Ariel 6 Observations of Cyg X-1 in the High State

1981 ◽  
pp. 369-371
Author(s):  
C. G. Page ◽  
A. J. Bennetts ◽  
M. J. Ricketts
Keyword(s):  
1997 ◽  
Vol 481 (1) ◽  
pp. 433-446 ◽  
Author(s):  
D. W. Hoard ◽  
Paula Szkody
Keyword(s):  

2011 ◽  
Vol 143 (1) ◽  
pp. 23 ◽  
Author(s):  
Haritma Gaur ◽  
Alok C. Gupta ◽  
Paul J. Wiita

2021 ◽  
Vol 4 ◽  
Author(s):  
Vasileios Ioakeimidis ◽  
Nareg Khachatoorian ◽  
Corinna Haenschel ◽  
Thomas A. Papathomas ◽  
Attila Farkas ◽  
...  

Abstract The hollow-mask illusion is an optical illusion where a concave face is perceived as convex. It has been demonstrated that individuals with schizophrenia and anxiety are less susceptible to the illusion than controls. Previous research has shown that the P300 and P600 event-related potentials (ERPs) are affected in individuals with schizophrenia. Here, we examined whether individual differences in neuroticism and anxiety scores, traits that have been suggested to be risk factors for schizophrenia and anxiety disorders, affect ERPs of healthy participants while they view concave faces. Our results confirm that the participants were susceptible to the illusion, misperceiving concave faces as convex. We additionally demonstrate significant interactions of the concave condition with state anxiety in central and parietal electrodes for P300 and parietal areas for P600, but not with neuroticism and trait anxiety. The state anxiety interactions were driven by low-state anxiety participants showing lower amplitudes for concave faces compared to convex. The P300 and P600 amplitudes were smaller when a concave face activated a convex face memory representation, since the stimulus did not match the active representation. The opposite pattern was evident in high-state anxiety participants in regard to state anxiety interaction and the hollow-mask illusion, demonstrating larger P300 and P600 amplitudes to concave faces suggesting impaired late information processing in this group. This could be explained by impaired allocation of attentional resources in high-state anxiety leading to hyperarousal to concave faces that are unexpected mismatches to standard memory representations, as opposed to expected convex faces.


Energy ◽  
2022 ◽  
Vol 238 ◽  
pp. 121809
Author(s):  
Shanshan Guo ◽  
Ruixin Yang ◽  
Weixiang Shen ◽  
Yongsheng Liu ◽  
Shenggang Guo

1988 ◽  
Vol 231 (1) ◽  
pp. 69-84 ◽  
Author(s):  
C. S. R. Day ◽  
A. F. Tennant ◽  
A. C. Fabian
Keyword(s):  

2005 ◽  
Vol 29 (2) ◽  
pp. 131-135
Author(s):  
Ming-xuan Zhang ◽  
Jin-lu Qu
Keyword(s):  

2003 ◽  
Vol 342 (4) ◽  
pp. 1083-1092 ◽  
Author(s):  
M. Gierlinski ◽  
C. Done
Keyword(s):  
X Ray ◽  

2001 ◽  
Vol 553 (1) ◽  
pp. 375-381 ◽  
Author(s):  
A. La Barbera ◽  
L. Burderi ◽  
T. Di Salvo ◽  
R. Iaria ◽  
N. R. Robba

2002 ◽  
Vol 54 (6) ◽  
pp. 1033-1039 ◽  
Author(s):  
Taichi Kato ◽  
Ryoko Ishioka ◽  
Makoto Uemura
Keyword(s):  

2020 ◽  
Vol 499 (2) ◽  
pp. 3006-3018
Author(s):  
Bangzheng Sun ◽  
Marina Orio ◽  
Andrej Dobrotka ◽  
Gerardo Juan Manuel Luna ◽  
Sergey Shugarov ◽  
...  

ABSTRACT We present X-ray observations of novae V2491 Cyg and KT Eri about 9 yr post-outburst of the dwarf nova and post-nova candidate EY Cyg, and of a VY Scl variable. The first three objects were observed with XMM–Newton, KT Eri also with the Chandra ACIS-S camera, V794 Aql with the Chandra ACIS-S camera and High Energy Transmission Gratings. The two recent novae, similar in outburst amplitude and light curve, appear very different at quiescence. Assuming half of the gravitational energy is irradiated in X-rays, V2491 Cyg is accreting at $\dot{m}=1.4\times 10^{-9}{\!-\!}10^{-8}\,{\rm M}_\odot \,{\rm yr}^{-1}$, while for KT Eri, $\dot{m}\lt 2\times 10^{-10}{\rm M}_\odot \,{\rm yr}$. V2491 Cyg shows signatures of a magnetized WD, specifically of an intermediate polar. A periodicity of  39 min, detected in outburst, was still measured and is likely due to WD rotation. EY Cyg is accreting at $\dot{m}\sim 1.8\times 10^{-11}{\rm M}_\odot \,{\rm yr}^{-1}$, one magnitude lower than KT Eri, consistently with its U Gem outburst behaviour and its quiescent UV flux. The X-rays are modulated with the orbital period, despite the system’s low inclination, probably due to the X-ray flux of the secondary. A period of  81 min is also detected, suggesting that it may also be an intermediate polar. V794 Aql had low X-ray luminosity during an optically high state, about the same level as in a recent optically low state. Thus, we find no clear correlation between optical and X-ray luminosity: the accretion rate seems unstable and variable. The very hard X-ray spectrum indicates a massive WD.


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