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2017:groups:higgs:2h [2017/06/17 14:46] stefania.gori |
2017:groups:higgs:2h [2017/06/17 15:35] jose_miguel.no |
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- | Interested: | + | Interested people: Jose Miguel No, Jose Zurita, |
1. V phi, with phi -> gamma gamma, what does the LHC can say? | 1. V phi, with phi -> gamma gamma, what does the LHC can say? | ||
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bounds from H coupling measurements to ZZ and EWPT | bounds from H coupling measurements to ZZ and EWPT | ||
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2. Complementarity with phi single production together with a ISR | 2. Complementarity with phi single production together with a ISR | ||
- | 3. h->ss->SM (eventually scalars with different masses h-> s1s2) | + | Light scalars (m_{phi} < m_h = 125 GeV) with no phi V V coupling (V = SM gauge boson) but coupling to fermions. Motivated in extended Higgs sectors (e.g. light Higgses in 2HDM) when the 125 GeV is SM like (2HDM "alignment limit"). |
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+ | Weakly constrained by LEP (no V phi production). Maybe challenging @ LHC? phi recoiling against a hard jet could allow to trigger on this (phi -> gamma gamma? tau tau?). | ||
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+ | 3. Exotic Higgs decays: What are the holes? | ||
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+ | h -> a a, Z a, a a' with a, a' scalar/pseudoscalar (for Z a, a is pseudoscalar) | ||
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+ | * Current searches for h -> a a: 4 muon, 2 mu 2 b, 4 tau, 2 tau 2 mu, 4 b... | ||
+ | * Interesting to look at signatures with resolved/not resolved photons: 2b 2gamma, 4 gamma (for unresolved 2 gamma pairs, measurement of h->gamma gamma could yield weak constrain) | ||
+ | * h -> Z a (a -> gamma gamma) has been initially studied by Bauer, Neubert, Thamm in , for a being an ALP (axion-like particle) | ||
+ | * h -> a a': if ma is different from ma', h -> a a searches would miss it (also depends on final state) | ||
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+ | h->chi1 chi2 | ||
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+ | h->ss->SM (eventually scalars with different masses h-> s1s2) | ||
what are the holes? | what are the holes? | ||
- | * signatures with resolved/not resolved photons: 2b 2gamma, 4 gamma, s Z with s->gamma gamma | + | |
* decays involving missing energy: h->chi1 chi2 with chi1 invisible | * decays involving missing energy: h->chi1 chi2 with chi1 invisible |