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Two-scale structure of the current layer controlled by meandering motion during steady-state collisionless driven reconnection
A steady two-scale structure of current layer is demonstrated in the collisionless driven reconnections without a guide field by means of two-dimensional full-particle simulations in an open system. The current density profile along the inflow direction consists of two parts. One is a low shoulder controlled by the ion-meandering motion, which is a bouncing motion in a field reversal region. The other is a sharp peak caused mainly by the electron-meandering motion. The shoulder structure is clearly separated from the sharp peak for the case of a large mass ratio calculation mi/m_e = 200 because the ratio of the ion-meandering orbit amplitude to the electron-meandering orbit amplitude is proportional to (mi/m_e)^1/4. Although the ion frozen-in constraint is broken within a distance of the ion skin depth c/omega_pi, the violation due to the ion inertia is weak compared to the strong violation caused by the ion-meandering motion. The violation of the electron frozen-in constraint caused by the electron-meandering motion is stronger than the violation due to the electron inertia, and thus the electron-meandering motion produces the reconnection electric field in the central region where the current has the sharp peak structure
Two-Scale Structure of the Current Layer Controlled by Meandering Motion during Steady-State Collisionless Driven Reconnection
Conversion Process of Electron Kinetic Energy in the Electron Dissipation Region in Steady Collisionless Driven Reconnection
Strong Electron Outflow and its Influence on the Downstream Structure of the Electron Dissipation Region in the Steady Collisionless Driven Reconnection
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