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2017
DOI: 10.3847/1538-4357/835/1/112
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ERRATUM: “EXCITATION MECHANISMS FOR HCN (1-0) AND HCO+ (1-0) IN GALAXIES FROM THE GREAT OBSERVATORIES ALL-SKY LIRG SURVEY” (2015, ApJ, 814, 39)

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Cited by 35 publications
(63 citation statements)
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“…The ratios of PLCK_G244.8+54.9 are more ambiguous as they lie just at the limit between the two regimes. While this also corroborates the lack of XDR imprints on the high-to-low-J CO line ratios in C18, we emphasize that an enhanced HCO + /HCN is not sufficient to firmly rule out the presence of XDRs (see Privon et al 2015). The elevated cosmic-ray fields expected from the intense star-formation activity of the GEMS may also play an important role in setting the HCO + /HCN ratios in dense cloud cores shielded from UV fields, as argued for instance by Schirm et al (2016) for the Antennae overlap region.…”
Section: Diagnostics From Hco + /Hcnsupporting
confidence: 71%
See 1 more Smart Citation
“…The ratios of PLCK_G244.8+54.9 are more ambiguous as they lie just at the limit between the two regimes. While this also corroborates the lack of XDR imprints on the high-to-low-J CO line ratios in C18, we emphasize that an enhanced HCO + /HCN is not sufficient to firmly rule out the presence of XDRs (see Privon et al 2015). The elevated cosmic-ray fields expected from the intense star-formation activity of the GEMS may also play an important role in setting the HCO + /HCN ratios in dense cloud cores shielded from UV fields, as argued for instance by Schirm et al (2016) for the Antennae overlap region.…”
Section: Diagnostics From Hco + /Hcnsupporting
confidence: 71%
“…The HCO + /HCN line-intensity ratio is also widely used to discriminate between active galactic nuclei-(AGN) and starburstdominated galaxies, given the apparent dichotomy between both populations (e.g., Krips et al 2008;Imanishi & Nakanishi 2014;Imanishi et al 2016;Izumi et al 2016). Other studies, such as that of Privon et al (2015), nonetheless find additional dependences on ISM density and the surrounding radiation fields (e.g., IRpumping, Krips et al 2008), and demonstrate that HCO + /HCN can strongly vary in LIRGs and ULIRGs experiencing both AGN and star formation feedback within their unresolved central regions. In NGC 1068, the HCO + /HCN ratio is even enhanced by the central AGN (García-Burillo et al 2014).…”
Section: Introductionmentioning
confidence: 99%
“…According to Salak et al (2018), all molecular clouds along the SF ring have density and high HCN(1−0)/HCO + (1−0) line ratio (of order ∼1), possibly indicating that the excitation mechanisms are from shocks, free-free emission from Hii regions, and synchrotron emission from SNRs. This ratio even is higher towards the nucleus, with HCN/HCO + ∼ 1.5, which is consistent with the scenario of a composite starburst plus AGN (Privon et al 2015;Salak et al 2018). In addition, they also detected SiO(2−1), a shock tracer, only around the nuclear region of NGC 1808.…”
Section: Ionized and Warm Molecular Gassupporting
confidence: 82%
“…The CO (1−0) 1 line, which is associated with a critical density (n c ) on the order of 10 3 cm −3 and an excitation temperature (T ex ) of 5.5 K, has been widely used to trace the total molecular gas content. However, SF occurs mainly in the denser parts of molecular clouds as evidenced by correlations in local (U)LIRGs between L IR and dense gas tracers such as HCN (1−0) (e.g., Gao & Solomom 2004;Wu et al 2005;Privon et al 2015), and heats up the surrounding dense molecular gas substantially. The resulting warm dense gas can be better traced by a mid-J CO line transition, such as CO (6−5), which has n c ∼ 10 5 cm −3 and T ex = 116 K (Carilli & Walter 2013).…”
Section: Introductionmentioning
confidence: 99%