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首页> 外文期刊>The Astrophysical journal >FIRST SPECTRAL OBSERVATIONS OF THE DIFFUSE BACKGROUND WITH THE EXTREME ULTRAVIOLET EXPLORER
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FIRST SPECTRAL OBSERVATIONS OF THE DIFFUSE BACKGROUND WITH THE EXTREME ULTRAVIOLET EXPLORER

机译:极端紫外线探测器对弥散背景的首次光谱观察

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We present the first results from the analysis of the spectroscopic observations of diffuse extreme ultraviolet (EUV) emission taken with the Extreme Ultraviolet Explorer (EUVE) spectrometers in the wavelength range 160-740 A. Although not designed or optimized for diffuse observation, the EUVE spectrometers are the most sensitive diffuse EUV spectrometer in orbit. The spectral resolution for diffuse emission of the medium and long-wavelength spectrometers are 17 and 34 A FWHM, respectively. During the period from 1992 July 25 to 1992 August 19, the spectrometers surveyed a 2.0° x 20° field scanned from (l, b) = (24°, -28°) to (44°, -74°) with a total effective exposure time of 575,232 s. The only emission lines detected were those of He Ⅰ and He Ⅱ (584, 537, and 304 A) with intensities consistent with local geocoronal and/or interplanetary scattering of solar radiation (584 A = 1.30 rayleighs; 537 A = 0.040 R; and 304 A = 0.029 R). Models of the soft X-ray background, which results from a 10~6 K plasma (Local Bubble) surrounding the neutral gas near the Sun (Local Cloud), predict that most of the flux from the hot plasma appears as emission lines in the EUV. We have compared these spectral predictions with our observations to place limits on the emission measure versus temperature of the proposed hot plasma. Using the same plasma model, we derived emission measures for our data and the C and B soft X-ray bands of the Wisconsin rocket survey. We find that our limits for the plasma emission measure are a factor of 5-10 below the C- and B-band emission measures over the temperature range from 10~(5.7) to 10~(6.4) K. We explore possible scenarios that could reconcile our results with the X-ray surveys and conclude that depletion or a nonequilibrium plasma state rather than absorption are the more likely explanations of the discrepancy. We also show that our spectrum is inconsistent with the spectrum from the ~10~5 K gas at the conductive interface between the hot Local Bubble and the cooler Local Cloud given by Slavin (1989). In addition, we place new limits on the helium ionization parameter in the Sun's vicinity caused by the 10~6 K plasma in the Local Bubble.
机译:我们提供了使用波长范围为160-740 A的极紫外探测器(EUVE)光谱仪对弥散极紫外(EUV)发射光谱进行观察的分析结果。尽管未针对弥散观察进行设计或优化,但EUVE光谱仪是轨道上最灵敏的扩散EUV光谱仪。中波谱仪和长波谱仪的漫射光谱分辨率分别为17和34 A FWHM。在1992年7月25日至1992年8月19日期间,光谱仪对从(l,b)=(24°,-28°)到(44°,-74°)扫描的2.0°x 20°场进行了总计有效曝光时间为575,232 s。唯一检测到的发射线是HeⅠ和HeⅡ(584、537和304 A),其强度与太阳辐射的局部冠冕和/或行星际散射一致(584 A = 1.30瑞利; 537 A = 0.040 R;和304 A = 0.029 R)。软X射线背景的模型是由围绕太阳(局部云)附近的中性气体的10〜6 K等离子体(局部气泡)产生的,该模型预测,来自热等离子体的大部分通量以辐射线的形式出现在EUV。我们将这些光谱预测值与我们的观察结果进行了比较,以对发射量度与拟议的热等离子体的温度进行限制。使用相同的等离子体模型,我们得出了我们的数据以及威斯康星州火箭调查的C和B软X射线波段的发射量度。我们发现,在10〜(5.7)到10〜(6.4)K的温度范围内,等离子发射量度的极限比C和B波段发射量度低5-10倍。我们探索了可能的情况,可以使我们的结果与X射线调查相一致,并得出结论,耗尽或非平衡血浆状态而非吸收是更可能的差异解释。我们还表明,我们的光谱与热的局部气泡和较冷的局部云(由Slavin(1989)给出)之间的导电界面处的〜10〜5 K气体的光谱不一致。此外,我们对由局部气泡中的10〜6 K等离子体引起的太阳附近氦电离参数设置了新的限制。

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