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Triple-core structure of the double-core vortex in superfluid $^3$He-B

Riku Rantanen

Abstract

The order parameter of superfluid $^3$He involves nine complex components, and the multicomponent structure allows quantized vortices in superfluid $^3$He to have complicated cores. One of the vortices found in the B phase is the double-core vortex, which has been often described as a pair of two half-quantum vortices (HQVs) connected by a domain wall. Our numerical calculations of the core structure suggest an alternative representation of the vortex as a combination of three vortices, one in each component of the spin-triplet superfluid. Based on the results we present a qualitative analytical model for the triple-core structure of the double-core vortex. Additionally we numerically calculate the structure of a double-core vortex stretched between pinning sites, and show that the HQV picture becomes more applicable when separation between subcores becomes large.

Triple-core structure of the double-core vortex in superfluid $^3$He-B

Abstract

The order parameter of superfluid He involves nine complex components, and the multicomponent structure allows quantized vortices in superfluid He to have complicated cores. One of the vortices found in the B phase is the double-core vortex, which has been often described as a pair of two half-quantum vortices (HQVs) connected by a domain wall. Our numerical calculations of the core structure suggest an alternative representation of the vortex as a combination of three vortices, one in each component of the spin-triplet superfluid. Based on the results we present a qualitative analytical model for the triple-core structure of the double-core vortex. Additionally we numerically calculate the structure of a double-core vortex stretched between pinning sites, and show that the HQV picture becomes more applicable when separation between subcores becomes large.
Paper Structure (5 sections, 15 equations, 2 figures)

This paper contains 5 sections, 15 equations, 2 figures.

Figures (2)

  • Figure 1: A double-core vortex with the two half-cores aligned along the $y$ axis. The data is taken from a numerical calculation at $p = 20$ bar and $T = 0.80T_{\rm{c}}$. Distances are given in units of the temperature and pressure dependent Ginzburg-Landau coherence length $\xi\approx 30\text{ nm}$. (Left) The spatial profile of the order parameter in the angular momentum basis in the region $x,y\in [-10\xi, 10\xi]$. The amplitudes are shown for all nine components and the phase for the three components with phase winding in the bulk. The three distinct subcores are clearly visible in the $C_{-+}$, $C_{00}$, and $C_{+-}$ components. (Right) The same order parameter amplitudes on the $y$ axis. The half-cores are located at $y = \pm 3.5\xi$.
  • Figure 2: The order parameter along the $y$ axis for a stretched double-core vortex calculated at $p = 20\text{ bar}$ and $T = 0.80T_{\rm{c}}$. The lines represent the components as labeled in Figure \ref{['fig:doublecorecomponents']}. The pinning sites are cylindrical obstacles with a diameter of $\xi$, marked by the grey regions. The state shown in panel (a) corresponds to $7\xi$ distance between cores, which is the equilibrium distance found in the bulk. Panels (b), (c) and (d) correspond to spacings of $15\xi$, $25\xi$ and $40\xi$, respectively.