JWST/MIRI 对原行星盘 HH 48 NE 中的冰分布和多环芳烃辐射的分析

J. Sturm, M. McClure, D. Harsono, J. Bergner, E. Dartois, A. Boogert, M. Cordiner, M. Drozdovskaya, S. Ioppolo, C.J. Law, D. Lis, B. A. McGuire, G. J. Melnick, J. A. Noble, K. Öberg, M. E. Palumbo, Y. Pendleton, G. Perotti, W. Rocha, R. Urso, E. V. van Dishoeck
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We present JWST Mid-InfraRed Imager (MIRI) observations of the edge-on disk HH 48 NE carried out as part of the Director’s Discretionary Early Release Science program Ice Age, completing the ice inventory of HH 48 NE by combining the MIRI data (5 -- 28 with those of NIRSpec (2.7 -- 5 We used radiative transfer models tailored to the system, including silicates, ices, and polycyclic aromatic hydrocarbons (PAHs) to reproduce the observed spectrum of HH 48 NE with a parameterized model. \n The model was then used to identify ice species and constrain spatial information about the ices in the disk. The mid-infrared spectrum of HH 48 NE is relatively flat, with weak ice absorption features. \n We detect CO2 NH3 H2O and tentatively CH4 and NH4+ .\n Radiative transfer models suggest that ice absorption features are produced predominantly in the 50 -- 100 au region of the disk. 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引用次数: 0

摘要

冰涂层尘粒是挥发物的主要储藏库,在行星形成过程中发挥着重要作用,并可能融入行星大气。 然而,由于观测方面的挑战,原行星盘中的冰丰度分布并没有得到很好的约束。 随着詹姆斯-韦伯太空望远镜(JWST)的问世,我们处于一个独特的位置,可以用近红外到中红外光谱观测这些冰,并对它们在II类原系星盘中的性质进行约束。我们展示了JWST中红外成像仪(MIRI)对边缘盘HH 48 NE的观测结果,这是 "冰河时代"(Ice Age)主任酌情早期发布科学计划的一部分,通过将MIRI数据(5--28)与NIRSpec数据(2.7--5)相结合,完成了HH 48 NE的冰清单。 我们使用了针对该系统量身定制的辐射传递模型,包括硅酸盐、冰和多环芳烃(PAHs),用参数化模型重现了HH 48 NE的观测光谱。 然后利用该模型来识别冰的种类,并对圆盘中冰的空间信息进行约束。HH 48 NE 的中红外光谱相对平坦,具有微弱的冰吸收特征。 我们探测到了 CO2 NH3 H2O,并初步探测到了 CH4 和 NH4+。辐射传递模型表明,冰吸收特征主要产生于磁盘的 50-100 au 区域。与 4.3 处的相应特征($z/r$ = 0.2-0.6)相比,15 处的 CO2 特征探测的区域更接近中面($z/r$ = 0.1-0.15),但所有观测都追踪了明显高于中面储层的区域,我们预计大部分冰体都位于中面储层。冰必须达到较高的尺度高度($z/r 0.6$;对应于模型尘埃消光 v 0.1$),才能与观测到的冰光学深度峰值的垂直分布相一致。相对于 4.3 特征,15 点的 CO2 特征较弱,而且 4.3 CO2 特征的红色发射翼与冰位于星盘高处的情况一致。检索到的 NH3 丰度和相对于 H2O 的 CH3OH 丰度上限明显低于星际介质,但与彗星观测结果一致。多环芳烃的发射特征与连续面的对比比类似的面朝上的原行星盘更强烈,这可能是边缘系统几何形状的结果。 根据发射特征的相对强度建立的模型表明,PAH 发射源于盘表层而非冰吸收层。要正确研究盘中冰的丰度分布,就必须覆盖全部波长。为了解释在磁盘高空出现冰的原因,我们提出了两种可能的情况:一种是磁盘风夹带了足够多的尘埃,从而阻挡了部分恒星紫外线辐射;另一种是垂直混合,使足够多的冰循环到磁盘上层,以平衡冰粒的光吸收。
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A JWST/MIRI analysis of the ice distribution and polycyclic aromatic hydrocarbon emission in the protoplanetary disk HH 48 NE
Ice-coated dust grains provide the main reservoir of volatiles that play an important role in planet formation processes and may become incorporated into planetary atmospheres. However, due to observational challenges, the ice abundance distribution in protoplanetary disks is not well constrained. With the advent of the James Webb Space Telescope (JWST), we are in a unique position to observe these ices in the near- to mid-infrared and constrain their properties in Class II protoplanetary disks. We present JWST Mid-InfraRed Imager (MIRI) observations of the edge-on disk HH 48 NE carried out as part of the Director’s Discretionary Early Release Science program Ice Age, completing the ice inventory of HH 48 NE by combining the MIRI data (5 -- 28 with those of NIRSpec (2.7 -- 5 We used radiative transfer models tailored to the system, including silicates, ices, and polycyclic aromatic hydrocarbons (PAHs) to reproduce the observed spectrum of HH 48 NE with a parameterized model. The model was then used to identify ice species and constrain spatial information about the ices in the disk. The mid-infrared spectrum of HH 48 NE is relatively flat, with weak ice absorption features. We detect CO2 NH3 H2O and tentatively CH4 and NH4+ . Radiative transfer models suggest that ice absorption features are produced predominantly in the 50 -- 100 au region of the disk. The CO2 feature at 15 probes a region closer to the midplane ($z/r$ = 0.1 -- 0.15) than the corresponding feature at 4.3 ($z/r$ = 0.2 -- 0.6), but all observations trace regions significantly above the midplane reservoirs where we expect the bulk of the ice mass to be located. Ices must reach a high scale height ($z/r 0.6$; corresponding to a modeled dust extinction v 0.1$), in order to be consistent with the observed vertical distribution of the peak ice optical depths. The weakness of the CO2 feature at 15 relative to the 4.3 feature and the red emission wing of the 4.3 CO2 feature are both consistent with ices being located at a high elevation in the disk. The retrieved NH3 abundance and the upper limit on the CH3OH abundance relative to H2O are significantly lower than those in the interstellar medium, but consistent with cometary observations. The contrast of the PAH emission features with the continuum is stronger than for similar face-on protoplanetary disks, which is likely a result of the edge-on system geometry. Modeling based on the relative strength of the emission features suggests that the PAH emission originates in the disk surface layer rather than the ice absorbing layer. Full wavelength coverage is required to properly study the abundance distribution of ices in disks. To explain the presence of ices at high disk altitudes, we propose two possible scenarios: a disk wind that entrains sufficient amounts of dust, and thus blocks part of the stellar UV radiation, or vertical mixing that cycles enough ices into the upper disk layers to balance ice photodesorption from the grains.
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