Abstract
The transverse autocorrelation function at an arbitrary temperature is calculated rigorously for a system with an arbitrary number of quantum spins, each of which is coupled to all the other spins with equal exchange. It is shown that the cluster approximation, formed by a model for a real magnet, explains short- and intermediate-time (up to the time to reach the spin-diffusion regime) experimental measurements in the paramagnetic phase.
Original language | English (US) |
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Pages (from-to) | 3974-3977 |
Number of pages | 4 |
Journal | Physical Review B |
Volume | 51 |
Issue number | 6 |
DOIs | |
State | Published - 1995 |
Externally published | Yes |
ASJC Scopus subject areas
- Condensed Matter Physics