Exact beta function from the holographic loop equation of large-N QCD_4
| dc.creator | Bochicchio, Marco | |
| dc.date | 2007-05-01 | |
| dc.date | 2007-06-08 | |
| dc.date.accessioned | 2026-07-07T13:06:27Z | |
| dc.date.available | 2026-07-07T13:06:27Z | |
| dc.description | We construct and study a previously defined quantum holographic effective action whose critical equation implies the holographic loop equation of large-N QCD_4 for planar self-avoiding loops in a certain regularization scheme. We extract from the effective action the exact beta function in the given scheme. For the Wilsonean coupling constant the beta function is exacly one loop and the first coefficient agrees with its value in perturbation theory. For the canonical coupling constant the exact beta function has a NSVZ form and the first two coefficients agree with their value in perturbation theory. | |
| dc.description | 42 pages, latex. The exponent of the Vandermonde determinant in the quantum effective action has been changed, because it has been employed a holomorphic rather than a hermitean resolution of identity in the functional integral. Beta function unchanged. New explanations and references added, typos corrected | |
| dc.identifier | https://arxiv.org/abs/0705.0082 | |
| dc.identifier | http://arxiv.org/abs/0705.0082 | |
| dc.identifier | JHEP 0709:033,2007 | |
| dc.identifier | doi:10.1088/1126-6708/2007/09/033 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/227785 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Exact beta function from the holographic loop equation of large-N QCD_4 | |
| dc.type | text |