| dc.creator |
Delgado, Antonio |
|
| dc.creator |
Quirós, Mariano |
|
| dc.date |
2007-12-26T08:52:30Z |
|
| dc.date |
2007-12-26T08:52:30Z |
|
| dc.date |
2000-04-13 |
|
| dc.date.accessioned |
2017-01-31T00:59:30Z |
|
| dc.date.available |
2017-01-31T00:59:30Z |
|
| dc.identifier |
Phys.Lett. B484 (2000) 355-361 |
|
| dc.identifier |
arXiv:hep-ph/0004124v1 |
|
| dc.identifier |
http://hdl.handle.net/10261/2588 |
|
| dc.identifier.uri |
http://dspace.mediu.edu.my:8181/xmlui/handle/10261/2588 |
|
| dc.description |
In the four-dimensional supersymmetric standard model extended with gauge singlets the lightest Higgs boson mass, $M_H$, has an important contribution proportional to the squared of the superpotential coupling $\lambda$ of singlets to Higgs fields, $\lambda SH_1\cdot H_2$. The requirement of perturbativity up to the unification scale yields an upper bound on $M_H\sim 140$ GeV. In extensions to theories with (longitudinal) extra dimensions at the TeV where such coupling exists and massive Kaluza-Klein states fall into N=2 representations, if either of the Higgs or singlet fields live in the bulk of the extra dimensions, the $\beta$-function of $\lambda$ is suppressed due to the absence of anomalous dimension of hypermultiplets to leading order. This implies a slower running of $\lambda$ and an enhancement of its low energy value. The $M_H$ upper bound increases to values $M_H\lesssim 165$ GeV. |
|
| dc.description |
Work supported in part by EU under TMR contract ERBFMRX-CT96-0045, and by CICYT (Spain)under contract AEN98-0816. |
|
| dc.description |
Peer reviewed |
|
| dc.format |
174534 bytes |
|
| dc.format |
application/pdf |
|
| dc.language |
eng |
|
| dc.rights |
openAccess |
|
| dc.subject |
High Energy Physics |
|
| dc.subject |
Phenomenology |
|
| dc.title |
The lightest Higgs mass in supersymmetric models with extra dimensions |
|
| dc.type |
Artículo |
|