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Supercooling of the A phase of (3)He
Because of the extreme purity, lack of disorder, and complex order parameter, the first-order superfluid (3)He A–B transition is the leading model system for first order transitions in the early universe. Here we report on the path dependence of the supercooling of the A phase over a wide range of p...
Autores principales: | , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9832038/ https://www.ncbi.nlm.nih.gov/pubmed/36627275 http://dx.doi.org/10.1038/s41467-022-35532-7 |
Sumario: | Because of the extreme purity, lack of disorder, and complex order parameter, the first-order superfluid (3)He A–B transition is the leading model system for first order transitions in the early universe. Here we report on the path dependence of the supercooling of the A phase over a wide range of pressures below 29.3 bar at nearly zero magnetic field. The A phase can be cooled significantly below the thermodynamic A–B transition temperature. While the extent of supercooling is highly reproducible, it depends strongly upon the cooling trajectory: The metastability of the A phase is enhanced by transiting through regions where the A phase is more stable. We provide evidence that some of the additional supercooling is due to the elimination of B phase nucleation precursors formed upon passage through the superfluid transition. A greater understanding of the physics is essential before (3)He can be exploited to model transitions in the early universe. |
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