JWST Observations of Cosmic-Ray-excited H <sub>2</sub> in Barnard 68: Spatial Variations and Constraints on Cosmic-Ray Attenuation

Abstract We present James Webb Space Telescope (JWST) NIRSpec observations of the starless dark cloud Barnard 68 (B68) that reveal the spatially resolved signature of cosmic-ray-excited molecular hydrogen (CRXH 2 ) emissions for the first time. Following up on our initial detection of CRXH 2 emissions from B68, we now exploit JWST’s sensitivity and spatial multiplexing to map CRXH 2 rovibrational lines across 16 sight lines through the cloud. By disentangling the CRXH 2 and UV-pumped H 2 components, we isolate the para-H 2 -dominated spectrum attributable to cosmic-ray (CR) excitation. We find that there are significant spatial variations in the ratio of the CRXH 2 line intensity to the line-of-sight H 2 column density; these cannot be accounted for by dust extinction alone and demonstrate a clear attenuation of the CR flux with increasing shielding column. Modeling B68 as a Bonnor–Ebert sphere, we constrain both the unshielded CR ionization rate, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>ζ</mml:mi> </mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">H</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>2</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:msub> </mml:math> , and how it decreases with shielding column. At a reference depth of N (H 2 ) = 3 × 10 21 cm −2 , we infer <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>ζ</mml:mi> </mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">H</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>2</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:msub> <mml:mo>≈</mml:mo> <mml:mn>1.4</mml:mn> <mml:mo>×</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>16</mml:mn> </mml:mrow> </mml:msup> </mml:math> s −1 , a factor of ≈3 higher than the average value derived from H <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow/> <mml:mrow> <mml:mn>3</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> </mml:mrow> </mml:msubsup> </mml:math> absorption studies. These results provide the most direct probe to date of CR penetration into cold, dense gas, offering new constraints on both the microphysics of CR–H 2 interactions and the attenuation of low-energy CRs in molecular clouds. Our findings establish CRXH 2 emission as a powerful new diagnostic of the CR environment in interstellar space.

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Publication Details

Journal
The Astrophysical Journal
Published
2026-02-03
DOI
https://doi.org/10.3847/1538-4357/ae22cd
Primary Topic
Astrophysics and Star Formation Studies
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article
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article

JWST Observations of Cosmic-Ray-excited H 2 in Barnard 68: Spatial Variations and Constraints on Cosmic-Ray Attenuation

Kedron Silsbee, James Muzerolle Page, Brandt A. L. Gaches, Sirio Belli et al.
The Astrophysical Journal
Astrophysics and Star Formation Studies
article

JWST Observations of Cosmic-Ray-excited H 2 in Barnard 68: Spatial Variations and Constraints on Cosmic-Ray Attenuation

Kedron Silsbee, James Muzerolle Page, Brandt A. L. Gaches, Sirio Belli, B. Godard, David Neufeld, Amit Chemke, Shmuel Bialy, Padovani Marco, Christian Rab, Thomas G. Bisbas, Alexei V. Ivlev
article en

Abstract

Abstract We present James Webb Space Telescope (JWST) NIRSpec observations of the starless dark cloud Barnard 68 (B68) that reveal the spatially resolved signature of cosmic-ray-excited molecular hydrogen (CRXH 2 ) emissions for the first time. Following up on our initial detection of CRXH 2 emissions from B68, we now exploit JWST’s sensitivity and spatial multiplexing to map CRXH 2 rovibrational lines across 16 sight lines through the cloud. By disentangling the CRXH 2 and UV-pumped H 2 components, we isolate the para-H 2 -dominated spectrum attributable to cosmic-ray (CR) excitation. We find that there are significant spatial variations in the ratio of the CRXH 2 line intensity to the line-of-sight H 2 column density; these cannot be accounted for by dust extinction alone and demonstrate a clear attenuation of the CR flux with increasing shielding column. Modeling B68 as a Bonnor–Ebert sphere, we constrain both the unshielded CR ionization rate, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>ζ</mml:mi> </mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">H</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>2</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:msub> </mml:math> , and how it decreases with shielding column. At a reference depth of N (H 2 ) = 3 × 10 21 cm −2 , we infer <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>ζ</mml:mi> </mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">H</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>2</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:msub> <mml:mo>≈</mml:mo> <mml:mn>1.4</mml:mn> <mml:mo>×</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>16</mml:mn> </mml:mrow> </mml:msup> </mml:math> s −1 , a factor of ≈3 higher than the average value derived from H <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow/> <mml:mrow> <mml:mn>3</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> </mml:mrow> </mml:msubsup> </mml:math> absorption studies. These results provide the most direct probe to date of CR penetration into cold, dense gas, offering new constraints on both the microphysics of CR–H 2 interactions and the attenuation of low-energy CRs in molecular clouds. Our findings establish CRXH 2 emission as a powerful new diagnostic of the CR environment in interstellar space.

The Astrophysical JournalVol. 998(1)
Openalex Percentile: Top 66%
Astrophysics and Star Formation Studies
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