Abstract

The composite cosmological objects -- Kibble-Lazarides-Shafi (KLS) walls bounded by strings and cosmic strings terminated by Nambu monopoles -- could be produced during the phase transitions in the early Universe. Recent experiments in superfluid $^3$He reproduced the formation of the KLS domain walls, which opened the new arena for the detailed study of those objects in human controlled system with different characteristic lengths. These composite defects are formed by two successive symmetry breaking phase transitions. In the first transition the strings are formed, then in the second transition the string becomes the termination line of the KLS wall. In the same manner, in the first transition monopoles are formed, and then in the second transition these monopoles become the termination points of strings. Here we show that in the vicinity of the second transition the composite defects can be described by relative homotopy groups. This is because there are two well separated length scales involved, which give rise to two different classes of the degenerate vacuum states, $R_1$ and $R_2$, and the composite objects correspond to the nontrivial elements of the group $\pi_n(R_1,R_2)$. We discuss this on example of the so-called polar distorted B phase, which is formed in the two-step phase transition in liquid $^3$He distorted by aerogel. In this system the string monopoles terminate spin vortices with even winding number, while KLS string walls terminate on half quantum vortices. In the presence of magnetic field, vortex-skyrmions are formed, and the string monopole transforms to the nexus. We also discuss the integer-valued topological invariants of those objects. Our consideration can be applied to the composite defects in other condensed matter and cosmological systems.

Highlights

  • The combined topological objects, such as strings terminated by Nambu monopoles [1] and Kibble-Lazarides-Shafi (KLS) walls bounded by strings [2,3], typically appear at two successive symmetry breaking phase transitions [4]

  • We discussed the topology, which emerges in two-step phase transition in the vicinity of the second transition

  • An example is provided by the second-order phase transition from the normal 3He to the polar phase followed by the secondorder phase transition from the polar phase to the PdB phase experimentally observed in superfluid 3He in nafen [9]

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Summary

INTRODUCTION

The combined topological objects, such as strings terminated by Nambu monopoles [1] and Kibble-Lazarides-Shafi (KLS) walls bounded by strings [2,3], typically appear at two successive symmetry breaking phase transitions [4]. Earlier it was shown that the nonaxisymmetric core of the singly quantized vortex [29,30], which was observed in bulk superfluid 3He-B [31], can be considered as a pair of HQVs connected by the KLS wall [32,33] This wall is rather short: only of few coherence length size. VI we summarize our results and discuss the role of these objects in formation of the numerous superfluid glass states, which may exist in aerogel [45,46,47]

CONVENTIONAL SYMMETRY BREAKING SCHEME
Transition from normal phase to polar phase
From polar phase to PdB phase
From normal phase to PdB phase
Defects in polar phase due to transition from the normal phase vacuum
Defects in PdB phase due to transition from polar phase vacuum
Spin vortices
Defects in PdB phase due to transition from normal phase vacuum
The fate of monopoles and half-quantum vortices in the PdB phase
The fate of half-quantum vortices in the PdB phase and the KLS wall
Combined objects and classification by relative homotopy groups
Wall bounded by string—KLS string wall
Strings terminated by monopole—string monopole
SKYRMIONS AND NEXUS IN THE PRESENCE OF MAGNETIC FIELD
CONCLUSION AND DISCUSSION
No magnetic field
In the presence of magnetic field
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