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# The cosmic-ray ionisation rate in the pre-stellar core L1544

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### Abstract

Context. Cosmic rays (CRs) play an important role in the chemistry and dynamics of the interstellar medium. In dense environments, they represent the main ionising agent, driving the rich chemistry of molecular ions and determining the ionisation fraction, which regulates the degree of coupling between the gas and magnetic fields. Estimates of the CR ionisation rate ($$\zeta_2$$) span several orders of magnitude, depending on the targeted sources and on the used method. Aims. Recent theoretical models have characterised the CR attenuation with increasing density. We aim to test these models for the attenuation of CRs in the low-mass pre-stellar core L1544. Methods. We use a state-of-the-art gas-grain chemical model, which accepts the CR ionisation rate profile as input, to predict the abundance profiles of four ions: $$\rm N_2H^+$$, $$\rm N_2D^+$$, $$\rm HC^{18}O^+$$, and $$\rm DCO^+$$. Non-LTE radiative transfer is performed to produce synthetic spectra based on the derived abundances. These are compared with observations obtained with the Institut de Radioastronomie Millim\'etrique (IRAM) 30m telescope. Results. Our results indicate that a model with $$\zeta_2 > 10^{-16} \rm \, s^{-1}$$ is excluded by the observations. Also the model with the standard $$\zeta_2 = 1.3 \times 10^{-17} \rm \, s^{-1}$$ produces a worse agreement with respect to the attenuation model based on Voyager observations, which has an average $$\zeta_2 = 3 \times 10^{-17} \rm \, s^{-1}$$ at the column densities typical of L1544. The single-dish data, however, are not sensitive to the attenuation of the CR profile, which changes only by a factor of two in the range of column densities spanned by the core model. Interferometric observations at higher spatial resolution, combined with observations of transitions with lower critical density are needed to observe a decrease of $$\zeta_2$$ with density.

### Author and article information

###### Journal
16 September 2021
###### Article
2109.08169