symons, T., Zemcov, M., Cooray, A., Lisse, C., & Poppe, A. R. 2023, ApJ, 945, 45, doi: 10.3847/1538-4357/acaa37
2023 doi
-
[81]
D., Henry, R
Tennyson, P. D., Henry, R. C., Feldman, P. D., & Hartig, G. F. 1988, ApJ, 330, 435, doi: 10.1086/166481
1988 doi
-
[82]
Vallerga, J. V. 1998, ApJ, 497, 921
1998
-
[83]
A., Cheng, A
Weaver, H. A., Cheng, A. F., Morgan, F., et al. 2020, PASP, 132, 035003, doi: 10.1088/1538-3873/ab67ec
2020 doi
-
[84]
2000, A&AS, 143, 9, doi: 10.1051/aas:2000332
Wenger, M., Ochsenbein, F., Egret, D., et al. 2000, A&AS, 143, 9, doi: 10.1051/aas:2000332
2000 doi
-
[85]
N., Friedmann, B
Witt, A. N., Friedmann, B. C., & Sasseen, T. P. 1997, ApJ, 481, 809
1997
-
[86]
N., & Petersohn, J
Witt, A. N., & Petersohn, J. K. 1994, in Astronomical Society of the Pacific Conference Series, Vol. 58, The First Symposium on the Infrared Cirrus and Diffuse Interstellar Clouds, ed. R. M. Cutri & W. B. Latter, 91
1994
-
[87]
K., Donas, J., Arnouts, S., et al
Xu, C. K., Donas, J., Arnouts, S., et al. 2005, ApJL, 619, L11, doi: 10.1086/425252
2005 doi
-
[88]
2017, Nature Communications, 8, 15003, doi: 10.1038/ncomms15003
Zemcov, M., Immel, P., Nguyen, C., et al. 2017, Nature Communications, 8, 15003, doi: 10.1038/ncomms15003
2017 doi
-
[89]
2018, PASP, 130, 115001, doi: 10.1088/1538-3873/aadb77
Zemcov, M., Arcavi, I., Arendt, R., et al. 2018, PASP, 130, 115001, doi: 10.1088/1538-3873/aadb77
2018 doi
Reviewed August 10, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.