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PreprintCC BY-NC-SA 4.0arXiv

The size and mass distribution of cold classical TNOs for 5<H<13

Abstract

The cold classical trans-Neptunian objects (CCs) are the only observable \textit{in situ} population of planetesimal remnants believed to have escaped collisional grinding. Recent JWST observations make it possible to fit the differential absolute magnitude distribution dN/dH of the CCs from 5<Hr<13, and infer the differential mass distribution dN/dM across ≥5 orders of magnitude in mass. We find dN/dM well fit by a lognormal distribution, and equally well by a generalized Γ distribution or a double power law. The maximum fraction of the total CC mass per log interval in M is in bodies near 75~km diameter, or ≈10−7.5M⊕. Extrapolation of the fitted dN/dH functions to Hr>13 is unwise, as the different analytic forms diverge. It remains unclear if dN/dH turns over at faint H. The uncertainty in the total mass of the CC belt is dominated by uncertainty in the relation between M and H. A calibration using CC binaries suggests a total CC mass of 1.7--2.7×10−3 M⊕. A trend toward lower density and/or higher albedo for smaller bodies may be present in the data, and would lower the estimated total CC mass. Qualitative comparison of the derived mass distribution to the results of numerical simulations of the streaming instability (SI) suggest the simulations produce dN/dM distributions that are more sharply peaked, and steeper at the bright end, than the CCs. Such differences could be ascribed to inhomogeneous formation conditions in the classical belt that are not yet included in modeling. The variety and uncertainty of dN/dM derived from state-of-the-art SI simulations currently preclude any definitive test of the SI hypothesis.

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BibTeX
@misc{bernstein2026size,
  title = {{The size and mass distribution of cold classical TNOs for $5<H<13$}},
  author = {Gary M. Bernstein and Wesley C. Fraser and Marielle R. Eduardo and William M. Grundy and Bryan Hilbert and Matthew J. Holman and Anastasia N. Morgan and Kevin J. Napier and John A. Stansberry and David E. Trilling},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.09063},
  eprint = {2609.09063},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.09063},
  note = {CC BY-NC-SA 4.0},
}
RIS
TY  - UNPB
TI  - The size and mass distribution of cold classical TNOs for 5<H<13
AU  - Gary M. Bernstein
AU  - Wesley C. Fraser
AU  - Marielle R. Eduardo
AU  - William M. Grundy
AU  - Bryan Hilbert
AU  - Matthew J. Holman
AU  - Anastasia N. Morgan
AU  - Kevin J. Napier
AU  - John A. Stansberry
AU  - David E. Trilling
PY  - 2026
DA  - 2026/09/08
PB  - arXiv
DO  - 10.48550/arxiv.2609.09063
UR  - https://arxiv.org/abs/2609.09063
AB  - The cold classical trans-Neptunian objects (CCs) are the only observable \textit{in situ} population of planetesimal remnants believed to have escaped collisional grinding. Recent JWST observations make it possible to fit the differential absolute magnitude distribution dN/dH of the CCs from 5<H_r<13, and infer the differential mass distribution dN/dM across ≥5 orders of magnitude in mass. We find dN/dM well fit by a lognormal distribution, and equally well by a generalized Γ distribution or a double power law. The maximum fraction of the total CC mass per log interval in M is in bodies near 75~km diameter, or ≈10^−7.5M_⊕. Extrapolation of the fitted dN/dH functions to H_r>13 is unwise, as the different analytic forms diverge. It remains unclear if dN/dH turns over at faint H. The uncertainty in the total mass of the CC belt is dominated by uncertainty in the relation between M and H. A calibration using CC binaries suggests a total CC mass of 1.7--2.7×10^−3 M_⊕. A trend toward lower density and/or higher albedo for smaller bodies may be present in the data, and would lower the estimated total CC mass. Qualitative comparison of the derived mass distribution to the results of numerical simulations of the streaming instability (SI) suggest the simulations produce dN/dM distributions that are more sharply peaked, and steeper at the bright end, than the CCs. Such differences could be ascribed to inhomogeneous formation conditions in the classical belt that are not yet included in modeling. The variety and uncertainty of dN/dM derived from state-of-the-art SI simulations currently preclude any definitive test of the SI hypothesis.
ER  -