Noncommutative BTZ Black Hole in Different Coordinates
| dc.creator | Chang-Young, Ee | |
| dc.date | 2009-01-12 | |
| dc.date.accessioned | 2026-07-07T12:28:23Z | |
| dc.date.available | 2026-07-07T12:28:23Z | |
| dc.description | We consider noncommutative BTZ black hole solutions in two different coordinate systems, the polar and rectangular coordinates. The analysis is carried out by obtaining noncommutative solutions of $U(1,1)\times U(1,1)$ Chern-Simons theory on $AdS_3$ in the two coordinate systems via the Seiberg-Witten map. This is based on the noncommutative extension of the equivalence between the classical BTZ solution and the solution of ordinary $SU(1,1)\times SU(1,1)$ Chern-Simons theory on $AdS_3$. The obtained solutions in these noncommutative coordinate systems become different in the first order of the noncommutativity parameter $θ$. | |
| dc.description | 6 pages, Talk given at CosPA2008, October 2008 | |
| dc.identifier | https://arxiv.org/abs/0901.1516 | |
| dc.identifier | http://arxiv.org/abs/0901.1516 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/215520 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Noncommutative BTZ Black Hole in Different Coordinates | |
| dc.type | text |