Dynamics near the inner dead-zone edges in a proprotoplanetary disk

Author:

Iwasaki Kazunari1ORCID,Tomida Kengo2ORCID,Takasao Shinsuke3ORCID,Okuzumi Satoshi4ORCID,Suzuki Takeru K5ORCID

Affiliation:

1. Center for Computational Astrophysics, National Astronomical Observatory of Japan , 2-21-1 Osawa, Mitaka, Tokyo 181-8588 , Japan

2. Astronomical Institute, Tohoku University , Aramaki, Aoba-ku, Sendai, Miyagi 980-8578 , Japan

3. Department of Earth and Space Science, Osaka University , 1-1 Machikaneyama-cho, Toyonaka, Osaka 560-0043 , Japan

4. Department of Earth and Planetary Sciences, Tokyo Institute of Technology , 2-12-1 Ookayama, Meguro, Tokyo 152-8551 , Japan

5. School of Arts & Sciences, The University of Tokyo , 3-8-1 Komaba, Meguro, Tokyo 153-8902 , Japan

Abstract

Abstract We perform three-dimensional global non-ideal magnetohydrodynamic simulations of a protoplanetary disk containing the inner dead-zone edge. We take into account realistic diffusion coefficients of the Ohmic resistivity and ambipolar diffusion based on detailed chemical reactions with single-size dust grains. We found that the conventional dead zone identified by the Elsässer numbers of the Ohmic resistivity and ambipolar diffusion is divided into two regions: “the transition zone” and “the coherent zone.” The coherent zone has the same properties as the conventional dead zone, and extends outside of the transition zone in the radial direction. Between the active and coherent zones, we discover the transition zone, the inner edge of which is identical to that of the conventional dead zone. The transition zone extends out over the regions where thermal ionization determines diffusion coefficients. The transition zone has completely different physical properties than the conventional dead zone, the so-called undead zone, and the zombie zone. The combination of amplification of the radial magnetic field owing to the ambipolar diffusion and a steep radial gradient of the Ohmic diffusivity causes the efficient evacuation of the net vertical magnetic flux from the transition zone within several rotations. Surface gas accretion occurs in the coherent zone but not in the transition zone. The presence of the transition zone prohibits mass and magnetic flux transport from the coherent zone to the active zone. Mass accumulation occurs at both edges of the transition zone as a result of mass supply from the active and coherent zones.

Funder

National Astronomical Observatory of Japan

Publisher

Oxford University Press (OUP)

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