5,337 research outputs found

    Explanation of the ATLAS Z-peaked excess by squark pair production in the NMSSM

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    The ATLAS collaboration recently reported a 3σ3\sigma excess in the leptonic-Z+jets+ETmissZ+jets+E_{T}^{miss} channel. We intend to interpret this excess by squark pair production in the Next-to-Minimal Supersymmetric Standard Model (NMSSM). The decay chain we employ is q~→qχ~20→qχ~10Z\tilde{q} \to q \tilde{\chi}_2^0 \to q \tilde{\chi}_1^0 Z, where χ~10\tilde{\chi}_1^0 and χ~20\tilde{\chi}_2^0 denote the lightest and the next-to-lightest neutralinos with singlino and bino as their dominant components respectively. Our simulations indicate that after considering the constraints from the ATLAS searches for jets+ETmissjets + E_{T}^{miss} signal the central value of the excess can be obtained for mq~≲1.2TeVm_{\tilde{q}} \lesssim 1.2 {\rm TeV}, and if the constraint from the CMS on-ZZ search is further considered, more than 10 signal events are still attainable for mq~≲750GeVm_{\tilde{q}} \lesssim 750 {\rm GeV}. Compared with the interpretation by gluino pair production, the squark explanation allows for a significantly wider range of mq~m_{\tilde{q}} as well as a less compressed SUSY mass spectrum. We also show that the squark explanation will be readily tested at the initial stage of the 14 TeV LHC.Comment: 19 pages, 4 figure

    Twist-3 contribution to the pion electromagnetic form factor

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    Non-leading contribution to the pion electromagnetic form factor which comes from the pion twist-3 wave function is analyzed in the modified hard scattering approach (MHSA) proposed by Li and Sterman. This contribution is enhanced significantly due to bound state effect (the twist-3 wave function is independent of the fractional momentum carried by the parton and has a large factor ∼mπ2/m0\sim m_\pi^2/m_0 with mπm_\pi being the pion meson mass and m0m_0 being the mean u- and d-quark masses). Consequently, although it is suppressed by the factor 1/Q21/Q^2, the twist-3 contribution is comparable with and even larger than the leading twist (twist-2) contribution at intermediate energy region of Q2Q^2 being 2∼40GeV22 \sim 40 {GeV}^2.Comment: 10 pages, 2 fgures, latex. More discussions on the Sudakov effect added, references added. To appear in European Physical Journal C (Zeitschrift fur Physik C

    Explanation of the ATLAS Z-peaked excess in the NMSSM

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    Recently the ATLAS collaboration reported a 3σ3\sigma excess in the leptonic-Z+jets+ETmissZ+jets+E_{T}^{miss} channel. This may be interpreted in the Next-to-Minimal Supersymmetric Standard Model (NMSSM) by gluino pair production with the decay chain g~→qqˉχ~20→qqˉZχ~10\tilde{g} \to q \bar{q} \tilde{\chi}_2^0 \to q \bar{q} Z \tilde{\chi}_1^0, where χ~10\tilde{\chi}_1^0 and χ~20\tilde{\chi}_2^0 denote the lightest and the next-to-lightest neutralinos with singlino and bino as their dominant components respectively. After exploring the relevant parameter space of the NMSSM by considering the constraints from the ATLAS searches for jets+ETmissjets + E_{T}^{miss} signals, we conclude that the NMSSM is able to explain the excess at 1σ1 \sigma level with the number of the signal events reaching its measured central value in optimal cases, and the best explanation comes from a compressed spectrum such as mg~≃650GeVm_{\tilde{g}} \simeq 650 {\rm GeV}, mχ~20≃565GeVm_{\tilde{\chi}_2^0} \simeq 565 {\rm GeV} and mχ~10≃465GeVm_{\tilde{\chi}_1^0} \simeq 465 {\rm GeV}. We also check the consistency of the ATLAS results with the null result of the CMS on-ZZ search. We find that under the CMS limits at 95%95\% C.L., the event number of the ATLAS on-ZZ signal can still reach 11 in our scenario, which is about 1.2σ1.2 \sigma away from the measured central value.Comment: 18 pages, 2 figure

    Sneutrino DM in the NMSSM with inverse seesaw mechanism

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    In supersymmetric theories like the Next-to-Minimal Supersymmetric Standard Model (NMSSM), the lightest neutralino with bino or singlino as its dominant component is customarily taken as dark matter (DM) candidate. Since light Higgsinos favored by naturalness can strength the couplings of the DM and thus enhance the DM-nucleon scattering rate, the tension between naturalness and DM direct detection results becomes more and more acute with the improved experimental sensitivity. In this work, we extend the NMSSM by inverse seesaw mechanism to generate neutrino mass, and show that in certain parameter space the lightest sneutrino may act as a viable DM candidate, i.e. it can annihilate by multi-channels to get correct relic density and meanwhile satisfy all experimental constraints. The most striking feature of the extension is that the DM-nucleon scattering rate can be naturally below its current experimental bounds regardless of the higgsino mass, and hence it alleviates the tension between naturalness and DM experiments. Other interesting features include that the Higgs phenomenology becomes much richer than that of the original NMSSM due to the relaxed constraints from DM physics and also due to the presence of extra neutrinos, and that the signatures of sparticles at colliders are quite different from those with neutralino as DM candidate.Comment: 33 page

    Interpreting The 750 GeV Diphoton Excess Within Topflavor Seesaw Model

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    We propose to interpret the 750 GeV diphoton excess in a typical topflavor seesaw model. The new resonance X can be identified as a CP-even scalar emerging from a certain bi-doublet Higgs field. Such a scalar can couple to charged scalars, fermions as well as heavy gauge bosons predicted by the model, and consequently all of the particles contribute to the diphoton decay mode of the X. Numerical analysis indicates that the model can predict the central value of the diphoton excess without contradicting any constraints from 8 TeV LHC, and among the constraints, the tightest one comes from the Z \gamma channel, \sigma_{8 {\rm TeV}}^{Z \gamma} \lesssim 3.6 {\rm fb}, which requires \sigma_{13 {\rm TeV}}^{\gamma \gamma} \lesssim 6 {\rm fb} in most of the favored parameter space.Comment: Major changes, 17 pages, 4 figure, typos corrected, calculation details adde

    Exploring the Higgs Sector of a Most Natural NMSSM and its Prediction on Higgs Pair Production at the LHC

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    As a most natural realization of the Next-to Minimal Supersymmetry Standard Model (NMSSM), {\lambda}-SUSY is parameterized by a large {\lambda} around one and a low tanβ\beta below 10. In this work, we first scan the parameter space of {\lambda}-SUSY by considering various experimental constraints, including the limitation from the Higgs data updated by the ATLAS and CMS collaborations in the summer of 2014, then we study the properties of the Higgs bosons. We get two characteristic features of {\lambda}-SUSY in experimentally allowed parameter space. One is the triple self coupling of the SM-like Higgs boson may get enhanced by a factor over 10 in comparison with its SM prediction. The other is the pair production of the SM-like Higgs boson at the LHC may be two orders larger than its SM prediction. All these features seems to be unachievable in the Minimal Supersymmetric Standard Model and in the NMSSM with a low {\lambda}. Moreover, we also find that naturalness plays an important role in selecting the parameter space of {\lambda}-SUSY, and that the Higgs χ2\chi^2 obtained with the latest data is usually significantly smaller than before due to the more consistency of the two collaboration measurements
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