Results for 'Allbrooke Bmm'

7 found
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  1.  23
    Search for Supersymmetry in Events with Large Missing Transverse Momentum, Jets, and at Least One Tau Lepton in 20 Fb−1of √s= 8 TeV Proton-Proton Collision Data with the ATLAS Detector. [REVIEW]A. The Atlas Collaboration, G. Aad, B. Abbott, Abdallah Jm, S. Abdel Khalek, Abdinov Ob, R. Aben, Abi Ba, Abolins Ma, Abouzeid Os, H. Abramowicz, H. Abreu, R. Abreu, Y. Abulaiti, Acharya Bs, L. Adamczyk, Adams Dl, J. Adelman, S. Adomeit, Adye Tj, T. Agatonovic-Jovin, Aguilar-Saavedra Ja, M. Agustoni, Ahlen Sp, F. Ahmadov, G. Aielli, Åkerstedt Ho, Åkesson Tpa, G. Akimoto, Akimov Av, Alberghi Gl, Albert Jb, S. Albrand, Alconada Verzini Mj, M. Aleksa, Aleksandrov In, C. Alexa, Alexander Gk, G. Alexandre, Alexopoulos Ta, M. Alhroob, G. Alimonti, L. Alio, Alison Jm, Allbrooke Bmm, Allison Lj, Allport Pp, Almond Je, A. Aloisio, A. Alonso, F. Alonso, C. Alpigiani, Altheimer Ad, B. Álvarez González, Alviggi Mg, K. Amako, Y. Amaral Coutinho, C. Amelung, D. Amidei, Amor Dos Santos Sp, Amorim As, S. Amoroso, N. Amram, G. Amundsen, C. Anastopoulos, Ancu Ls, N. Andari, Andeen Tr, Anders Cf, G. Anders, Anderson Kj, A. Andreazza, V. Andrei, Anduaga Xs, S. Angelidakis, I. Angelozzi, P. Anger, A. Angerami, F. Anghinolfi, Anisenkov Av, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli & A. - unknown
    © 2014, The Author. A search for supersymmetry in events with large missing transverse momentum, jets, at least one hadronically decaying tau lepton and zero or one additional light leptons, has been performed using 20.3fb−1of proton-proton collision data at √ s= 8 TeV recorded with the ATLAS detector at the Large Hadron Collider. No excess above the Standard Model background expectation is observed in the various signal regions and 95% confidence level upper limits on the visible cross section for new (...)
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  2.  34
    Search for the Direct Production of Charginos, Neutralinos and Staus in Final States with at Least Two Hadronically Decaying Taus and Missing Transverse Momentum in Pp Collisions at √ $$ \Sqrt{s}=8 $$ TeV with the ATLAS Detector.The Atlasc, G. Aad, B. Abbott, J. Abdallah, Khalek Sa, O. Abdinov, R. Aben, B. Abi, M. Abolins, Abouzeid Os, H. Abramowicz, H. Abreu, R. Abreu, Y. Abulaiti, Acharya Bs, L. Adamczyk, Adams Dl, J. Adelman, S. Adomeit, T. Adye, T. Agatonovic-Jovin, Aguilar-Saavedra Ja, M. Agustoni, Ahlen Sp, F. Ahmadov, G. Aielli, H. Akerstedt, Åkesson Tpa, G. Akimoto, Akimov Av, Alberghi Gl, J. Albert, S. Albrand, Alconada Verzini Mj, M. Aleksa, Aleksandrov In, C. Alexa, G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, G. Alimonti, L. Alio, J. Alison, Allbrooke Bmm, Allison Lj, Allport Pp, J. Almond, A. Aloisio, A. Alonso, F. Alonso, C. Alpigiani, A. Altheimer, Gonzalez Ba, Alviggi Mg, K. Amako, Y. Amaral Coutinho, C. Amelung, D. Amidei, Amor Dos Santos Sp, A. Amorim, S. Amoroso, N. Amram, G. Amundsen, C. Anastopoulos, Ancu Ls, N. Andari, T. Andeen, Anders Cf, G. Anders, Anderson Kj, A. Andreazza, V. Andrei, Anduaga Xs, S. Angelidakis, I. Angelozzi, P. Anger, A. Angerami, F. Anghinolfi, Anisenkov Av, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, A. Antonov, J. Antos, F. Anulli & A. - unknown
    : Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb−1 of proton-proton collisions at recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the (...)
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  3.  6
    Bounded Martin’s Maximum with an Asterisk.David Asperó & Ralf Schindler - 2014 - Notre Dame Journal of Formal Logic 55 (3):333-348.
    We isolate natural strengthenings of Bounded Martin’s Maximum which we call ${\mathsf{BMM}}^{*}$ and $A-{\mathsf{BMM}}^{*,++}$, and we investigate their consequences. We also show that if $A-{\mathsf{BMM}}^{*,++}$ holds true for every set of reals $A$ in $L$, then Woodin’s axiom $$ holds true. We conjecture that ${\mathsf{MM}}^{++}$ implies $A-{\mathsf{BMM}}^{*,++}$ for every $A$ which is universally Baire.
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  4.  26
    Semi-Proper Forcing, Remarkable Cardinals, and Bounded Martin's Maximum.Ralf Schindler - 2004 - Mathematical Logic Quarterly 50 (6):527-532.
    We show that L absoluteness for semi-proper forcings is equiconsistent with the existence of a remarkable cardinal, and hence by [6] with L absoluteness for proper forcings. By [7], L absoluteness for stationary set preserving forcings gives an inner model with a strong cardinal. By [3], the Bounded Semi-Proper Forcing Axiom is equiconsistent with the Bounded Proper Forcing Axiom , which in turn is equiconsistent with a reflecting cardinal. We show that Bounded Martin's Maximum is much stronger than BSPFA in (...)
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  5.  11
    Martin’s Maximum Revisited.Matteo Viale - 2016 - Archive for Mathematical Logic 55 (1-2):295-317.
    We present several results relating the general theory of the stationary tower forcing developed by Woodin with forcing axioms. In particular we show that, in combination with class many Woodin cardinals, the forcing axiom MM++ makes the Π2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\Pi_2}$$\end{document}-fragment of the theory of Hℵ2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${H_{\aleph_2}}$$\end{document} invariant with respect to stationary set preserving forcings that preserve BMM. We argue that this is a promising generalization to (...)
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  6.  9
    On a Convenient Property About $${[\Gamma]^{\Aleph_0}}$$.David Asperó - 2009 - Archive for Mathematical Logic 48 (7):653-677.
    Several situations are presented in which there is an ordinal γ such that ${\{ X \in [\gamma]^{\aleph_0} : X \cap \omega_1 \in S\,{\rm and}\, ot(X) \in T \}}$ is a stationary subset of ${[\gamma]^{\aleph_0}}$ for all stationary ${S, T\subseteq \omega_1}$ . A natural strengthening of the existence of an ordinal γ for which the above conclusion holds lies, in terms of consistency strength, between the existence of the sharp of ${H_{\omega_2}}$ and the existence of sharps for all reals. Also, an (...)
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  7.  1
    On a Convenient Property About [FORMULA].David Asperó - 2009 - Archive for Mathematical Logic 48 (7):653-677.
    Several situations are presented in which there is an ordinal γ such that \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\{ X \in [\gamma]^{\aleph_0} : X \cap \omega_1 \in S\,{\rm and}\, ot \in T \}}$$\end{document} is a stationary subset of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${[\gamma]^{\aleph_0}}$$\end{document} for all stationary \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${S, T\subseteq \omega_1}$$\end{document}. A natural strengthening of the existence of an ordinal γ for which the above (...)
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