Abstract
We describe an apparatus allowing the observation of the NMR static longitudinal component of nuclear magnetizationM z by a SQUID at low magnetic fields and atT=4.2 K in Plexiglas, Teflon, and CaF2. The higher order NMR Larmor lines at 2f 0, 3f 0, and 4f 0, wheref 0 is the Larmor frequency of the allowed NMR line, were measured. These lines correspond to a flip of two, three, and four spins, respectively, by one photon. The amplitudes of 2f 0 and 3f 0 lines and their field dependences show that the common assertion that the forbidden lines at 2f 0 and 3f 0 appear in the same order of perturbation theory and that their intensity decreases with static magnetic fieldB 0 asB −20 is wrong. In fact, the third Larmor line 3f 0 appears at higher order than the second Larmor line 2f 0 and its intensity decreases asB −40 . This is also shown by a theoretical calculation of its intensity. For the first time the NMR SQUID technique allowed the detection of the 4f 0 line, corresponding to the simultaneous flip of four spins by one photon.
Similar content being viewed by others
References
A. H. Silver and J. E. Zimmerman,Appl. Phys. Lett. 10, 142 (1967).
E. P. Day,Phys. Lett. 29, 540 (1972).
R. A. Webb,Rev. Sci. Instrum. 48, 1585 (1977).
D. J. Meredith, G. R. Pickett, and O. G. Symko,J. Low Temp. Phys. 13, 607 (1973).
J. H. Van Vleck,Phys. Rev. 74, 1168 (1948).
A. Abragam,The Principles of Nuclear Magnetism (Oxford University Press, 1961), p. 105.
C. P. Slichter,Principles of Magnetic Resonance (Springer-Verlag, Berlin, 1978), p. 61.
G. E. Pake,Paramagnetic Resonance (Benjamin, New York, 1962), p. 82.
A. Lösche,Kerninduktion (VEB Deutcher der Wissenschaften, Berlin, 1957), p. 271.
A. G. Anderson,Phys. Rev. 115, 863 (1959).
A. G. Anderson,Phys. Rev. 125, 1517 (1962).
A. I. Ahonen, T. Kodama, M. A. Paalanen, R. C. Richardson, W. Schoepe, and Y. Takano,J. Phys. C 9, 1665 (1976).
J. R. Franz and C. P. Slichter,Phys. Rev. 148, 287 (1966).
R. V. Chamberlin, L. A. Moberly, and O. G. Symko,J. Low. Temp. Phys. 35, 337 (1979).
J. P. Eckström, J. F. Jacquinot, M. T. Loponen, J. K. Soini, and P. Kumar,Physica 98B, 45 (1979).
D. Konotop,Fiz. Nizk. Temp. 8, 665 (1982).
L. J. F. Broer,Physica X, 51 (1943).
A. Wright,Phys. Rev. 76, 1826 (1949).
H. Cheng,Phys. Rev. 124, 1359 (1961).
H. Goldman,Spin Temperature and Nuclear Magnetic Resonance in Solids (Clarendon Press, Oxford, 1970), p. 138.
M. Kohl, M. Odehnal, V. Petříček, and R. Tichý,SQUID '85 (Walter de Gruyter, Berlin, 1985), p. 879.
M. Kohl, M. Odehnal, V. Petříček, and R. Tichý, inProceedings of the 17th International Symposium on Low Temperature Physics (F. S. Universität Jena, German Democratic Republic, 1985), p. 117.
M. Kohl, M. Odehnal, V. Petříček, R. Tichý, and J. Chalupecký, inProceedings 4th Czechloslovak Symposium on Weak Superconductivity (Electrotechnical Institute, Smolenice, 1986), p. 194.
L. S. Vlasenko, N. V. Zavarickij, C. V. Sorokin, and V. G. Fleisher,Zh. Eksp. Teor. Fiz. 91, 1496 (1986).
W. P. Slichter,J. Polymer Sci. 24, 173 (1957).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Kohl, M., Odehnal, M., Petříěek, V. et al. Observation of higher order NMR larmor lines by SQUID in solids at low magnetic field. J Low Temp Phys 72, 319–343 (1988). https://doi.org/10.1007/BF00682103
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF00682103