skip to main content
US FlagAn official website of the United States government
dot gov icon
Official websites use .gov
A .gov website belongs to an official government organization in the United States.
https lock icon
Secure .gov websites use HTTPS
A lock ( lock ) or https:// means you've safely connected to the .gov website. Share sensitive information only on official, secure websites.


Title: Low-energy Explosions in a Gravitational Field: Implications for Sub-energetic Supernovae and Fast X-Ray Transients
Abstract Observations and theory suggest that core-collapse supernovae can span a range of explosion energies, and when sub-energetic the shockwave initiating the explosion can decelerate to speeds comparable to the escape speed of the progenitor. In these cases, gravity will complicate the explosion hydrodynamics and conceivably cause the shock to stall at large radii within the progenitor star. To understand these unique properties of weak explosions, we develop a perturbative approach for modeling the propagation of an initially strong shock into a time-steady, infalling medium in the gravitational field of a compact object. This method writes the shock position and the post-shock velocity, density, and pressure as series solutions in the (time-dependent) ratio of the freefall speed to the shock speed, and predicts that the shock stalls within the progenitor if the explosion energy is below a critical value. We show that our model agrees very well with hydrodynamic simulations, and accurately predicts (for example) the time-dependent shock position and velocity and the radius at which the shock stalls. Our results have implications for black hole formation and the newly detected class of fast X-ray transients (FXTs). In particular, we propose that a “phantom shock breakout”—where the outer edge of the star falls through a stalled shock—can yield a burst of X-rays without a subsequent optical/UV signature, similar to FXTs. This model predicts the rise time of the X-ray burst,td, and the mean photon energy,kT, are anticorrelated, approximately as T t d 5 / 8 more » « less
Award ID(s):
2006684
PAR ID:
10487226
Author(s) / Creator(s):
; ; ;
Publisher / Repository:
DOI PREFIX: 10.3847
Date Published:
Journal Name:
The Astrophysical Journal
Volume:
961
Issue:
2
ISSN:
0004-637X
Format(s):
Medium: X Size: Article No. 158
Size(s):
Article No. 158
Sponsoring Org:
National Science Foundation
More Like this
  1. Abstract We analyze pre-explosion near- and mid-infrared (IR) imaging of the site of SN 2023ixf in the nearby spiral galaxy M101 and characterize the candidate progenitor star. The star displays compelling evidence of variability with a possible period of ≈1000 days and an amplitude of Δm≈ 0.6 mag in extensive monitoring with the Spitzer Space Telescope since 2004, likely indicative of radial pulsations. Variability consistent with this period is also seen in the near-IRJandKsbands between 2010 and 2023, up to just 10 days before the explosion. Beyond the periodic variability, we do not find evidence for any IR-bright pre-supernova outbursts in this time period. The IR brightness ( M K s = 10.7 mag) and color (J−Ks= 1.6 mag) of the star suggest a luminous and dusty red supergiant. Modeling of the phase-averaged spectral energy distribution (SED) yields constraints on the stellar temperature ( T eff = 3500 1400 + 800 K) and luminosity ( log L / L = 5.1 ± 0.2 ). This places the candidate among the most luminous Type II supernova progenitors with direct imaging constraints, with the caveat that many of these rely only on optical measurements. Comparison with stellar evolution models gives an initial mass ofMinit= 17 ± 4M. We estimate the pre-supernova mass-loss rate of the star between 3 and 19 yr before explosion from the SED modeling at M ̇ 3 × 10 5 to 3 × 10−4Myr−1for an assumed wind velocity ofvw= 10 km s−1, perhaps pointing to enhanced mass loss in a pulsation-driven wind. 
    more » « less
  2. Abstract We present the stellar population properties of 69 short gamma-ray burst (GRB) host galaxies, representing the largest uniformly modeled sample to date. Using theProspectorstellar population inference code, we jointly fit photometry and/or spectroscopy of each host galaxy. We find a population median redshift of z = 0.64 0.32 + 0.83 (68% confidence), including nine photometric redshifts atz≳ 1. We further find a median mass-weighted age oftm= 0.8 0.53 + 2.71 Gyr, stellar mass of log(M*/M) = 9.69 0.65 + 0.75 , star formation rate of SFR = 1.44 1.35 + 9.37 Myr−1, stellar metallicity of log(Z*/Z) = 0.38 0.42 + 0.44 , and dust attenuation of A V = 0.43 0.36 + 0.85 mag (68% confidence). Overall, the majority of short GRB hosts are star-forming (≈84%), with small fractions that are either transitioning (≈6%) or quiescent (≈10%); however, we observe a much larger fraction (≈40%) of quiescent and transitioning hosts atz≲ 0.25, commensurate with galaxy evolution. We find that short GRB hosts populate the star-forming main sequence of normal field galaxies, but do not include as many high-mass galaxies as the general galaxy population, implying that their binary neutron star (BNS) merger progenitors are dependent on a combination of host star formation and stellar mass. The distribution of ages and redshifts implies a broad delay-time distribution, with a fast-merging channel atz> 1 and a decreased neutron star binary formation efficiency from high to low redshifts. If short GRB hosts are representative of BNS merger hosts within the horizon of current gravitational wave detectors, these results can inform future searches for electromagnetic counterparts. All of the data and modeling products are available on the Broadband Repository for Investigating Gamma-ray burst Host Traits website. 
    more » « less
  3. Abstract Magnetic reconnection is often invoked as a source of high-energy particles, and in relativistic astrophysical systems it is regarded as a prime candidate for powering fast and bright flares. We present a novel analytical model—supported and benchmarked with large-scale three-dimensional kinetic particle-in-cell simulations in electron–positron plasmas—that elucidates the physics governing the generation of power-law energy spectra in relativistic reconnection. Particles with Lorentz factorγ≳ 3σ(here,σis the magnetization) gain most of their energy in the inflow region, while meandering between the two sides of the reconnection layer. Their acceleration time is t acc γ η rec 1 ω c 1 20 γ ω c 1 , whereηrec≃ 0.06 is the inflow speed in units of the speed of light andωc=eB0/mcis the gyrofrequency in the upstream magnetic field. They leave the region of active energization aftertesc, when they get captured by one of the outflowing flux ropes of reconnected plasma. We directly measuretescin our simulations and find thattesc∼taccforσ≳ few. This leads to a universal (i.e.,σ-independent) power-law spectrum dN free / d γ γ 1 for the particles undergoing active acceleration, and dN / d γ γ 2 for the overall particle population. Our results help to shed light on the ubiquitous presence of power-law particle and photon spectra in astrophysical nonthermal sources. 
    more » « less
  4. Abstract We present comprehensive optical observations of SN 2021gmj, a Type II supernova (SN II) discovered within a day of explosion by the Distance Less Than 40 Mpc survey. Follow-up observations show that SN 2021gmj is a low-luminosity SN II (LL SN II), with a peak magnitudeMV= −15.45 and an Feiivelocity of ∼1800 km s−1at 50 days past explosion. Using the expanding photosphere method, we derive a distance of 17.8 0.4 + 0.6 Mpc. From the tail of the light curve we obtain a radioactive nickel mass of M 56 Ni = 0.014 ± 0.001M. The presence of circumstellar material (CSM) is suggested by the early-time light curve, early spectra, and high-velocity Hαin absorption. Analytical shock-cooling models of the light curve cannot reproduce the fast rise, supporting the idea that the early-time emission is partially powered by the interaction of the SN ejecta and CSM. The inferred low CSM mass of 0.025Min our hydrodynamic-modeling light-curve analysis is also consistent with our spectroscopy. We observe a broad feature near 4600 Å, which may be high-ionization lines of C, N, or/and Heii. This feature is reproduced by radiation-hydrodynamic simulations of red supergiants with extended atmospheres. Several LL SNe II show similar spectral features, implying that high-density material around the progenitor may be common among them. 
    more » « less
  5. Abstract Let$$\mathbb {F}_q^d$$ F q d be thed-dimensional vector space over the finite field withqelements. For a subset$$E\subseteq \mathbb {F}_q^d$$ E F q d and a fixed nonzero$$t\in \mathbb {F}_q$$ t F q , let$$\mathcal {H}_t(E)=\{h_y: y\in E\}$$ H t ( E ) = { h y : y E } , where$$h_y:E\rightarrow \{0,1\}$$ h y : E { 0 , 1 } is the indicator function of the set$$\{x\in E: x\cdot y=t\}$$ { x E : x · y = t } . Two of the authors, with Maxwell Sun, showed in the case$$d=3$$ d = 3 that if$$|E|\ge Cq^{\frac{11}{4}}$$ | E | C q 11 4 andqis sufficiently large, then the VC-dimension of$$\mathcal {H}_t(E)$$ H t ( E ) is 3. In this paper, we generalize the result to arbitrary dimension by showing that the VC-dimension of$$\mathcal {H}_t(E)$$ H t ( E ) isdwhenever$$E\subseteq \mathbb {F}_q^d$$ E F q d with$$|E|\ge C_d q^{d-\frac{1}{d-1}}$$ | E | C d q d - 1 d - 1
    more » « less