Ion Anisotropy in Earth's Magnetotail: Importance of High‐Energy Ions
Journal of Geophysical Research: Space Physics American Geophysical Union (AGU) 131:6 (2026) e2026JA035223
Abstract:
Eccentric Stellar-mass Binary Black Holes: Population, Detectability, and Waveform Analysis in the LISA and LIGO Era
(2026)
Dynamical evolution of quasi-hierarchical triples
Monthly Notices of the Royal Astronomical Society Oxford University Press 549:2 (2026) stag944
Abstract:
We study the gravitational dynamics of quasi-hierarchical triple systems, where the outer orbital period is significantly longer than the inner one, but the outer orbit is extremely eccentric, rendering the time at pericentre comparable to the inner period. Such systems are not amenable to the standard techniques of perturbation theory and orbit-averaging. Modelling the evolution of these triples as a sequence of impulses at the outer pericentre, we show, by comparing with direct three-body integrations, that such triples lend themselves to a description as an analytical map between subsequent outer pericentre passages. This map exhibits secular oscillations, going beyond the von Zeipel–Lidov–Kozai mechanism. We show that the time to coalescence due to gravitational waves in such systems is modified. We then study the long-term evolution under this map, which lead to a random-walk-like behaviour of the inner eccentricity. While this behaviour is probably absent from isolated triples, it could exist in triples where the outer orbit is weakly coupled to a system with which it can exchange angular momentum, and we describe some properties of this random walk.Actions of highly eccentric orbits
Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 549:1 (2026) stag839
Abstract:
ABSTRACT The challenge presented by computing actions for eccentric orbits in axisymmetric potentials is discussed. In the limit of vanishing angular momentum about the potential’s symmetry axis, there is a clean distinction between box and loop orbits. We show that this distinction persists into the regime of non-zero angular momentum. In the case of a Stäckel potential, there is a critical value $I_{3\rm crit}(E)$ of the third integral $I_3$ below which $I_3$ does not contribute to the centrifugal barrier. An orbit is of box or loop type according as its value of $I_3$ is smaller or greater than $I_{3\rm crit}$. We give algorithms for determining $I_{3\rm crit}(E)$ and the critical action $J_{z\rm crit}$ below which orbits in any given potential are boxes. It is hard to compute the actions and especially the frequencies of orbits that have $J_z\simeq J_{z\rm crit}$ using the Stäckel Fudge. A modification of the Fudge that alleviates the problem is described.Turbulent damping of fast tidal oscillations by three-dimensional Rayleigh–Bénard convection with a radiating free surface
Monthly Notices of the Royal Astronomical Society Oxford University Press 549:3 (2026) stag909