Abstract:Ferromagnetic spin-1 Bose-Einstein condensates in the broken-axisymmetric phase support polar-core spin vortices (PCVs), which are intimately linked to the nonequilibrium dynamics of the system. For a purely transversely magnetized system, the Turner point-vortex model predicts that PCVs behave like massive charged particles interacting via a two-dimensional Coulomb potential. We test the accuracy of the Turner model for two oppositely charged PCVs, via comparisons with numerical simulations. While the bare Tu… Show more
“…As already mentioned, it would be interesting to deepen the study of more complex ghostvortex configurations, both within a suitable analytical model and by means of numerical experiments. Besides this, another possibility is certainly the investigation of the normal (Tkachenko-like) modes of a massive-vortex N -gon (possibly in the presence of mass imbalance [66] or damping [67]), which will thus generalize the results of Ref. [45] obtained in the massless case and further stimulate the current experimental research in real-time vortex dynamics [19,68,69].…”
Ghost vortices constitute an elusive class of topological excitations in quantum fluids since the relevant phase singularities fall within regions where the superfluid density is almost zero. Here we present a platform that allows for the controlled generation and observation of such vortices. Upon rotating an imbalanced mixture of two-component Bose-Einstein condensates (BECs), one can obtain necklaces of real vortices in the majority component whose cores get filled by particles from the minority one. The wavefunction describing the state of the latter is shown to harbour a number of ghost vortices which are crucial to support the overall dynamics of the mixture. Their arrangement typically mirrors that of their real counterpart, hence resulting in a "dual" ghostvortex necklace, whose properties are thoroughly investigated in the present paper. We also present a viable experimental protocol for the direct observation of ghost vortices in a 23 Na + 39 K ultracold mixture. Quenching the inter-component scattering length, some atoms are expelled from the vortex cores and, while diffusing, swirl around unpopulated phase singularities, thus turning them directly observable.
“…As already mentioned, it would be interesting to deepen the study of more complex ghostvortex configurations, both within a suitable analytical model and by means of numerical experiments. Besides this, another possibility is certainly the investigation of the normal (Tkachenko-like) modes of a massive-vortex N -gon (possibly in the presence of mass imbalance [66] or damping [67]), which will thus generalize the results of Ref. [45] obtained in the massless case and further stimulate the current experimental research in real-time vortex dynamics [19,68,69].…”
Ghost vortices constitute an elusive class of topological excitations in quantum fluids since the relevant phase singularities fall within regions where the superfluid density is almost zero. Here we present a platform that allows for the controlled generation and observation of such vortices. Upon rotating an imbalanced mixture of two-component Bose-Einstein condensates (BECs), one can obtain necklaces of real vortices in the majority component whose cores get filled by particles from the minority one. The wavefunction describing the state of the latter is shown to harbour a number of ghost vortices which are crucial to support the overall dynamics of the mixture. Their arrangement typically mirrors that of their real counterpart, hence resulting in a "dual" ghostvortex necklace, whose properties are thoroughly investigated in the present paper. We also present a viable experimental protocol for the direct observation of ghost vortices in a 23 Na + 39 K ultracold mixture. Quenching the inter-component scattering length, some atoms are expelled from the vortex cores and, while diffusing, swirl around unpopulated phase singularities, thus turning them directly observable.
“…Possible future research directions include the study of massive-vortex dynamics on curved surfaces, thus generalizing the analysis developed in Refs. [21,26,27,28] to the case of nonzero core mass, the introduction of an inter-component coherent coupling [29,30] which may result in time-dependant core masses, component-selective potentials [31,32], dissipation [33], the extension to three-dimensional systems [34,35] and to miscible components [36,37,38]. Also, we are going to investigate the properties of massive-vortex lattices and their associated Tkachenko-like oscillation modes [23].…”
Section: Conclusion and Future Perspectivesmentioning
We consider the dynamical properties of quantum vortices with filled massive cores, hence the term “massive vortices”. While the motion of massless vortices is described by first-order motion equations, the inclusion of core mass introduces a second-order time derivative in the motion equations and thus doubles the number of independent dynamical variables needed to describe the vortex. The simplest possible system where this physics is present, i.e. a single massive vortex in a circular domain, is thoroughly discussed. We point out that a massive vortex can exhibit various dynamical regimes, as opposed to its massless counterpart, which can only precess at a constant rate. The predictions of our analytical model are validated by means of numerical simulations of coupled Gross-Pitaevskii equations, which indeed display the signature of the core inertial mass. Eventually, we discuss a nice formal analogy between the motion of massive vortices and that of massive charges in two-dimensional domains pierced by magnetic fields.
“…17 A detailed knowledge with mechanics of quantifying vortex systems to monopoles 18 to more specific Lagrangian and Hamiltonian derivation mathematically of vortex systems suitable to analyze vacuum quagmire with monopole & the dipole had already been modeled. 2,[19][20][21][22][23] These studies show that monopoles' physics had mechanics like the fluid system's hydro dynamical vortex systems Searches for monopoles, with scientists all over the world, consisted of two categories experimentally typically: (1) detecting preexisting monopoles, (2) creating and detecting then new monopoles. [24][25][26][27][28][29][30][31][32][33] Mathematical techniques explored here to solve eigen value problem might set a precedence to abstract who listic observational physics with mathematical preciseness, applicable further to provable generalized quantum relativistic grand formalism.…”
Section: Introductionmentioning
confidence: 99%
“….i) and(21.ii) together form Equation(21).Equations(19),(20), & (21) will give result: .i) and(22.ii) together form Equation(22).Performing differential algebraic manipulations, like Equation (19), having set of differential equations, for | λ >=…”
Our observations of magneton with Ferrolens shows evidence pointing to such magneton entity, and more evidently in recent results with the synthetic vacuum unipole experiments. Physics formalism ansatz novel model analyses demonstrate how vacuum quanta may have sufficient energy for vacuum genesis, by constructing eigen spinors of zero_point microblackhole Hamiltonian quantum mechanics with Helmholtz decomposition matrix of gradient and rotational tensors, that are characteristic of translational vortex fields. With these mathematical physics processes, we obtain resulting energy fields spatial property partial differential equations characterizing eigen state energetics of zero point vacuum quagmire, as well as eigen state vortex fields of micro black hole, both together making up plasmodial zones within quagmire. Specific eigen spinors Hamiltonian partial differential equations quantifying energy and fields eigen functions. Vacuum that is dipole vacuum may have superposition of complex input of quagmire vortex fields acting to create nonhermitian quantum relativistic physics.
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