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arXiv 2403.09780astro-ph.EP
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T Cha 的 JWST MIRI-MRS 观测建模:中红外惰性气体发射示踪致密盘风

Modeling JWST MIRI-MRS Observations of T Cha: Mid-IR Noble Gas Emission Tracing a Dense Disk Wind

Andrew D. Sellek, Naman S. Bajaj, Ilaria Pascucci, Cathie J. Clarke, Richard Alexander, Chengyan Xie, Giulia Ballabio, Dingshan Deng, Uma Gorti, Andras Gaspar, Jane Morrison

AI总结:

本文通过 JWST MIRI-MRS 对 T Cha 的中红外惰性气体发射进行光致电离辐射转移建模,揭示其谱线特征要求一个致密且延展的盘风,并据此区分光致蒸发与磁驱动风的贡献。

摘要:

[Ne II] 12.81 μm 发射因其蓝移谱线轮廓而成为原行星盘风的常用示踪剂。MIRI-MRS 最近观测了 T Cha,探测到这条谱线以及 [Ne III]、[Ar II] 和 [Ar III] 谱线,发现 [Ne II] 和 [Ne III] 谱线具有空间延展性,而 [Ar II] 则没有。在这项补充工作中,我们利用这些谱线来解决关于原行星盘风长期争论的问题,涉及它们的质量损失率、电离起源,以及磁驱动风相对于光致蒸发的作用。为此,我们对简单的流体动力学风模型进行光致电离辐射转移,以绘制谱线发射图。我们将模型积分光度与 MIRI-MRS 观测到的光度进行比较,以确定哪些模型最接近地再现数据,并从这些模型生成合成图像,以理解谱线延展度测量所捕获的信息。除了谱线比所暗示的低电离度之外,[Ar II] 相对于 [Ne II] 的相对致密性尤其具有约束力。这要求在一个延展的(≳10 au)风中,硬 X 射线产生 Ne II,软 X 射线(和/或 EUV)产生 Ar II,且该风被屏蔽于软 X 射线之外——这需要一个致密的风,其物质发射尺度小至约 1 au。这样的条件可以由光致蒸发产生,而一个产生同等屏蔽效果的延展 MHD 风则可能低估谱线通量。然而,一个稀薄的内部 MHD 风可能仍然有助于屏蔽延展风。这一图景与光谱分辨谱线轮廓的约束条件一致。

英文摘要:

[Ne II] 12.81 $μ\mathrm{m}$ emission is a well-used tracer of protoplanetary disk winds due to its blueshifted line profile. MIRI-MRS recently observed T Cha, detecting this line along with lines of [Ne III], [Ar II] and [Ar III], with the [Ne II] and [Ne III] lines found to be extended while the [Ar II] was not. In this complementary work, we use these lines to address long-debated questions about protoplanetary disk winds regarding their mass-loss rate, the origin of their ionization, and the role of magnetically-driven winds as opposed to photoevaporation. To this end, we perform photoionization radiative transfer on simple hydrodynamic wind models to map the line emission. We compare the integrated model luminosities to those observed with MIRI-MRS to identify which models most closely reproduce the data and produce synthetic images from these to understand what information is captured by measurements of the line extents. Along with the low degree of ionization implied by the line ratios, the relative compactness of [Ar II] compared to [Ne II] is particularly constraining. This requires Ne II production by hard X-rays and Ar II production by soft X-rays (and/or EUV) in an extended ($\gtrsim 10$ au) wind that is shielded from soft X-rays - necessitating a dense wind with material launched on scales down to ~1 au. Such conditions could be produced by photoevaporation, whereas an extended MHD wind producing equal shielding would likely underpredict the line fluxes. However, a tenuous inner MHD wind may still contribute to shielding the extended wind. This picture is consistent with constraints from spectrally-resolved line profiles.

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