C. L. Fryer’s research while affiliated with Los Alamos National Laboratory and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (235)


Occurrence of Gravitational Collapse in the Accreting Neutron Stars of Binary-driven Hypernovae
  • Article

November 2024

·

10 Reads

The Astrophysical Journal

L. M. Becerra

·

·

C. L. Fryer

·

[...]

·

The binary-driven hypernova (BdHN) model proposes long gamma-ray bursts (GRBs) originate in binaries composed of a carbon–oxygen (CO) star and a neutron star (NS) companion. The CO core collapse generates a newborn NS and a supernova that triggers the GRB by accreting onto the NSs, rapidly transferring mass and angular momentum to them. This article aims to determine the conditions under which a black hole (BH) forms from NS collapse induced by the accretion and the impact on the GRB’s observational properties and taxonomy. We perform three-dimensional, smoothed particle hydrodynamics simulations of BdHNe using up-to-date NS nuclear equations of state, with and without hyperons, and calculate the structure evolution in full general relativity. We assess the binary parameters leading either NS in the binary to the critical mass for gravitational collapse into a BH and its occurrence time, t col . We include a nonzero angular momentum of the NSs and find that t col ranges from a few tens of seconds to hours for decreasing NS initial angular momentum values. BdHNe I are the most compact (about 5 minute orbital period), promptly form a BH, and release ≳10 ⁵² erg of energy. They form NS–BH binaries with tens of kiloyears merger timescales by gravitational-wave emission. BdHNe II and III do not form BHs, and release ∼10 ⁵⁰ –10 ⁵² erg and ≲10 ⁵⁰ erg of energy, respectively. They form NS–NS binaries with a range of merger timescales larger than for NS–BH binaries. In some compact BdHNe II, either NS can become supramassive, i.e., above the critical mass of a nonrotating NS. Magnetic braking by a 10 ¹³ G field can delay BH formation, leading to BH–BH or NS–BH with tens of kiloyears merger timescales.


The Green Monster Hiding in Front of Cas A: JWST Reveals a Dense and Dusty Circumstellar Structure Pockmarked by Ejecta Interactions

November 2024

·

15 Reads

The Astrophysical Journal Letters

JWST observations of the young Galactic supernova remnant Cassiopeia A revealed an unexpected structure seen as a green emission feature in colored composite MIRI F1130W and F1280W images—hence dubbed the Green Monster—that stretches across the central parts of the remnant in projection. Combining the kinematic information from NIRSpec and the MIRI Medium Resolution Spectrograph with the multiwavelength imaging from NIRCam and MIRI, we associate the Green Monster with circumstellar material (CSM) that was lost during an asymmetric mass-loss phase. MIRI images are dominated by dust emission, but their spectra show emission lines from Ne, H, and Fe with low radial velocities indicative of a CSM nature. An X-ray analysis of this feature in a companion paper supports its CSM nature and detects significant blueshifting, thereby placing the Green Monster on the nearside, in front of the Cas A supernova remnant. The most striking features of the Green Monster are dozens of almost perfectly circular 1″–3″ sized holes, most likely created by interaction between high-velocity supernova ejecta material and the CSM. Further investigation is needed to understand whether these holes were formed by small 8000–10,500 km s ⁻¹ N-rich ejecta knots that penetrated and advanced out ahead of the remnant’s 5000–6000 km s ⁻¹ outer blast wave or by narrow ejecta fingers that protrude into the forward-shocked CSM. The detection of the Green Monster provides further evidence of the highly asymmetric mass loss that Cas A’s progenitor star underwent prior to its explosion.




Figure 1. Angular momentum for 3 different mechanisms coupling the angular momenta between burning layers. The Genec models (GZ0.006, GZ0.002) use no magnetic coupling between burning layers correspond to a 32 M⊙ star with metallicities set to 0.006 and 0.002. Metallicity only mildly affects the spin rates for the 32 M⊙ star. The Kepler models (KM15, KM20) using a mild Taylor-Spruit dynamo that reproduces pulsar spin velocities. These models use 15 and 20 M⊙ solar metallicity progenitors. The primary differences in the angular momentum profiles between the Genec and Kepler models lies in this burning layer coupling. The Kepler models are evolved to collapse. The MESA models (M0.006, M0.0004) were run with strong magnetic coupling between burning layers for a 40 M⊙ star. This coupling highlights the strong dependence of the spin on the prescription for magnetic coupling.
Figure 5. Black Hole dimensionless spin parameter versus of orbital separation (in Roche radii) for 4 models assuming He and CO stars for 25, 32 M⊙ zero-age main-sequence mass progenitors. Spin rates above 0.4 are expected for models that produce reasonable disks.
Figure 6. Available rotational energy for neutron stars in stellar collapse as a function of zero-age main sequence mass. Because the neutron star only exists in its hot, extended state for the BH-forming, progenitor masses above 25 M⊙ can only have weak magnetars.
Figure 7. Disk accretion rate as a function of time for tight-binary (fR = 1.0) systems with zero age main-sequence masses ranging from 20-75 M⊙. The more common, 20 M⊙ progenitors continue to accrete for over 1000 s.
Figure 8. Top panel: Accretion rate versus time after the formation of the disk for a 30 M⊙ zero-age main-sequence progenitor as a function of time after the formation of the disk. Disk formation occurs later for wider binaries. Middle panel: Corresponding black hole spin rate as a function of this time. Bottom Panel: GRB jet power as a function of time using Equation 19.

+1

Explaining Non-Merger Gamma-Ray Bursts and Broad-Lined Supernovae with Close Binary Progenitors with Black Hole Central Engine
  • Preprint
  • File available

October 2024

·

5 Reads

For over 25 years, the origin of long-duration gamma-ray bursts (lGRBs) has been linked to the collapse of rotating massive stars. However, we have yet to pinpoint the stellar progenitor powering these transients. Moreover, the dominant engine powering the explosions remains open to debate. Observations of both lGRBs, supernovae associated with these GRBs, such as broad-line (BL) stripped-envelope (type Ic) supernovae (hereafter, Ic-BL) supernovae (SNe) and perhaps superluminous SNe, fast blue optical transients, and fast x-ray transients, may provide clues to both engines and progenitors. In this paper, we conduct a detailed study of the tight-binary formation scenario for lGRBs, comparing this scenario to other leading progenitor models. Combining this progenitor scenario with different lGRB engines, we can compare to existing data and make predictions for future observational tests. We find that the combination of the tight-binary progenitor scenario with the black hole accretion disk (BHAD) engine can explain lGRBs, low-luminosity GRBs, ultra-long GRBs, and Ic-BL. We discuss the various progenitor properties required for these different subclasses and note such systems would be future gravitational wave merger sources. We show that the current literature on other progenitor-engine scenarios cannot explain all of these transient classes with a single origin, motivating additional work. We find that the tight-binary progenitor with a magnetar engine is excluded by existing observations. The observations can be used to constrain the properties of stellar evolution, the nature of the GRB and the associated SN engines in lGRBs and Ic-BL. We discuss the future observations needed to constrain our understanding of these rare, but powerful, explosions.

Download



Figure 7. Multi-wavelength view on the GM ring in position P2 (see Figure 1) showing the NIRCam F162M (PSF FWHM: 0.055 ′′ ), F356W (PSF FWHM: 0.116 ′′ ) and F444W (PSF FWHM: 0.145 ′′ ) images (top row), NIRCam+MIRI RGB image (F444W, F1000W, F1800W with PSF FWHMs of 0.145 ′′ , 0.328 ′′ and 0.591 ′′ , respectively) and MRS MRS line flux maps for [Ne ii] 12.81 µm (PSF FWHM: ∼ 0.529 ′′ ) and [Ne iii] 15.56 µm (PSF FWHM: ∼ 0.619 ′′ ) lines (middle row) and MRS [Fe ii] 17.94 µm (PSF FWHM: ∼ 0.698 ′′ ) and NIRSpec Br α 4.05 µm (PSF FWHM: ∼ 0.15 ′′ ) line flux maps for the near v rad = 0 km s −1 velocity component and a multi-color RGB image comparing the dust with the line emission (bottom row). The images are at their native resolution; the FWHM of the PSF has been indicated between parentheses here for guidance. Each of the cut-outs has the same 5 arcsec × 5 arcsec field of view. The green or black circle with radius of 0.8 arcsec overlaid on the continuum and line emission maps serves to guide the eye when comparing dust continuum, synchrotron and line emission in this region.
Figure 8. Left: The locations of dense CSM clumps, often called quasi-stationary flocculi (QSFs), as traced by Hα emission. The figure was adapted from Fesen (2001) to show a green outline of the location of the GM, which nicely fits in the middle of the formerly identified dense CSM knots. Right: Multi-color MIRI image (blue: F1000W, green: F1130W, red: F2550W) with contours indicating the locations of these dense QSFs as identified by Koo et al. (2018).
Figure 10. A comparison between holes and rings observed with JWST (left panels) and analogous structures predicted by hydrodynamic simulations (right panels; Orlando et al. 2022) and identified in the white squared regions in Figure 9.
Figure 11. Spectral mapping of the GM ring region in position P2 (see Figure 1) near rest-frame velocities. Maps are shown of the line flux (left column), line velocity (middle column) and FWHM line width (right column) for low-velocity components of the [Ne ii] 12.81 µm (first row), [Ne iii] 15.56 µm (second row), [Fe ii] 17.94 µm (third row) and Br α (fourth row) lines. The green circle roughly outlines the position of the ring in MIRI dust continuum maps, with the same circle overlaid on the GM images shown in Figure 7.
The Green Monster hiding in front of Cas A: JWST reveals a dense and dusty circumstellar structure pockmarked by ejecta interactions

October 2024

·

22 Reads

JWST observations of the young Galactic supernova remnant Cassiopeia A revealed an unexpected structure seen as a green emission feature in colored composite MIRI F1130W and F1280W images - hence dubbed the Green Monster - that stretches across the central parts of the remnant in projection. Combining the kinematic information from NIRSpec and MIRI MRS with the multi-wavelength imaging from NIRCam and MIRI, we associate the Green Monster with circumstellar material that was lost during an asymmetric mass-loss phase. MIRI images are dominated by dust emission but its spectra show emission lines from Ne, H and Fe with low radial velocities indicative of a CSM nature. An X-ray analysis of this feature in a companion paper (Vink et al. 2024) supports its CSM nature and detects significant blue shifting, thereby placing the Green Monster on the near side, in front of the Cas A SN remnant. The most striking features of the Green Monster are dozens of almost perfectly circular 1" - 3" sized holes, most likely created by interaction between high-velocity SN ejecta material and the CSM. Further investigation is needed to understand whether these holes were formed by small 8000-10500 km/s N-rich ejecta knots that penetrated and advanced out ahead of the remnant's 5000 - 6000 km/s outer blastwave, or by narrow ejecta fingers that protrude into the forward-shocked CSM. The detection of the Green Monster provides further evidence of the highly asymmetric mass-loss that Cas A's progenitor star underwent prior to explosion.


Occurrence of gravitational collapse in the accreting neutron stars of binary-driven hypernovae

September 2024

·

13 Reads

The binary-driven hypernova (BdHN) model proposes long gamma-ray bursts (GRBs) originate in binaries composed of a carbon-oxygen (CO) star and a neutron star (NS) companion. The CO core collapse generates a newborn NS and a supernova that triggers the GRB by accreting onto the NSs, rapidly transferring mass and angular momentum to them. We perform three-dimensional, smoothed-particle-hydrodynamics simulations of BdHNe using up-to-date NS nuclear equations of state (EOS), with and without hyperons, and calculate the structure evolution in full general relativity. We assess the binary parameters leading either NS to the critical mass for gravitational collapse into a black hole (BH) and its occurrence time, tcolt_\textrm{col}. We include a non-zero angular momentum of the NSs and find that tcolt_\textrm{col} ranges from a few tens of seconds to hours for decreasing NS initial angular momentum values. BdHNe I are the most compact (about five minutes orbital period), promptly form a BH and release 1052\gtrsim 10^{52} erg. They form NS-BH binaries with tens of kyr merger timescale by gravitational-wave emission. BdHNe II and III do not form BHs, release 1050\sim 10^{50}-105210^{52} erg and 1050\lesssim 10^{50} erg. They form NS-NS with a wider range of merger timescales. In some compact BdHNe II, either NS can become supramassive, i.e., above the critical mass of a non-rotating NS. Magnetic braking by a 101310^{13} G field can delay BH formation, leading to BH-BH or NS-BH of tens of kyr merger timescale.


A spectroscopic analysis code for spatially resolved x-ray absorption data from the COAX platform

September 2024

·

12 Reads

Sophisticated tools such as computer vision techniques in combination with 1D lineout type analyses have been used in automating the analysis of spectral data for high energy density (HED) plasmas. Standardized automation can solve the problems posed by the complexity of HED spectra and the quantity of data. We present a spectroscopic code written for automated and streamlined analysis of spatially resolved x-ray absorption data from the COAX platform on Omega-60. COAX uses radiographs and spectroscopic diagnostics to provide shock position and density information. We also obtain the more novel spectral-derived spatial profile of the supersonic radiation flow into a low-density foam. Considerable effort has been spent modernizing our previous spectroscopic analysis method, including the development of new tools characterized by a faster runtime and minimal user input to reduce bias and a testing suite for verifying the accuracy of the various functions within the code. The new code analyzes our spectroscopic images in 1–2 min, with added uncertainty and confidence.


Citations (55)


... A more thorough construction of synthetic nebular models with careful consideration of hydrogen ejecta distributions and velocities to reproduce the unique line profiles of SN 2023ufx is beyond the scope of the current paper and will be part of future work. There has been growing evidence that most CCSNe are inherently asymmetric in their explosion mechanisms (e.g., Janka et al. 2007;Maeda et al. 2008;Lopez et al. 2009;Chornock et al. 2010;Wongwathanarat et al. 2013;Grefenstette et al. 2014Grefenstette et al. , 2017Larsson et al. 2023;Milisavljevic et al. 2024;van Baal et al. 2024;Shrestha et al. 2024b). The distribution of radioactive 44 Ti, synthesized in the core-collapse that formed the supernova remnant Cassiopeia A was revealed to be from a highly asymmetric bipolar explosion (Grefenstette et al. 2014(Grefenstette et al. , 2017. ...

Reference:

Luminous Type II Short-Plateau SN 2023ufx: Asymmetric Explosion of a Partially-Stripped Massive Progenitor
A JWST Survey of the Supernova Remnant Cassiopeia A

The Astrophysical Journal Letters

... The detection rate of galactic supernovae (SN) has been calculated to be about 1.63 ± 0.46 per century [68], and with SN1987A the last detected supernova in our galaxy, the next galactic SN event is already heading our way with detection imminent. With veteran GW detectors and neutrino detectors lying in wait, together with a host of electro-magnetic (EM) detectors, the next detectable CCSNe is expected to be the most significant event in multi-messenger astronomy (MMA) [69,70]. The event is expected to provide a wealth of information on the composition and the EoS of NSs and on the CCSNe evolution itself. ...

Multimessenger Diagnostics of the Engine behind Core-collapse Supernovae

The Astrophysical Journal

... They are physically interesting and important probes of both the explosion and nature of progenitor stars (see, e.g., the reviews of Vink 2012 andDubner &Giacani 2015). For example, estimates of ejecta masses, velocities, and energies constrain the progenitor and explosions (e.g., Temim et al. 2022;Braun et al. 2023). They are laboratories for shock physics (e.g., Raymond et al. 2020aRaymond et al. , 2020b. ...

Progenitors and explosion properties of supernova remnants hosting central compact objects: II. A global systematic study with a comparison to nucleosynthesis models
  • Citing Article
  • August 2023

Monthly Notices of the Royal Astronomical Society

... The Gamma-ray burst GRB 221009A, named because it was the first GRB detected on October 9, 2022, likely indicated the birth of a black hole. Fermi's Large Area Telescope (Fermi-LAT) recorded gamma-ray photons for more than 10 hours from the burst [70]. Photons with energies of over 100 MeV were detected. ...

Fermi-GBM Discovery of GRB 221009A: An Extraordinarily Bright GRB from Onset to Afterglow

The Astrophysical Journal Letters

... * These authors contributed equally † Neil Gehrels Fellow Many collaborations such as the Zwicky Transient Facility (ZTF; Bellm et al. 2019a;Graham et al. 2019;Dekany et al. 2020 Hu et al. 2023), KM3Net 2 and VINROUGE 3 undertook targeted efforts during IGWN's third observing run (O3) to identify any associated electromagnetic counterparts. However, despite extensive tiling and galaxy-targeted searches, no EM counterparts were found (Coughlin et al. 2019;Goldstein et al. 2019;Andreoni et al. 2020aAndreoni et al. , 2019Antier et al. 2020;Vieira et al. 2020;Kilpatrick et al. 2021;Alexander et al. 2021;de Wet et al. 2021;Thakur et al. 2021;Tucker et al. 2022;Rastinejad et al. 2022;Dobie et al. 2022). Amongst the 6 BNS and 9 NSBH merger candidates announced in O3, only 1 BNS merger (GW190425) and 4 NSBH merger candidates (GW190426, GW190814, GW200105, and GW200115) passed the False Alarm Rate (FAR) threshold for inclusion in the Gravitational Wave Transient Catalog (GWTC-3; ) as highconfidence signals, rendering the remainder of the candidates as subthreshold astrophysical events or noise sources. ...

Erratum: A search for optical and near-infrared counterparts of the compact binary merger GW190814
  • Citing Article
  • January 2021

Monthly Notices of the Royal Astronomical Society

... ic physics in the neutrino sector are also being investigated (S. Ando 2003; G. L. Fogli et al. 2004;A. de Gouvêa et al. 2020A. de Gouvêa et al. , 2022Z. Tabrizi & S. Horiuchi 2021;P. Iváñez-Ballesteros & M. C. Volpe 2023). Furthermore, the DSNB flux may be related to other cosmic background radiation such as MeV γ-rays (L. E. Strigari et al. 2005;S. Anandagoda et al. 2023) and nonthermal high-energy neutrinos (Y. Ashida 2024). Incidentally, neutrinos emitted from accretion disks formed around SNe may contribute to cosmic background radiation (T. S. H. Schilbach et al. 2019;Y.-F. Wei et al. 2024). The basics of DSNB are covered in several previous reviews (S. Ando & K. Sato 2004;J. F. Beacom 2010;C. Lunar ...

Cosmic Supernova Neutrino and Gamma-Ray Backgrounds in the MeV Regime

The Astrophysical Journal

... Surrogate modeling with GP was used to lower the cost of candidate period evaluation as an optimization in the pulsar period search process [19]. Pulsar models have also been used to test new gravity theories [20] or to model the light curve of pulsar mergers [21]. ...

Surrogate light curve models for kilonovae with comprehensive wind ejecta outflows and parameter estimation for AT2017gfo

Physical Review Research

... For instance, assuming B = 10 11 G, M NS = 0.9M ⊙ , R NS = 10 6 cm, and I = 10 45 g cm 2 , Eq. (6) tells that at t = 4.5 kyr, the NS rotation frequency will be ≈ 531 Hz. This is an upper limit for the rotation frequency since additional effects could also contribute to the NS spin-down, e.g., the gravitational waves in early evolution (see, e.g., Ostriker & Gunn 1969;Ferrari & Ruffini 1969;Ruffini & Wheeler 1971;Chandrasekhar 1970;Miller 1974), multipolar magnetic field components (see, e.g., Tiengo et al. 2013;Mastrano et al. 2013;Pétri 2015;Rodríguez Castillo et al. 2016;Pons & Viganò 2019;Rueda et al. 2022;Wang et al. 2023), or the magnetic field could have been larger at earlier times at then be buried by fallback accretion (see, e.g., Ho 2011;Fraija et al. 2018). Thus, the rotation effect on the NS structure at these times is negligible, so a slow-rotation or non-rotation approximation may suffice to estimate the mass and radius (see, e.g., Cipolletta et al. 2015). ...

GRB 171205A: Hypernova and Newborn Neutron Star

The Astrophysical Journal

... The current and funded suite of gamma-ray telescopes, including Fermi (Atwood et al. 2009), Integral (Ubertini et al. 2003) and COSI (Tomsick et al. 2019), are all capable of these transient observations and will detect nearby supernova events, but not out to this distance. A number of mission concepts have been proposed to increase the distance of detection of radioactive decay emission from supernovae: AMEGO-X (Caputo et al. 2022), LOX (Miller et al. 2019;Miller et al. 2023), and ASCENT (Kislat et al. 2023). Similarly, detectors such as the UltraSAT (Ben-Ami et al. 2022) and CASTOR (Ménesguen et al. 2017) satellites are designed to increase the number of shock-breakout detections in the UV. ...

ASCENT: a balloon-borne hard x-ray imaging spectroscopy telescope using transition edge sensor microcalorimeter detectors
  • Citing Article
  • February 2023

Journal of Astronomical Telescopes Instruments and Systems

... This results in a mixing of the hot and cold layers in the star, known as convection. The convective engine provides the means to convert potential energy released in the collapse into explosion energy in the form of a supernovae (Fryer et al. 2012;Fryer et al. 2021). The commonly accepted supernova explosion mechanism is neutrino driven, where some of the neutrinos emitted during the core collapse are reabsorbed, powering an explosion (Janka et al. 2007;Marek & Janka 2009;Janka 2012Janka , 2017. ...

Understanding Convection in the Core-Collapse Supernovae Engine
  • Citing Article
  • October 2021

Astronomy Reports