Samar Safi-Harb’s research while affiliated with University of Manitoba and other places

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Publications (191)


Figure 1. The summed XMM-EPIC MOS1 and MOS2 rate map, showing the LHAASO regions (white dashed lines-LHAASO J0341 is the source described in Z. Cao et al. 2021, while the others are the KM2A and WCDA sources from Z. Cao et al. 2024), the primary source region (green line), the selected background region (yellow dashed line), the nearby 4FGL 95% uncertainty ellipse (red line), and the 11 detected secondary point sources (numbered in cyan). The lime insert shows the primary source in greater detail, along with the fitted absorbed power-law slopes in each annular analysis region.
Figure 2. The average flux density along four tracks extended in the cardinal directions (east-red solid; west-blue dashed; north-lime dotted-dashed; and south-cyan dotted) from the primary source center, along with the EPIC-MOS PSF for a ¢ 10 offset and 3 keV energy (black). The insert shows the regions used in the extraction of these count rates. The uncertainties (black for east, cyan for south) assume Poisson statistics and are displayed every ¢ 0.36.
Figure 3. 0.3-8.0 keV XMM-Newton spectrum of the primary source, fitted with an absorbed power law. An instrumental feature of the EPIC-MOS detector at 1.7 keV is masked out for our fitting.
Figure 4. 0.5-500 GeV Fermi-LAT TS map after removing 4FGL J0340.4 +5302 from the gamma-ray background model. We include the 1LHAASO J0343+5254u WCDA and KM2A regions (white), the 95% error ellipse of 4FGL J0340.4+5302 (blue ellipse), and the extent of the XMMNewton primary source (small blue circle). The red points are two X-ray point sources described in upcoming works. NRO CO line contours are shown for velocity ranges of [−20, −4] (yellow) and [−4, +10] (green) km s −1 .
Figure 5. Detections (green dots) and constraining upper limits (black arrows) for our PWN candidate, along with the MCMC best-fit leptonic model (blue). The faint red curve is the leptonic IC spectrum, but with κ = 1 photon fields fixed at solar-neighborhood values. The components of the gamma-ray emission are included as thin lines of the same color for each model (SSC is not visible on this scale).

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Discovery of a Pulsar Wind Nebula Candidate Associated with the Galactic PeVatron 1LHAASO J0343+5254u
  • Article
  • Full-text available

April 2025

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6 Reads

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1 Citation

The Astrophysical Journal

Stephen DiKerby

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Shuo Zhang

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[...]

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Jooyun Woo

The astronomical origins of the most energetic galactic cosmic rays and gamma rays are still uncertain. X-ray follow-up of candidate “PeVatrons”—systems producing cosmic rays with energies exceeding 1 PeV—can constrain their spatial origin, identify likely counterparts, and test particle emission models. Using ∼120 ks of XMM-Newton observations, we report the discovery of a candidate pulsar wind nebula, a possible counterpart for the LHAASO PeVatron J0343+5254u. This extended source has a power-law X-ray spectrum with spectral index Γ X = 1.9—softer at greater distance from the center—and asymmetric spatial extension out to ≈ 2 ′ . We conduct leptonic modeling of the X-ray and gamma-ray radiation from this complex system, showing that a fully leptonic model with elevated IR photon fields can explain the multiwavelength emission from this source, similar to other very high-energy pulsar wind nebulas; excess gamma-ray emissivity not explained by a leptonic model may be due to hadronic interactions in nearby molecular cloud regions, which might also produce detectable astroparticle flux.

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Figure 8. The 12 CO(J = 1-0) map with V LSR = −40 to 10 km s −1 , overlaid with the gamma-ray emission of the first LHAASO catalogs (cyan circles), a known counterpart of PSR J0343+5312 (the green small circle), 4FGL J0340.4+5302 (the magenta circle), ROSAT sources from the 2RXS catalog (green crosses), and a newly detected XMM-Newton source (the green circle; S. DiKerby et al. 2025). Clouds A-E are marked in white.
LHAASO Sources in the J0341 Region
Radio Continuum Flux in J0341
Detection of Molecular Clouds in the PeVatron Candidate Source LHAASO J0341+5258 by the Nobeyama 45-m Radio Telescope

April 2025

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6 Reads

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1 Citation

The Astrophysical Journal

We report a new CO observation survey of LHAASO J0341+5258, using the Nobeyama Radio Observatory 45-m telescope. LHAASO J0341+5258 is one of the unidentified ultra-high-energy (UHE; E > 100 TeV) gamma-ray sources detected by LHAASO. Our CO observations were conducted in 2024 February and March, with a total observation time of 36 hr, covering the LHAASO source (∼0 . ° 3–0 . ° 5 in radius) and its surrounding area (1° × 1 . ° 5). Within the LHAASO source extent, we identified five compact (<2 pc) molecular clouds at nearby distances (<1–4 kpc). These clouds can serve as proton–proton collision targets, producing hadronic gamma rays via neutral pion decays. Based on the hydrogen densities (700–5000 cm ⁻³ ) estimated from our CO observations and archived H i data from the Dominion Radio Astrophysical Observatory survey, we derive the total proton energy of W p ( E > 1 TeV) ∼ 10 ⁴⁵ erg to account for the gamma-ray flux. One of the molecular clouds appears to be likely associated with an asymptotic giant branch (AGB) star with an extended CO tail, which may indicate some particle acceleration activities. However, the estimated maximum particle energy below 100 TeV makes the AGB-like star unlikely to be a PeVatron site. We conclude that the UHE emission observed in LHAASO J0341+5258 could be due to hadronic interactions between the newly discovered molecular clouds and TeV–PeV protons originating from a distant SNR or due to leptonic emission from a pulsar wind nebula candidate, which is reported in our companion X-ray observation paper.


Detection of molecular clouds in the PeVatron candidate source LHAASO J0341+5258 by the Nobeyama 45-m radio telescope

February 2025

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14 Reads

We report a new CO observation survey of LHAASO J0341+5258 using the Nobeyama Radio Observatory (NRO) 45-m telescope. LHAASO J0341+5258 is one of the unidentified ultra-high-energy (UHE; E >>100 TeV) gamma-ray sources detected by LHAASO. Our CO observations were conducted in February and March 2024, with a total observation time of 36 hours, covering the LHAASO source (\sim0.3-0.5 degrees in radius) and its surrounding area (1×\times1.5 degrees). Within the LHAASO source extent, we identified five compact (<< 2 pc) molecular clouds at nearby distances (<< 1-4 kpc). These clouds can serve as proton-proton collision targets, producing hadronic gamma rays via neutral pion decays. Based on the hydrogen densities (700-5000 cm3^{-3}) estimated from our CO observations and archived HI data from the DRAO survey, we derived the total proton energy of WpW_p (E >> 1 TeV) \sim 1045^{45} erg to account for the gamma-ray flux. One of the molecular clouds appears to be likely associated with an asymptotic giant branch (AGB) star with an extended CO tail, which may indicate some particle acceleration activities. However, the estimated maximum particle energy below 100 TeV makes the AGB-like star unlikely to be a PeVatron site. We conclude that the UHE emission observed in LHAASO J0341+5258 could be due to hadronic interactions between the newly discovered molecular clouds and TeV-PeV protons originating from a distant SNR or due to leptonic emission from a pulsar wind nebula candidate, which is reported in our companion X-ray observation paper (DiKerby et al. 2025).


Discovery of a Pulsar Wind Nebula Candidate Associated with the Galactic PeVatron 1LHAASO J0343+5254u

February 2025

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3 Reads

The astronomical origin of the most energetic galactic cosmic rays and gamma rays is still uncertain. X-ray followup of candidate "PeVatrons", systems producing cosmic rays with energies exceeding 1 PeV, can constrain their spatial origin, identify likely counterparts, and test particle emission models. Using 120 ks of XMM-Newton observations, we report the discovery of a candidate pulsar wind nebula, a possible counterpart for the LHAASO PeVatron J0343+5254u. This extended source has a power law X-ray spectrum with spectral index of 1.9 - softer at greater distance from the center - and asymmetric spatial extension out to 2'. We conduct leptonic modeling of the X-ray and gamma ray radiation from this complex system, showing that a fully leptonic model with elevated IR photon fields can explain the multiwavelength emission from this source, similar to other VHE pulsar wind nebulae; excess gamma ray emissivity not explained by a leptonic model may be due to hadronic interactions in nearby molecular cloud regions, which might also produce detectable astroparticle flux.


Constraining Disk-to-Corona Power Transfer Fraction, Soft X-ray Excess Origin, and Black Hole Spin Population of Type-1 AGN across Mass Scales

January 2025

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4 Reads

Understanding the nature of the accretion disk, its interplay with the X-ray corona, and assessing black hole spin demographics are some open challenges in astrophysics. In this work, we examine the predictions of the standard α\alpha-disk model, origin of the soft X-ray excess, and measure the black hole spin parameter by applying the updated high-density disk reflection model to the XMM-Newton/NuSTAR broadband (0.3-78 keV) X-ray spectra of a sample of Type-1 AGN. Our Bayesian analysis confirms that the high-density relativistic reflection model with a broken power-law emissivity profile can simultaneously fit the soft X-ray excess, broad iron K line, and Compton hump for \sim70% of the sample, while an additional warm Comptonization model is still required to describe the observed soft X-ray excess for the remaining sources. Our first-ever calculation of the disk-to-corona power transfer fraction reveals that the fraction of power released from the accretion disk into the hot corona can have diverse values, the sample median of which is 0.70.4+0.20.7_{-0.4}^{+0.2}. We find that the transferred power from the accretion disk can potentially soften the X-ray spectrum of the hot corona. The median values of the hot coronal temperature and optical depth for the sample are estimated to be 6311+2363_{-11}^{+23} keV and 0.850.27+0.120.85_{-0.27}^{+0.12}, respectively. Finally, through joint XMM-Newton+NuSTAR relativistic reflection spectroscopy, we systematically constrain the black hole spin parameter across the broad range of black hole masses, log(MBH/M)5.59.0\log(M_{\rm BH}/M_{\odot}) \sim 5.5-9.0, and increase the available spin measurements in the AGN population by \sim20%.


Figure 2. The 15-50 keV flux maps of Cas A for 2013 (a) and 2023 (b), and a difference map between 2013 and 2023 (c). For (a) and (b), background-subtracted count maps were divided by vignetting-corrected exposure maps and then iteratively deconvolved using the on-axis NuSTAR point-spread function (PSF; see Section 2.4). The two images were scaled equally to ensure direct comparison. Part (c) was generated by subtracting (b) from (a). All three images were smoothed with a Gaussian kernel (σ = 3  .5 = 1.5 pixel). The L-band radio contour (V. Domček et al. 2021) is overlaid in black. A circle with diameter 14″ is overlaid in the bottomright corner of each image to indicate the size of the NuSTAR PSF (14″ FWHM). Fading over the entire remnant is clearly noticeable. Most prominently, the brightest knots inside the remnant (in the middle and in the west) dimmed significantly.
Figure 4. Synchrotron spectra for 2013 and 2023 calculated with the temporal synchrotron cooling and injection model. The black (red) solid line is the synchrotron spectrum calculated using the best-fit parameters in Table 2 for 2013 (2023). The red dashed line is the synchrotron spectrum of the preexisting electrons for 2023, and the red dotted line shows the contribution of the injected electrons to the synchrotron spectrum for 2023. The NuSTAR spectrum from this work and the radio spectrum from A. S. Trotter et al. (2017) are overlaid. The error bars of the data points are for 1σ uncertainties in this figure and all the figures hereafter.
List of Archival and New Observations
Best-fit Parameters for the Synchrotron Cooling and Injection Model
Spectrum and Location of Ongoing Extreme Particle Acceleration in Cassiopeia A

January 2025

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11 Reads

The Astrophysical Journal

Young supernova remnants (SNRs) are believed to be the origin of energetic cosmic rays (CRs) below the “knee” of their spectrum at ∼3 PeV (10 ¹⁵ eV). Nevertheless, the precise location, duration, and operation of CR acceleration in young SNRs are open questions. Here, we report on multiepoch X-ray observations of Cassiopeia A (Cas A), a 350 yr old SNR, in the 15–50 keV band that probes the most energetic CR electrons. The observed X-ray flux decrease (15% ± 1% over 10 yr), contrary to the expected >90% decrease based on previous radio, X-ray, and gamma-ray observations, provides unambiguous evidence for CR electron acceleration operating in Cas A. A temporal model for the radio and X-ray data accounting for electron cooling and continuous injection finds that the freshly injected electron spectrum is significantly harder (exponential cutoff power-law index q = 2.15), and its cutoff energy is much higher ( E cut = 36 TeV), than the relic electron spectrum ( q = 2.44 ± 0.03, E cut = 4 ± 1 TeV). Both electron spectra are naturally explained by the recently developed modified nonlinear diffusive shock acceleration (mNLDSA) mechanism. The CR protons producing the observed gamma rays are likely accelerated at the same location by the same mechanism as the injected electrons. The Cas A observations and spectral modeling represent the first time radio, X-ray, gamma-ray, and CR spectra have been self-consistently tied to a specific acceleration mechanism—mNLDSA—in a young SNR.


Figure 2. (a) A 1.2-7.0 keV XRISM Xtend image with the regions for the spectral analysis. (b) Same with a course binning. (c) The image after the particlebackground subtraction and vignetting correction and with the HAWC gamma-ray contours (>1 TeV; R. Alfaro et al. 2024) and the Xtend field of view (FoV) overlaid. The 68% containment circle of the point-spread function at 6.4 keV is shown as a reference. The images are shown on the Equatorial coordinates (J2000).
Detection of Extended X-Ray Emission around the PeVatron Microquasar V4641 Sgr with XRISM

January 2025

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15 Reads

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1 Citation

The Astrophysical Journal Letters

A recent report on the detection of very-high-energy gamma rays from V4641 Sagittarii (V4641 Sgr) up to ≈0.8 PeV has made it the second confirmed “PeVatron” microquasar. Here we report on the observation of V4641 Sgr with X-Ray Imaging and Spectroscopy Mission (XRISM) in 2024 September. Thanks to the large field of view and low background, the CCD imager Xtend successfully detected for the first time X-ray extended emission around V4641 Sgr with a significance of ≳4.5 σ and >10 σ based on our imaging and spectral analysis, respectively. The spatial extent is estimated to have a radius of 7′ ± 3′ (13 ± 5 pc at a distance of 6.2 kpc) assuming a Gaussian-like radial distribution, which suggests that the particle acceleration site is within ~10 pc of the microquasar. If the X-ray morphology traces the diffusion of accelerated electrons, this spatial extent can be explained by either an enhanced magnetic field (∼80 μ G) or a suppressed diffusion coefficient (∼10 ²⁷ cm ² s ⁻¹ at 100 TeV). The integrated X-ray flux, (4–6) × 10 ⁻¹² erg s ⁻¹ cm ⁻² (2–10 keV), would require a magnetic field strength higher than the Galactic mean (≳8 μ G) if the diffuse X-ray emission originates from synchrotron radiation and the gamma-ray emission is predominantly hadronic. If the X-rays are of thermal origin, the measured extension, temperature, and plasma density can be explained by a jet with a luminosity of ∼2 × 10 ³⁹ erg s ⁻¹ , which is comparable to the Eddington luminosity of this system.


Figure 2. (a) 3-20 keV NuSTAR FPMA (left) and FPMB (right) images made with the 2023 observation. While J1714 appears to be heavily contaminated by stray light in the FPMB image, it was detected outside the contamination in FPMA. We smoothed and logarithmically scaled the images to enhance legibility. (b) and (c) Result of our pulsation search (b) and backgroundsubtracted 1.6-5 keV pulse profile (c) of J1714 measured using the 2023 NuSTAR data.
-Ray Data Used in This Study
Results of Joint Fits of the XMM-Newton and NuSTAR Spectra
Parameters for the NTB Model in Figure 4
Investigation of the Nonthermal X-Ray Emission from the Supernova Remnant CTB 37B Hosting the Magnetar CXOU J171405.7-381031

December 2024

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4 Reads

The Astrophysical Journal

We present a detailed X-ray investigation of a region (S1) exhibiting nonthermal X-ray emission within the supernova remnant (SNR) CTB 37B hosting the magnetar CXOU J171405.7−381031. Previous analyses modeled this emission with a power law (PL), inferring various values for the photon index (Γ) and absorbing column density ( N H ). Based on these, S1 was suggested to be an SNR shell, a background pulsar wind nebula, or an interaction region between the SNR and a molecular cloud. Our analysis of a larger data set favors a steepening (broken or curved PL) spectrum over a straight PL, with the best-fit broken power-law (BPL) parameters of Γ = 1.23 ± 0.23 and 2.24 ± 0.16 below and above a break at 5.57 ± 0.52 keV, respectively. However, a simple PL or srcut model cannot be definitively ruled out. For the BPL model, the inferred N H = (4.08 ± 0.72) × 10 ²² cm ⁻² towards S1 is consistent with that of the SNR, suggesting a physical association. The BPL-inferred spectral break ΔΓ ≈ 1 and hard Γ can be naturally explained by a nonthermal bremsstrahlung (NTB) model. We present an evolutionary NTB model that reproduces the observed spectrum, which indicates the presence of subrelativistic electrons within S1. However, alternate explanations for S1, an unrelated PWN or the SNR shock with unusually efficient acceleration, cannot be ruled out. We discuss these explanations and their implications for gamma-ray emission from CTB 37B and describe future observations that could settle the origin of S1.


Figure 1. MAXI/GSC light curves of V4641 Sgr showing the bursting activity in September 2024, obtained from http: //maxi.riken.jp/star data/J1819-254/J1819-254.html. The observation period with XRISM is indicated with the blue transparent region.
Figure 3. (a) A 1.2-7.0 keV XRISM Xtend image with the radial-profile extraction region centered at V4641 Sgr (green). (b) Extracted radial profile with the models for the point spread function at 6.4 keV, sky background, particle background, and extended emission modeled with a Gaussian function. The transparent regions indicate the systematic uncertainty ranges (see text for details).
Detection of extended X-ray emission around the PeVatron microquasar V4641 Sgr with XRISM

December 2024

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25 Reads

A recent report on the detection of very-high-energy gamma rays from V4641 Sagittarii (V4641 Sgr) up to ~0.8 peta-electronvolt has made it the second confirmed "PeVatron" microquasar. Here we report on the observation of V4641 Sgr with X-Ray Imaging and Spectroscopy Mission (XRISM) in September 2024. Thanks to the large field of view and low background, the CCD imager Xtend successfully detected for the first time X-ray extended emission around V4641 Sgr with a significance of > 4.5 sigma and > 10 sigma based on our imaging and spectral analysis, respectively. The spatial extent is estimated to have a radius of 7±37 \pm 3 arcmin (13±513 \pm 5 pc at a distance of 6.2 kpc) assuming a Gaussian-like radial distribution, which suggests that the particle acceleration site is within ~10 pc of the microquasar. If the X-ray morphology traces the diffusion of accelerated electrons, this spatial extent can be explained by either an enhanced magnetic field (~80 uG) or a suppressed diffusion coefficient (~102710^{27} cm2^2 s1^{-1} at 100 TeV). The integrated X-ray flux, (4-6)×1012\times 10^{-12} erg s1^{-1} cm2^{-2} (2-10 keV), would require a magnetic field strength higher than the galactic mean (> 8 uG) if the diffuse X-ray emission originates from synchrotron radiation and the gamma-ray emission is predominantly hadronic. If the X-rays are of thermal origin, the measured extension, temperature, and plasma density can be explained by a jet with a luminosity of ~2×10392\times 10^{39} erg s1^{-1}, which is comparable to the Eddington luminosity of this system.


Figure 1. A composite image of combined SUMSS (843 MHz;
Figure 2. (a) 3-20 keV NuSTAR FPMA (left) and FPMB (right) images made with the 2023 observation. While J1714 appears to be heavily contaminated by stray light in the FPMB image, it was detected outside the contamination in FPMA. We smoothed and logarithmically scaled the images to enhance legibility. (b and c) Result of our pulsation search (b) and backgroundsubtracted 1.6-5 keV pulse profile (c) of J1714 measured using the 2023 NuSTAR data. P =3.852450(5) s on MJD 60233 (Figure 2 (b) and (c)). Unfortunately, owing to limited statistics resulting from a large off-axis angle and elevated background due to stray light, we were unable to confirm the previously reported phase reversal of the pulse profile at higher energies (>6 keV; Gotthelf et al. 2019) with the new data. However, the obtained P value aligns with the trend presented in Gotthelf et al. (2019); by comparing our result with the previous Chandra measurement on MJD 54856, we estimated an average ˙ P of 6 × 10 −11 s s −1 , falling within the previously reported range of (5-7)×10 −11 s s −1 .
X-ray data used in this study
Results of joint fits of the XMM-Newton and NuSTAR spectra
Investigation of the non-thermal X-ray emission from the supernova remnant CTB 37B hosting the magnetar CXOU J171405.7-381031

November 2024

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5 Reads

We present a detailed X-ray investigation of a region (S1) exhibiting non-thermal X-ray emission within the supernova remnant (SNR) CTB 37B hosting the magnetar CXOU J171405.7-381031. Previous analyses modeled this emission with a power law (PL), inferring various values for the photon index (Γ\Gamma) and absorbing column density (NHN_{\rm H}). Based on these, S1 was suggested to be the SNR shell, a background pulsar wind nebula (PWN), or an interaction region between the SNR and a molecular cloud. Our analysis of a larger dataset favors a steepening (broken or curved PL) spectrum over a straight PL, with the best-fit broken power-law (BPL) parameters of Γ=1.23±0.23\Gamma=1.23\pm0.23 and 2.24±0.162.24\pm0.16 below and above a break at 5.57±0.525.57\pm0.52 keV, respectively. However, a simple PL or srcut model cannot be definitively ruled out. For the BPL model, the inferred NH=(4.08±0.72)×1022 cm2N_{\rm H}=(4.08\pm0.72)\times 10^{22}\rm \ cm^{-2} towards S1 is consistent with that of the SNR, suggesting a physical association. The BPL-inferred spectral break ΔΓ1\Delta \Gamma \approx 1 and hard Γ\Gamma can be naturally explained by a non-thermal bremsstrahlung (NTB) model. We present an evolutionary NTB model that reproduces the observed spectrum, which indicates the presence of sub-relativistic electrons within S1. However, alternate explanations for S1, an unrelated PWN or the SNR shock with unusually efficient acceleration, cannot be ruled out. We discuss these explanations and their implications for gamma-ray emission from CTB 37B, and describe future observations that could settle the origin of S1.


Citations (42)


... We have been conducting observations of radio line emissions using the Nobeyama Radio Observatory (NRO) 45 m radio telescope, to search for associated molecular clouds in the 1LHAASO J0343+5254u region (N. Tsuji et al. 2025). Five molecular clouds are detected within the gamma-ray regions of the LHAASO sources; four have derived distances and n H in the range 0.3-1 kpc and 200-800 cm −3 , with the fifth having d = 4.0 ± 1.0 kpc and n H = 2 × 10 3 cm −3 (related to a nearby optical/IR asymptotic giant star). ...

Reference:

Discovery of a Pulsar Wind Nebula Candidate Associated with the Galactic PeVatron 1LHAASO J0343+5254u
Detection of Molecular Clouds in the PeVatron Candidate Source LHAASO J0341+5258 by the Nobeyama 45-m Radio Telescope

The Astrophysical Journal

... roughly 200 TeV, either in leptonic or hadronic. Although there are three ROSAT X-ray point-like sources within the gamma-ray extension, there is no known extended X-ray emission so far. As part of an approved AO-22 XMM-Newton Large Program, the J0341 region was observed in 2024 February (Figure 1), and an associated publication is in preparation (S. DiKerby et al. 2025). ...

Discovery of a Pulsar Wind Nebula Candidate Associated with the Galactic PeVatron 1LHAASO J0343+5254u

The Astrophysical Journal

... Ivezić et al. 2019) monitored over increasing baselines. Upcoming and proposed X-ray observatories-such as the Advanced X-ray Imaging Satellite (C. S. Reynolds et al. 2024), which will have ∼100× greater sensitivity than Swift and NICER, as well as faster slew and longer monitoring capabilities than XMM-Newton-will be crucial in extending our reach to a larger sample of QPEs at higher z and longer timescales. Systematic searches will yield valuable insights into the nature of these transient accretion events and help constrain astrophysical processes in galactic nuclei, including stellar dynamics and capture, accretion disk formation evolutions, and the rates and properties of extreme mass-ratio inspirals. ...

The Advanced X-ray Imaging Satellite (AXIS)
  • Citing Conference Paper
  • August 2024

... However, this model was also found to be insensitive during spectral fitting of X2 observation. Such a lower value of the N H was previously seen in other systems (Laha et al. 2014;Matzeu et al. 2020;Nandi et al. 2024;Madathil-Pottayil et al. 2024;Porquet et al. 2024). This indicates that no significant warm absorbing gas exists along our line of sight towards this AGN, thereby supporting its classification as a bare Seyfert 1 galaxy. ...

Accretion properties of a low-mass active galactic nucleus: UGC 6728
  • Citing Article
  • June 2024

Monthly Notices of the Royal Astronomical Society

... ration. Furthermore, in the hadronic scenario, the same proton-proton interactions produce charged pions, decaying into muons and secondary electrons and positrons. Thus, measuring the synchrotron radiation from these secondary electrons can be a strong indication for hadronic gamma rays, although it has not been detected yet (F. A. Aharonian 2013;N. Tsuji et al. 2024). ...

Search for Synchrotron Emission from Secondary Electrons of Proton–Proton Interactions in Galactic PeVatron Candidate HESS J1641–463

The Astrophysical Journal

... In addition, we take into account the molecular ionisation induced by low-energy (< 280 MeV) CRs. Two CR ionization rates are adopted: = 2.6 × 10 −17 s −1 typical of Galactic value (van der Tak & van Dishoeck 2000) and = 2.6 × 10 −15 s −1 for the gas ionized by SNR-accelerated CRs (e.g., Ceccarelli et al. 2011;Vaupré et al. 2014;Zhou et al. 2022;Tu et al. 2024b). The calculation results are shown in Figure 10. ...

Shock and Cosmic-Ray Chemistry Associated with the Supernova Remnant W28

The Astrophysical Journal

... ± 0.379) × 10 −15 cm −2 s −1 MeV −1 , and the energy scale E 0 is fixed to 20,000 MeV. Kim et al. (2024) To investigate the systematic errors in the local γ-ray Galactic background and the effective area, we altered the normalization of the diffuse background by ±5% and used the isotropic diffuse background version P8R3_SOURCE_V2 instead of P8R3_SOURCE_V3 (Acero et al. 2013). The spectral points we obtained are shown in Figure 3, and they are well connected to the TeV spectrum of HESS J1849-000 and ASγ. ...

X-Ray Characterization of the Pulsar PSR J1849−0001 and Its Wind Nebula G32.64+0.53 Associated with TeV Sources Detected by H.E.S.S., HAWC, Tibet ASγ, and LHAASO

The Astrophysical Journal

... 20 cm −2 for LF. Thus, Mrk 590 can essentially be classified as a 'bare' AGN, defined by Nandi et al. (2023) as sources with intrinsic column densities below 10 20 cm −2 . While these constraints only directly apply to measurements along our line-of-sight, we note a few other indications that the central engine of Mrk 590 may be gas poor. 1) Mrk 590 displays an unusually strong (for AGN) UV response to X-ray variability (Paper 1); this suggests unobscured sight-lines between the X-ray continuum and the reprocessor. ...

Survey of Bare Active Galactic Nuclei in the Local Universe (z < 0.2). I. On the Origin of Soft Excess

The Astrophysical Journal Supplement Series

... 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

... This size is similar to other X-ray PWNs related to teraelectronvolt emission regions, like those linked to G75.2+0.1 (J. Woo et al. 2023, having X-ray size » ¢ 1 ) and HAWC J1826-128 (D. A. Burgess et al. 2022, » ¢ 3 ), an indication that this new source may be a PWN like those objects. ...

Hard X-Ray Observation and Multiwavelength Study of the PeVatron Candidate Pulsar Wind Nebula “Dragonfly”

The Astrophysical Journal