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Ultraviolet, X-Ray, and Optical Radiation from the Geminga Pulsar*

机译:Geminga脉冲星发出的紫外线,X射线和光辐射*

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We observed the γ-ray pulsar Geminga with the FUV-MAMA and NUV-MAMA detectors of the Space Telescope Imaging Spectrometer to measure Geminga's spectrum and pulsations in the ultraviolet. The slope of the far-ultraviolet (FUV) spectrum is close to that of a Rayleigh-Jeans spectrum, suggesting that the FUV radiation is dominated by thermal emission from the neutron star (NS) surface. The measured FUV flux, FFUV = (3.7 ± 0.2) × 10-15 ergs cm-2 s-1 in the 1155-1702 ? band, corresponds to a brightness temperature TRJ ≈ (0.3-0.4)(d200/R13)2 MK, depending on the interstellar extinction (d = 200d200 pc and R = 13R13 km are the distance and the NS radius, respectively). The soft thermal component of Geminga's X-ray spectrum measured with the XMM-Newton observatory corresponds to a temperature Ts = 0.49 ± 0.01 MK and radius Rs = (12.9 ± 1.0)d200 km. Contrary to other NSs detected in the UV-optical, for which the extrapolation of the X-ray thermal component into the optical underpredicts the observed flux of thermal radiation, the FUV spectrum of Geminga lies slightly below the extrapolation of the soft thermal component, which might be associated with Geminga's very low temperature. Surprisingly, the thermal FUV radiation is strongly pulsed, showing a narrow dip at a phase close to that of a broader minimum of the soft X-ray light curve. The strong pulsations might be attributed to partial occultations of the thermal UV radiation by regions of the magnetosphere filled with electron/positron plasma. In contrast to the FUV spectrum, the near-infrared (NIR) through near-ultraviolet (NUV) spectrum of Geminga is clearly nonthermal. It can be described by a power-law model, Fν ∝ ν-Γ+1, with a photon index Γ = 1.43 ± 0.15, close to the slope Γ = 1.56 ± 0.24 of the hard X-ray (E 2.5 keV) magnetospheric component. The extrapolation of the X-ray magnetospheric spectrum into the optical is marginally consistent with (or perhaps lies slightly above) the observed NIR-optical-NUV spectrum. The NUV pulsations, however, do not show a clear correlation with the hard X-ray pulsations.
机译:我们使用太空望远镜成像光谱仪的FUV-MAMA和NUV-MAMA探测器观察了γ射线脉冲星Geminga,以测量Geminga的光谱和紫外线脉动。远紫外(FUV)光谱的斜率接近瑞利-吉恩斯光谱的斜率,这表明FUV辐射主要来自中子星(NS)表面的热辐射。在1155-1702?中测得的FUV通量FFUV =(3.7±0.2)×10-15 ergs cm-2 s-1。波段,对应于亮度温度TRJ≈(0.3-0.4)(d200 / R13)2 MK,取决于星际消光(d = 200d200 pc和R = 13R13 km分别是距离和NS半径)。用XMM-牛顿天文台测量的Geminga X射线光谱的软热分量对应于温度Ts = 0.49±0.01 MK,半径Rs =(12.9±1.0)d200 km。与在紫外光学中检测到的其他NSs相反,对于这些NSs,X射线热成分外推到光学中会不足以预测观察到的热辐射通量,Geminga的FUV光谱略低于软热成分的外推,后者可能与Geminga的低温有关。令人惊讶地,热FUV辐射被强脉冲化,在接近软X射线光曲线的更宽最小值的相位处显示出窄的倾角。强烈的脉动可能归因于充满电子/正电子等离子体的磁层区域对紫外线热辐射的部分掩盖。与FUV光谱相反,Geminga的近红外(NIR)到近紫外(NUV)光谱显然是非热的。可以用幂律模型Fν∝ν-Γ+ 1来描述,其光子指数Γ= 1.43±0.15,接近硬X射线的斜率Γ= 1.56±0.24(E> 2.5 keV)磁层成分。 X射线的磁层光谱外推到光学上与观察到的NIR-光学-NUV光谱在一定程度上是一致的(或者可能略高于)。但是,NUV脉动与硬X射线脉动没有明显的相关性。

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