2024ApJ...973..142O


Query : 2024ApJ...973..142O

2024ApJ...973..142O - Astrophys. J., 973, 142 (2024/October-1)

Reevaluation of the Cosmic-Ray Ionization Rate in Diffuse Clouds.

OBOLENTSEVA M., IVLEV A.V., SILSBEE K., NEUFELD D.A., CASELLI P., EDENHOFER G., INDRIOLO N., BISBAS T.G. and LOMELI D.

Abstract (from CDS):

All current estimates of the cosmic-ray (CR) ionization rate rely on assessments of the gas density along the probed sight lines. Until now, these have been based on observations of different tracers, with C2 being the most widely used in diffuse molecular clouds for this purpose. However, dust extinction maps have recently reached sufficient accuracy to give an independent measurement of the gas density on parsec scales. In addition, they allow us to identify the gas clumps along each sight line, thus localizing the regions where CR ionization is probed. We reevaluate ${{\rm{H}}}_{3}^{+}$ observations, which are often considered as the most reliable method to measure the H2 ionization rate ${\zeta }_{{{\rm{H}}}_{2}}$ in diffuse clouds. The peak density values derived from the extinction maps for 12 analyzed sight lines turn out to be, on average, an order of magnitude lower than the previous estimates and agree with the values obtained from revised analysis of C2 data. We use the extinction maps in combination with the 3D-PDR code to self-consistently compute the ${{\rm{H}}}_{3}^{+}$ and H2 abundances in the identified clumps for different values of ${\zeta }_{{{\rm{H}}}_{2}}$. For each sight line, we obtain the optimum value by comparing the simulation results with observations. We show that ${\zeta }_{{{\rm{H}}}_{2}}$ is systematically reduced with respect to the earlier estimates by a factor of ≈9 on average, to ≈6 × 10–17 s–1, primarily as a result of the density reduction. We emphasize that these results have profound consequences for all available measurements of the ionization rate.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Diffuse molecular clouds - Galactic cosmic rays

Simbad objects: 19

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Number of rows : 19
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 21856 Pu* 03 32 40.0150232424 +35 27 42.207495156 4.96 5.807 5.900     B1V 192 0
2 * o Per * 03 42 22.6459308614 +33 57 54.093701142 4.13 4.912 4.972     B0.5V 315 0
3 * omi Per SB* 03 44 19.1337687984 +32 17 17.687367960 3.13 3.91 3.91 3.71 3.71 B1III 628 0
4 * zet Per s*b 03 54 07.9224751 +31 53 01.081262 2.19 2.97 2.85 2.71 2.62 B1Ib 881 0
5 V* X Per HXB 03 55 23.0777456088 +31 02 45.039836148 6.090 6.840 6.720     O9.5III 1037 0
6 * 62 Tau * 04 23 59.7627483096 +24 18 03.527065188 6.18 6.499 6.337     B3V 237 0
7 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 4971 0
8 LDN 1544 DNe 05 04 16.6 +25 10 48           ~ 965 0
9 * chi02 Ori s*b 06 03 55.1843706432 +20 08 18.428141364 4.24 4.91 4.63 4.32 4.10 B2Ia 465 0
10 HD 73882 ** 08 39 09.53412 -40 25 09.2608 7.07 7.59 7.19 6.67 6.30 O8.5IV 261 1
11 HD 110432 HXB 12 42 50.2663572384 -63 03 31.052981412 4.79 5.58 5.31     B0.5IVpe 334 0
12 * chi Oph Be* 16 27 01.4355697915 -18 27 22.499961252 3.95 4.71 4.43 3.97 3.73 B2Vne 624 0
13 HD 149404 s*b 16 36 22.5628499784 -42 51 31.902127776 5.23 5.88 5.52 6.90   O8.5Iab(f)p 265 0
14 * zet Oph Be* 16 37 09.5400587698 -10 34 01.509742704 1.73 2.58 2.56 2.46 2.50 O9.2IVnn 1908 0
15 HD 154368 s*b 17 06 28.3687759224 -35 27 03.760593156 6.10 6.63 6.13 7.12   O9.5Iab 316 0
16 * lam Sco bC* 17 33 36.52012 -37 06 13.7648 0.52 1.49 1.63     B2IV+DA7.9 404 0
17 * lam Cep s*b 22 11 30.5765111040 +59 24 52.154264880 4.55 5.29 5.05 4.77 4.62 O6.5I(n)fp 705 1
18 NAME Local Bubble ISM ~ ~           ~ 1059 0
19 NAME Per-Tau reg ~ ~           ~ 54 0

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