Triply Heavy Baryons
| dc.creator | Nobary, M. A. Gomshi | |
| dc.date | 2006-09-13 | |
| dc.date.accessioned | 2026-07-07T10:42:01Z | |
| dc.date.available | 2026-07-07T10:42:01Z | |
| dc.description | The triply heavy baryons are very different in their mass. They are essentially $Ω_{ccc}$, $Ω_{ccb}$, $Ω_{cbb}$ and $Ω_{bbb}$ baryons which may be produced in a $c$ or a $b$ quark fragmentation. Here we briefly review the direct fragmentation production of these states and choose $Ω_{ccc}$ and $Ω_{bbb}$ baryons as prototype of them to consider their production at the hadron colliders with different $\sqrt{s}$. It becomes clear that their production cross sections fall within a rather diverse range according to $\sqrt{s}$, minimum transverse momentum and rapidity. We present and compare transverse momentum distributions of the differential cross sections, $p_T^{\rm min}$ distributions of total cross sections and the integrated total cross sections for all triply heavy baryons at CERN LHC and simlar quantities for $Ω_{ccc}$ and $Ω_{bbb}$ at RHIC, Tevatron Run II and the CERN LHC. While some of them possess considerable event rates even at RHIC proton-proton collider, others need much more energetic hadron collider with appropriate kinematical cuts to be produced. | |
| dc.description | 6 pages, 4 figures; Seminar presented at IPM-LHP06 May 2006 | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0609123 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0609123 | |
| dc.identifier | ECONFC0605151:0010,2006 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/181807 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Triply Heavy Baryons | |
| dc.type | text |