๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Nuclear relaxation in an antiferromagnetic single crystal

โœ Scribed by G.E.G. Hardeman; N.J. Poulis; W. v.d. Lugt


Publisher
Elsevier Science
Year
1956
Weight
370 KB
Volume
22
Category
Article
ISSN
0031-8914

No coin nor oath required. For personal study only.

โœฆ Synopsis


The proton spin relaxation time in the antiferromagnetic single crystal of CuC12. 2H,O Was measured in the temperature region of liquid helium. A strong temperature dependence was found, the relaxation time increasing to a few seconds at 1.2ยฐK. Up to 2.5ยฐK the results can be described in terms of a simple model concerning the fluctuating magnetic moments of the Cu ions.

I. Introduction.

Previous experiments on the decomposed proton magnetic resonance line in single crystals of paramagnetic CuSO4.5H20 1) and CuC12. 2KC1.2H20 z) showed saturation effects for high RF amplitudes at the lowest temperatures (about 1.2ยฐK). During later measurements on the proton resonance in single crystals of antiferromagnetic CuCI~.2HzO 3), the same effects were observed. Various experiments have been carried out cn this crystal, resulting in detailed information about its magnetic properties.

To extend the data we carried out relaxation time measurements on the antiferromagnetic single crystal of CuC1,.2H,O. In the following we describe the temperature dependence of the proton magnetic relaxation time t 1 for one specified resonance line and at a certain fixed direction of the external field. Further experiments are being made in order to determine t 1 as a function of the direction of the external field to the crystal axes. Measurements on t 1 are also being carried out in the paramagnetic state for which the single crystal of CuClz. 2KCI. 2HzO is being used. In our theoretical discussion we assume that the major contribution to the relaxation originates from the time dependence of the interaction between the protons and their surrounding copper ions. Because ot the low temperatures involved, only the time variations of the electron spin coordinates are taken into account. In principle, the model for the rapidly fluctuating copper magnetic moment was already assumed in one of our earlier papers 4).

  1. Experimental arrangement. Several methods of determining ~1 were tried. As the oscillator method 3) 4) proved to be convenient in our previous --48 --

๐Ÿ“œ SIMILAR VOLUMES


Nuclear relaxation in antiferromagnetic
โœ J. Van Kranendonk; M. Bloom ๐Ÿ“‚ Article ๐Ÿ“… 1956 ๐Ÿ› Elsevier Science โš– 881 KB

A general theory of the spin-lattice relaxation process of nuclear spins in antiferromagnetic crystals, resulting from the magnetic dipolar interaction between the nuclear spins and the antiferromagnetic spins is developed. A detailed calculation of the relaxation time t I is carried out on the basi

The threshold field phenomenon in an ant
โœ N.J. Poulis; G.E.G. Hardeman ๐Ÿ“‚ Article ๐Ÿ“… 1954 ๐Ÿ› Elsevier Science โš– 289 KB

## Synop sis The threshold field in an antiferromagnetic single crystal of CuC12.2H20 is measured as a function of the temperature. A change in character of the proton magnetic resonance of CuC12.2H20 was used as a criterion for the threshold field phenomenon. The proton resonance in paraffin wax