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<title>Research Papers</title>
<link>http://localhost:8080/xmlui/handle/123456789/17</link>
<description/>
<pubDate>Mon, 20 Apr 2026 15:21:28 GMT</pubDate>
<dc:date>2026-04-20T15:21:28Z</dc:date>
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<title>Research Papers</title>
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<link>http://localhost:8080/xmlui/handle/123456789/17</link>
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<title>Very-high-frequency oscillations in the main  peak of a magnetar giant flare</title>
<link>http://localhost:8080/xmlui/handle/123456789/1660</link>
<description>Very-high-frequency oscillations in the main  peak of a magnetar giant flare
Castro-Tirado, A. J. et.al.; Pandey, S. B.
Magnetars are strongly magnetized, isolated neutron stars1–3&#13;
 with magnetic felds &#13;
up to around 1015 gauss, luminosities of approximately 1031–1036 ergs per second &#13;
and rotation periods of about 0.3–12.0 s. Very energetic giant fares from galactic &#13;
magnetars (peak luminosities of 1044–1047 ergs per second, lasting approximately 0.1 s) &#13;
have been detected in hard X-rays and soft γ-rays4&#13;
, and only one has been detected &#13;
from outside our galaxy5&#13;
. During such giant fares, quasi-periodic oscillations (QPOs) &#13;
with low (less than 150 hertz) and high (greater than 500 hertz) frequencies have been &#13;
observed6–9&#13;
, but their statistical signifcance has been questioned10. High-frequency &#13;
QPOs have been seen only during the tail phase of the fare9&#13;
. Here we report the &#13;
observation of two broad QPOs at approximately 2,132 hertz and 4,250 hertz in &#13;
the main peak of a giant γ-ray fare11 in the direction of the NGC 253 galaxy12–17, &#13;
disappearing after 3.5 milliseconds. The fare was detected on 15 April 2020 by the &#13;
Atmosphere–Space Interactions Monitor instrument18,19 aboard the International &#13;
Space Station, which was the only instrument that recorded the main burst phase &#13;
(0.8–3.2 milliseconds) in the full energy range (50 × 103&#13;
 to 40 × 106&#13;
 electronvolts) &#13;
without sufering from saturation efects such as deadtime and pile-up. Along with &#13;
sudden spectral variations, these extremely high-frequency oscillations in the burst &#13;
peak are a crucial component that will aid our understanding of magnetar giant fares
</description>
<pubDate>Wed, 01 Dec 2021 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://localhost:8080/xmlui/handle/123456789/1660</guid>
<dc:date>2021-12-01T00:00:00Z</dc:date>
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<item>
<title>Investigation of two coronal mass ejections from circular ribbon source region: Origin, Sun-Earth propagation and Geoeffectiveness</title>
<link>http://localhost:8080/xmlui/handle/123456789/1659</link>
<description>Investigation of two coronal mass ejections from circular ribbon source region: Origin, Sun-Earth propagation and Geoeffectiveness
Ibrahim, Syed ,et.al.; Uddin, Wahab
In this article, we compare the properties of two coronal mass ejections (CMEs) that show&#13;
similar source region characteristics but different evolutionary behaviors in the later phases. We discuss&#13;
the two events in terms of their near-Sun characteristics, interplanetary evolution and geoeffectiveness. We&#13;
carefully analyzed the initiation and propagation parameters of these events to establish the precise CME interplanetary CME (ICME) connection and their near-Earth consequences. The first event is associated&#13;
with poor geomagnetic storm disturbance index (Dst ≈-20 nT) while the second event is associated&#13;
with an intense geomagnetic storm of DST ≈-119 nT. The configuration of the sunspots in the active&#13;
regions and their evolution are observed by Helioseismic and Magnetic Imager (HMI). For source region&#13;
imaging, we rely on data obtained from Atmospheric Imaging Assembly (AIA) on board Solar Dynamics&#13;
Observatory (SDO) and Hα filtergrams from the Solar Tower Telescope at Aryabhatta Research Institute of&#13;
Observational Sciences (ARIES). For both the CMEs, flux rope eruptions from the source region triggered&#13;
flares of similar intensities (≈M1). At the solar source region of the eruptions, we observed a circular&#13;
ribbon flare (CRF) for both cases, suggesting fan-spine magnetic configuration in the active region corona.&#13;
The multi-channel SDO observations confirm that the eruptive flares and subsequent CMEs were intimately&#13;
related to the filament eruption. Within the Large Angle and Spectrometric Coronograph (LASCO) field of&#13;
view (FOV) the two CMEs propagated with linear speeds of 671 and 631 km s−1&#13;
, respectively. These CMEs&#13;
were tracked up to the Earth by Solar Terrestrial Relations Observatory (STEREO) instruments. We find&#13;
that the source region evolution of CMEs, guided by the large-scale coronal magnetic field configuration,&#13;
along with near-Sun propagation characteristics, such as CME-CME interactions, played important roles in&#13;
deciding the evolution of CMEs in the interplanetary medium and subsequently their geoeffectiveness.
</description>
<pubDate>Tue, 01 Feb 2022 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://localhost:8080/xmlui/handle/123456789/1659</guid>
<dc:date>2022-02-01T00:00:00Z</dc:date>
</item>
<item>
<title>Deciphering Solar Magnetic Activity: 140 Years of the ‘Extended Solar Cycle’ – Mapping the Hale Cycle</title>
<link>http://localhost:8080/xmlui/handle/123456789/1658</link>
<description>Deciphering Solar Magnetic Activity: 140 Years of the ‘Extended Solar Cycle’ – Mapping the Hale Cycle
McIntosh, Scott W. ,et.al.; Banerjee, Dipankar
We investigate the occurrence of the “extended solar cycle” (ESC) as it occurs in a host of&#13;
observational data spanning 140 years. Investigating coronal, chromospheric, photospheric,&#13;
and interior diagnostics, we develop a consistent picture of solar activity migration linked to&#13;
the 22-year Hale (magnetic) cycle using superposed epoch analysis (SEA) and previously&#13;
identified Hale cycle termination events as the key time for the SEA. Our analysis shows&#13;
that the ESC and Hale cycle, as highlighted by the terminator-keyed SEA, is strongly recur rent throughout the entire observational record studied, some 140 years. Applying the same&#13;
SEA method to the sunspot record confirms that Maunder’s butterfly pattern is a subset of&#13;
the underlying Hale cycle, strongly suggesting that the production of sunspots is not the&#13;
fundamental feature of the Hale cycle, but the ESC is. The ESC (and Hale cycle) pattern&#13;
highlights the importance of 55◦ latitude in the evolution, and possible production, of solar&#13;
magnetism.
</description>
<pubDate>Wed, 01 Dec 2021 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://localhost:8080/xmlui/handle/123456789/1658</guid>
<dc:date>2021-12-01T00:00:00Z</dc:date>
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<item>
<title>X-ray confirmation of the intermediate polar IGR J16547-1916</title>
<link>http://localhost:8080/xmlui/handle/123456789/1657</link>
<description>X-ray confirmation of the intermediate polar IGR J16547-1916
Joshi, A.,et.al.; Pandey, J. C.; Rawat, N.
Using X-ray observations from the NuSTAR and Swift satellites, we present temporal and spectral properties of an intermediate polar&#13;
(IP) IGR J16547-1916. A persistent X-ray period at ∼546 s confirming the optical spin period obtained from previous observations&#13;
is detected. The detection of a strong X-ray spin pulse reinforces the classification of this system as an intermediate polar. The lack&#13;
of orbital or side-band periodicities in the X-rays implies that the system is accreting predominantly via a disk. A variable covering&#13;
absorber appears to be responsible for the spin pulsations in the low energy range. In the high energy band, the pulsations are likely due&#13;
to the self occultation of tall shocks above the white dwarf surface. The observed double-humped X-ray spin pulse profile indicates&#13;
two-pole accretion geometry with tall accretion regions in short rotating IP IGR J16547-1916. We present the variation of the spin&#13;
pulse profile over an orbital phase to account for the effects of orbital motion on the spin pulsation. X-ray spectra obtained from the&#13;
contemporaneous observations of Swift and NuSTAR in the 0.5–78.0 keV energy band are modeled with a maximum temperature of&#13;
31 keV and a blackbody temperature of 64 eV, along with a common column density of 1.8 × 1023 cm−2&#13;
and a power-law index of&#13;
−0.22 for the covering fraction. An additional Gaussian component and a reflection component are needed to account for a fluorescent&#13;
emission line at 6.4 keV and the occurrence of X-ray reflection in the system. We also present the spin phase-resolved spectral&#13;
variations of IGR J16547-1916 in the 0.5–78.0 keV energy band and find dependencies in the X-ray spectral parameters during the&#13;
rotation of the white dwarf.
</description>
<pubDate>Sat, 01 Jan 2022 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://localhost:8080/xmlui/handle/123456789/1657</guid>
<dc:date>2022-01-01T00:00:00Z</dc:date>
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