A Schrödinger equation is derived which allows an improvement in the wave function of a quantum crystal inside the tunneling duct for exchange. This equation is used to derive a simple estimate of the exchange rate accurate enough to be used to compare various exchange mechanisms (two-body, three-body cyclic, etc.). We find that the 3He bulk hcp crystal and 3He surface triangular crystals have their exchange dominated by three-body cyclic exchange. Therefore the dominant part of the spin Hamiltonian will be Heisenberg nearest neighbor ferromagnetic. This result explains the ferro-magnetic tendency observed in adsorbed 3He films. A ferromagnetic transition in hcp 3He at the lowest pressures is predicted at 0.05±0.01 mK, corresponding to a Curie-Weiss constant of 0.075 \+ -0.015 mK.
Similar content being viewed by others
References
J. H. Hetherington and F. D. C. Willard, Phys. Rev. Lett. 35, 1442 (1975).
M. Roger, J. M. Delrieu, and A. Landesman, Phys. Lett. 62A, 449 (1977).
J. M. Delrieu and M. Roger, J. Phys. (Paris) (Coll. C6), 39, C-123 (1978).
I. Okada and K. Ishikawa, Prog. Theor. Phys. 60, 11 (1978); I. Izuyana and K. Utsumi, in Proc. ULT Hakone Symposium (1977), p. 199.
A. K. McMahan and J. W. Wilkins, Phys. Rev. Lett. 35, 376 (1975).
W. Mullin, Phys. Rev. B 12, 3718 (1975).
R. A. Guyer, Phys. Rev. A 9, 1452 (1974).
A. K. McMahan and R. A. Guyer, Phys. Rev. A 7, 1105 (1973).
D. J. Thouless, Proc. Phys. Soc. 86, 893 (1965).
C. Herring, in Magnetism, C. T. Rado and H. Suhl, eds. (Academic Press, London, 1966), Vol. II
F. London, in Superfluids (Wiley, New York, 1954), Vol. II, Section 56, pp. 29–31.
J. P. Hansen, D. Levesque, and D. Schiff, Phys. Rev. A 3, 776 (1971).
M. H. Kalos, D. Levesque, and L. Verlet, Phys. Rev. A 9, 2178 (1974).
A. Landesman, Ann. Phys. (France) 8, (1973–74), Fig. 9.
A. Abragam, C. R. Acad. Sci. Paris 284, 255 (1977).
A. F. Andreev, J. Phys. (Paris) (Coll. C6) 39, C6–1257 (1978).
A. I. Ahonen, T. A. Alvesalo, T. Haavasoja, and M. C. Veuro, J. Phys. (Paris) (Coll. C6) 39, C6–285 (1978); J. Phys. C 9, 1665 (1976).
H. M. Bozler, T. Bartolac, K. Lueyand, and A. L. Thomson, J. Phys. (Paris) (Coll. C 6) 39, C6–283 (1978).
K. SatŌ and T. Sugawara, J. Phys. (Paris) (Coll C6) 39, C6–281 (1978).
H. Godfrin, G. Frossati, D. Thoulouze, M. Chapellier, and W. G. Clark, J. Phys. (Paris) (Coll. C6) 39, C6–287 (1978).
R. A. Guyer, Phys. Rev. Lett. 39, 1091 (1977).
M. Heritier and P. Lederer, Phys. Rev. Lett. 42, 1068 (1979).
M. T. Beal-Monod and D. L. Mills, J. Phys. (Paris) (Coll. C6) 39, C6–290 (1978).
T. Banks, C. N. Bender, and T. S. Wu, Phys. Rev. D 8, 3345, 3366 (1973).
G. S. Rushbrooke, G. A. Baker, and P. J. Wood, in Phase Transitions and Critical Phenomena, C. Domb and M. S. Green (Academic Press, New York,G. S. Rushbrooke 1974), Vol. 3, Chapter 5.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Delrieu, J.M., Roger, M. & Hetherington, J.H. Exchange and magnetic order in HCP 3He and adsorbed 3He with triangular lattice. J Low Temp Phys 40, 71–87 (1980). https://doi.org/10.1007/BF00115983
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF00115983