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SPECTROSCOPY OF MOLECULAR HYDROGEN EMISSION FROM KH 15D

机译:KH 15D分子氢发射光谱

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We report infrared spectroscopy of the unusual eclipsing pre-main-sequence object KH 15D, obtained using NIRSPEC on Keck Ⅱ. During eclipse, observations using low spectral resolution (λ/δλ ~ 1000) reveal the presence of prominent molecular hydrogen emission in five lines near 2 μm. The relative line strengths are consistent with thermal excitation at T ~ 2800 +- 300 K. Observations out of eclipse, at both low and high spectral resolution (λ/δλ ~ 2 x 10~4), show reduced contrast with the stellar continuum. The change in contrast for the strongest line, 1-0 S(1), is consistent with an approximately constant emission line superposed on a variable stellar continuum. Emission in the 1-0 S(1) line is observed to extend by approx> 4″ both east and west of the stellar point-spread function (PSF; approx> 3000 AU). Observed at high spectral resolution, the velocity and the intensity structure of the 1-0 S(1) profile are both asymmetric. East of the stellar PSF (by 1.1″-2.3″) the emission is blueshifted (-63 km s~(-1)) and has significantly greater intensity than the marginally redshifted component (+ 2 km s~(-1), approximately consistent with zero) that dominates west of the stellar PSF. The spatial extent of the emission and the excitation temperature suggest shock excitation of ambient gas by a bipolar outflow from the star and/or the disk. However, it is difficult to account for the observed radial velocity unless the outflow axis is inclined significantly to the plane of the sky.
机译:我们报道了使用NIRSPEC在KeckⅡ上获得的不寻常的食前主序列对象KH 15D的红外光谱。在日食期间,使用低光谱分辨率(λ/δλ〜1000)进行的观测表明,在2μm附近的五条线中存在明显的分子氢发射。相对线强度与在T〜2800 +-300 K时的热激发一致。在日食之外,在低和高光谱分辨率下(λ/δλ〜2 x 10〜4)观察到的图像,与恒星连续体的对比度降低。最强的线1-0 S(1)的对比度变化与叠加在可变恒星连续体上的近似恒定的发射线一致。观测到1-0 S(1)线中的发射在恒星点扩展函数(PSF;大约> 3000 AU)的东边和西边都延伸了大约> 4“。在高光谱分辨率下观察到的1-0 S(1)轮廓的速度和强度结构都是不对称的。在恒星PSF的东部(1.1“ -2.3”),发射是蓝移的(-63 km s〜(-1)),其强度比边缘红移的分量(+ 2 km s〜(-1))大得多。与零一致),在恒星PSF的西边占主导地位。发射的空间范围和激发温度表明,环境气体通过恒星和/或盘的双极流出而受到激振。但是,除非流出轴相对于天空平面明显倾斜,否则很难考虑观测到的径向速度。

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