![]() |
![]() |
![]() |
|
|
Home | About | Table of Contents | Advanced Search | Copyright | Feedback | Privacy |
|||||||||||||||
|
|||||||||||||||
|
Unless otherwise stated this page contains Version 1.0 content (Read more about versions) 3.8.3 Nuclear spin relaxation timeWhen a material is in thermal equilibrium, the nuclear spins are either randomly oriented or have a distribution of orientations related to the crystal structure. This equilibrium distribution of nuclear spins may be altered by various re-orienting processes, but after such a process is removed the spin orientations (and hence the nuclear magnetization of the sample) will revert to their original equilibrium distribution exponentially with time. The time constant for this reversion is known as the spin-lattice relaxation time, τ. Relaxation times are usually temperature sensitive but are not very dependent on magnetic field. In the table a magnetic field of about 1 tesla (10 kilogauss) is assumed and the temperature T, or temperature range of the observations, is listed. The relaxation times in insulating diamagnetic materials are often very much reduced if paramagnetic impurities are present.
References A. Abragam (1961) The Principles of Nuclear Magnetism, Oxford University Press. L.E.Drain |
|
Home | About | Table of Contents | Advanced Search | Copyright | Feedback | Privacy | ^ Top of Page ^ |
||
|
This site is hosted and maintained by the National Physical Laboratory |
||