Tea Temim’s research while affiliated with Princeton University and other places

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Publications (141)


JWST and Ground-based Observations of the Type Iax Supernovae SN 2024pxl and SN 2024vjm: Evidence for Weak Deflagration Explosions
  • Preprint
  • File available

May 2025

Lindsey A. Kwok

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Saurabh W. Jha

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We present panchromatic optical + near-infrared (NIR) + mid-infrared (MIR) observations of the intermediate-luminosity Type Iax supernova (SN Iax) 2024pxl and the extremely low-luminosity SN Iax 2024vjm. JWST observations provide unprecedented MIR spectroscopy of SN Iax, spanning from +11 to +42 days past maximum light. We detect forbidden emission lines in the MIR at these early times while the optical and NIR are dominated by permitted lines with an absorption component. Panchromatic spectra at early times can thus simultaneously show nebular and photospheric lines, probing both inner and outer layers of the ejecta. We identify spectral lines not seen before in SN Iax, including [Mg II] 4.76 μ\mum, [Mg II] 9.71 μ\mum, [Ne II] 12.81 μ\mum, and isolated O I 2.76 μ\mum that traces unburned material. Forbidden emission lines of all species are centrally peaked with similar kinematic distributions, indicating that the ejecta are well mixed in both SN 2024pxl and SN 2024vjm, a hallmark of pure deflagration explosion models. Radiative transfer modeling of SN 2024pxl shows good agreement with a weak deflagration of a near-Chandrasekhar-mass white dwarf, but additional IR flux is needed to match the observations, potentially attributable to a surviving remnant. We favor a weak deflagration origin for SN 2024vjm because of its panchromatic spectral similarity to SN 2024pxl, despite the large difference in luminosity. However, our comparison weak deflagration models are all too luminous and rapidly fading compared to SN 2024vjm; future modeling should push to even weaker explosions and include the contribution of a bound remnant. Our observations demonstrate the diagnostic power of panchromatic spectroscopy for unveiling explosion physics in thermonuclear supernovae.

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Figure 7. The results of the MCMC analysis of the mocassin models for the Spitzer/WISE 2009-10 epoch on the left and for the JWST 2023 epoch on the right. The parameters are silicate fraction, heating source luminosity, dust mass, grain size, and distance. Vertical dashed lines indicate 1σ confidence intervals. Blue crosshairs in the left panel indicate the values found by R. Wesson et al. (2023) from an analysis of a much smaller grid of models than used here.
Figure 8. Best-fit mocassin models for the new JWST spectrum; see Table 1.
Best mocassin Models
Very Late-Time JWST and Keck Spectra of the Oxygen-Rich Supernova 1995N

May 2025

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2 Reads

We present new {\it JWST}/MIRI MRS and Keck spectra of SN 1995N obtained in 2022--2023, more than 10,000 days after the supernova (SN) explosion. These spectra are among the latest direct detections of a core-collapse SN, both through emission lines in the optical and thermal continuum from infrared dust emission. The new infrared data show that dust heating from radiation produced by the ejecta interacting with circumstellar matter is still present, but greatly reduced from when SN 1995N was observed by the {\it Spitzer Space Telescope} and {\it WISE} in 2009/2010 and 2018, when the dust mass was estimated to be 0.4 M(Sun). New radiative-transfer modeling suggests that the dust mass and grain size may have increased between 2010 and 2023. The new data can alternatively be well fit with a dust mass of 0.4 M(Sun) and a much reduced heating source luminosity. The new late-time spectra show unusually strong oxygen forbidden lines, stronger than the H-alpha emission. This indicates that SN 1995N may have exploded as a stripped-envelope SN which then interacted with a massive H-rich circumstellar shell, changing it from intrinsically Type Ib/c to Type IIn. The late-time spectrum results when the reverse shock begins to excite the inner H-poor, O-rich ejecta. This change in the spectrum is rarely seen, but marks the start of the transition from SN to SN remnant.


Figure 5. Left and Middle: Spitzer IRAC images of SN 2005af taken on February 2006 and August 2008 (Szalai & Vinkó 2013) Right: JWST/MIRI image of SN 2005af taken in July 2023 in filter band F1500W.
Figure 6. JWST/MIRI composite image of SN 2005af, taken on 2023-07-21, which is 6767 days post-explosion. The white tick marks show the position of the supernova.
The results of the Spitzer/IRAC photometry of SN 2005af. Numbers marked with italic show the photometric values previously published in Szalai & Vinkó (2013).
Two Decades of Dust Evolution in SN 2005af through JWST, Spitzer, and Chemical Modeling

April 2025

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6 Reads

The evolution of dust in core-collapse supernovae (SNe), in general, is poorly constrained owing to a lack of infrared observations after a few years from explosion. Most theories of dust formation in SNe heavily rely only on SN 1987A. In the last two years, the James Webb Space Telescope (JWST) has enabled us to probe the dust evolution in decades-old SNe, such as SN 2004et, SN 2005ip, and SN 1980K. In this paper, we present two decades of dust evolution in SN 2005af, combining early-time infrared observations with Spitzer Space Telescope and recent detections by JWST. We have used a chemical kinetic model of dust synthesis in SN ejecta to develop a template of dust evolution in SN 2005af. Moreover, using this approach, for the first time, we have separately quantified the dust formed in the pre-explosion wind that survived after the explosion, and the dust formed in the metal-rich SN ejecta post-explosion. We report that in SN 2005af, predominantly carbon-rich dust is formed in the ejecta, where the total mass of ejecta dust is about 0.02-0.03 Msun, while in the circumstellar medium the amount of surviving oxygen-rich dust is 0.001-0.004 Msun.


Large Cold Dust Reservoir Revealed in Transitional SN Ib 2014C by James Webb Space Telescope Mid-Infrared Spectroscopy

April 2025

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3 Reads

Supernova (SN) 2014C is a rare transitional event that exploded as a hydrogen-poor, helium-rich Type Ib SN and subsequently interacted with a hydrogen-rich circumstellar medium (CSM) a few months post explosion. This unique interacting object provides an opportunity to probe the mass-loss history of a stripped-envelope SN progenitor. Using the James Webb Space Telescope (JWST), we observed SN 2014C with the Mid-InfraRed Instrument Medium Resolution Spectrometer at 3477 days post explosion (rest frame), and the Near-InfraRed Spectrograph Integral Field Unit at 3568 days post explosion, covering 1.7 to 25 μ\mum. The bolometric luminosity indicates that the SN is still interacting with the same CSM that was observed with the Spitzer Space Telescope 40--1920 days post explosion. JWST spectra and near-contemporaneous optical and near-infrared spectra show strong [Ne II] 12.831 μ\mum, He 1.083 μ\mum, Hα\alpha, and forbidden oxygen ([O I] λ\lambdaλ\lambda6300, 6364, [O II] λ\lambdaλ\lambda7319, 7330, and [O III] λ\lambdaλ\lambda4959, 5007) emission lines with asymmetric profiles, suggesting a highly asymmetric CSM. The mid-IR continuum can be explained by ~0.036 MM_\odot of carbonaceous dust at ~300 K and ~0.043 MM_\odot of silicate dust at \sim200 K. The observed dust mass has increased tenfold since the last Spitzer observation 4 yr ago, with evidence suggesting that new grains have condensed in the cold dense shell between the forward and reverse shocks. This dust mass places SN 2014C among the dustiest SNe in the mid-IR and supports the emerging observational trend that SN explosions produce enough dust to explain the observed dust mass at high redshifts.


JWST/MIRI detects the dusty SN1993J about 30 years after explosion

April 2025

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5 Reads

Astronomy and Astrophysics

Core-collapse supernovae (CCSNe) have long been considered to contribute significantly to the cosmic dust budget. Newly-formed dust in the SN ejecta cools quickly and is therefore detectable at mid-infrared (mid-IR) wavelengths. However, before the era of the James Webb Space Telescope (JWST), direct observational evidence for dust condensation was found in only a handful of nearby CCSNe, and dust masses (∼ 10^ generally limited to <5< 5 yr and to >500> 500 K temperatures) have been two to three orders of magnitude smaller than theoretical predictions and dust amounts found by far-IR/submillimeter observations of Galactic SN remnants and in the very nearby SN 1987A. As recently demonstrated, the combined angular resolution and mid-IR sensitivity of JWST finally allow hidden cool (∼ 100--200 K) dust reservoirs in extragalactic SNe beyond SN 1987A to be revealed. Our team received JWST/MIRI time for studying a larger sample of CCSNe to fill the currently existing gap in their dust formation histories. The first observed target of this program was the well-known Type IIb SN 1993J that appeared in M81. We generated its spectral energy distribution (SED) from the current JWST/MIRI F770W, F1000W, F1500W, and F2100W fluxes. We fit single- and two-component silicate and carbonaceous dust models to the SED in order to determine the dust parameters. We find that SN 1993J still contains a significant amount (∼ 0.01 of dust ∼ 30 yr after explosion. Comparing our results to those from the analysis of earlier Spitzer Space Telescope data, we observed a similar amount of dust as was detected ∼ 15--20 yr ago, but at a lower temperature (noting that the modeling results of the earlier Spitzer SEDs have strong limitations). We also found residual background emission near the SN site (after point-spread-function subtraction on the JWST/MIRI images) that may plausibly be attributed to an IR echo from more distant interstellar dust grains heated by the SN shock-breakout luminosity or ongoing star formation in the local environment.


Fig. 5. 3D volumetric renderings of the shocked circumstellar shell (green, first two columns) and ejecta distributions (red, right column). The green renderings in the first two columns show results from models W15-IIb-sh-HD+dec-hr (top row) and W15-IIb-sh-MHD+dec-rl-hr (bottom row) at two evolutionary stages: approximately 100 years before the current age of Cas A (left column) and at the present age of Cas A (center column). The red volumetric rendering in the rightmost column illustrates the corresponding ejecta distributions at the present age of Cas A.
Fig. 8. Left panels: cross-sections of the density distribution for selected ejecta species in a plane aligned with the LoS, corresponding to the region shown in Fig. 6. The color bar in each panel represents the density in log scale. The light blue contour outlines the material of the shocked shell. Right panels: corresponding 3D volumetric renderings of the same quantities as seen from Earth's vantage point. The color bar on the right of each panel shows the column density in linear scale. The vertical dashed line marks the location of the cross-sections shown in the left panels. The results are derived from the W15-IIb-sh-MHD+dec-rl-hr model at the evolutionary stage corresponding to Cas A.
Fig. 10. Examples of hole and ring structures observed in the GM with JWST (De Looze et al. 2024; first row) compared to those produced in run W15-IIb-sh-MHD+dec-rl-hr at two different epochs: 258 years (second row) and 367 years (third row). The latter epoch corresponds approximately to the current age of Cas A. The bottom panels highlight the selected regions within the context of the entire shocked shell; the dashed box indicates the region analyzed in Figs. 6, 8, and 9. Hole dimensions are shown in arcseconds, assuming a distance of 3.4 kpc to Cas A.
Fig. A.1. Radiative losses from optically thin plasma as a function of electron temperature for selected values of ionization age, derived from SPEX version 3.08.01 (Kaastra et al. 1996, 2018). The upper left panel illustrates the cooling function assuming solar metal abundances from Lodders et al. (2009), highlighting the dependence on ionization time. The remaining panels show radiative losses for plasmas composed of the individual elements indicated in the labels.
Origin of holes and rings in the Green Monster of Cassiopeia A: Insights from 3D magnetohydrodynamic simulations

March 2025

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4 Reads

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1 Citation

Astronomy and Astrophysics

Context. The supernova remnant (SNR) Cassiopeia A (Cas A) offers a unique opportunity to study supernova (SN) explosion dynamics and remnant interactions with the circumstellar medium (CSM). Recent observations with the James Webb Space Telescope have unveiled an enigmatic structure within the remnant, termed “Green Monster” (GM), whose properties indicate a CSM origin. Aims. Our goal is to investigate the properties of the GM and uncover the origin of its intriguing pockmarked structure, characterized by nearly circular holes and rings. We aim to examine the role of small-scale ejecta structures in shaping these features through their interaction with a dense circumstellar shell. Methods. We adopted a neutrino-driven SN model to trace the evolution of its explosion from core collapse to the age of the Cas A remnant using high-resolution 3D magnetohydrodynamic simulations. Besides other processes, the simulations include self-consistent calculations of radiative losses, accounting for deviations from electron-proton temperature equilibration and ionization equilibrium, as well as the ejecta composition derived from the SN. Results. The observed GM morphology can be reproduced by the interaction of dense ejecta clumps and fingers with an asymmetric, forward-shocked circumstellar shell. The clumps and fingers form by hydrodynamic instabilities growing at the interface between SN ejecta and shocked CSM. Radiative cooling accounting for effects of non-equilibrium of ionization enhances the ejecta fragmentation, forming dense knots and thin filamentary structures that penetrate the shell, producing a network of holes and rings with properties similar to those observed. Conclusions. The origin of the holes and rings in the GM can be attributed to the interaction of ejecta with a shocked circumstellar shell. By constraining the timing of this interaction and analyzing the properties of these structures, we provide a distinction of this scenario from an alternative hypothesis, which attributes these features to fast-moving ejecta knots penetrating the shell ahead of the forward shock.


Fig. 5. The green volumetric renderings in the first two columns represent the shocked circumstellar shell as derived from models W15-IIb-shHD+dec-hr (upper panels) and W15-IIb-sh-MHD+dec-rl-hr (lower panels) at two evolutionary stages: approximately 100 years before the age of Cas A (left column) and at the age of Cas A (center column). The red volumetric rendering in the last column illustrates the corresponding ejecta distributions at the age of Cas A.
Fig. 7. Normalized LoS velocity distribution of the shocked ejecta (black curve), shocked shell (orange curve), and the shocked ejecta filling the holes (blue curve) in the region shown in Fig. 6. The analysis is restricted to plasma with coordinates y < −1.5 pc, corresponding to the domain where the shocked shell interacts with the ejecta. The results are derived from the W15-IIb-sh-MHD+dec-rl-hr model at the evolutionary stage corresponding to Cas A.
Fig. 10. Examples of hole and ring structures observed in the GM with JWST (De Looze et al. 2024; first row) compared to those produced in run W15-IIb-sh-MHD+dec-rl-hr at two different epochs: 258 years (second row) and 367 years (third row). The latter epoch corresponds approximately to the current age of Cas A. The bottom panels highlight the selected regions within the context of the entire shocked shell; the dashed box indicates the region analyzed in Figs. 6, 8, and 9. Hole dimensions are shown in arcseconds, assuming a distance of 3.4 kpc to Cas A.
Origin of holes and rings in the Green Monster of Cassiopeia A: Insights from 3D magnetohydrodynamic simulations

March 2025

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10 Reads

[Abridged] Cassiopeia A (Cas A) provides a unique opportunity to study supernova (SN) dynamics and interactions with the circumstellar medium (CSM). Recent JWST observations revealed the "Green Monster" (GM), a structure with a likely CSM origin. We investigate its pockmarked morphology, characterized by circular holes and rings, by examining the role of small-scale ejecta structures interacting with a dense circumstellar shell. We adopted a neutrino-driven SN model to trace the evolution of its explosion from core collapse to the age of the Cas A remnant using high-resolution 3D magnetohydrodynamic simulations. Besides other processes, the simulations include self-consistent calculations of radiative losses, accounting for deviations from electron-proton temperature equilibration and ionization equilibrium, as well as the ejecta composition derived from the SN. The GM's morphology is reproduced by dense ejecta clumps and fingers interacting with an asymmetric, forward-shocked circumstellar shell. The clumps and fingers form by hydrodynamic instabilities growing at the interface between SN ejecta and shocked CSM. Radiative cooling accounting for effects of non-equilibrium of ionization enhances the ejecta fragmentation, forming dense knots and thin filamentary structures that penetrate the shell, producing a network of holes and rings with properties similar to those observed. The origin of the holes and rings in the GM can be attributed to the interaction of ejecta with a shocked circumstellar shell. By constraining the timing of this interaction and analyzing the properties of these structures, we provide a distinction of this scenario from an alternative hypothesis, which attributes these features to fast-moving ejecta knots penetrating the shell ahead of the forward shock.


JWST/MIRI detects the dusty SN1993J about 30 years after explosion

March 2025

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4 Reads

Core-collapse supernovae (CCSNe) have long been considered to contribute significantly to the cosmic dust budget. New dust cools quickly and is therefore detectable at mid-infrared (mid-IR) wavelengths. However, before the era of the James Webb Space Telescope (JWST), direct observational evidence for dust condensation was found in only a handful of nearby CCSNe, and dust masses (~102103M^{-2}-10^{-3} M_{\odot}, generally limited to <5 yr and to >500K temperatures) have been 2-3 orders of magnitude smaller than either theoretical predictions or dust amounts found by far-IR/submm observations of Galactic SN remnants and in the very nearby SN 1987A. The combined angular resolution and mid-IR sensitivity of JWST finally allow us to reveal hidden cool (~100-200K) dust reservoirs in extragalactic SNe beyond SN 1987A. Our team received JWST/MIRI time for studying a larger sample of CCSNe to fill the currently existing gap in their dust formation histories. The first observed target of this program is the well-known Type IIb SN~1993J appeared in M81. We generated its spectral energy distribution (SED) from the current JWST/MIRI F770W, F1000W, F1500W, and F2100W fluxes. We fit single- and two-component silicate and carbonaceous dust models to the SED. We found that SN 1993J still contains a significant amount (~0.01 MM_{\odot}) of dust ~30 yr after explosion. Comparing these results to those of the analysis of earlier {Spitzer Space Telescope data, we see a similar amount of dust now that was detected ~15-20 yr ago, but at a lower temperature. We also find residual background emission near the SN site (after point-spread-function subtraction on the JWST/MIRI images) that may plausibly be attributed to an IR echo from more distant interstellar dust grains heated by the SN shock-breakout luminosity or ongoing star formation in the local environment.


Filamentary ejecta network in Cassiopeia A reveals fingerprints of the supernova explosion mechanism

March 2025

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5 Reads

Astronomy and Astrophysics

Context . Recent observations with the James Webb Space Telescope (JWST) have revealed unprecedented details of an intricate filamentary structure of unshocked ejecta within the young supernova remnant (SNR) Cassiopeia A (Cas A), offering new insights into the mechanisms governing supernova (SN) explosions and the subsequent evolution of ejecta. Aims . We aim to investigate the origin and evolution of the newly discovered web-like network of ejecta filaments in Cas A. Our specific objectives are: (i) to characterize the three-dimensional (3D) structure and kinematics of the filamentary network and (ii) to identify the physical mechanisms responsible for its formation. Methods . We performed high-resolution, 3D hydrodynamic (HD) and magneto-hydrodynamic (MHD) simulations to model the evolution of a neutrino-driven SN from the explosion to its remnant with the age of 1000 years. The initial conditions, set shortly after the shock breakout at the stellar surface, are based on a 3D neutrino-driven SN model that closely matches the basic properties of Cas A. Results . We found that the magnetic field has little impact on the evolution of unshocked ejecta, so we focused most of the analysis on the HD simulations. A web-like network of ejecta filaments, with structures compatible with those observed by JWST (down to scales ≈0.01 pc), naturally forms during the SN explosion. The filaments result from the combined effects of processes occurring soon after the core collapse, including the expansion of neutrino-heated bubbles formed within the first second after the explosion, hydrodynamic instabilities triggered during the blast propagation through the stellar interior, and the Ni-bubble effect following the shock breakout. The interaction of the reverse shock with the ejecta progressively disrupts the filaments through the growth of hydrodynamic instabilities. By around 700 years, the filamentary network becomes unobservable. Conclusions . According to our models, the filaments observed by JWST in Cas A most likely preserve a “memory” of the early explosion conditions, reflecting the processes active during and immediately after the SN event. Notably, a filamentary network closely resembling that observed in Cas A is naturally produced by a neutrino-driven SN explosion.


Filamentary Ejecta Network in Cassiopeia~A Reveals Fingerprints of the Supernova Explosion Mechanism

February 2025

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3 Reads

[Abridged] Recent JWST observations have revealed an intricate filamentary network of unshocked ejecta in the young supernova remnant (SNR) Cassiopeia A (Cas A), offering new insights into supernova (SN) explosions and ejecta evolution. We investigate the origin and evolution of this structure by (i) characterizing its 3D morphology and kinematics and (ii) identifying the physical mechanisms driving its formation. Using high-resolution hydrodynamic (HD) and magneto-hydrodynamic (MHD) simulations, we model the evolution of a neutrino-driven SN from explosion to a remnant age of 1000 years. The initial conditions, set just after shock breakout, are based on a 3D neutrino-driven SN model matching Cas A's basic properties. We find that magnetic fields have little impact on unshocked ejecta evolution, so we focus on HD simulations. A web-like filamentary structure, consistent with JWST observations (down to 0.01\sim 0.01 pc), naturally forms during the explosion. These filaments arise from early post-collapse processes, including neutrino-heated bubble expansion, hydrodynamic instabilities during blast propagation, and the Ni-bubble effect after shock breakout. The reverse shock later disrupts the filaments via hydrodynamic instabilities, rendering them unobservable by 700\sim 700 years. Our models suggest that JWST-detected filaments in Cas A preserve a 'memory' of early explosion conditions, tracing processes active during and immediately after the SN event. Notably, a filamentary network akin to Cas A's emerges naturally from a neutrino-driven SN explosion.


Citations (48)


... This shell is included to account for significant asymmetries of the reverse shock, which cannot be explained by models assuming a spherically symmetric stellar wind from the progenitor (see Orlando et al. 2022). Recent JWST observations support the existence of this shell, having revealed evidence of a shocked, dense CSM structure around Cas A (the so-called "Green Monster"), consistent with past interactions between the remnant and a dense region of CSM material De Looze et al. 2024;Orlando et al. 2025). In the MHD simulations, the ambient magnetic field is represented by a "Parker spiral" configuration, resulting from the progenitor star's rotation and the corresponding outward flow of the stellar wind (Parker 1958;see Orlando et al. 2019a for further details). ...

Reference:

Filamentary ejecta network in Cassiopeia A reveals fingerprints of the supernova explosion mechanism
Origin of holes and rings in the Green Monster of Cassiopeia A: Insights from 3D magnetohydrodynamic simulations

Astronomy and Astrophysics

... However, SPHEREx operates at the longer wavelengths, where its impact is less severe. Moreover, the focus of our search on the Milky Way is not on regions with very high dust density, as, e.g., towards the Galactic Center [26]. The LMC, however, has regions with strong extinction, such as Doradus 30. ...

Sensitivity of JWST to eV-Scale Decaying Axion Dark Matter

Physical Review Letters

... Studies in the frame of the neutrino-driven mechanism argue for the successful shaping of different structures in CCSN remnants. For example, several papers address the shaping of Cassiopeia A, mainly the inner parts of the remnant (e.g., Orlando et al. 2021Orlando et al. , 2022Orlando et al. , 2025De Looze et al. 2024), but these papers do not address the point-symmetric morphology. ...

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

The Astrophysical Journal Letters

... An isolated (or otherwise wide-binary) magnetar interpretation remains viable with our lack of a counterpart detection. Indeed, spectra of such objects may appear as red, largely featureless, spectra (Hare et al. 2024), which are abundant in the vicinity of GLEAM-X J1627-52 (Fig. B1). Although the optical and NIR emission of magnetars is relatively poorly understood, largely due to the difficulty in observations (Mignani et al. 2009;Chrimes et al. 2022), they are known to be subtly variable on short timescales linked to their spin period (Dhillon et al. 2011), as well as more dramatically on longer timescales of years . ...

Probing the Spectrum of the Magnetar 4U 0142+61 with JWST

The Astrophysical Journal

... Observations of trace elements using the James Webb Space Telescope: JWST (J. Rho et al. 2024) and X-Ray Imaging and Spectroscopy Mission: XRISM (M. Audard et al. 2024) will be important for understanding these properties. ...

Shockingly Bright Warm Carbon Monoxide Molecular Features in the Supernova Remnant Cassiopeia A Revealed by JWST

The Astrophysical Journal Letters

... 0 51 erg for the SN explosion energy, and require the outer boundary R pwn to reach 2 pc at the present age, which corresponds to an ejecta mass of 9 M e consistent with R. Bandiera et al. (2020). Note that the explosion energy is an open question, and some studies suggest a lower energy of 10 50 erg (e.g., N. Smith 2013; G. Stockinger et al. 2020;T. Temim et al. 2024). Details of the parameters can be found in Table 1, and the result is shown in Figure 1. We obtain a magnetic field at the termination shock B 0 = 234 μG with the profile index β = 0.5 or ...

Dissecting the Crab Nebula with JWST: Pulsar Wind, Dusty Filaments, and Ni/Fe Abundance Constraints on the Explosion Mechanism

The Astrophysical Journal Letters

... Hwang et al. 2011;A. P. Huxor et al. 2013), and of a disk with an ongoing star formation activity (see, e.g., M. Tantalo et al. 2022, hereafter Paper I; L. Lenkić et al. 2024). Moreover, NGC 6822 is the closest dIrr to the MW after the MCs (d ∼ 510 ± 10 kpc; F. Fusco et al. 2014), and one of the most investigated dIrr galaxies, due its position in the sky (R.A.(J2000) = 19 44 58.56 ...

A JWST/MIRI and NIRCam Analysis of the Young Stellar Object Population in the Spitzer I Region of NGC 6822

The Astrophysical Journal

... Many of these are MIR-bright or foreground stars, including young stellar objects (YSOs; e.g. Jones et al. 2023;Nally et al. 2024). Some may be young clusters. ...

JWST MIRI and NIRCam unveil previously unseen infrared stellar populations in NGC 6822
  • Citing Article
  • May 2024

Monthly Notices of the Royal Astronomical Society

... Recent JWST observations in the MIR of both normal and peculiar SN Ia provide a new probe of progenitor and explosion models DerKacy et al. 2023;Chen et al. 2023;Siebert et al. 2024;Kwok et al. 2024;DerKacy et al. 2024;Ashall et al. 2024). Spectral lines in the nearinfrared (NIR) and MIR are more isolated, making the contribution from individual lines easier to distinguish (e.g., Pinto & Eastman 2000;Gerardy et al. 2007;Kwok et al. 2023). ...

Ground-based and JWST Observations of SN 2022pul. II. Evidence from Nebular Spectroscopy for a Violent Merger in a Peculiar Type Ia Supernova

The Astrophysical Journal