A new analytic approach to infer the cosmic-ray ionization rate in hot molecular cores from HCO+, N2H+, and CO observations

被引:0
作者
Luo, Gan [1 ]
Bisbas, Thomas G. [2 ]
Padovani, Marco [3 ]
Gaches, Brandt A. L. [4 ]
机构
[1] Inst Radioastron Millimetr, 300 Rue Piscine, F-38400 St Martin Dheres, France
[2] Zhejiang Lab, Res Ctr Intelligent Comp Platform, Hangzhou 311100, Peoples R China
[3] INAF Osservatorio Astrofis Arcetri, Largo E Fermi 5, I-50125 Florence, Italy
[4] Chalmers Univ Technol, Dept Space Earth & Environm, SE-41296 Gothenburg, Sweden
关键词
astrochemistry; stars: formation; ISM: abundances; ISM: clouds; cosmic rays; ISM: molecules; DENSE INTERSTELLAR GAS; STAR-FORMING REGIONS; CHEMICAL EVOLUTION; NONTHERMAL EMISSION; EARLY PHASES; MILKY-WAY; ABUNDANCE; CLOUDS; OXYGEN; DUST;
D O I
10.1051/0004-6361/202450285
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Context. The cosmic-ray ionization rate (zeta(2)) is one of the key parameters in star formation, since it regulates the chemical and dynamical evolution of molecular clouds by ionizing molecules and determining the coupling between the magnetic field and gas. Aims. However, measurements of zeta(2) in dense clouds (e.g., n(H) >= 10(4) cm(-3)) are difficult and sensitive to the model assumptions. The aim is to find a convenient analytic approach that can be used in high-mass star-forming regions (HMSFRs), especially for warm gas environments such as hot molecular cores (HMCs). Methods. We propose a new analytic approach to calculate zeta(2) through HCO+, N2H+, and CO measurements. By comparing our method with various astrochemical models and with observations found in the literature, we identify the parameter space for which the analytic approach is applicable. Results. Our method gives a good approximation, to within 50%, of zeta(2) in dense and warm gas (e.g., n(H) >= 10(4) cm(-3), T = 50, 100 K) for A(V) >= 4 mag and t >= 2 x 10(4) yr at Solar metallicity. The analytic approach gives better results for higher densities. However, it starts to underestimate zeta(2) at low metallicity (Z = 0.1 Z(circle dot)) when the value is too high (zeta(2) >= 3 x 10(-15) s(-1)). By applying our method to the OMC-2 FIR4 envelope and the L1157-B1 shock region, we find zeta(2) values of (1.0 +/- 0.3) x 10(-14) s(-1) and (2.2 +/- 0.4) x 10(-16) s(-1), consistent with those previously reported. Conclusions. We calculate zeta(2) toward a total of 82 samples in HMSFRs, finding that the average value of zeta(2) toward all HMC samples (zeta(2) = (7.4 +/- 5.0)x10(-16) s(-1)) is more than an order of magnitude higher than the theoretical prediction of cosmic-ray attenuation models, favoring the scenario that locally accelerated cosmic rays in embedded protostars should be responsible for the observed high zeta(2).
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页数:13
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