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Spiral Structure in the Gas Disk of TW Hya
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abstract
We report the detection of spiral substructure in both the gas velocity and temperature structure of the disk around TW~Hya, suggestive of planet-disk interactions with an unseen planet. Perturbations from Keplerian rotation tracing out a spiral pattern are observed in the SE of the disk, while significant azimuthal perturbations in the gas temperature are seen in the outer disk, outside 90~au, extending the full azimuth of the disk. The deviation in velocity is either $\Delta v_{\phi} \, / \, v_{\rm kep} \sim 0.1$ or $\Delta v_{z} \, / \, v_{\rm kep} \sim 0.01$ depending on whether the perturbation is in the rotational or vertical direction, while radial perturbations can be ruled out. Deviations in the gas temperature are $\pm 4$ K about the azimuthally averaged profile, equivalent to deviations of $\Delta T_{\rm gas} \, / \, T_{\rm gas} \sim 0.05$. Assuming all three structures can be described by an Archimedean spiral, measurements of the pitch angles of both velocity and temperature spirals show a radially decreasing trend for all three, ranging from 9$^{\circ}$ at 70 au, dropping to 3$^{\circ}$ at 200 au. Such low pitch-angled spirals are not readily explained through the wake of an embedded planet in the location of previously reported at 94 au, but rather require a launching mechanism which results in much more tightly wound spirals. Molecular emission tracing distinct heights in the disk is required to accurately distinguish between spiral launching mechanisms.
Forward citations
Cited by 2 Pith papers
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Dust and Gas Transport in Substructured Nonideal MHD Wind-Launching Disks with Embedded Planets
In magnetized wind-launching disks, planet-opened gaps remain partially permeable: small grains and gas leak through, while large grains are filtered, making substructures regulators rather than barriers.
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Unstable magnetospheric accretion on the T Tauri star TW Hya
TW Hya’s large-scale field is a ~0.83 kG tilted dipole that varies yearly; accretion is unstable (rmag/rcor ≈ 0.33–0.40) and no close-in planet is detected above ~0.3–1 Mjup.
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