• • • We do not use the following data for averages, fits, limits, etc. • • • |
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ATLS |
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CDF |
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ATLS |
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ATLS |
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CMS |
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ATLS |
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CDF |
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CMS |
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CMS |
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CMS |
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ATLS |
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CDF |
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SIRUNYAN 2020A search for SUSY and LQ production using mT2 or presence of long-lived charged particle; no signal, limits placed in various mass planes for different BSM scenarios and various assumed lifetimes.
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ALCANTARA 2019 place limits on m(WIMPzilla=${{\mathit X}}$) vs lifetime from upper bound on ultra high energy cosmic rays at Auger experiment: e.g. ${{\mathit \tau}}({{\mathit X}}$) $<$ $4 \times 10^{22}$ yr for m(${{\mathit X}}$) = $10^{16}$ GeV.
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PORAYKO 2018 search for deviations in the residuals of pulsar timing data using PPTA. No signal observed. Limits set on fuzzy DM with $3 \times 10^{-24}$ $<$ m(DM) $<2 \times 10^{-22}$ eV.
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AAD 2015AT search for events with a top quark and mssing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 20.3 fb${}^{-1}$.
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KHACHATRYAN 2015F search for events with a top quark and mssing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 19.7 fb${}^{-1}$.
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AALTONEN 2014J examine events with a ${{\mathit W}}$ and two jets in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = 8.9 fb${}^{-1}$. Invariant mass distributions of the two jets are consistent with the Standard Model expectation.
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AAD 2013A search for resonant ${{\mathit W}}{{\mathit W}}$ production in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.7 fb${}^{-1}$.
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AAD 2013C search for events with a photon and missing $\not E_T$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.6 fb${}^{-1}$.
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AALTONEN 2013I search for events with a photon and missing $\mathit E_{T}$, where the photon is detected after the expected timing, in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = 6.3 fb${}^{-1}$. The data are consistent with the Standard Model expectation.
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CHATRCHYAN 2013 search for events with an opposite-sign lepton pair, jets, and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.98 fb${}^{-1}$.
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AAD 2012C search for events with a ${{\mathit t}}{{\overline{\mathit t}}}$ pair and missing $\not E_T$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 1.04 fb${}^{-1}$.
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AALTONEN 2012M search for events with a jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = 6.7 fb${}^{-1}$.
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CHATRCHYAN 2012AP search for events with a jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 5.0 fb${}^{-1}$.
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CHATRCHYAN 2012Q search for events with a ${{\mathit Z}}$, jets, and missing $\not E_T$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.98 fb${}^{-1}$.
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CHATRCHYAN 2012T search for events with a photon and missing $\not E_T$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 5.0 fb${}^{-1}$.
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AAD 2011S search for events with one jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 33$~$pb${}^{-1}$.
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AALTONEN 2011AF search for high-$p_T$ like-sign dileptons in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96$~$TeV with $\mathit L$ = 6.1 fb${}^{-1}$.
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CHATRCHYAN 2011C search for events with an opposite-sign lepton pair, jets, and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 34 pb${}^{-1}$.
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CHATRCHYAN 2011U search for events with one jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 36$~$pb${}^{-1}$.
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AALTONEN 2010AF search for ${{\mathit \gamma}}{{\mathit \gamma}}$ events with ${{\mathit e}}$, ${{\mathit \mu}}$, ${{\mathit \tau}}$, or missing $\mathit E_{T}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = $1.1 - 2.0$ fb${}^{-1}$.
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AALTONEN 2009AF search for ${{\mathit \ell}}{{\mathit \gamma}}{{\mathit b}}$ events with missing $\mathit E_{T}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = 1.9 fb${}^{-1}$. The observed events are compatible with Standard Model expectation including ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit \gamma}}$ production.
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AALTONEN 2009G search for ${{\mathit \mu}}{{\mathit \mu}}{{\mathit \mu}}$ and ${{\mathit \mu}}{{\mathit \mu}}{{\mathit e}}$ events with missing $\mathit E_{T}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = 976 pb${}^{-1}$.
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