Abstract
There are very few formalisms available to solve the Liouville equation for energy-conserved systems. The continued fraction formalism, introduced through the works of Zwanzig, Mori, Kubo, Lee, Grigolini and others is described here. A detailed discussion is presented on ways to apply the continued fraction formalism to solve for relaxation functions and for the dynamical variable itself for a simple and exactly solvable quantum spin system.
| Original language | English |
|---|---|
| Pages (from-to) | 304-324 |
| Number of pages | 21 |
| Journal | Physica A: Statistical Mechanics and its Applications |
| Volume | 360 |
| Issue number | 2 |
| DOIs | |
| State | Published - Feb 1 2006 |
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