This shows you the differences between two versions of the page.
Both sides previous revision Previous revision Next revision | Previous revision Next revision Both sides next revision | ||
2015:groups:higgs:morehiggs:forbidden [2015/06/12 14:14] giacomo.cacciapaglia |
2015:groups:higgs:morehiggs:forbidden [2015/06/12 14:30] giacomo.cacciapaglia |
||
---|---|---|---|
Line 1: | Line 1: | ||
**Responsible:** Antonio Delgado | **Responsible:** Antonio Delgado | ||
- | **Members:** Mariano Quiros, Roberto-Vega Morales, Jose Santiago, Marco Nardecchia, Giaccomo Cacciapaglia, Aram Apyan, Thomas Flacke | + | **Members:** Mariano Quiros, Roberto-Vega Morales, Jose Santiago, Marco Nardecchia, Giacomo Cacciapaglia, Aram Apyan, Thomas Flacke |
**Some Papers:** | **Some Papers:** | ||
Line 11: | Line 11: | ||
**Experimental searches:** | **Experimental searches:** | ||
http://arXiv.org/pdf/1503.04233.pdf | http://arXiv.org/pdf/1503.04233.pdf | ||
+ | |||
+ | **H'H' pair production (Giacomo):** | ||
+ | Searching for typical production cross sections, I found this paper on NLO computation for sleptons: | ||
+ | http://arxiv.org/pdf/1310.2621v3.pdf | ||
+ | I think that, taking into account the s-channel W, the fact that it's a triplet, and the 13 TeV energy at Run II, we may hope to have sizable xsections up to masses of 500 GeV (roughly). | ||
+ | |||
+ | Suggestion for suitable final states: | ||
+ | gamma gamma V V, with hadronic V decays (and double invariant-mass reconstruction); | ||
+ | ... | ||
+ | |||
+ | |||
+ | |||
+ |