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Hub Formation and Filament-Filament Collision: An Analytical Model

Published 13 Mar 2026 in astro-ph.GA | (2603.12876v1)

Abstract: Filaments are ubiquitous throughout the Galaxy. Massive star formation is often observed in hub-filament systems, where multiple filaments appear to be interconnected and merging. Filament-filament collisions are therefore a likely triggering mechanism for massive star formation. We derive basic physical properties of filament-filament collisions, such as the collision cross section (CCS), the hub mass, and its mass function, based on a simple cylindrical filament model. We assume a cylindrical filament with length $2p$, full width $2q$, and line-mass λ<em>0λ<em>0, and consider the CCS between two identical filaments. The collision is specified by three vectors: the directions of the colliding filaments (n1n_1 and n2n_2) and the direction of the relative velocity between the two filaments (nv=v/vn_v=v/|v|). For the thin filament, pqp\gg q, the CCS is expressed as $S=4p<sup>2|n&#39;_1\times</sup> n&#39;_2|$, where $n&#39;_1$ and $n&#39;_2$ represent the directional vectors projected onto a plane perpendicular to the relative velocity nvn_v. As the angle between $n&#39;_1$ and $n&#39;_2$ becomes smaller, the cross section proportional to pqp\cdot q becomes relatively important. We propose a simple model in which the hub mass is estimated by the overlapping portion of the two colliding filaments. The hub mass function is derived using the CCSs and the geometrically estimated overlapping mass. When the directions and relative velocities of the filaments are isotropically distributed, the mass function expected from a single species of filaments fits well to a power law and the power exponent is γM2.96γ_M\simeq -2.96 ~ 3.78-3.78. The power exponent of the global hub mass function is the same as that of the line-mass distribution function, γ</em>λ1.5γ</em>λ\simeq -1.5. This means that a massive hub is formed by the collision of two massive filaments.

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