The Ionization Structure of the Narrow-Line Region of NGC 1068 and Its Relationship to the Extended Radio Emission
The Ionization Structure of the Narrow-Line Region of NGC 1068 and Its Relationship to the Extended Radio Emission
复制标题
NGC 1068窄线区电离结构及其与扩展射电发射的关系
DOI:
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发表时间:
1997
期刊:
影响因子:
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通讯作者:
F. Macchetto
中科院分区:
文献类型:
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作者:
A. Capetti;D. Axon;F. Macchetto
Hubble Space Telescope (HST)/WFPC2 imaging has been used to investigate the emission-line structure of the narrow-line region (NLR) of the Seyfert 2 galaxy NGC 1068 and its relationship to the extended radio emission. We find that the morphology and the ionization properties of the NLR of NGC 1068 are dominated by the interaction with the radio jet, in full agreement with similar results obtained for other Seyfert galaxies with extended radio emission. The emission lines originate in two distinct regions: a large-scale cocoon enveloping the northeastern radio lobe and a small-scale broken network of filaments and knots surrounding the radio jet. The material along the radio jet, although denser than the surrounding gas, is in a much higher ionization state than the remainder of the NLR. We believe that this requires the presence of a source of ionizing radiation that locally dominates over the nuclear emission, e.g., free-free emission from the gas heated by the interaction with the radio jet. At a distance of approximately 4' (~300 pc) from the nucleus, corresponding to the transition in the radio structure from jetlike to lobelike, the ionization structure of the NLR shows a sharp and well-defined boundary between an inner low-ionization zone and an outer higher ionization zone. This ionization change is easily explained if there is a density increase where the jet enters the lobe, presumably due to the compression of the backflowing radio cocoon at the jet working surface. A color image reveals the presence of a nuclear dust lane projected onto the location of the hidden nucleus. Nuclear dust lanes appear to be ubiquitous in Seyfert 2 galaxies observed with HST and can be naturally associated with the material responsible for the obscuration of the active nucleus.