MRI乱流におけるAlfven的揺動と圧縮的揺動の散逸比

(2020) 824-824

Authors:

川面 洋平, A Schekochihin, MA Barnes, W Dorland, SA Balbus

Formation and Evolution of Compact Object Binaries in AGN Disks

(2019)

Authors:

Hiromichi Tagawa, Zoltan Haiman, Bence Kocsis

Anisotropic Mass Segregation in Rotating Globular Clusters

ASTROPHYSICAL JOURNAL American Astronomical Society 887:2 (2019) ARTN 123

Authors:

Akos Szolgyen, Yohai Meiron, Bence Kocsis

Abstract:

We investigate the internal dynamics of anisotropic, rotating globular clusters with a multimass stellar population by performing new direct N-body simulations. In addition to the well-known radial mass segregation effect, where heavy stars and stellar remnants sink toward the center of the cluster, we find a mass segregation in the distribution of orbital inclinations as well. This newly discovered anisotropic mass segregation leads to the formation of a disk-like structure of massive objects near the equatorial plane of a rotating cluster. This result has important implications on the expected spatial distribution of black holes in globular clusters.

Binary intermediate-mass black hole mergers in globular clusters

(2019)

Authors:

Alexander Rasskazov, Giacomo Fragione, Bence Kocsis

Impact of main ion pressure anisotropy on stellarator impurity transport

Nuclear Fusion IOP Publishing 60 (2019) 016035

Authors:

I Calvo, F Parra Diaz, JL Velasco, JM García-Regaña

Abstract:

Main ions influence impurity dynamics through a variety of mechanisms; in particular, via impurity-ion collisions. To lowest order in an expansion in the main ion mass over the impurity mass, the impurity-ion collision operator only depends on the component of the main ion distribution that is odd in the parallel velocity. These lowest order terms give the parallel friction of the impurities with the main ions, which is typically assumed to be the main cause of collisional impurity transport. Next-order terms in the mass ratio expansion of the impurity-ion collision operator, proportional to the component of the main ion distribution that is even in the parallel velocity, are usually neglected. However, in stellarators, the even component of the main ion distribution can be very large. In this article, such next-order terms in the mass ratio expansion of the impurity-ion collision operator are retained, and analytical expressions for the neoclassical radial flux of trace impurities are calculated in the Pfirsch-Schl\"uter, plateau and $1/\nu$ regimes. The new terms provide a drive for impurity transport that is physically very different from parallel friction: they are associated to anisotropy in the pressure of the main ions, which translates into impurity pressure anisotropy. It is argued that main ion pressure anisotropy must be taken into account for a correct description of impurity transport in certain realistic stellarator plasmas. Examples are given by numerically evaluating the analytical expressions for the impurity flux.