WILSON LOOP AND CONTOUR SHAPES
| dc.citation.epage | 4164 | en_US |
| dc.citation.issue | 12 | en_US |
| dc.citation.spage | 4159 | en_US |
| dc.citation.volume | 42 | en_US |
| dc.citation.woscount | 0 | en_US |
| dc.contributor.author | KAO, WF | en_US |
| dc.contributor.department | 電子物理學系 | zh_TW |
| dc.contributor.department | Department of Electrophysics | en_US |
| dc.date.accessioned | 2019-04-03T06:37:48Z | |
| dc.date.available | 2019-04-03T06:37:48Z | |
| dc.date.issued | 1990-12-15 | en_US |
| dc.description.abstract | By computing the Wilson loop expectation value W[C] in the two-dimensional Schwinger model on R1 x S1, we show that nonleading terms depend on the shape of the contours both on R1 x R1 and R1 x S1. We also find that the rhombic contour and triangular contour lead to the same static potentials both on R1 x R1 and R1 x S1. The binding energy is also affected by the choice of contour shapes on the R1 x S1 model. This indicates that the model on R1 x S1 deserves more study. | en_US |
| dc.identifier.doi | 10.1103/PhysRevD.42.4159 | en_US |
| dc.identifier.issn | 0556-2821 | en_US |
| dc.identifier.journal | PHYSICAL REVIEW D | en_US |
| dc.identifier.uri | http://dx.doi.org/10.1103/PhysRevD.42.4159 | en_US |
| dc.identifier.uri | https://ir.lib.nycu.edu.tw/handle/11536/3948 | |
| dc.identifier.wosnumber | WOS:A1990EP27800025 | en_US |
| dc.language.iso | en_US | en_US |
| dc.title | WILSON LOOP AND CONTOUR SHAPES | en_US |
| dc.type | Article | en_US |