Neural Network Constraints on the Cosmic-Ray Ionization Rate and Other Physical Conditions in NGC 253 with ALCHEMI Measurements of HCN and HNC
We use a neural network model and ALMA observations of HCN and HNC to constrain the physical conditions, most notably the cosmic-ray ionization rate (CRIR, zeta), in the Central Molecular Zone (CMZ) of the starburst galaxy NGC 253. Using output from the chemical code UCLCHEM, we train a neural netwo...
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Zusammenfassung: | We use a neural network model and ALMA observations of HCN and HNC to
constrain the physical conditions, most notably the cosmic-ray ionization rate
(CRIR, zeta), in the Central Molecular Zone (CMZ) of the starburst galaxy NGC
253. Using output from the chemical code UCLCHEM, we train a neural network
model to emulate UCLCHEM and derive HCN and HNC molecular abundances from a
given set of physical conditions. We combine the neural network with radiative
transfer modeling to generate modeled integrated intensities, which we compare
to measurements of HCN and HNC from the ALMA Large Program ALCHEMI. Using a
Bayesian nested sampling framework, we constrain the CRIR, molecular gas volume
and column densities, kinetic temperature, and beam-filling factor across NGC
253's CMZ. The neural network model successfully recovers UCLCHEM molecular
abundances with about 3 percent error and, when used with our Bayesian
inference algorithm, increases the parameter inference speed tenfold. We create
images of these physical parameters across NGC 253's CMZ at 50 pc resolution
and find that the CRIR, in addition to the other gas parameters, is spatially
variable with zeta a few times 10^{14} s^{-1} at greater than 100 pc from the
nucleus, increasing to zeta greater than 10^{-13} s^{-1} at its center. These
inferred CRIRs are consistent within 1 dex with theoretical predictions based
on non-thermal emission. Additionally, the high CRIRs estimated in NGC 253's
CMZ can be explained by the large number of cosmic-ray-producing sources as
well as a potential suppression of cosmic-ray diffusion near their injection
sites. |
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DOI: | 10.48550/arxiv.2409.13821 |