REVIEW 4 major objections 5 minor 76 references
Multi-epoch spectro-photometric characterization of the minimoon 2024 PT$_5$ in the visible and near-infrared
T0 review · 4 major / 5 minor · reviewed 2026-08-06 · deepseek-v4-flash
Pith's one-line read The paper derives the first geometric albedo for the minimoon 2024 PT5 — 0.26±0.07 — and uses it to estimate an equivalent diameter of 7.4±1.0 m.
desk verdict First albedo for 2024 PT5, but the quoted uncertainty likely understates rotational-phase and calibration systematics. 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 V-band photometric phase curve of 2024 PT5, built from simultaneous $g$, $r$, $i$, and $z$ photometry on three nights together with $Y$, $J$, $H$, and $K$ photometry on two further nights. The curve is fitted with the standard $H$-$G$ phase function, giving $H_{V,HG}=27.72\pm0.09$ and $G_V=0.223\pm0.073$, and with a linear model giving the phase slope $b=0.029\pm0.002$ mag deg$^{-1}$. The albedo step is the named Belskaya-Shevchenko identity $b=C_1-C_2\log_{10}p_V$ with updated constants, which converts a shallow phase slope into a high geometric albedo. The tumbling claim is carried by periodogram searches showing no significant periodicity even though the lightcurves vary by roughly 0.3 mag on tens-of-minutes timescales, with the multicolor measurements taken simultaneously so that the color results are not biased by the changing brightness.
What would settle it
Measure the thermal infrared flux of 2024 PT5 with a mid-infrared facility and derive an independent geometric albedo from a standard thermal model; if the thermal albedo falls outside the $0.26\pm0.07$ range, or if a carefully measured phase curve of a known small S-complex asteroid breaks the slope-albedo calibration at this size, the central albedo and diameter estimates would be invalidated.
Extended reading notes
Core claim
On its own terms, the paper establishes that the minimoon 2024 PT5 has a geometric albedo of $0.26\pm0.07$, the first reported for this object. The claim is based on fitting the V-band phase curve, assembled from observations at phase angles $14.3$ to $26.8$ degrees, with both a linear model and the $H$-$G$ model; the fitted slope $b=0.029\pm0.002$ mag deg$^{-1}$ is converted to an albedo through the empirical Belskaya-Shevchenko relation $b=C_1-C_2\log_{10}p_V$. With the fitted absolute magnitude $H_{V,HG}=27.72\pm0.09$ and slope parameter $G_V=0.223\pm0.073$, this albedo yields an equivalent diameter of $7.4\pm1.0$ m. The paper further claims that 2024 PT5 is tumbling, because all of its lightcurves, including a more than two-hour arc on one night, show roughly 0.3 mag brightness variations over tens of minutes without a single detectable period in standard periodograms. The measured visible and near-infrared colors ($g-r=0.567\pm0.044$, $r-i=0.155\pm0.009$, $r-z=0.147\pm0.066$, $Y-J=0.557\pm0.046$, $J-H=0.672\pm0.078$, $H-K_s=0.148\pm0.098$) identify it as an S-complex asteroid, and its near-infrared reflectance is close to lunar rock samples, consistent with previous suggestions that 2024 PT5 is lunar ejecta.
Load-bearing premise
The albedo value rests on an empirical relation between phase-curve slope and geometric albedo that was calibrated on comparatively large asteroids, and the paper explicitly flags that this relation may not hold for a roughly 7 m, tumbling, possibly irregular object.
Editorial extensions
If this is right
- The first reported albedo of $0.26\pm0.07$ and diameter of $7.4\pm1.0$ m give concrete physical parameters for planning any spacecraft reconnaissance of 2024 PT5 or of minimoons with similar sizes.
- An S-complex classification with an albedo typical of S- and Q-type near-Earth asteroids strengthens the spectral link to lunar rock and to other lunar-like co-orbital asteroids, making a lunar-ejecta origin a quantitatively testable hypothesis.
- The inferred tumbling state, if real, is what a fragment produced by a lunar impact would be expected to show, and it warns that single-night color snapshots of minimoons can be biased by a changing visible hemisphere.
- Wide-phase-angle, multi-filter photometry from a medium-sized telescope appears sufficient to recover albedo, size, and rotation state for meter-scale near-Earth objects, a capability that will matter as surveys begin discovering minimoons more routinely.
Reading between the lines
- A direct test of the slope-albedo calibration would be to apply this same phase-curve method to a well-observed asteroid whose albedo is already known from thermal-infrared data; if the recovered value is systematically off at small sizes, the 2024 PT5 albedo could be a size-dependent bias rather than a true surface property.
- If the visible and near-infrared portions of the 2024 PT5 spectrum genuinely cannot be joined because the observed hemisphere changed between observing epochs, then the surface is heterogeneous on the 7 m scale; time-resolved multicolor photometry over a full tumbling cycle could map that heterogeneity and test the lunar-ejecta interpretation directly.
- The derived albedo is higher than the Moon's average value and closer to lunar highland material, so a lunar origin would point toward a bright highland source region; this is a testable prediction for future band-center and sample-matching analyses.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents new visible (Seimei/TriCCS, 2025 January 4/7/10) and near-infrared (Keck/MOSFIRE, January 16/17) photometry of the minimoon 2024 PT5. It derives Pan-STARRS g, r, i, z colors and 2MASS Y, J, H, Ks colors, reports roughly 0.3 mag brightness variations over tens of minutes, and finds no significant periodicity in the Lomb-Scargle analysis of the January 4 r-band lightcurve. The authors fit linear and H-G phase curves to three nightly averaged V magnitudes, obtaining H_V,linear = 28.06±0.05, b = 0.029±0.002 mag/deg, H_V,HG = 27.72±0.09, and G_V = 0.223±0.073. Using the linear phase slope with the Belskaya-Shevchenko albedo relation, they derive a geometric albedo of 0.26±0.07 and, with the absolute magnitude, an equivalent diameter of 7.4±1.0 m. They conclude that 2024 PT5 is an S-complex, tumbling object whose colors are compatible with lunar rock samples and with previous studies.
Significance. If the albedo and tumbling inferences hold, this is the first geometric albedo and a refined diameter for 2024 PT5, and the color/spectral comparison provides new constraints on the lunar-ejecta versus asteroid-origin debate for this rare minimoon. The photometric calibration is a clear strength: strict reference-star color cuts, simultaneous three-band imaging, in-field solar-like calibrators for the near-infrared, Monte Carlo uncertainty propagation, and an independent MPC phase-curve cross-check in Section 3.3. The authors also explicitly flag the uncertain applicability of the Belskaya-Shevchenko relation to a roughly 7 m body, which is the right scientific instinct. The principal new quantitative claims nevertheless rest on a three-point phase curve of a target whose rotational/tumbling phase is unconstrained, so the central numbers need a systematic-error treatment or a more cautious presentation before they can be taken at face value.
major comments (4)
- [§3.1, §3.3, Eq. (7), Eq. (12), Fig. 9] The geometric albedo pV = 0.26±0.07 is derived from the linear phase slope b = 0.029±0.002, fitted to only three nightly averaged V points spanning 14.3–26.8 deg. The target shows approximately 0.3 mag variations over tens of minutes, and the Lomb-Scargle analysis in Section 3.1 finds no unique periodicity, so the rotational/tumbling phase sampled by each nightly mean is unconstrained. A single-epoch offset of 0.1 mag, half the observed amplitude, changes the fitted slope by roughly 0.008 mag/deg over the 12.5 deg phase-angle lever arm; propagating that through Eq. (12) shifts pV from 0.26 to roughly 0.11–0.59, a range far larger than the quoted ±0.07. The Monte Carlo errors quoted in Section 3.3 include only the random errors of the nightly mean magnitudes, not this rotational-phase systematic. Please add a systematic-error term for rotational-phase sampling, or restrict the albedo and diameter claims to reflect this additional uncertainty.
- [§4.1, Fig. 6] The conclusion that 2024 PT5 is in a tumbling state goes beyond what the presented data show. The Lomb-Scargle periodogram in Fig. 6 shows no significant periodicity, and the text itself states that "the possibility that these variations are due to noise cannot be excluded." Aperiodic brightness variations could be produced by rotation with a non-sinusoidal or changing lightcurve, by albedo variegation, or by residual systematics, and do not uniquely imply tumbling. Because the later lunar-ejecta argument in Section 4.1 relies on the tumbling inference, the abstract's unqualified statement that "2024 PT5 is in a tumbling state" should be softened to "consistent with a tumbling state" or similar unless a tumbling model is explicitly fitted to the lightcurves.
- [§4.1, Eq. (12)] The albedo derivation depends entirely on the empirical Belskaya-Shevchenko relation calibrated with WISE/AKARI albedos of relatively large asteroids. The authors correctly identify this as a caveat for a roughly 7 m object, but the caveat is not reflected in the quoted uncertainty: ±0.07 in pV is purely the propagation of the statistical error in the phase slope. If the slope-albedo calibration does not transfer to very small, possibly tumbling and irregular bodies, the central albedo value and the diameter derived from it would be systematically wrong. Please state explicitly that the reported error bars exclude calibration systematics and recast the albedo as provisional pending independent validation by thermal-infrared or polarimetric measurements.
- [§3.2, Abstract, §5] There is a direct reporting inconsistency for the Y-J color. Section 3.2 derives Y-J = 0.557±0.046 but then states that this color is excluded from subsequent analysis because of MOSFIRE/Pan-STARRS Y-band filter systematics. Nevertheless, the abstract and Section 5 list Y-J = 0.557±0.046 among the headline color indices with no caveat. Please either remove Y-J from the abstract and conclusions or add the caveat there, and ensure that the reflectance construction in Section 4.2 is consistent with the stated exclusion.
minor comments (5)
- [§3.3, Fig. 9] The text reports fitting parameters from the Monte Carlo resampling, while the Fig. 9 caption describes medians of the fitted model curves; please clarify whether the quoted values are medians, best fits, or the peak of the posterior distribution.
- [§3.2] The color uncertainties are given as standard deviations of nightly mean colors, but for comparison with literature values the standard errors of the mean would be more appropriate; please state explicitly which quantity is plotted in Fig. 7 and used in Table 3.
- [§4.1 and Abstract] The sentence "The diameter of 2024 PT5 is estimated to be 7.4±1.0 using the albedo and absolute magnitude" is missing the unit 'm' in Section 4.1 and in the conclusion; please add it.
- [Fig. 8] The axis label in Fig. 8 uses "H-Ks" while the text and table consistently use "H-Ks" with a subscript; please standardize the notation.
- [§3.2] The phrase "The Y-J color of 2024 PT5 is estimated to be Y−J=0.557±0.046" appears before the statement that this color is excluded due to systematics; consider moving the derivation to a clearly labeled diagnostic section or adding a caution immediately after the first mention.
Circularity Check
No circularity: the albedo rests on an external phase-slope/albedo calibration, not on the target result.
full rationale
The central result, pV = 0.26±0.07, follows from the fitted phase-curve slope b = 0.029±0.002 mag/deg (Section 3.3) through the external Belskaya–Shevchenko relation b = C1 − C2 log10 pV (Eq. 12), with constants taken from Shevchenko et al. (2021). The target albedo is therefore an output of the analysis, not an input. H and G are fitted parameters reported as such, not disguised predictions, and the diameter 7.4±1.0 m is a standard propagation of H and pV through Eq. 13. The MPC phase-curve fit in Section 3.3 is an independent consistency test using 404 external observations. The paper explicitly flags the main limitation, that Eq. 12 is calibrated on larger asteroids and may not transfer to a ~7 m body, which is a validity caveat about the external calibration, not circularity. Self-citations (Bolin et al. 2025a for prior spectrophotometry, Bolin et al. 2025b for the 2024 YR4 comparison, and Beniyama et al. for photometric methodology) serve as comparison datasets or method references and are not load-bearing for the albedo claim. The tumbling inference is drawn from observed ~0.3 mag variability and the absence of a unique period, not from the definition of tumbling. The inclusion of Y−J in the abstract despite its exclusion in Section 3.2 is a reporting inconsistency, not a circular step. No equation in the paper is equivalent to its own input by construction.
Assumptions & free parameters
free parameters (5)
- Phase curve slope b (linear model) =
0.029 ± 0.002 mag deg^-1
- Absolute magnitude H_V,HG =
27.72 ± 0.09
- Slope parameter G_V =
0.223 ± 0.073
- Geometric albedo p_V =
0.26 ± 0.07
- Lightcurve amplitude m(alpha) =
0.3 mag
assumptions (6)
- domain assumption The H-G phase function model (Bowell et al. 1989) adequately describes the photometric phase curve of 2024 PT5 over the observed phase-angle range.
- domain assumption The empirical Belskaya-Shevchenko relation between phase-curve slope and geometric albedo applies to small minimoons.
- domain assumption The photometric transformations of Tonry et al. (2012) between Pan-STARRS and SDSS systems (Eqs. 2-5) and to Johnson V (Eq. 6) are valid.
- domain assumption The asteroid is a triaxial ellipsoid with an aspect angle of 90 degrees for the axial ratio estimate.
- ad hoc to paper The observed brightness variations are due to rotational or tumbling motion rather than noise or systematic effects.
- domain assumption Solar colors from Willmer (2018) are accurate for computing reflectance spectra.
Cite this review
Pith. "Pith review of Multi-epoch spectro-photometric characterization of the minimoon 2024 PT$_5$ in the visible and near-infrared." pith.science (2026). https://pith.science/paper/4PYF4SLD
@misc{pith2026250710527,
author = {Pith},
title = {Pith review of: Multi-epoch spectro-photometric characterization of the minimoon 2024 PT$_5$ in the visible and near-infrared},
year = {2026},
howpublished = {\url{https://pith.science/paper/4PYF4SLD}},
note = {Machine review of arXiv:2507.10527}
}
abstract
2024 PT$_5$ is a tiny ($D\leq10$ m) near-Earth asteroid (NEA) discovered in August 2024. 2024 PT$_5$ was gravitationally bound to the Earth-Moon system from September to November 2024 and classified as a minimoon. Several quick response observations suggest the lunar ejecta origin of 2024 PT$_5$, while rotation state and albedo, essential properties to investigate its origin, are not well constrained. We performed visible to near-infrared multicolor photometry of 2024 PT$_5$ from data taken using the TriColor CMOS Camera and Spectrograph (TriCCS) on the Seimei 3.8 m telescope during 2025 January 4-10. The Seimei/TriCCS observations of 2024 PT$_5$ cover phase angles from 14 deg to 27 deg, and were obtained in the $g$, $r$, $i$, and $z$ bands in the Pan-STARRS system. In addition, we analyzed $Y$, $J$, $H$, and $K$ photometry taken with the Multi-Object Spectrograph for Infrared Exploration (MOSFIRE) on the Keck I 10-m telescope taken on 2025 January 16-17. Our lightcurves show brightness variations over time periods of several tens of minutes. We infer that 2024 PT$_5$ is in a tumbling state and has a lightcurve amplitude of about 0.3 mag. Visible and near-infrared color indices of 2024 PT$_5$, $g-r=0.567\pm0.044$, $r-i=0.155\pm0.009$, $r-z=0.147\pm0.066$, $Y-J=0.557\pm0.046$, $J-H=0.672\pm0.078$, and $H-Ks=0.148\pm0.098$, indicate that 2024 PT$_5$ is an S-complex asteroid, largely consistent with previous observations. Using the $H$-$G$ model, we derived an absolute magnitude $H_{V,HG}$ of $27.72\pm0.09$ and a slope parameter $G_V$ of $0.223\pm0.073$ in V-band. A geometric albedo of 2024 PT$_5$ is derived to be $0.26\pm0.07$ from the slope of its photometric phase curve. This albedo value is typical of the S- and Q-type NEAs. The color properties of 2024 PT$_5$ derived from our observations match rock samples taken from the lunar surface, which agrees with previous studies.
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Works this paper leans on
-
[1]
Ballouz, R. L., Agrusa, H., Barnouin, O. S., et al. 2024, PSJ, 5, 251
work page 2024
-
[2]
Belskaya, I. N. & Shevchenko, V . G. 2000, Icarus, 147, 94
work page 2000
-
[3]
Beniyama, J., Sergeyev, A. V ., Tholen, D. J., & Micheli, M. 2024, A&A, 690, A180
work page 2024
-
[4]
Benson, C. J., Scheeres, D. J., & Moskovitz, N. A. 2020, Icarus, 340, 113518
work page 2020
-
[5]
P., Morbidelli, A., Merouane, S., et al
Binzel, R. P., Morbidelli, A., Merouane, S., et al. 2010, Nature, 463, 331
work page 2010
-
[6]
Bolin, B., Jedicke, R., Granvik, M., et al. 2014, Icarus, 241, 280
work page 2014
-
[7]
T., Ahumada, T., van Dokkum, P., et al
Bolin, B. T., Ahumada, T., van Dokkum, P., et al. 2022, MNRAS, 517, L49
work page 2022
-
[8]
Bolin, B. T., Fernandez, Y . R., Lisse, C. M., et al. 2021, AJ, 161, 116
work page 2021
Show all 76 references
-
[9]
T., Fremling, C., Holt, T
Bolin, B. T., Fremling, C., Holt, T. R., et al. 2020, ApJ, 900, L45
2020
-
[10]
1989, in Asteroids II, ed
Bowell, E., Hapke, B., Domingue, D., et al. 1989, in Asteroids II, ed. R. P. Binzel, T. Gehrels, & M. S. Matthews (Tucson, AZ: Univ. Arizona Press), 524–556
1989
-
[11]
2024, A&A, 687, A38
Carry, B., Peloton, J., Le Montagner, R., Mahlke, M., & Berthier, J. 2024, A&A, 687, A38
2024
-
[12]
C., Magnier, E
Chambers, K. C., Magnier, E. A., Metcalfe, N., et al. 2016, arXiv:1612.05560, arXiv:1612.05560
2016 arXiv
-
[13]
Chapman, C. R. & Morrison, D. 1976, Icarus, 28, 91
1976
-
[14]
T., Ernst, C
Daly, R. T., Ernst, C. M., Barnouin, O. S., et al. 2023, Nature, 616, 443 de la Fuente Marcos, C. & de la Fuente Marcos, R. 2018, MNRAS, 473, 2939 de la Fuente Marcos, C. & de la Fuente Marcos, R. 2020, MNRAS, 494, 1089 de la Fuente Marcos, R., de León, J., de la Fuente Marcos...
2023
-
[15]
E., Binzel, R
DeMeo, F. E., Binzel, R. P., Slivan, S. M., & Bus, S. J. 2009, Icarus, 202, 160
2009
-
[16]
2024, Minor Planet Electronic Circulars, 2024-P170
Denneau, L., Robinson, J., Fitzsimmons, A., et al. 2024, Minor Planet Electronic Circulars, 2024-P170
2024
-
[17]
2017, Icarus, 285, 83
Fedorets, G., Granvik, M., & Jedicke, R. 2017, Icarus, 285, 83
2017
-
[18]
Fowler, J. W. & Chillemi, J. R. 1992, Phillips Lab. Tech. Rep., 2049, 17
1992
-
[19]
M., Brasseur, C
Ginsburg, A., Sip˝ocz, B. M., Brasseur, C. E., et al. 2019, AJ, 157, 98
2019
-
[20]
J., Burns, J
Gladman, B. J., Burns, J. A., Duncan, M. J., & Levison, H. F. 1995, Icarus, 118, 302
1995
-
[21]
Glass, I. S. 1999, Handbook of Infrared Astronomy
1999
-
[22]
2013, in Aster- oids: Prospective Energy and Material Resources, ed
Granvik, M., Jedicke, R., Bolin, B., Chyba, M., & Patterson, G. 2013, in Aster- oids: Prospective Energy and Material Resources, ed. V . Badescu, 151–167
2013
-
[23]
2012, Icarus, 218, 262
Granvik, M., Vaubaillon, J., & Jedicke, R. 2012, Icarus, 218, 262
2012
-
[24]
Harris, A. W. 1994, Icarus, 107, 209
1994
-
[25]
K., Cruikshank, D
Hartmann, W. K., Cruikshank, D. P., & Degewij, J. 1982, Icarus, 52, 377
1982
-
[26]
H., Della Corte, V ., Pravec, P., et al
Hasselmann, P. H., Della Corte, V ., Pravec, P., et al. 2024, PSJ, 5, 91
2024
-
[27]
2021, Advances in Space Re- search, 68, 1533
Hirabayashi, M., Mimasu, Y ., Sakatani, N., et al. 2021, Advances in Space Re- search, 68, 1533
2021
-
[28]
J., Pieters, C
Isaacson, P. J., Pieters, C. M., Besse, S., et al. 2011, Journal of Geophysical Research (Planets), 116, E00G11
2011
-
[29]
2003, PASJ, 55, 691
Ishiguro, M., Abe, M., Ohba, Y ., et al. 2003, PASJ, 55, 691
2003
-
[30]
2014, ApJ, 792, 74 Ivezi´c, Ž., Kahn, S
Ishiguro, M., Kuroda, D., Hasegawa, S., et al. 2014, ApJ, 792, 74 Ivezi´c, Ž., Kahn, S. M., Tyson, J. A., et al. 2019, ApJ, 873, 111
2014
-
[31]
L., Rozitis, B., Dover, L
Jackson, S. L., Rozitis, B., Dover, L. R., et al. 2022, MNRAS, 513, 3076
2022
-
[32]
M., Wiedner, N., et al
Jedicke, R., Alessi, E. M., Wiedner, N., et al. 2025, arXiv e-prints, arXiv:2504.17985
2025 arXiv
-
[33]
T., Bottke, W
Jedicke, R., Bolin, B. T., Bottke, W. F., et al. 2018, Frontiers in Astronomy and Space Sciences, 5, 13
2018
-
[34]
2024, Nature Astronomy, 8, 819
Jiao, Y ., Cheng, B., Huang, Y ., et al. 2024, Nature Astronomy, 8, 819
2024
-
[35]
Kareta, T., Fuentes-Muñoz, O., Moskovitz, N., Farnocchia, D., & Sharkey, B. N. L. 2025, ApJ, 979, L8
2025
-
[36]
Kary, D. M. & Dones, L. 1996, Icarus, 121, 207
1996
-
[37]
V ., Velikodsky, Y
Korokhin, V . V ., Velikodsky, Y . I., Shkuratov, Y . G., & Mall, U. 2007, Solar System Research, 41, 19
2007
-
[38]
2020, PASJ, 72, 48
Kurita, M., Kino, M., Iwamuro, F., et al. 2020, PASJ, 72, 48
2020
-
[39]
& Kryszczynska, A
Kwiatkowski, T. & Kryszczynska, A. 1992, in Liege International Astrophys- ical Colloquia, V ol. 30, Liege International Astrophysical Colloquia, ed. A. Brahic, J. C. Gerard, & J. Surdej, 353
1992
-
[40]
2009, A&A, 495, 967
Kwiatkowski, T., Kryszczy´nska, A., Poli´nska, M., et al. 2009, A&A, 495, 967
2009
-
[41]
W., Mierle, K., Blanton, M., & Roweis, S
Lang, D., Hogg, D. W., Mierle, K., Blanton, M., & Roweis, S. 2010, AJ, 139, 1782
2010
-
[42]
Lomb, N. R. 1976, Ap&SS, 39, 447
1976
-
[43]
Mahlke, M., Carry, B., & Mattei, P. A. 2022, A&A, 665, A26
2022
-
[44]
E., Burt, B., et al
Marsset, M., DeMeo, F. E., Burt, B., et al. 2022, AJ, 163, 165
2022
-
[45]
2018, Astropy/Astroscrappy: V1.0.5 Zenodo Release, Zenodo
McCully, C., Crawford, S., Kovacs, G., et al. 2018, Astropy/Astroscrappy: V1.0.5 Zenodo Release, Zenodo
2018
-
[46]
E., Thomas, C
McGraw, L. E., Thomas, C. A., Lister, T. A., et al. 2024, ApJ, 977, L25
2024
-
[47]
S., Steidel, C
McLean, I. S., Steidel, C. C., Epps, H. W., et al. 2012, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, V ol. 8446, Ground- based and Airborne Instrumentation for Astronomy IV , ed. I. S. McLean, S. K. Ramsay, & H. Takami, 84460J
2012
-
[48]
C., et al
Michel, P., Küppers, M., Bagatin, A. C., et al. 2022, PSJ, 3, 160
2022
-
[49]
2019, The Journal of Open Source Software, 4, 1426 Article number, page 11 of 12 A&A proofs:manuscript no
Mommert, M., Kelley, M., de Val-Borro, M., et al. 2019, The Journal of Open Source Software, 4, 1426 Article number, page 11 of 12 A&A proofs:manuscript no. main_clean 0.4 0.5 0.6 0.7 0.8 0.9 1.0 Wavelength [ m] 0.70 0.80 0.90 1.00 1.10 1.20 1.30 1.40 Normalized reflectance 20...
2019
-
[50]
A., Benson, C
Moskovitz, N. A., Benson, C. J., Scheeres, D., et al. 2020, Icarus, 340, 113519
2020
-
[51]
P., Micheli, M., Farnocchia, D., et al
Naidu, S. P., Micheli, M., Farnocchia, D., et al. 2021, ApJ, 913, L6
2021
-
[52]
Pieters, C. M. 1983, J. Geophys. Res., 88, 9534
1983
-
[53]
Popescu, M., Birlan, M., & Nedelcu, D. A. 2012, A&A, 544, A130
2012
-
[54]
M., et al
Popescu, M., Licandro, J., Carvano, J. M., et al. 2018, A&A, 617, A12
2018
-
[55]
2016, A&A, 591, A115
Popescu, M., Licandro, J., Morate, D., et al. 2016, A&A, 591, A115
2016
-
[56]
& Harris, A
Pravec, P. & Harris, A. W. 2007, Icarus, 190, 250
2007
-
[57]
L., Sanchez, J
Reddy, V ., Gary, B. L., Sanchez, J. A., et al. 2015, ApJ, 811, 65
2015
-
[58]
S., Farnocchia, D., et al
Reddy, V ., Kelley, M. S., Farnocchia, D., et al. 2019, Icarus, 326, 133
2019
-
[59]
S., Chabot, N
Rivkin, A. S., Chabot, N. L., Stickle, A. M., et al. 2021, PSJ, 2, 173
2021
-
[60]
Scargle, J. D. 1982, ApJ, 263, 835
1982
-
[61]
E., Jones, R
Schwamb, M. E., Jones, R. L., Yoachim, P., et al. 2023, ApJS, 266, 22
2023
-
[62]
R., et al
Selmi, E., Devogèle, M., Masiero, J. R., et al. 2025, PSJ, 6, 26
2025
-
[63]
Sergeyev, A. V . & Carry, B. 2021, A&A, 652, A59
2021
-
[64]
Sharkey, B. N. L., Reddy, V ., Malhotra, R., et al. 2021, Communications Earth and Environment, 2, 231
2021
-
[65]
G., Belskaya, I
Shevchenko, V . G., Belskaya, I. N., Slyusarev, I. G., et al. 2012, Icarus, 217, 202
2012
-
[66]
G., Mikhalchenko, O
Shevchenko, V . G., Mikhalchenko, O. I., Belskaya, I. N., et al. 2021, Planet. Space Sci., 202, 105248
2021
-
[67]
F., Cutri, R
Skrutskie, M. F., Cutri, R. M., Stiening, R., et al. 2006, AJ, 131, 1163
2006
-
[68]
2014, PASJ, 66, 53
Takahashi, J., Urakawa, S., Terai, T., et al. 2014, PASJ, 66, 53
2014
-
[69]
L., Stubbs, C
Tonry, J. L., Stubbs, C. W., Lykke, K. R., et al. 2012, ApJ, 750, 99
2012
-
[70]
2019, AJ, 157, 155 van Dokkum, P
Urakawa, S., Ohsawa, R., Sako, S., et al. 2019, AJ, 157, 155 van Dokkum, P. G. 2001, PASP, 113, 1420
2019
-
[71]
VanderPlas, J. T. 2018, ApJS, 236, 16
2018
-
[72]
2004, Icarus, 167, 271
Warell, J. 2004, Icarus, 167, 271
2004
-
[73]
D., Harris, A
Warner, B. D., Harris, A. W., & Pravec, P. 2009, Icarus, 202, 134
2009
-
[74]
Willmer, C. N. A. 2018, ApJS, 236, 47
2018
-
[75]
M., Fulchignoni, M., & Lupishko, D
Zappala, V ., Cellino, A., Barucci, A. M., Fulchignoni, M., & Lupishko, D. F. 1990, A&A, 231, 548
1990
-
[76]
2021, Nature Astronomy, 5, 730 Article number, page 12 of 12
Zhang, T., Xu, K., & Ding, X. 2021, Nature Astronomy, 5, 730 Article number, page 12 of 12
2021
Reviewed August 6, 2026 · model on record in the stance chip above.
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