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THE FASCINATING PHYSICS OF SOLID 3He

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Title: THE FASCINATING PHYSICS OF SOLID 3He


1
Le coche et la mouche Sur un chemin montant,
sablonneux, malaise, Et de tous les cotes au
soleil expose, Six forts chevaux tiraient un
coche Jean de La Fontaine
M. Roger
?
The coach and the fly Over a hilly, sandy and
difficult road, From every side exposed to the
sun, Six strong horses were pulling a coach
... Jean de La Fontaine
2
THE FASCINATING PHYSICS OF SOLID 3He ITS IMPACT
IN OTHER FIELDS
  • Michel Roger
  • CEA DRECAM SPEC

3
Historical survey 1
  • Theory
  • 1926-1930
  • Heisenberg1, Dirac2 general concept of an
    effective exchange Hamiltonian for almost
    localised identical fermions
  • Hex ? (-1)p JP P?
  • Experiment
  • up to 1975
  • No evidence for any experimental system for
    which permutations involving more than two
    particles
  • are relevant
  • (Nothing beyond the so-called Heisenberg model)

4
Historical survey 2
  • Theory
  • 1965
  • Thouless3
  • Puts forward the idea that three and four-spin
    exchange might be important in solid 3He and lay
    out the basis for a calculation of their
    frequencies JP from first principles
  • Proves that 2, 4, particle cyclic exchanges are
    antiferromagnetic while 3, 5, particle cyclic
    exchanges are ferromagnetic.
  • Experiment
  • Nothing new!

5
Historical survey 3
  • Theory
  • 1975
  • J. H. Hetherington5
  • The data of D. Adams et al. are explained by
    significant four-particle exchange processes
  • Experiment
  • 1975
  • D. Adams et al.4
  • Experimental evidence of a first order
    transition at 1mK to some antiferromagnetic order
    in solid bcc 3He incompatible with a simple
    Heisenberg model

6
Historical survey 4
  • Theory
  • 1977-1980
  • Delrieu, Hetherington, Roger9
  • Quantitative interpretation of all experimental
    data with a multiple spin exchange Hamiltonian
  • In particular, the competition between the two
    exotic phases is a signature of the  quantum
    frustration  resulting from the competition
    between ferromagnetic three-particle exchange and
    antiferromagnetic four-spin exchange
  • Experiment
  • 1977-1980
  • Adams et al.6, Godfrin et al7
  • Experimental evidence for a competition between
    two ordered phases.
  • A low field phase
  • A (moderately-high) -field phase with exotic
    properties.
  • 1980
  • Osheroff et al.8 Indirect proof byNMR of the
    unexpected symmetry  uudd  of the low-field
    phase

7
Historical survey 5
  • Theory
  • 1980
  • J. M Delrieu10 prediction of the ferromagnetism
    of the hcp phase based on the argument that
    steric hinderance favor 3 particle exchange in a
    compact lattice.
  • Experiment
  • 1985
  • Takano et al.11 measurement of the
    susceptibility of hcp solid 3He showing
    ferromagnetic behavior
  • 1996
  • Adams, Takano et al.12 reach the ferromagnetic
    phase by direct nuclear adiabatic demagnetization

8
Historical survey 6
  • Theory
  • 1981-84
  • Delrieu13 Roger14 justification of the
    hierarchy of various exchange processes from
    first principles through WKB approximation
  • 1987
  • Ceperley Jacucci15 calculation of exchange
    frequencies from first principles though
    Monte-Carlo methods.
  • Experiment
  • 1985
  • Benoit, Bossy et al16. direct observation of the
    low field  uudd  phase of bcc 3He through
    neutron diffraction

9
Present situation
  • A unique model system for which we are able to
    start from the first principles, predict
    quantitatively the expected thermodymamic
    properties and compare quantitatively with
    experimental results
  • Most  indirect  consequences of the
    Multiple-Spin-Exchange model, as the behavior of
    a large number thermodynamic properties, have
    been verified experimentally.
  • Nevertheless, the direct observation by neutron
    diffraction of the most important prediction
    which results from the intrisically  quantum
    frustrated  nature of the model the exotic high
    field phase, is missing.
  • Neutron critical scattering also offer the most
    direct measurement of various exchange parameter,
    which should be interesting to compare with
    Monte-Carlo theoretical predictions.

10
The role of Saclay Il semble que ce soit Un
sergent de bataille allant en chaque endroit
Faire avancer ses gens, et hater la victoire
.  (La Fontaine)
  • Will be crucial in the last year of the project
    to participate with experimentalists to the
    quantitative interpretation of the results.
  • ? A postdoctoral theoretician will be appointed
    from next october
  • Preparation of the project of direct
    characterisation of exchange processes through
    inelastic neutron scattering, in close
    collaboration with HMI and the University of
    Liverpool.
  • Spreading of our results to a large community,
    including physicists interested in other
    strongly interacting fermion systems where
    relevant four-particle exchange processes have
    been theoretically predicted.
  • ? Organisation of a largely open spring school
    in April 2003

11
Multiple-spin exchange in the Wigner Solid
  • 1984
  • Delrieu13 Roger14 WKB calculation of exchange
    processes in the two-dimensional Wigner Solid of
    electrons. Three-particle exchange is dominant
    near the classical limit (low density), four
    particle exchange might be also significant at
    higher densities.
  • 2000
  • Bernu Ceperley17 Ab initio Monte-Carlo
    calculation of exchange processes in the Wigner
    Solid. Confirmation of the WKB results near the
    classical limit. Close to melting the hierarchy
    of various exchange processe is similar to that
    calculated and observed for two-dimensional solid
    3He layers adsorbed on graphite.
  • Present experimental situation
  • A lot of excitement and controversies about the
    possible observation of the 2D Wigner solid in
    AgGa and Si MOSFET inversion layers!

12
Four-spin exchange in the CuO2 planes of hight Tc
superconducting cuprates
  • 1988
  • Delrieu Roger18 theoretical prediction of
    significant four-spin exchange in the CuO2 planes
    of high Tc superconducting cuprates, based on a
    large U expansion of a three-band Hubbard model.
  • 2000
  • Calzado Malrieu19 same conclusion through
    ab-initio quantum-chemical calculations on finite
    clusters.
  • Present experimental situation
  • Although most experimental thermodynamic
    properties of the anti-ferromagnetic phase of
    these compounds are generally interpreted with a
    simple Heisenberg model, some results, which are
    in contradiction with the pure Heisenberg model
    can be explained with a small but significant
    amount of four-spin exchange
  • - The susceptibility data M. Roger20
  • - The anomalously broad two (and four?) magnon
    Raman spectra S. Sugai et al21, 1990
  • - Magnon spectrum obtained through
    high-resolution inelastic neutron scattering
  • Coldea et al22, 2000

13
Conclusion
  • Solid 3He a model system involving fundamental
    quantum mechanical processes
  • Has long been considered, from theoretical point
    of view, as marginal.
  • Should be now advertised as an archetype among
    other strongly interacting identical-fermion
    systems illustrating the same fundamental
    physics
  • - Wigner solid
  • - High Tc superconducting cuprates
  • - Other magnetic systems (the list is open! )

14
References
  • 1 Heisenberg, Z. Phys. 38, 411 (1926)
  • 2 P.A.M Dirac, Proc. Roy. Soc. A123, 714
    (1929)
  • 3 D.J. Thouless, Proc. Phys. Soc. 86, 893
    (1965)
  • 4 R.B. Kummer, E.D. Adams, W.P. Kirk, A.S.
    Greenberg, R.M. Mueller, C.Y Britton
  • and D.M. Lee, Phys. Rev. Lett. 34, 517 (1975)
  • 5 J.H. Hetherington, Phys. Rev. Lett. 35, 1442
    (1975)
  • 6 E.D. Adams, J.M. Delrieu and A. Landesman,
    J. Phys. Lett. 39, L190 (1978)
  • 7 H. Godfrin, G. Frossati, A. Greenberg, B.
    Hebral and D. Thoulouze, Phys. Rev. Lett.
  • 44, 1695 (1980).
  • 8 D.D. Osheroff, M.C. Cross and D.E. Fisher,
    Phys. Rev. Lett. 44, 792 (1980)
  • 9 M. Roger, J.M. Delrieu and J.H.
    Hetherington, Rev. Mod. Phys. 55, 1 (1980).
  • 10 J.M. Delrieu et al. J. Low. Temp. Phys. 40,
    71 (1980)
  • 11 Y. Takano, N. Nishida, Y. Miura, H.
    Fukuyama, H. Ishimoto and S. Ogawa,
  • Phys. Rev. Lett. 55, 1490 (1985)

15
References
  • 12 T. Lang, P.L. Moyland, D.A. Sergatskov,
    E.D. Adams and Y. Takano, Phys. Rev. Lett.
  • 77, 322 (1996)
  • 13 J.M. Delrieu, unpublished (1981)
  • 14 M. Roger, Phys. Rev. B 30, 6432 (1984)
  • 15 D.M. Ceperley and G. Jacucci, Phys. Rev.
    Lett. 58, 1648 (1987)
  • 16 A. Benoit, J. Bossy, J. Flouquet, J.
    Schweizer, J. de Physique Lettres, L923 (1985)
  • 17 B. Bernu, L. Candido, and D.M. Ceperley
    Phys. Rev. Lett. 86, 870 (2001)
  • 18 M. Roger and J.M. Delrieu, Phys. Rev. B39,
    2299 (1989)
  • 19 C.J. Calzado and J.P. Malrieu, Phys. Rev.
    B63, 214520 (2001)
  • 20 M. Roger, to be published.
  • 21 S. Sugai et al. Phys. Rev. B42, 1405 (1990)
  • 22 R. Coldea et al. Phys. Rev. Lett. 86, 5377
    (2001)

16
The moral of the fable
  • Ainsi certaines gens, faisant les empresses,
  • S introduisent dans les affaires,
  • Ils font partout les nécessaires,
  • Et, partout importuns, devraient être chasses.
  • Jean de La Fontaine.
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