Light Higgses at the Tevatron and at the LHC and observable dark matter in SUGRA and D-branes
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摘要
Sparticle landscapes in mSUGRA, in SUGRA models with nonuniversalities (NUSUGRA), and in D-brane models are analyzed. The analysis exhibits the existence of Higgs Mass Patterns (HPs) (for MXD-3&_mathId=mml35&_user=1067359&_cdi=5539&_rdoc=17&_acct=C000050221&_version=1&_userid=10&md5=dc390996cda28c7473f9bb9b22e5704d" title="Click to view the MathML source" alt="Click to view the MathML source">μ>0) where the CP odd Higgs could be the next heavier particle beyond the LSP and sometimes even lighter than the LSP. It is shown that the Higgs production cross sections from the HPs are typically the largest enhancing the prospects for their detection at the LHC. Indeed it is seen that the recent Higgs production limits from CDF/DØ are beginning to put constraints on the HPs. It is also seen that the 710357ca8db0c" title="Click to view the MathML source" alt="Click to view the MathML source">Bsμ+μ limits constrain the HPs more stringently. Predictions of the Higgs production cross sections for these patterns at the LHC are made. We compute the neutralino–proton cross sections 38ff64967c412ce3def92a5f12c81">View the MathML source for dark matter experiments and show that the largest 38">38&_user=1067359&_cdi=5539&_rdoc=17&_acct=C000050221&_version=1&_userid=10&md5=d5e99ef5170c8ae0ffe9927d23d4f0b7">View the MathML source also arise from the HPs and further that the HPs and some of the other patterns are beginning to be constrained by the most recent data from CDMS and from Xenon10 experiments. Finally, it is shown that the prospects are bright for the discovery of dark matter with View the MathML source in the range 10−44±0.5 cm2 due to a “Wall” consisting of a copious number of parameter points in the Chargino Patterns (CPs) where the chargino is the NLSP. The Wall, which appears in all models considered (mSUGRA, NUSUGRA and D-branes) and runs up to about a TeV in LSP mass, significantly enhances the chances for the observation of dark matter by SuperCDMS, ZEPLIN-MAX, or LUX experiments which are expected to achieve a sensitivity of 10−45 cm2 or more.

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