# Thermal physics of the inner coma: ALMA studies of the methanol   distribution and excitation in comet C/2012 K1 (PanSTARRS)

**Authors:** M. A. Cordiner, N. Biver, J. Crovisier, D. Bockelee-Morvan, M. J., Mumma, S. B. Charnley, G. Villanueva, L. Paganini, D. C. Lis, S. N. Milam, A., J. Remijan, I. M. Coulson, Y.-J. Kuan, J. Boissier

arXiv: 1701.08258 · 2017-03-22

## TL;DR

This study uses ALMA observations to analyze the spatial distribution and excitation of methanol in comet C/2012 K1, revealing temperature variations and cooling processes in the inner coma with implications for cometary physics.

## Contribution

First detailed ALMA-based analysis of methanol excitation and temperature distribution in a comet's inner coma, highlighting the importance of radiative cooling and additional heating sources.

## Key findings

- Temperature drops from 60 K to 20 K within 2500 km on June 28
- Temperature drops from 120 K to 40 K within 1000 km on June 29
- Radiative cooling dominates over collisional cooling in the coma

## Abstract

We present spatially and spectrally-resolved observations of CH$_3$OH emission from comet C/2012 K1 (PanSTARRS) using The Atacama Large Millimeter/submillimeter Array (ALMA) on 2014 June 28-29. Two-dimensional maps of the line-of-sight average rotational temperature ($T_{rot}$) were derived, covering spatial scales $0.3''-1.8''$ (corresponding to sky-projected distances $\rho\sim500$-2500 km). The CH$_3$OH column density distributions are consistent with isotropic, uniform outflow from the nucleus, with no evidence for extended sources of CH$_3$OH in the coma. The $T_{rot}(\rho)$ radial profiles show a significant drop within a few thousand kilometers of the nucleus, falling from about 60 K to 20 K between $\rho=0$ and 2500 km on June 28, whereas on June 29, $T_{rot}$ fell from about 120 K to 40 K between $\rho=$ 0 km and 1000 km. The observed $T_{rot}$ behavior is interpreted primarily as a result of variations in the coma kinetic temperature due to adiabatic cooling of the outflowing gas, as well as radiative cooling of the CH$_3$OH rotational levels. Our excitation model shows that radiative cooling is more important for the $J=7-6$ transitions (at 338 GHz) than for the $K=3-2$ transitions (at 252 GHz), resulting in a strongly sub-thermal distribution of levels in the $J=7-6$ band at $\rho\gtrsim1000$ km. For both bands, the observed temperature drop with distance is less steep than predicted by standard coma theoretical models, which suggests the presence of a significant source of heating in addition to the photolytic heat sources usually considered.

## Full text

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## Figures

25 figures with captions in the complete paper: https://tomesphere.com/paper/1701.08258/full.md

## References

36 references — full list in the complete paper: https://tomesphere.com/paper/1701.08258/full.md

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Source: https://tomesphere.com/paper/1701.08258