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1. CLEAR: High-ionization [Ne v] λ3426 Emission-line Galaxies at 1.4 < z < 2.3

   https://doi.org/10.3847/1538-4357/acc1e6  

   Cleri, Nikko J.; Yang, Guang; Papovich, Casey; Trump, Jonathan R.; Backhaus, Bren E.; Estrada-Carpenter, Vicente; Finkelstein, Steven L.; Giavalisco, Mauro; Hutchison, Taylor A.; Ji, Zhiyuan; et al (May 2023, The Astrophysical Journal)

   Abstract We analyze a sample of 25 [Nev] (λ3426) emission-line galaxies at 1.4 <z< 2.3 using Hubble Space Telescope/Wide Field Camera 3 G102 and G141 grism observations from the CANDELS LyαEmission at Reionization (CLEAR) survey. [Nev] emission probes extremely energetic photoionization (creation potential of 97.11 eV) and is often attributed to energetic radiation from active galactic nuclei (AGNs), shocks from supernovae, or an otherwise very hard ionizing spectrum from the stellar continuum. In this work, we use [Nev] in conjunction with other rest-frame UV/optical emission lines ([Oii]λλ3726, 3729, [Neiii]λ3869, Hβ, [Oiii]λλ4959, 5007, Hα+[Nii]λλ6548, 6583, [Sii]λλ6716, 6731), deep (2–7 Ms) X-ray observations (from Chandra), and mid-infrared imaging (from Spitzer) to study the origin of this emission and to place constraints on the nature of the ionizing engine. The majority of the [Nev]-detected galaxies have properties consistent with ionization from AGNs. However, for our [Nev]-selected sample, the X-ray luminosities are consistent with local (z≲ 0.1) X-ray-selected Seyferts, but the [Nev] luminosities are more consistent with those fromz∼ 1 X-ray-selected QSOs. The excess [Nev] emission requires either reduced hard X-rays or a ∼0.1 keV excess. We discuss possible origins of the apparent [Nev] excess, which could be related to the “soft (X-ray) excess” observed in some QSOs and Seyferts and/or be a consequence of a complex/anisotropic geometry for the narrow-line region, combined with absorption from a warm, relativistic wind ejected from the accretion disk. We also consider implications for future studies of extreme high-ionization systems in the epoch of reionization (z≳ 6) with the James Webb Space Telescope. 

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2. Ne viii in the Warm-hot Circumgalactic Medium of FIRE Simulations and in Observations

   https://doi.org/10.3847/1538-4357/ad63a0  

   Wijers, Nastasha_A; Faucher-Giguère, Claude-André; Stern, Jonathan; Byrne, Lindsey; Sultan, Imran (September 2024, The Astrophysical Journal)

   Abstract The properties of warm-hot gas around ∼L_*galaxies can be studied with absorption lines from highly ionized metals. We predict Neviiicolumn densities from cosmological zoom-in simulations of halos with masses in ∼10¹²and ∼10¹³M_☉from the Feedback in Realistic Environments (FIRE) project. Neviiitraces the volume-filling, virial-temperature gas in ∼10¹²M_☉halos. In ∼10¹³M_☉halos the Neviiigas is clumpier, and biased toward the cooler part of the warm-hot phase. We compare the simulations to observations from the COS Absorption Survey of Baryon Harbors (or CASBaH) and COS Ultraviolet Baryon Survey (or CUBS). We show that when inferring halo masses from stellar masses to compare simulated and observed halos, it is important to account for the scatter in the stellar-mass–halo-mass relation, especially atM_⋆≳ 10^10.5M_☉. Median Neviiicolumns in the fiducial FIRE-2 model are about as high as observed upper limits allow, while the simulations analyzed do not reproduce the highest observed columns. This suggests that the median Neviiiprofiles predicted by the simulations are consistent with observations, but that the simulations may underpredict the scatter. We find similar agreement with analytical models that assume a product of the halo gas fraction and metallicity (relative to solar) ∼0.1, indicating that observations are consistent with plausible circumgalactic medium temperatures, metallicities, and gas masses. Variants of the FIRE simulations with a modified supernova feedback model and/or active galactic nuclei feedback included (as well as some other cosmological simulations from the literature) more systematically underpredict Neviiicolumns. The circumgalactic Neviiiobservations therefore provide valuable constraints on simulations that otherwise predict realistic galaxy properties. 

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3. Modeling Ionized Gas in the Small Magellanic Cloud: The Wolf–Rayet Nebula N76

   https://doi.org/10.3847/1538-4357/ad3def  

   Tarantino, Elizabeth; Bolatto, Alberto_D; Indebetouw, Rémy; Rubio, Mónica; Sandstrom, Karin_M; Smith, J-D_T; Stapleton, Daniel; Wolfire, Mark (July 2024, The Astrophysical Journal)

   Abstract We presentCloudymodeling of infrared emission lines in the Wolf–Rayet (WR) nebula N76 caused by one of the most luminous and hottest WR stars in the low metallicity Small Magellanic Cloud. We use spatially resolved mid-infrared Spitzer/InfRared Spectrograph and far-infrared Herschel/PACS spectroscopy to establish the physical conditions of the ionized gas. The spatially resolved distribution of the emission allows us to constrain properties much more accurately than using spatially integrated quantities. We construct models with a range of constant hydrogen densities between n_H= 4–10 cm⁻³and a stellar wind-blown cavity of 10 pc, which reproduces the intensity and shape of most ionized gas emission lines, including the high ionization lines [Oiv] and [Nev], as well as [Siii], [Siv], [Oiii], and [Neiii]. Our models suggest that the majority of [Siii] emission (91%) is produced at the edge of the Hiiregion around the transition between ionized and atomic gas while very little of the [Cii] (<5%) is associated with the ionized gas. The physical conditions of N76 are characterized by a hot HII region with a maximum electron temperature ofT_e∼ 24,000 K, electron densities that range fromn_e∼ 4 to 12 cm⁻³, and high ionization parameters of $\log \left(U\right)\sim -1.15\mathrm{to}-1.77.$By analyzing a low-metallicity WR nebula with a single ionization source, this work gives valuable insights into the impact WR stars have on the galaxy-integrated ionized gas properties in nearby dwarf galaxies. 

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4. The Baryonic Content of Galaxies Mapped by MaNGA and the Gas Around Them

   https://doi.org/10.3847/1538-4357/ace329  

   Klimenko, Viacheslav_V; Kulkarni, Varsha; Wake, David_A; Poudel, Suraj; Bershady, Matthew_A; Péroux, Celine; Lundgren, Britt (August 2023, The Astrophysical Journal)

   Abstract We analyze the cool gas in and around 14 nearby galaxies (atz< 0.1) mapped with the Sloan Digital Sky Survey IV MaNGA survey by measuring absorption lines produced by gas in spectra of background quasars/active galactic nuclei at impact parameters of 0–25 effective radii from the galactic centers. Using Hubble Space Telescope/Cosmic Origins Spectrograph, we detect absorption at the galactic redshift and measure or constrain column densities of neutral (Hi, Ni, Oi, and Ari), low-ionization (Siii, Sii, Cii, Nii, and Feii), and high-ionization (Siiii, Feiii, Nv, and Ovi) species for 11 galaxies. We derive the ionization parameter and ionization-corrected metallicity usingcloudyphotoionization models. The Hicolumn density ranges from ∼10¹³to ∼10²⁰cm⁻²and decreases with impact parameter forr≳R_e. Galaxies with higher stellar mass have weaker Hiabsorption. Comparing absorption velocities with MaNGA radial velocity maps of ionized gas line emissions in galactic disks, we find that the neutral gas seen in absorption corotates with the disk out to ∼10R_e. Sight lines with lower elevation angles show lower metallicities, consistent with the metallicity gradient in the disk derived from MaNGA maps. Higher-elevation angle sight lines show higher ionization, lower Hicolumn density, supersolar metallicity, and velocities consistent with the direction of galactic outflow. Our data offer the first detailed comparisons of circumgalactic medium (CGM) properties (kinematics and metallicity) with extrapolations of detailed galaxy maps from integral field spectroscopy; similar studies for larger samples are needed to more fully understand how galaxies interact with their CGM. 

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5. The ⁴¹ Ar(n,y) ⁴² Ar reaction

   https://doi.org/10.1051/epjconf/202328401037  

   Sahoo, R. N.; Paul, M.; Köster, U.; Scott, R.; Tessler, M.; Zylstra, A.; Avila, M. L.; Dickerson, C.; Jayatissa, H.; Kohen, M.S.; et al (January 2023, EPJ Web of Conferences)

   Mattoon, C.M.; Vogt, R.; Escher, J.; Thompson, I. (Ed.)

   The cross-section of the thermal neutron capture⁴¹Ar(n,γ)⁴²Ar(t_1/2=32.9 y) reaction was measured by irradiating a⁴⁰Ar sample at the high-flux reactor of Institut Laue-Langevin (ILL) Grenoble, France. The signature of the two-neutron capture has been observed by measuring the growth curve and identifying the 1524.6 keV γ-lines of the shorter-lived⁴²K(12.4 h) β⁻daughter of⁴²Ar. Our preliminary value of the⁴¹Ar(n,γ)⁴²Ar thermal cross section is 240(80) mb at 25.3 meV. For the first time, direct counting of⁴²Ar was performed using the ultra-high sensitivity technique of noble gas accelerator mass spectrometry (NOGAMS) at Argonne National Laboratory, USA. 

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