Abstract
The integrable quantum many-body systems associated with the classical root systems are formulated in terms of the (trigonometric) Dunkl operators. We define the Dunkl operators by use of the infinite-dimensional representation of the R and K matrices for the Yang-Baxter equation and the reflection equation. The eigenvalues of systems are also given.
Original language | English |
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Pages (from-to) | 394-401 |
Number of pages | 8 |
Journal | Journal of the Physical Society of Japan |
Volume | 65 |
Issue number | 2 |
DOIs | |
Publication status | Published - 1996 |
Externally published | Yes |
All Science Journal Classification (ASJC) codes
- Physics and Astronomy(all)