Abstract
Yang-Lee analysis of the grand canonical partition function for a Hubbard Model at finite doping is presented. Evaluating the zeros of this function in the complex chemical-potential plane, we observe an onset of a phase transition when the zeros approach the positive real half-axis with spatial increase of the simulated system. The peak of electronic susceptibility is located in the vicinity of the relevant zeros. © 1995.
| Original language | English |
|---|---|
| Pages (from-to) | 702-704 |
| Number of pages | 3 |
| Journal | Physica B: Condensed Matter |
| Volume | 206-207 |
| Issue number | C |
| Publication status | Published - 1 Feb 1995 |
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