TY - JOUR
T1 - High-resolution H I observations of H II regions. III. Photodissociation regions and the magnetic field near orion B
AU - Van Der Werf, Paul P.
AU - Goss, W. M.
AU - Heiles, Carl
AU - Crutcher, R. M.
AU - Troland, T. H.
N1 - Copyright:
Copyright 2018 Elsevier B.V., All rights reserved.
PY - 1993/7/1
Y1 - 1993/7/1
N2 - H I observations of the H II region Orion B are presented with an angular resolution of 50″ (0.1 pc) and velocity resolution of 0.64 km s-1. Three kinematically distinct H I layers are detected in absorption. It is argued that one of these H I components originates in a photodissociation region (PDR) directly outside the ionization front in front of the H II region. In addition to the H I absorption, H I emission is detected, most likely originating in a PDR behind the H II region. Combining the H I emission and absorption data yields the conclusion that a range of temperatures exists in the PDRs, a conclusion corroborated by existing [C II] 158 μm line measurements of the PDRs. While the H I absorption data show the presence of gas colder than ∼20 K (which is too cold to contribute significantly to the [C II] emission), the H I and [C II] data can be brought in agreement if the emitting H I is a temperature of at least several hundred degrees. These results are interpreted in terms of a clumpy PDR model, where the colder gas is located in dense clumps, which are embedded in a warmer, low-density interclump medium. An analysis of the Zeeman effect as determined from the observed circular polarization yields line-of-sight magnetic fields of 28 and 63 μG for two of the H I layers, at a reduced angular resolution of 100″. It is concluded that the magnetic field strength and the total pressure in the dense PDR are higher than in the more tenuous cloud envelope. However, in the cloud envelope the pressure is dominated by the magnetic field, while in the PDR turbulent pressure dominates.
AB - H I observations of the H II region Orion B are presented with an angular resolution of 50″ (0.1 pc) and velocity resolution of 0.64 km s-1. Three kinematically distinct H I layers are detected in absorption. It is argued that one of these H I components originates in a photodissociation region (PDR) directly outside the ionization front in front of the H II region. In addition to the H I absorption, H I emission is detected, most likely originating in a PDR behind the H II region. Combining the H I emission and absorption data yields the conclusion that a range of temperatures exists in the PDRs, a conclusion corroborated by existing [C II] 158 μm line measurements of the PDRs. While the H I absorption data show the presence of gas colder than ∼20 K (which is too cold to contribute significantly to the [C II] emission), the H I and [C II] data can be brought in agreement if the emitting H I is a temperature of at least several hundred degrees. These results are interpreted in terms of a clumpy PDR model, where the colder gas is located in dense clumps, which are embedded in a warmer, low-density interclump medium. An analysis of the Zeeman effect as determined from the observed circular polarization yields line-of-sight magnetic fields of 28 and 63 μG for two of the H I layers, at a reduced angular resolution of 100″. It is concluded that the magnetic field strength and the total pressure in the dense PDR are higher than in the more tenuous cloud envelope. However, in the cloud envelope the pressure is dominated by the magnetic field, while in the PDR turbulent pressure dominates.
KW - H II regions
KW - ISM: individual (Orion B)
KW - ISM: magnetic fields
KW - ISM: structure
KW - Radio lines: ISM
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U2 - 10.1086/172824
DO - 10.1086/172824
M3 - Article
AN - SCOPUS:12044251821
SN - 0004-637X
VL - 411
SP - 247
EP - 259
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
ER -