Abstract:For L IR - The best-fit lines in Figure 6 of the original article are correct and the conclusions of the paper are not affected. We thank Iván Oteo for bringing the discrepancy in the original paper to our attention. , and J HNC 1 0 ( ) = , for a sample of 58 local luminous and ultraluminous infrared galaxies from the Great Observatories All-sky LIRG Survey (GOALS). By combining our new IRAM data with literature data and Spitzer/IRS spectroscopy, we study the correspondence between these putative tracers o… Show more
“…Assuming a fundamental relationship between the amount of dense gas and the star formation rate exists, then scatter in the relationship between the HCN 1-0 intensity and the actual amount of dense gas would contribute to the observed scatter in the GaoSolomon relationship. Our identification of HCN abundance variations and self absorption as sources of this scatter could help explain the increased scatter and systematic deviations seen when testing the Gao Solomon relationship for larger samples of more extreme sources, including ULIRGs (Privon et al 2015) and AGN (Davies et al 2012;Imanishi et al 2009;Kohno et al 2003). Wu et al (2005) interpret the Gao-Solomon relationship as indicating that individual, sub-parsec scale dense cores are the fundamental unit of dense gas mass associated with star formation, and that the Gao Solomon relation on larger scales is essentially counting the number of these structures.…”
Section: The Interpretation Of the Gao-solomon Relationmentioning
confidence: 92%
“…HCN 1-0 is observed to be anomalously bright in active galactic nuclei (AGN), compared to CO and HCO + (Davies et al 2012;Imanishi et al 2009;Kohno et al 2003). Graciá-Carpio et al (2006) also find that HCN 1-0 may be overluminous compared to HCO + in ultraluminous infrared galaxies (ULIRGs), and Privon et al (2015) also find that overluminous HCN 1-0 is not limited to galaxies containing AGN. In addition to these indications that HCN 1-0 is overluminous in some environments, there are observations that a single power-law spectrum is insufficient to describe both normal galaxies and ULIRGs.…”
We investigate the correlation of HCN 1-0 with gas mass in the central 300 pc of the Galaxy. We find that on the ∼ 10 pc size scale of individual cloud cores, HCN 1-0 is well correlated with dense gas mass when plotted as a log-log relationship. There is ∼0.75 dex of scatter in this relationship from clouds like Sgr B2, which has an integrated HCN 1-0 intensity of a cloud less than half its mass, and others that have HCN 1-0 enhanced by a factor of 2-3 relative to clouds of comparable mass. We identify the two primary sources of scatter to be self-absorption and variations in HCN abundance. We also find that the extended HCN 1-0 emission is more intense per unit mass than in individual cloud cores. In fact the majority (80%) of HCN 1-0 emission comes from extended gas with column densities below 7 × 10 22 cm −2 , accounting for 68% of the total mass. We find variations in the brightness of HCN 1-0 would only yield a ∼ 10% error in the dense gas mass inferred from this line in the Galactic center. However, the observed order of magnitude HCN abundance variations, and the systematic nature of these variations, warn of potential biases in the use of HCN as dense gas mass tracer in more extreme environments such as AGN and shock-dominated regions. We also investigate other 3 mm tracers, finding that HNCO is better correlated with mass than HCN, and might be a better tracer of cloud mass in this environment.
“…Assuming a fundamental relationship between the amount of dense gas and the star formation rate exists, then scatter in the relationship between the HCN 1-0 intensity and the actual amount of dense gas would contribute to the observed scatter in the GaoSolomon relationship. Our identification of HCN abundance variations and self absorption as sources of this scatter could help explain the increased scatter and systematic deviations seen when testing the Gao Solomon relationship for larger samples of more extreme sources, including ULIRGs (Privon et al 2015) and AGN (Davies et al 2012;Imanishi et al 2009;Kohno et al 2003). Wu et al (2005) interpret the Gao-Solomon relationship as indicating that individual, sub-parsec scale dense cores are the fundamental unit of dense gas mass associated with star formation, and that the Gao Solomon relation on larger scales is essentially counting the number of these structures.…”
Section: The Interpretation Of the Gao-solomon Relationmentioning
confidence: 92%
“…HCN 1-0 is observed to be anomalously bright in active galactic nuclei (AGN), compared to CO and HCO + (Davies et al 2012;Imanishi et al 2009;Kohno et al 2003). Graciá-Carpio et al (2006) also find that HCN 1-0 may be overluminous compared to HCO + in ultraluminous infrared galaxies (ULIRGs), and Privon et al (2015) also find that overluminous HCN 1-0 is not limited to galaxies containing AGN. In addition to these indications that HCN 1-0 is overluminous in some environments, there are observations that a single power-law spectrum is insufficient to describe both normal galaxies and ULIRGs.…”
We investigate the correlation of HCN 1-0 with gas mass in the central 300 pc of the Galaxy. We find that on the ∼ 10 pc size scale of individual cloud cores, HCN 1-0 is well correlated with dense gas mass when plotted as a log-log relationship. There is ∼0.75 dex of scatter in this relationship from clouds like Sgr B2, which has an integrated HCN 1-0 intensity of a cloud less than half its mass, and others that have HCN 1-0 enhanced by a factor of 2-3 relative to clouds of comparable mass. We identify the two primary sources of scatter to be self-absorption and variations in HCN abundance. We also find that the extended HCN 1-0 emission is more intense per unit mass than in individual cloud cores. In fact the majority (80%) of HCN 1-0 emission comes from extended gas with column densities below 7 × 10 22 cm −2 , accounting for 68% of the total mass. We find variations in the brightness of HCN 1-0 would only yield a ∼ 10% error in the dense gas mass inferred from this line in the Galactic center. However, the observed order of magnitude HCN abundance variations, and the systematic nature of these variations, warn of potential biases in the use of HCN as dense gas mass tracer in more extreme environments such as AGN and shock-dominated regions. We also investigate other 3 mm tracers, finding that HNCO is better correlated with mass than HCN, and might be a better tracer of cloud mass in this environment.
“…Privon et al (2015) have shown that some pure starburst and composite sources show similarly enhanced HCN emission. The origin of this enhancement is uncertain, but might be due to mid-infrared pumping associated with a compact obscured nucleus (CON; e.g., Aalto et al 2015).…”
We report the detection of a heavily obscured active galactic nucleus (AGN) in the luminous infrared galaxy (LIRG) NGC 6286 identified in a 17.5 ks Nuclear Spectroscopic Telescope Array observation. The source is in an early merging stage and was targeted as part of our ongoing NuSTAR campaign observing local luminous and ultraluminous infrared galaxies in different merger stages. NGC 6286 is clearly detected above 10 keV and by including the quasi-simultaneous Swift/XRT and archival XMM-Newton and Chandra data, we find that the source is heavily obscured (N H ;(0.95−1.32) × 10 24 cm −2 ) with a column density consistent with being Compton-thick (CT, N log cm 24The AGN in NGC 6286 has a low absorption-corrected luminosity (L 2−10 keV ∼ 3 −20 × 10 41 erg s −1 ) and contributes 1% to the energetics of the system. Because of its low luminosity, previous observations carried out in the soft X-ray band (<10 keV) and in the infrared did not notice the presence of a buried AGN. NGC 6286 has multiwavelength characteristics typical of objects with the same infrared luminosity and in the same merger stage, which might imply that there is a significant population of obscured low-luminosity AGNs in LIRGs that can only be detected by sensitive hard X-ray observations.
“…Recently the favored scenario for the enhancement of HCN around AGNs in observational data is high temperature chemistry likely due to mechanical heating (Harada et al 2010;Izumi et al 2013;Matsushita et al 2015). The increasing number of sources detected in these species seem to show in average an enhancement of the HCN/HCO + ratio in the presence of an AGN (Privon et al 2015;Izumi et al 2016;Imanishi et al 2016). However, the scatter is large among the ratios observed in both galaxies hosting AGNs and starbursts (Privon et al 2015), which makes it necessary to study individual cases at high resolution to understand the origin of such dispersion.…”
Section: Hcn/hcomentioning
confidence: 99%
“…The increasing number of sources detected in these species seem to show in average an enhancement of the HCN/HCO + ratio in the presence of an AGN (Privon et al 2015;Izumi et al 2016;Imanishi et al 2016). However, the scatter is large among the ratios observed in both galaxies hosting AGNs and starbursts (Privon et al 2015), which makes it necessary to study individual cases at high resolution to understand the origin of such dispersion. In addition, recent high resolution observations with ALMA have shown that this enhancement may occur in the surroundings and not towards the AGN itself (García-Burillo et al 2014;Martín et al 2015;Izumi et al 2016).…”
We present the distribution and kinematics of the molecular gas in the circumnuclear disk (CND, 400 pc × 200 pc) of Centaurus A with resolutions of ∼5 pc (0. 3) and shed light onto the mechanism feeding the Active Galactic Nucleus (AGN) using CO(3-2), HCO + (4-3), HCN(4-3), and CO(6-5) observations obtained with ALMA. Multiple filaments or streamers of tens to a hundred parsec scale exist within the CND, which form a ring-like structure with an unprojected diameter of 9 × 6 (162 pc × 108 pc) and a position angle P A 155• . Inside the nuclear ring, there are two leading and straight filamentary structures with lengths of about 30-60 pc at P A 120• on opposite sides of the AGN, with a rotational symmetry of 180• and steeper position-velocity diagrams, which are interpreted as nuclear shocks due to non-circular motions. Along the filaments, and unlike other nearby AGNs, several dense molecular clumps present low HCN/HCO + (4-3) ratios ( 0.5). The filaments abruptly end in the probed transitions at r 20 pc from the AGN, but previous near-IR H 2 (J=1-0)S(1) maps show that they continue in an even warmer gas phase (T∼1000 K), winding up in the form of nuclear spirals, and forming an inner ring structure with another set of symmetric filaments along the N-S direction and within r 10 pc. The molecular gas is governed primarily by non-circular motions, being the successive shock fronts at different scales where loss of angular momentum occurs, a mechanism which may feed efficiently powerful radio galaxies down to parsec scales.
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