| dc.contributor.author |
Bohr H. |
|
| dc.contributor.author |
Rajasekaran G. |
|
| dc.date.accessioned |
2023-10-13T12:37:31Z |
|
| dc.date.available |
2023-10-13T12:37:31Z |
|
| dc.date.issued |
1985 |
|
| dc.identifier |
10.1103/PhysRevD.32.1547 |
|
| dc.identifier.issn |
5562821 |
|
| dc.identifier.uri |
https://dspace.imsc.res.in/xmlui/handle/123456789/758 |
|
| dc.identifier.uri |
https://doi.org/10.1103/PhysRevD.32.1547 |
|
| dc.description.abstract |
A large-N gauge model is constructed entirely in terms of gauge-invariant composite fields. The model is formulated in a canonical framework where the Hamiltonian contains only the Wilson-loop and string operators and their canonical momenta. The quarks on the end of the strings are treated as scalar particles. © 1985 The American Physical Society. |
|
| dc.language.iso |
en |
|
| dc.relation.ispartof |
Physical Review D - Particles, Fields, Gravitation and Cosmology, Vol. 32, Issue. 6 |
|
| dc.rights |
Copyrighted by the Publisher |
|
| dc.source |
Physical Review D - Particles, Fields, Gravitation and Cosmology |
|
| dc.title |
Large-N gauge theory of loops and strings. I |
|
| dc.description.pages |
1547 - 1552 |
|
| dc.relation.url |
https://doi.org/10.1103/PhysRevD.32.1547 |
|
| dc.type |
Article |
|