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1. Interplanetary Type IV Solar Radio Bursts: A Comprehensive Catalog and Statistical Results

   https://doi.org/10.3847/1538-4357/ad5315  

   Mohan, Atul; Gopalswamy, Nat; Kumari, Anshu; Akiyama, Sachiko; G, Sindhuja (August 2024, The Astrophysical Journal)

   Abstract Decameter hectometric (DH; 1–14 MHz) type IV radio bursts are produced by flare-accelerated electrons trapped in postflare loops or the moving magnetic structures associated with the coronal mass ejections (CMEs). From a space weather perspective, it is important to systematically compile these bursts, explore their spectrotemporal characteristics, and study the associated CMEs. We present a comprehensive catalog of DH type IV bursts observed by the Radio and Plasma Wave Investigation instruments on board the Wind and Solar TErrestrial RElations Observatory spacecraft covering the period of white-light CME observations by the Large Angle and Spectrometric Coronagraph on board the Solar and Heliospheric Observatory mission between 1996 November and 2023 May. The catalog has 139 bursts, of which 73% are associated with a fast (>900 km s⁻¹) and wide (>60°) CME, with a mean CME speed of 1301 km s⁻¹. All DH type IV bursts are white-light CME-associated, with 78% of the events associated with halo CMEs. The CME source latitudes are within ±45°. Seventy-seven events had multiple-vantage-point observations from different spacecraft, letting us explore the impact of the line of sight on the dynamic spectra. For 48 of the 77 events, there were good data from at least two spacecraft. We find that, unless occulted by nearby plasma structures, a type IV burst is best viewed when observed within a ±60° line of sight. Also, bursts with a duration above 120 minutes have source longitudes within ±60°. Our inferences confirm the inherent directivity in the type IV emission. Additionally, the catalog forms a Sun-as-a-star DH type IV burst database. 

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2. The Demographics, Stellar Populations, and Star Formation Histories of Fast Radio Burst Host Galaxies: Implications for the Progenitors

   https://doi.org/10.3847/1538-4357/ace5aa  

   Gordon, Alexa C; Fong, Wen-fai; Kilpatrick, Charles D; Eftekhari, Tarraneh; Leja, Joel; Prochaska, J Xavier; Nugent, Anya E; Bhandari, Shivani; Blanchard, Peter K; Caleb, Manisha; et al (August 2023, The Astrophysical Journal)

   Abstract We present a comprehensive catalog of observations and stellar population properties for 23 highly secure host galaxies of fast radio bursts (FRBs). Our sample comprises 6 repeating FRBs and 17 apparent nonrepeaters. We present 82 new photometric and 8 new spectroscopic observations of these hosts. Using stellar population synthesis modeling and employing nonparametric star formation histories (SFHs), we find that FRB hosts have a median stellar mass of ≈10^9.9M_⊙, mass-weighted age ≈5.1 Gyr, and ongoing star formation rate ≈1.3M_⊙yr⁻¹but span wide ranges in all properties. Classifying the hosts by degree of star formation, we find that 87% (20 of 23 hosts) are star-forming, two are transitioning, and one is quiescent. The majority trace the star-forming main sequence of galaxies, but at least three FRBs in our sample originate in less-active environments (two nonrepeaters and one repeater). Across all modeled properties, we find no statistically significant distinction between the hosts of repeaters and nonrepeaters. However, the hosts of repeating FRBs generally extend to lower stellar masses, and the hosts of nonrepeaters arise in more optically luminous galaxies. While four of the galaxies with the clearest and most prolonged rises in their SFHs all host repeating FRBs, demonstrating heightened star formation activity in the last ≲100 Myr, one nonrepeating host shows this SFH as well. Our results support progenitor models with short delay channels (i.e., magnetars formed via core-collapse supernova) for most FRBs, but the presence of some FRBs in less-active environments suggests a fraction form through more delayed channels. 

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3. Dynamic spectra of solar radio emissions from weak-turbulence simulation

   https://doi.org/10.1051/0004-6361/202553752  

   Lazar, M; Ziebell, L F; Yoon, P H; López, R A; Poedts, S (April 2025, Astronomy & Astrophysics)

   Context.In recent decades, serious efforts have been made in the analytical and numerical modeling of solar radio bursts generated by the electron beam interacting with the background plasma, including the dynamic spectra with decreasing frequency over time/space. These are type II and type III radio bursts, with the fundamental components at the local plasma frequency (ω_p = 2πf_p) and the harmonics (nω_p = 2πnf_p). Synthetic spectra built for a number of radio events were able to reproduce the decreasing frequency profiles reasonably well, despite the limitations of the approximate analytical theory. Aims.We propose new modeling of dynamic radio emission spectra using weak-turbulence (WT) theory. This novel approach also aims at a self-consistent and quantitative evaluation of radio emissions, based on first-principles modeling of electron beam plasma instabilities and nonlinear wave interaction. Methods.We performed the WT simulation, which has the ability to quantitatively describe the standard plasma emission involving the nonlinear interaction of Langmuir (L), ion-sound (S), and transverse electromagnetic (T) waves. The composite dynamic spectra are constructed for type II- and type III-like events, against the background electron density model that behaves as an inverse square of the distance from the solar source. Results.The new dynamic spectra are obtained distinctly, with a rapid frequency shift for type III emissions (generated by fast electron beams from coronal sources), as well as a less steep frequency drop for type II spectra (whose sources move away from the Sun along with interplanetary shocks). Upon making a qualitative comparison with typical solar radio emission events, we find that our first-principle-based synthetic dynamic spectra are in good agreement. Conclusions.The findings of the present study demonstrate that the theoretical approach taken in this paper can be further applied to obtain (i) quantitatively relevant predictions and replications of the observed dynamic spectra of radio bursts, and (ii) more realistic large-scale models of the solar radio source, for example the type II and type III source models computed from the large-scale magnetohydrodynamics (MHD) simulations or even from direct spacecraft observations. 

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4. Novel scaling laws to derive spatially resolved flare and CME parameters from sun-as-a-star observables

   https://doi.org/10.1051/0004-6361/202451072  

   Mohan, Atul; Gopalswamy, Natchimuthuk; Raju, Hemapriya; Akiyama, Sachiko (November 2024, Astronomy & Astrophysics)

   Coronal mass ejections (CMEs) are often associated with X-ray (SXR) flares powered by magnetic reconnection in the low corona, while the CME shocks in the upper corona and interplanetary (IP) space accelerate electrons often producing the type II radio bursts. The CME and the reconnection event are part of the same energy release process as highlighted by the correlation between reconnection flux (ϕ_rec) that quantifies the strength of the released magnetic free energy during the SXR flare, and the CME kinetic energy that drives the IP shocks leading to type II bursts. Unlike the Sun, these physical parameters cannot be directly inferred in stellar observations. Hence, scaling laws between unresolved sun-as-a-star observables, namely SXR luminosity (L_X) and type II luminosity (L_R), and the physical properties of the associated dynamical events are crucial. Such scaling laws also provide insights into the interconnections between the particle acceleration processes across low-corona to IP space during solar-stellar “flare-CME-type II” events. Using long-term solar data in the SXR to radio waveband, we derived a scaling law between two novel power metrics for the flare and CME-associated processes. The metrics of “flare power” (P_flare = √(L_Xϕ_rec)) and “CME power” (P_CME = √(L_RV_CME²)), whereV_CMEis the CME speed, scale asP_flare ∝ P_CME^{0.76 ± 0.04}. In addition,L_Xandϕ_recshow power-law trends withP_CMEwith indices of 1.12 ± 0.05 and 0.61 ± 0.05, respectively. These power laws help infer the spatially resolved physical parameters,V_CMEandϕ_rec, from disk-averaged observables,L_XandL_Rduring solar-stellar flare-CME-type II events. 

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5. Multi-epoch sampling of the radio star population with the Australian SKA Pathfinder

   https://doi.org/10.1093/mnras/stae127  

   Pritchard, Joshua; Murphy, Tara; Heald, George; Wheatland, Michael S; Kaplan, David L; Lenc, Emil; O’Brien, Andrew; Wang, Ziteng (March 2024, Monthly Notices of the Royal Astronomical Society)

   ABSTRACT The population of radio-loud stars has to date been studied primarily through either targeted observations of a small number of highly active stars or wide-field, single-epoch surveys that cannot easily distinguish stellar emission from background extragalactic sources. As a result it has been difficult to constrain population statistics such as the surface density and fraction of the population producing radio emission in a particular variable or spectral class. In this paper, we present a sample of 36 radio stars detected in a circular polarization search of the multi-epoch Variables and Slow Transients (VAST) pilot survey with ASKAP at 887.5 MHz. Through repeat sampling of the VAST pilot survey footprint we find an upper limit to the duty cycle of M-dwarf radio bursts of $$8.5 \,\rm {per\,cent}$$, and that at least 10 ± 3 $$\rm {per\,cent}$$ of the population should produce radio bursts more luminous than $$10^{15} \,\rm {erg}\mathrm{s}^{-1} \,\mathrm{Hz}^{-1}$$. We infer a lower limit on the long-term surface density of such bursts in a shallow $$1.25 \,\mathrm{m}\rm {Jy}\rm\ {PSF}^{-1}$$ sensitivity survey of $${9}^{\, +{11}}_{-{7}}\times 10^{-3}$$  $$\,\deg ^{-2}$$ and an instantaneous radio star surface density of 1.7 ± 0.2 × 10−3  $$\,\deg ^{-2}$$ on 12 min time-scales. Based on these rates we anticipate ∼200 ± 50 new radio star detections per year over the full VAST survey and $${41\, 000}^{\, +{10\, 000}}_{-{9\, 000}}$$ in next-generation all-sky surveys with the Square Kilometre Array. 

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