On the interaction of nuclear spins in a crystalline lattice

Abstract The exchange of energy between a system of nuclear spins, immersed in a strong magnetic field H o , and the lattice vibrations of insulating crystals has been investigated experimentally by the method of nuclear magnetic resonance absorption. The resonance in calciumfluoride, some hydrated sulphates and some alkalihalides, has been observed between 300°K and 1°K, at 30.5 and 9.5 Mc/sec. The measured spin-lattice relaxation times T 1 range from 10 −3 to 10 4 sec, and disagree violenty — in many cases by more than a factor 10 6 — with Waller's theory of paramagnetic relaxation. It is shown that the relaxation time T 1 is determined by paramagnetic impurities occurring in the lattice. An order of magnitude theory is developed taking these impurities into account. The quanta absorbed by the system of nuclear spins from the external radiofrequeney field diffuse toward the impurities. The energy is then transferred to the lattice vibrations via the fluctuating magnetic field from the impurity. The first process depends on the concentration of the impurities, the second on H o and on the relaxation time ϱ of the impurity. The experimental data receive at least qualitative explanation in terms of these quantities. In some cases a direct heat contact between the system of nuclear spins and the system of impurity spins proves to be important. Then T i is independent of the lattice temperature.

[1]  J. Griffiths,et al.  Paramagnetic Resonance in Copper Sulphate , 1948, Nature.

[2]  E. Purcell,et al.  Relaxation Effects in Nuclear Magnetic Resonance Absorption , 1948 .

[3]  R. Kronig On the theory of absorption and dispersion in paramagnetic crystals under alternating magnetic fields , 1938 .

[4]  B. V. Rollin,et al.  Nuclear Paramagnetism at Low Temperatures , 1948 .

[5]  R. Kronig,et al.  On the theory of absorption and dispersion in paramagnetic and dielectric media , 1936 .

[6]  P. R. Weiss,et al.  Magnetic Resonance Absorption in the Chrome Alums , 1948 .

[7]  J. H. Van Vleck,et al.  The Dipolar Broadening of Magnetic Resonance Lines in Crystals , 1948 .

[8]  C. Gorter,et al.  Negative result of an attempt to observe nuclear magnetic resonance in solids , 1942 .

[9]  J. V. Vleck The Influence of Dipole‐Dipole Coupling on the Specific Heat and Susceptibility of a Paramagnetic Salt , 1937 .

[10]  H. Casimir,et al.  Measurememts on paramagnetic relaxation in chromium potassium alum , 1941 .

[11]  C. Bouwkamp,et al.  On the time of relaxation due to spin-spin interaction in paramagnetic crystals , 1938 .

[12]  J. V. Vleck Paramagnetic Relaxation Times for Titanium and Chrome Alum , 1940 .

[13]  J. V. Vleck,et al.  The Role of Exchange Interaction in Paramagnetic Absorption , 1947 .

[14]  R. Kronig On the mechanism of paramagnetic relaxation , 1939 .

[15]  R. Pound The Magnetic Moments of Cu 63 and Cu 65 , 1948 .

[16]  G. Pake Nuclear Resonance Absorption in Hydrated Crystals: Fine Structure of the Proton Line , 1948 .

[17]  I. Waller Über die Magnetisierung von paramagnetischen Kristallen in Wechselfeldern , 1932 .