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1. How Large Is a Disk—What Do Protoplanetary Disk Gas Sizes Really Mean?

   https://doi.org/10.3847/1538-4357/ace7d1  

   Trapman, Leon; Rosotti, Giovanni; Zhang, Ke; Tabone, Benoît (August 2023, The Astrophysical Journal)

   Abstract It remains unclear what mechanism is driving the evolution of protoplanetary disks. Direct detection of the main candidates, either turbulence driven by magnetorotational instabilities or magnetohydrodynamical disk winds, has proven difficult, leaving the time evolution of the disk size as one of the most promising observables able to differentiate between these two mechanisms. But to do so successfully, we need to understand what the observed gas disk size actually traces. We studied the relation betweenR_CO,90%, the radius that encloses 90% of the¹²CO flux, andR_c, the radius that encodes the physical disk size, in order to provide simple prescriptions for conversions between these two sizes. For an extensive grid of thermochemical models, we calculateR_CO,90%from synthetic observations and relate properties measured at this radius, such as the gas column density, to bulk disk properties, such asR_cand the disk massM_disk. We found an empirical correlation between the gas column density atR_CO,90%and disk mass: $N_{\mathrm{gas}}{\left(R_{\mathrm{CO},90\%}\right)\approx 3.73\times {10}^{21}\left(M_{\mathrm{disk}}/M_{\odot }\right)}^{0.34}{\mathrm{cm}}^{-2}$ . Using this correlation we derive an analytical prescription ofR_CO,90%that only depends onR_candM_disk. We deriveR_cfor disks in Lupus, Upper Sco, Taurus, and the DSHARP sample, finding that disks in the older Upper Sco region are significantly smaller (〈R_c〉 = 4.8 au) than disks in the younger Lupus and Taurus regions (〈R_c〉 = 19.8 and 20.9 au, respectively). This temporal decrease inR_cgoes against predictions of both viscous and wind-driven evolution, but could be a sign of significant external photoevaporation truncating disks in Upper Sco. 

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2. Molecular Outflows in the Nucleus of the Nearby Compton-thick AGN NGC 3079

   https://doi.org/10.3847/1538-4357/ae6654  

   Lin, Ming-Yi; Medling, Anne M; Davies, Richard I; Krips, Melanie; Barcos-Muñoz, L; Genzel, R; González-Alfonso, E; Gracia-Carpio, J; Lutz, D; Neri, R; et al (June 2026, The Astrophysical Journal)

   Abstract We present Northern Extended Millimeter Array observations of the CO (2–1) molecular gas kinematics in the nearby Compton-thick Seyfert 2 galaxy NGC 3079, with an angular resolution of 0 $\stackrel{\text{″}}{.}$ 5 (∼40 pc). To interpret the observed CO (2–1) kinematics, we model the rotating disk using two software tools, 3D-Barolo and DysmalPy, to generate mock 3D data cubes. Both models indicate, in addition to the rotating disk, the presence of a spatially unresolved nuclear component characterized by high velocity dispersion. Analysis of the visibility data reveals that the blueshifted, high-velocity component is spatially offset from the continuum peak by 0 $\stackrel{\text{″}}{.}$ 17 (∼14 pc) and exhibits line-of-sight velocities ofv−v_sys= −350 to −450 km s⁻¹, which we interpret as a nuclear molecular outflow. We calculate a molecular gas mass outflow rate of 8.82M_⊙yr⁻¹, with a kinetic power ( ${\dot{E}}_{\text{out}}$ ) of 3.8 ×10⁴¹erg s⁻¹and a momentum rate ( ${\dot{p}}_{\text{out}}$ ) of 2.05 × 10³⁴Dyne. The momentum rate exceeds the AGN radiation momentum rate by a factor of ∼15, suggesting an energy-driven outflow. Furthermore, we argue that the derived kinetic power of the nuclear molecular outflow favors a jet-powered scenario that explains the slowdown and brightening of the parsec-scale radio source observed with the Very Long Baseline Array. 

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3. Pre-peak Emission in Tidal Disruption Events

   https://doi.org/10.3847/1538-4357/ad6c39  

   Huang_黄, Xiaoshan 小珊; Davis, Shane W; Jiang_姜, Yan-fei 燕飞 (October 2024, The Astrophysical Journal)

   Abstract The rising part of a tidal disruption event light curve provides unique insight into early emission and the onset of accretion. Various mechanisms are proposed to explain the pre-peak emission, including shocks from debris interaction and reprocessing of disk emission. We study the pre-peak emission and its influence on the gas circularization by a series of gray radiation hydrodynamic simulations with varying black hole mass. We find that, given a super-Eddington fallback rate of $10{\dot{M}}_{\mathrm{Edd}}$ , the stream–stream collision can occur multiple times and drive strong outflows of up to $9{\dot{M}}_{\mathrm{Edd}}$ . By dispersing gas to ≳100r_s, the outflow can delay gas circularization and leads to sub-Eddington accretion rates during the first few stream–stream collisions. The stream–stream collision shock and circularization shock can sustain a luminosity of ∼10⁴⁴erg s⁻¹for days. The luminosity is generally sub-Eddington and shows a weak correlation with accretion rate at early times. The outflow is optically thick, yielding a reprocessing layer with a size of ∼10¹⁴cm and photospheric temperature of ∼4 × 10⁴K. 

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4. Jets with a Twist: The Emergence of FR0 Jets in a 3D GRMHD Simulation of Zero-angular-momentum Black Hole Accretion

   https://doi.org/10.3847/1538-4357/ad0974  

   Lalakos, Aretaios; Tchekhovskoy, Alexander; Bromberg, Omer; Gottlieb, Ore; Jacquemin-Ide, Jonatan; Liska, Matthew; Zhang, Haocheng (March 2024, The Astrophysical Journal)

   Abstract Spinning supermassive black holes (BHs) in active galactic nuclei magnetically launch relativistic collimated outflows, or jets. Without angular momentum supply, such jets are thought to perish within 3 orders of magnitude in distance from the BH, well before reaching kiloparsec scales. We study the survival of such jets at the largest scale separation to date, via 3D general relativistic magnetohydrodynamic simulations of rapidly spinning BHs immersed into uniform zero-angular-momentum gas threaded by a weak vertical magnetic field. We place the gas outside the BH sphere of influence, or the Bondi radius, chosen to be much larger than the BH gravitational radius,R_B= 10³R_g. The BH develops dynamically important large-scale magnetic fields, forms a magnetically arrested disk (MAD), and launches relativistic jets that propagate well outsideR_Band suppress BH accretion to 1.5% of the Bondi rate, ${\dot{M}}_{\mathrm{B}}$ . Thus, low-angular-momentum accretion in the MAD state can form large-scale jets in Fanaroff–Riley (FR) type I and II galaxies. Subsequently, the disk shrinks and exits the MAD state: barely a disk (BAD), it rapidly precesses, whips the jets around, globally destroys them, and lets 5%–10% of ${\dot{M}}_{\mathrm{B}}$ reach the BH. Thereafter, the disk starts rocking back and forth by angles 90°–180°: the rocking accretion disk (RAD) launches weak intermittent jets that spread their energy over a large area and suppress BH accretion to ≲2% ${\dot{M}}_{\mathrm{B}}$ . Because the BAD and RAD states tangle up the jets and destroy them well insideR_B, they are promising candidates for the more abundant, but less luminous, class of FR0 galaxies. 

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5. Winds and Disk Turbulence Exert Equal Torques on Thick Magnetically Arrested Disks

   https://doi.org/10.3847/1538-4357/ad323d  

   Manikantan, Vikram; Kaaz, Nicholas; Jacquemin-Ide, Jonatan; Musoke, Gibwa; Chatterjee, Koushik; Liska, Matthew; Tchekhovskoy, Alexander (April 2024, The Astrophysical Journal)

   Abstract The conventional accretion disk lore is that magnetized turbulence is the principal angular momentum transport process that drives accretion. However, when dynamically important large-scale magnetic fields thread an accretion disk, they can produce mass and angular momentum outflows, known as winds,that also drive accretion. Yet, the relative importance of turbulent and wind-driven angular momentum transport is still poorly understood. To probe this question, we analyze a long-duration (1.2 × 10⁵r_g/c) simulation of a rapidly rotating (a= 0.9) black hole feeding from a thick (H/r∼ 0.3), adiabatic, magnetically arrested disk (MAD), whose dynamically important magnetic field regulates mass inflow and drives both uncollimated and collimated outflows (i.e., winds and jets, respectively). By carefully disentangling the various angular momentum transport processes within the system, we demonstrate the novel result that disk winds and disk turbulence both extract roughly equal amounts of angular momentum from the disk. We find cumulative angular momentum and mass accretion outflow rates of $\dot{L}\propto r^{0.9}$ and $\dot{M}\propto r^{0.4}$ , respectively. This result suggests that understanding both turbulent and laminar stresses is key to understanding the evolution of systems where geometrically thick MADs can occur, such as the hard state of X-ray binaries, low-luminosity active galactic nuclei, some tidal disruption events, and possibly gamma-ray bursts. 

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