Visible Cascade Higgs Decays to Four Photons at Hadron Colliders
| dc.creator | Chang, Spencer | |
| dc.creator | Fox, Patrick J. | |
| dc.creator | Weiner, Neal | |
| dc.date | 2006-08-29 | |
| dc.date.accessioned | 2026-07-07T11:05:37Z | |
| dc.date.available | 2026-07-07T11:05:37Z | |
| dc.description | The presence of a new singlet scalar particle a can open up new decay channels for the Higgs boson, through cascades of the form h -> 2a -> X, possibly making discovery through standard model channels impossible. If a is CP-odd, its decay products are particularly sensitive to physics beyond the standard model. Quantum effects from heavy fields can naturally make gluonic decay, a -> 2g, the dominant decay mode, resulting in a h -> 4 g decay which is difficult to observe at hadron colliders, and is allowed by LEP for m_h > 82 GeV. However, there are usually associated decays with photons, either h -> 2g 2gamma or h -> 4gamma, which are more promising. The decay h -> 2g 2gamma only allows discovery of the a particle and not the Higgs whereas h -> 4gamma is a clean channel that can discover both particles. We determine what branching ratios are required for discovery at LHC and find that with 300 fb^-1 of luminosity, a branching ratio of order 10^-4 is sufficient for a large region of Higgs masses. Due to a lower expected luminosity of ~ 8 fb^-1, discovery at the Tevatron requires more than 5 x 10^-3 in branching ratio. | |
| dc.description | 6 pages, 2 color figures, revtex4 format | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0608310 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0608310 | |
| dc.identifier | Phys.Rev.Lett.98:111802,2007 | |
| dc.identifier | doi:10.1103/PhysRevLett.98.111802 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/189258 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | High Energy Physics - Experiment | |
| dc.title | Visible Cascade Higgs Decays to Four Photons at Hadron Colliders | |
| dc.type | text |