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Dynamical Instability of Helical Vortex Filaments and Impurity Trapping Dynamics in Periodically Modulated Bose-Einstein Condensates

Vakhtang Mchedlishvili

Published May 29, 2026• 0 citations
Publisher

Abstract

This work investigates the dynamical stability, parametric excitation, and impurity (tracer) trapping kinetics of quantized vortex filaments in periodically modulated superfluid systems (Bose-Einstein Condensates and Helium-II). Within the framework of the Local Induction Approximation (LIA) and linear perturbation theory, we show that external quadrupole pressure/density modulation couples counter-propagating Kelvin waves, which is modeled via the Rotating Wave Approximation (RWA) as a damped Mathieu-type autonomous system. By employing the microscopic theory of Bogoliubov phonon scattering off a quantized vortex core (Pitaevskii-Fetter theory), we integrate a T⁵ temperature dependence of the mutual friction drag force. Accounting for this thermodynamic damping and the mechanical cavitation limit ε_max ≈ c_s/ξ, we analytically derive the minimum parametric excitation threshold ε_min(T) = C₁ T⁵. For a ⁸⁷Rb condensate, we establish that the stable helical phase is strictly bounded by a critical crossover temperature T_cross ≈ 34 pK, above which the thermal phonon damping demands a driving amplitude that inevitably causes structural cavitation. Furthermore, the kinetics of neutral impurity trapping into the vortex core are evaluated in two distinct regimes. In the viscous (overdamped) Helium-II regime (T ~ 1-1.5 K), we obtain the characteristic trapping time scaling τ_trap ∝ T⁴ R_part⁻¹. In the ballistic (underdamped) BEC regime (34 pK < T ~ 10-50 nK for straight vortices, and T < 34 pK for helical vortices), the trapping is driven by acoustic bremsstrahlung. By evaluating the inertial acceleration of the tracer via orbital force balance, we show that the trapping time scales quadratically with the density ratio, yielding τ_trap(BEC) ∝ (ρ_part / ρ_s)², which is numerically evaluated as ≈ 6.5 s for a density-matched macroscopic tracer. Finally, we estimate the critical trapping velocity to be v_c ≈ 0.1–1 mm/s. Thermodynamic Crossover (T_cross): Establishes that the stable helical vortex phase in a ⁸⁷Rb BEC is strictly bounded by T_cross ≈ 34 pK due to the competition between T⁵ phonon damping and the mechanical cavitation limit. Dual-Regime Impurity Trapping Kinetics: Derives the trapping time scaling laws for both the viscous Helium-II regime (τ_trap ∝ T⁴) and the ballistic BEC regime where capturing is mediated by acoustic bremsstrahlung (τ_trap(BEC) ∝ (ρ_part / ρ_s)²). Experimental Verification: Connects the theoretical boundaries to state-of-the-art microgravity BEC platforms (Cold Atom Lab and QUANTUS) and Feshbach tuning methods.

DOI
10.5281/zenodo.20442409

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This work investigates the dynamical stability, parametric excitation, and impurity (tracer) trapping kinetics of quantized vortex filaments in periodically modulated superfluid systems (Bose-Einstein Condensates and Helium-II). Within the framework of the Local Induction Approximation (LIA) and linear perturbation theory, we show that external quadrupole pressure/density modulation couples counter-propagating Kelvin waves, which is modeled via the Rotating Wave Approximation (RWA) as a damped Mathieu-type autonomous system. By employing the microscopic theory of Bogoliubov phonon scattering off a quantized vortex core (Pitaevskii-Fetter theory), we integrate a T⁵ temperature dependence of the mutual friction drag force. Accounting for this thermodynamic damping and the mechanical cavitation limit ε_max ≈ c_s/ξ, we analytically derive the minimum parametric excitation threshold ε_min(T) = C₁ T⁵. For a ⁸⁷Rb condensate, we establish that the stable helical phase is strictly bounded by a critical crossover temperature T_cross ≈ 34 pK, above which the thermal phonon damping demands a driving amplitude that inevitably causes structural cavitation. Furthermore, the kinetics of neutral impurity trapping into the vortex core are evaluated in two distinct regimes. In the viscous (overdamped) Helium-II regime (T ~ 1-1.5 K), we obtain the characteristic trapping time scaling τ_trap ∝ T⁴ R_part⁻¹. In the ballistic (underdamped) BEC regime (34 pK < T ~ 10-50 nK for straight vortices, and T < 34 pK for helical vortices), the trapping is driven by acoustic bremsstrahlung. By evaluating the inertial acceleration of the tracer via orbital force balance, we show that the trapping time scales quadratically with the density ratio, yielding τ_trap(BEC) ∝ (ρ_part / ρ_s)², which is numerically evaluated as ≈ 6.5 s for a density-matched macroscopic tracer. Finally, we estimate the critical trapping velocity to be v_c ≈ 0.1–1 mm/s. Thermodynamic Crossover (T_cross): Establishes that the stable helical vortex phase in a ⁸⁷Rb BEC is strictly bounded by T_cross ≈ 34 pK due to the competition between T⁵ phonon damping and the mechanical cavitation limit. Dual-Regime Impurity Trapping Kinetics: Derives the trapping time scaling laws for both the viscous Helium-II regime (τ_trap ∝ T⁴) and the ballistic BEC regime where capturing is mediated by acoustic bremsstrahlung (τ_trap(BEC) ∝ (ρ_part / ρ_s)²). Experimental Verification: Connects the theoretical boundaries to state-of-the-art microgravity BEC platforms (Cold Atom Lab and QUANTUS) and Feshbach tuning methods.
Atomtronic quantum sensors based on trapped superfluids offer a promising platform for high-precision inertial measurements where the dynamics of quantized vortices can serve as sensitive probes of external forces. We analytically investigate the persistent current oscillations between two density-coupled Bose-Einstein condensate rings of equal radius and show that the vortex dynamics is governed by low-energy acoustic excitations circulating through the condensate bulk. The oscillation frequency and damping rate are quantitatively predicted by a simplified hydrodynamic model, in agreement with Bogoliubov–de Gennes analysis and Gross-Pitaevskii simulations. We identify the critical dissipation separating persistent oscillations from overdamped vortex localization. Furthermore, we demonstrate that periodic modulation of the interring barrier at resonant frequencies enables controlled vortex transfer even when the condensates are well separated in density. These results clarify the role of collective hydrodynamic modes in circulation transfer and establish a framework for employing vortex dynamics in atomtronic quantum technologies.
The dynamics of interacting quantized vortex filaments in a rotating Bose–Einstein condensate existing in the Thomas–Fermi regime at zero temperature and obeying the Gross–Pitaevskii equation has been considered in the hydrodynamic “nonelastic” approximation. A noncanonical Hamilton equation of motion for the macroscopically averaged vorticity has been derived for a smoothly inhomogeneous array of filaments (vortex lattice) taking into account spatial nonuniformity of the equilibrium density of the condensate, which is determined by the trap potential. The minimum of the corresponding Hamiltonian describes the static configuration of the deformed vortex lattice against the preset density background. The condition of minimum can be reduced to a nonlinear second-order partial differential vector equation for which some exact and approximate solutions are obtained. It has been shown that if the condensate density has an anisotropic Gaussian profile, the equation of motion for the averaged vorticity has solutions in the form of a vector exhibiting a nontrivial time dependence, but homogeneous in space. An integral representation has also been obtained for the matrix Green function that determines the nonlocal Hamiltonian of a system of several quantized vortices of an arbitrary shape in a Bose–Einstein condensate with the Gaussian density. In particular, if all filaments are straight and oriented along one of the principal axes of the ellipsoid, we have a finitedimensional reduction that can describe the dynamics of the system of pointlike vortices against an inhomogeneous background. A simple approximate expression is proposed for the 2D Green function with an arbitrary density profile and is compared numerically with the exact result in the Gaussian case. The corresponding approximate equations of motion, describing the long-wavelength dynamics of interacting vortex filaments in condensates with a density depending only on transverse coordinates, have been derived.
Bose-Einstein condensation is a quantum statistical phase transition which was theoretically predicted almost a hundred years ago. After years of seminal research, physicists realized the first almost ideal Bose-Einstein condensates in ultracold dilute atomic gases in 1995. Since then, the theoretical and experimental methods concerning such systems have been developing rapidly, and many fascinating phenomena have been found in these novel quantum systems.\n\nBose-Einstein condensation occurs in a system consisting of massive bosons when a single quantum state becomes macroscopically occupied as the temperature is lowered below the transition temperature. In general, condensates consisting of repulsively interacting bosons exhibit superfluidity: Particle currents can flow in the system without dissipation and viscosity. Moreover, the velocity fields of condensates have to be irrotational, which severely restricts the rotational characteristics of these systems. Apart from the center of mass motion, the system may carry angular momentum in the form of elementary excitations or so-called quantized vortices.\n\nThis Thesis is a theoretical study of subjects related to stability and dynamics of quantized vortices in dilute atomic Bose-Einstein condensates. The precession and instability of off-centered vortices in trapped condensates is investigated both in the zero-temperature limit and at finite temperatures. Dynamical stability of multiply quantized vortices and vortex clusters is studied in axisymmetric trap geometries. Splitting of energetically and dynamically unstable multiply quantized vortices into singly quantized vortices is also studied. Finally, as a separate subject, tunneling of a condensate through a potential barrier is investigated. Majority of this work relies on numerical methods for solving the Gross-Pitaevskii and Bogoliubov equations, which are of central importance in the study of dilute atomic Bose-Einstein condensates.
Dilute atomic Bose-Einstein condensates support intriguing macroscopic excitations in the form of quantized vortices and dark solitons. In this thesis we present extensive quantitative studies of the dynamics of these phenomena in the limit of zero temperature, performed by numerical simulation of the Gross- Pitaevskii equation. We show that vortices and dark solitons are inherently unstable to acceleration through the condensate, leading to the emission of sound waves. Indeed, for a single vortex/soliton, the power emitted is proportional to the square of the local acceleration. However, due to the finite size of the condensate, the vortex/soliton reinteracts with the emitted sound. This coupling has an important effect on the ensuing dynamics, and we illustrate how it can be engineered to induce net decay, stabilise, or even drive energy into the vortex/soliton. Under the harmonic confinement typically employed to trap the condensates, the acceleration-induced decay is stabilised by reabsorption of the emitted sound. However, by modifying the trap geometry, e.g. by adding an inner dimple in which the soliton resides or an optical lattice potential, it is possible to break this equilibrium and so induce a net decay of the vortex/soliton in a controllable manner. The decay rate can be considerable and should be observable under current experimental conditions. The dynamical stability of quantized vortices is also relevant to the field of turbulence in superfluid Helium, where the motion of the vortices is induced by the surrounding distribution of vortices rather than density. We extend these results to this field, and additionally consider the interactions between two and three vortices, which are also found to involve sound emission. By exciting the sound field of the condensate it is possible to drive parametrically energy into a dark soliton. In a real dissipative environment, this can be used to stabilise the soliton decay. Finally, we illustrate the links between dark solitons and vortices: a dark soliton embedded in a three-dimensional system is prone to decay into vortex rings, while a vortex in a quasi-one-dimensional geometry cannot be supported and exists as a hybrid between a vortex and dark soliton, known as a solitonic vortex.
We propose a different type of Landau instability in trapped Bose-Einstein condensates by a helically moving environment. In the presence of quantized vortices, the instability can cause spontaneous radiation and amplification of Kelvin waves. This study gives a microscopic understanding of the Donnelly-Glaberson instability which was known as the hydrodynamic instability in superfluid helium. The Donnelly-Glaberson instability can be a powerful tool for observing the dispersion relation of Kelvin waves, vortex reconnections, and quantum turbulence in atomic Bose-Einstein condensates.
We have theoretically investigated Kelvin waves of quantized vortex lines in trapped Bose-Einstein condensates. Counterrotating perturbation induces an elliptical instability to the initially straight vortex line, driven by a parametric resonance between a quadrupole mode and a pair of Kelvin modes of opposite momenta. Subsequently, Kelvin waves rapidly decay to longer wavelengths emitting sound waves in the process. We present a modified Kelvin wave dispersion relation for trapped superfluids and propose a simple method to excite Kelvin waves of specific wave number.