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The kinematic Kelvin–Helmholtz instability-driven dynamo: implications for merging compact objects

Nov 4, 2026·
James R. Beattie
James R. Beattie
,
Amitava Bhattacharjee
,
Elias R. Most
,
Bart Ripperda
,
Alexander Philippov
,
Ralf S. Klessen
,
Salvatore Cielo
· 1 min read
A density slice shows a Kelvin–Helmholtz billow rolling into a spiral, with fine secondary fingers along its folded layers. Density roll-up in a Kelvin–Helmholtz billow at Re = 8192 and 140 shear times. Detail from Figure 3a, Beattie et al. (2026).
Abstract
High-resolution visco-resistive simulations and analytical models trace magnetic amplification in Kelvin–Helmholtz shear layers. Initial shear winding gives way to three-dimensional breakup and dynamo growth. At high Reynolds number, growth rates become independent of Reynolds number and the mean vertical field is seeded rapidly. Applied to binary neutron-star mergers, the models predict magnetar-strength fields and a transition out of the kinematic regime on roughly 0.1 ms timescales.
Type
Publication
arXiv preprint (submitted)

A rapid dynamo between merging stars

When two neutron stars meet, their shear layer rolls into Kelvin–Helmholtz billows. How do these motions build the intense magnetic fields found in merger simulations?

We follow three stages: shear winds the initial field; secondary instabilities break the billows into three-dimensional motions; and a dynamo amplifies both the fluctuating field and a mean field perpendicular to the original flow plane. At high Reynolds number, the dynamo growth rates become independent of Reynolds number.

Applied to neutron-star mergers, our models predict rapid vertical-field seeding and magnetar-strength fields as the dynamo leaves its kinematic stage on roughly 0.1 ms timescales. This suggests that global simulations may not resolve the relevant amplification regime.

Read the preprint → · Watch the simulations →