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首页> 外文期刊>The Astrophysical journal >SOFT X-RAY PROPERTIES OF THE BINARY MILLISECOND PULSAR J0437-4715
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SOFT X-RAY PROPERTIES OF THE BINARY MILLISECOND PULSAR J0437-4715

机译:二值微距脉冲J0437-4715的软X射线性质

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摘要

We obtained a light curve for the 5.75 ms pulsar J0437 -4715 in the 65-120 A range with 0.5 ms time resolution using the Deep Survey instrument on the Extreme-Ultraviolet Explorer (EUVE) satellite. The single-peaked profile has a pulsed fraction of 0.27 ± 0.05, similar to the ROSAT data in the overlapping energy band. A combined analysis of the EUVE and ROSAT data is consistent with a power-law spectrum of energy index α = 1.2-1.5, intervening column density N_H = (5-8) x 10~(19) cm~(-2), and luminosity 5.0 x 10~(30) ergs s~(-1) in the 0.1-2.4 keV band. We also use a bright EUVE/ROSAT source only 4.2′ from the pulsar, the Seyfert galaxy RX J0437.4-4711 ( = EUVE J0437-471 = 1ES 0435-472), to obtain an independent upper limit on the intervening absorption to the pulsar, N_H < 1.2 x 10~(20) cm~(-2). Although a blackbody spectrum fails to fit the ROSAT data, two-component spectral fits to the combined EUVE/ROSAT data are used to limit the temperatures and surface areas of thermal emission that might make partial contributions to the flux. A hot polar cap of radius 50-600 m and temperature (1.0-3.3) x 10~6 K could be present. Alternatively, a larger region with T = (4-12) x 10~5 K and area less than 200 km~2 might contribute most of the EUVE and soft X-ray flux, but only if a hotter component were present as well. Any of these temperatures would require some mechanism(s) of surface reheating to be operating in this old pulsar, the most plausible being the impact of accelerated electrons and positrons onto the polar caps. The kinematically corrected spin-down power of PSR J0437—4715 is only 4 x 10~(33) ergs s~(-1), which is an order of magnitude less than that of the lowest luminosity γ-ray pulsars Geminga and PSR B1055 ?52. The absence of high-energy γ-rays from PSR J0437—4715 might signify an inefficient or dead outer gap accelerator, which in turn accounts for the lack of a more luminous reheated surface such as those intermediate-age γ-ray pulsars may have.
机译:我们使用极紫外探测器(EUVE)卫星上的Deep Survey仪器,以0.5 ms的时间分辨率在65-120 A范围内获得了5.75 ms脉冲星J0437 -4715的光曲线。单峰轮廓的脉冲分数为0.27±0.05,类似于重叠能带中的ROSAT数据。 EUVE和ROSAT数据的组合分析与能量指数α= 1.2-1.5,中间列密度N_H =(5-8)x 10〜(19)cm〜(-2)的幂律谱一致,并且在0.1-2.4 keV波段内的光度为5.0 x 10〜(30)ergs s〜(-1)。我们还使用了仅来自脉冲星的4.2'的明亮EUVE / ROSAT源,即塞弗特星系RX J0437.4-4711(= EUVE J0437-471 = 1ES 0435-472),以获得对星体的中间吸收的独立上限。脉冲星,N_H <1.2 x 10〜(20)cm〜(-2)。尽管黑体光谱无法拟合ROSAT数据,但是结合使用EUVE / ROSAT数据的两成分光谱拟合可限制可能对通量造成部分贡献的温度和热辐射表面积。可能存在半径为50-600 m和温度(1.0-3.3)x 10〜6 K的热极帽。另外,T =(4-12)x 10〜5 K且面积小于200 km〜2的较大区域可能会贡献大部分EUVE和软X射线通量,但前提是也必须存在更热的分量。这些温度中的任何一个都将需要某种表面再加热机制才能在这个旧的脉冲星中运行,最可能的是加速的电子和正电子撞击到极帽上。经运动学校正的PSR J0437—4715的旋转下降功率仅为4 x 10〜(33)ers s〜(-1),比最低发光度γ射线脉冲星Geminga和PSR B1055的数量级小。 52。 PSR J0437–4715中缺少高能γ射线可能表示效率低下或失效的外间隙加速器,这反过来又导致了缺少更明亮的再加热表面(例如那些中年γ射线脉冲星可能具有的)。

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