The behavior of the order parameter A ai (x) is investigated for a planar interface between 3He-A and 3He-B. Boundary conditions are derived and the surface energy is calculated in excellent agreement with experiment. Our energy is 30% lower than a previous estimate which assumed the presence of a planar phase in the transition region.
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References
D. D.Osheroff and M. C. Cross, Phys. Rev. Lett. 38, 905 (1977).
M. C. Cross, in Quantum Fluids and Solids, 1977, S. B. Trickey, E. D. Adams, and J. W. Dufty, eds. (Plenum Press, New York, 1977).
D. Mermin, Physica 90B, 1 (1977).
W. F. Brinkman, J. W. Serene, and P. W. Anderson, Phys. Rev. A 10, 2386 (1974).
R. C. Richardson, Erice Lectures 1977, in Quantum Liquids, J. Ruvalds and T. Regge, eds. (North-Holland, 1978).
Y. Kuroda and A. D. S. Nagi, J. Low Temp. Phys. 25, 569 (1978).
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Alexander von Humboldt Fellow.
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Kaul, R., Kleinert, H. Surface energy and textural boundary conditions between A and B phases of 3He. J Low Temp Phys 38, 539–552 (1980). https://doi.org/10.1007/BF00115487
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DOI: https://doi.org/10.1007/BF00115487