Jaegeun Park’s research while affiliated with Chungbuk National University and other places

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Publications (12)


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
  • Article
  • Full-text available

December 2024

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4 Reads

The Astrophysical Journal

Chanho Kim

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Jaegeun Park

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[...]

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Shuo Zhang

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.

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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.


Revisiting the Intrabinary Shock Model for Millisecond Pulsar Binaries: Radiative Losses and Long‐Term Variability

November 2024

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4 Reads

Astronomische Nachrichten

Spectrally hard x‐ray emission with double‐peak light curves (LCs) and orbitally modulated gamma rays have been observed in some millisecond pulsar binaries, phenomena attributed to intrabinary shocks (IBSs). While the existing IBS model by Sim et al. (2024; Astrophysical Journal 964(2):109) successfully explains these high‐energy features observed in three pulsar binaries, it neglects particle energy loss within the shock region. We refine this IBS model to incorporate radiative losses of x‐ray emitting electrons and positrons and verify that the losses have insignificant impact on the observed LCs and spectra of the three binaries. Applying our refined IBS model to the x‐ray bright pulsar binary PSR J1723‐2837, we predict that it can be detected by the Cherenkov Telescope Array. Additionally, we propose that the long‐term x‐ray variability observed in XSS J12270‐4859 and PSR J1723‐2837 is due to changes in the shape of their IBSs. Our modeling of the x‐ray variability suggests that these IBS shape changes may alter the extinction of the companion's optical emission, potentially explaining the simultaneous optical and x‐ray variability observed in XSS J12270‐4859. We present the model results and discuss their implications.


FIGURE 2 X-ray LC and broadband SED of J1723. (a) X-ray LC obtained with XMM-Newton in 2011 (Bogdanov et al., 2014). (b) Companion emission is represented by gray points. X-ray spectra were measured by XMM-Newton (black circles) and NuSTAR (blue triangles) (Kong et al., 2017), and Fermi-LAT data are shown as a gray band (Hui et al., 2014). Red curves in both panels represent our model computations (Table 1 ), while the sensitivity curves for AMEGO-X and CTA are as presented in Figure 1 .
Parameters used for models displayed in Figures 1 -3
Revisiting the Intrabinary Shock Model for Millisecond Pulsar Binaries: Radiative Losses and Long-Term Variability

Spectrally hard X-ray emission with double-peak light curves (LCs) and orbitally modulated gamma rays have been observed in some millisecond pulsar binaries, phenomena attributed to intrabinary shocks (IBSs). While the existing IBS model by Sim, An, and Wadiasingh (2024) successfully explains these high-energy features observed in three pulsar binaries, it neglects particle energy loss within the shock region. We refine this IBS model to incorporate radiative losses of X-ray emitting electrons and positrons, and verify that the losses have insignificant impact on the observed LCs and spectra of the three binaries. Applying our refined IBS model to the X-ray bright pulsar binary PSR J1723-2837, we predict that it can be detected by the Cherenkov Telescope Array. Additionally, we propose that the long-term X-ray variability observed in XSS J12270-4859 and PSR J1723-2837 is due to changes in the shape of their IBSs. Our modeling of the X-ray variability suggests that these IBS shape changes may alter the extinction of the companion's optical emission, potentially explaining the simultaneous optical and X-ray variability observed in XSS J12270-4859. We present the model results and discuss their implications.


What is the unknown “star” or “∼star” recorded in Korean historical books?

August 2024

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1 Read

Astronomische Nachrichten

This study discusses historical records of Korea that mention “stars” possibly related to astronomical transient events. We selected 19 such records and scrutinized them by cross‐checking with records of other countries to identify those events. Ten events were identified as comets based on their described motions and tails. We further confirmed this by comparing them with records from other countries. Five events were classified as meteors based on descriptions of their movements, sizes, and shapes. We speculate that two recordings about “big stars” (大星) are typographical errors for “Mars” (火星), as the descriptions of these big stars seem to be consistent with the properties of the latter. This leaves two unidentified events, and we search lists of astronomical transients for their counterparts. Our work emphasizes the uncertainties and challenges caused by the limited information in the historical records while exploring the usefulness of historical records to enhance the understanding of astrophysical transient events.


Figure 4. (Left) X-ray spectra of J1849 measured with XMM-Newton (black), NICER (purple), and NuSTAR (red and blue) and the best-fit logpar model (solid curves). The pulsar spectra were measured in the on-pulse interval by subtracting the off-pulse background (i.e., on−off) and averaged over a spin cycle. (Middle) PL fit of the on−off spectra of J1849. (Right) The PWN spectra measured with Chandra (yellow) and NuSTAR (red and blue) and the best-fit PL model. The bottom panels show the fit residuals.
Pulsar Timing Parameters
Spectral Analysis Results
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

December 2023

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35 Reads

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5 Citations

The Astrophysical Journal

We report on the X-ray emission properties of the pulsar PSR J1849−0001 and its wind nebula (PWN), as measured by Chandra, XMM-Newton, NICER, Swift, and NuSTAR. In the X-ray data, we detected the 38 ms pulsations of the pulsar up to ∼60 keV with high significance. Additionally, we found that the pulsar's on-pulse spectral energy distribution displays significant curvature, peaking at ≈60 keV. Comparing the phase-averaged and on-pulse spectra of the pulsar, we found that the pulsar's off-pulse emission exhibits a spectral shape that is very similar to its on-pulse emission. This characterization of the off-pulse emission enabled us to measure the >10 keV spectrum of the faint and extended PWN using NuSTAR's off-pulse data. We measured both the X-ray spectrum and the radial profiles of the PWN’s brightness and photon index, and we combined these X-ray measurements with published TeV results. We then employed a multizone emission scenario to model the broadband data. The results of the modeling suggest that the magnetic field within the PWN is relatively low (≈7 μ G) and that electrons are accelerated to energies ≳400 TeV within this PWN. The electrons responsible for the TeV emission outside the X-ray PWN may propagate to ∼30 pc from the pulsar in ∼10 kyr.


The high energy X-ray probe (HEX-P): Galactic PeVatrons, star clusters, superbubbles, microquasar jets, and gamma-ray binaries

December 2023

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11 Reads

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3 Citations

Frontiers in Astronomy and Space Sciences

HEX-P is a probe-class mission concept that will combine high spatial resolution X-ray imaging ( < 1 0 ″ FWHM) and broad spectral coverage (0.2–80 keV) with an effective area far superior to current facilities (including XMM-Newton and NuSTAR) to enable revolutionary new insights into a variety of important astrophysical problems. With the recent discoveries of over 40 ultra-high-energy gamma-ray sources (detected above 100 TeV) and neutrino emission in the Galactic Plane, we have entered a new era of multi-messenger astrophysics facing the exciting reality of Galactic PeVatrons. In the next decade, as more Galactic PeVatrons and TeV gamma-ray sources are expected to be discovered, the identification of their acceleration and emission mechanisms will be the most pressing issue in both particle and high-energy astrophysics. In this paper, along with its companion papers, we will present that HEX-P is uniquely suited to address important problems in various cosmic-ray accelerators, including Galactic PeVatrons, through investigating synchrotron X-ray emission of TeV–PeV electrons produced by both leptonic and hadronic processes. For Galactic PeVatron candidates and other TeV gamma-ray sources, HEX-P can fill in a large gap in the spectral-energy distributions (SEDs) of many objects observed in radio, soft X-rays, and gamma rays, constraining the maximum energies to which electrons can be accelerated, with implications for the nature of the Galactic PeVatrons and their contributions to the spectrum of Galactic cosmic rays beyond the knee at ∼ 3 PeV. In particular, X-ray observation with HEX-P and TeV observation with CTAO will provide the most powerful multi-messenger diagnostics to identify Galactic PeVatrons and explore a variety of astrophysical shock mechanisms. We present simulations of each class of Galactic TeV–PeV sources, demonstrating the power of both the imaging and spectral capabilities of HEX-P to advance our knowledge of Galactic cosmic-ray accelerators. In addition, we discuss HEX-P’s unique and complementary roles to upcoming gamma-ray and neutrino observatories in the 2030s.


A Broadband X-Ray Study of the Rabbit Pulsar Wind Nebula Powered by PSR J1418-6058

March 2023

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73 Reads

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9 Citations

The Astrophysical Journal

We report on broadband X-ray properties of the Rabbit pulsar wind nebula (PWN) associated with the pulsar PSR J1418−6058 using archival Chandra and XMM-Newton data, as well as a new NuSTAR observation. NuSTAR data above 10 keV allowed us to detect the 110 ms spin period of the pulsar, characterize its hard X-ray pulse profile, and resolve hard X-ray emission from the PWN after removing contamination from the pulsar and other overlapping point sources. The extended PWN was detected up to ∼20 keV and is described well by a power-law model with a photon index Γ ≈ 2. The PWN shape does not vary significantly with energy, and its X-ray spectrum shows no clear evidence of softening away from the pulsar. We modeled the spatial profile of X-ray spectra and broadband spectral energy distribution in the radio to TeV band to infer the physical properties of the PWN. We found that a model with low magnetic field strength ( B ∼ 10 μ G) and efficient diffusion ( D ∼ 10 ²⁷ cm ² s ⁻¹ ) fits the PWN data well. The extended hard X-ray and TeV emission, associated respectively with synchrotron radiation and inverse Compton scattering by relativistic electrons, suggest that particles are accelerated to very high energies (≳500 TeV), indicating that the Rabbit PWN is a Galactic PeVatron candidate.


Figure 2. The 2-7 keV Chandra images of the K3 PWN on various spatial scales (a-c) and a SUMSS 843 MHz image (d). The images are smoothed and the scales are adjusted for better legibility. The point-source-removed and exposure-corrected Chandra images are constructed following a CIAO science thread. The position of J1420 is denoted by a green cross. (a) Chandra image on a 40″ × 40″ scale. In addition to the two knots denoted in cyan, a faint jet (not visible in this panel) and a torus are marked. (b) Chandra image on a ¢ ´ ¢ 2 2 scale. The torus and the jet structures are shown in white and cyan ellipses, respectively. (c) Chandra image on a ¢ ´ ¢ 16 16 scale. A long northern tail region is denoted by a yellow ellipse and two short tails are marked. Regions of the Fermi-LAT (0° . 123; radius of a disk model) and H.E.S.S. (0° . 08; 1σ width of a Gaussian model) counterparts are displayed in cyan and white circles, respectively. (d) SUMSS 843 MHz image (Mauch et al. 2003). The image was downloaded from the Skyview webpage and truncated to match the X-ray emission region in panel (c). Note also that a box region in the lower right corner is excised because it contains a bright unrelated point source. The pulsar, northern X-ray tail, and Fermi-LAT and H.E.S.S. regions are overlaid for comparison.
Figure 3. Background-subtracted NuSTAR images (a and b) and radial profiles (c) in the 3-7 keV and 7-20 keV bands. (a and b) NuSTAR images in the 3-7 keV (a) and 7-20 keV bands (b). The images are smoothed and normalized to 1 at the maximum counts, and = ¢ R 2.5 circles are shown for reference. The image scales are adjusted for legibility. (c) 3-7 keV (black) and 7-20 keV (red) radial profiles of surface brightness (counts per area) are presented in the top panel. The green line is the radial profile of the PSF (pulsar), and the black and red dotted lines are background profiles in the low-and high-energy bands, respectively. Radial Gaussian functions that describe the PWN profiles in the low-and high-energy bands are shown in cyan and blue dotted lines, respectively. The summed models are presented in the cyan and blue dashed lines for the low-and high-energy profiles, respectively. Hardness ratios, defined by the high-energy to low-energy brightness ratio, are displayed in the bottom panel, and the red line is a linear fit to the hardness ratios.
Figure 4. Chandra (black) and NuSTAR (red and green) spectra of J1420 (empty circles) and the K3 PWN (crosses). The NuSTAR spectra of the pulsar were generated in the on-pulse phases by subtracting the off-pulse background and were averaged over the spin cycle. Best-fit models are presented as solid lines.
Figure 5. Broadband SED, radial profiles of X-ray photon index and brightness measured for the K3 PWN, and an optimized multizone emission model. (a) Spatially integrated broadband SED (Section 3.1) data and the optimized model. The radio points are the K3 excess (pink; Roberts et al. 1999) and the shell emission (purple; Van Etten & Romani 2010); we take these as the lower and upper limit, respectively, as was done by Van Etten & Romani (2010). The X-ray points are our measurements of the PWN emission within the = ¢ R 2.5 region, and the blue and green points show >20 GeV Fermi-LAT data (Fermi-LAT Collaboration et al. 2022) and the H.E.S.S. measurements taken from Aharonian et al. (2006), respectively. The curves are model-computed emission components: green for the synchrotron, red and blue for the ICS from IR and CMB seeds, and blue solid for the summed model. (b) Model-computed particle distributions in the inner (r < 100″; red) and the outer (100″ < r < 150″; blue) regions, and their sum (black), (c and d) radial profiles of X-ray photon index (c) and brightness (d). In panel (c), we also show Suzaku measurements (Kishishita et al. 2012) in blue for reference.
Parameters for the Multizone SED Model
X-Ray Studies of the Pulsar PSR J1420–6048 and Its TeV Pulsar Wind Nebula in the Kookaburra Region

March 2023

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726 Reads

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5 Citations

The Astrophysical Journal

We present a detailed analysis of broadband X-ray observations of the pulsar PSR J1420−6048 and its wind nebula (PWN) in the Kookaburra region with Chandra, XMM-Newton, and NuSTAR. Using the archival XMM-Newton and new NuSTAR data, we detected 68 ms pulsations of the pulsar and characterized its X-ray pulse profile, which exhibits a sharp spike and a broad bump separated by ∼0.5 in phase. A high-resolution Chandra image revealed a complex morphology of the PWN: a torus-jet structure, a few knots around the torus, one long (∼7′) and two short tails extending in the northwest direction, and a bright diffuse emission region to the south. Spatially integrated Chandra and NuSTAR spectra of the PWN out to 2.′5 are well-described by a power-law model with a photon index Γ ≈ 2. A spatially resolved spectroscopic study, as well as NuSTAR radial profiles of the 3–7 keV and 7–20 keV brightness, showed a hint of spectral softening with increasing distance from the pulsar. A multiwavelength spectral energy distribution (SED) of the source was then obtained by supplementing our X-ray measurements with published radio, Fermi-LAT, and H.E.S.S. data. The SED and radial variations of the X-ray spectrum were fit with a leptonic multizone emission model. Our detailed study of the PWN may be suggestive of (1) particle transport dominated by advection, (2) a low magnetic-field strength ( B ∼ 5 μ G), and (3) electron acceleration to ∼PeV energies.


A broadband X-ray study of the Rabbit pulsar wind nebula powered by PSR J1418-6058

February 2023

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3 Reads

We report on broadband X-ray properties of the Rabbit pulsar wind nebula (PWN) associated with the pulsar PSR J1418-6058 using archival Chandra and XMM-Newton data, and a new NuSTAR observation. NuSTAR data above 10 keV allowed us to detect the 110-ms spin period of the pulsar, characterize its hard X-ray pulse profile, and resolve hard X-ray emission from the PWN after removing contamination from the pulsar and other overlapping point sources. The extended PWN was detected up to \sim20 keV and is well described by a power-law model with a photon index Γ\Gamma\approx2. The PWN shape does not vary significantly with energy, and its X-ray spectrum shows no clear evidence of softening away from the pulsar. We modeled the spatial profile of X-ray spectra and broadband spectral energy distribution in the radio to TeV band to infer the physical properties of the PWN. We found that a model with low magnetic field strength (B10B\sim 10 μ\muG) and efficient diffusion (D1027D\sim 10^{27} cm2^2 s1^{-1}) fits the PWN data well. The extended hard X-ray and TeV emission, associated respectively with synchrotron radiation and inverse Compton scattering by relativistic electrons, suggests that particles are accelerated to very high energies (500\gtrsim500 TeV), indicating that the Rabbit PWN is a Galactic PeVatron candidate.


Citations (4)


... If it is a a radio galaxy, then it will be difficult to explain the observed UHE emission considering the CMB absorbtion. On the other hand microquasar is a possible PeVatron candidate (Abaroa et al., 2024;Mori et al., 2023). Presence of molecular cloud (MC) in this region hints towards a hadronic emission scenario, and protons from microquasar also can interact with the MCs to produce UHE gamma-rays. ...

Reference:

uGMRT observation of the unidentified PeVatron candidate LHAASO J2108+5157
The high energy X-ray probe (HEX-P): Galactic PeVatrons, star clusters, superbubbles, microquasar jets, and gamma-ray binaries

Frontiers in Astronomy and Space Sciences

... ± 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

... In Scenario 1, the S1 size of R 1 » ¢ (∼4 pc for an assumed distance of 13 kpc scaled by N H ) may indicate a middle-aged PWN. Such a PWN could exhibit a TeV flux comparable to its X-ray flux (e.g., J. Park et al. 2023), which is an order of magnitude lower than the measured gamma-ray flux of the SNR shell (peaking at ∼100 GeV). IC emission from the electrons emitting synchrotron photons at ∼10 keV would appear at TeV energies, as observed in other middle-aged PWNe. ...

A Broadband X-Ray Study of the Rabbit Pulsar Wind Nebula Powered by PSR J1418-6058

The Astrophysical Journal

... The degeneracy can be broken to a certain extent if we can constrain some of the parameters; e.g., measuring the expansion speed of the PWN can help determine V 0 and α V (Equation (2)), and B 0 can be well constrained if u CMB + u IR are known. Nonetheless, the values presented in Table 3, which are similar to the values inferred for Table 3 Parameters for the SED Model in Figure 5 Parameter Symbol Value other PWNe (e.g., Park et al. 2023b), can account for the measurements. ...

X-Ray Studies of the Pulsar PSR J1420–6048 and Its TeV Pulsar Wind Nebula in the Kookaburra Region

The Astrophysical Journal