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We performed a signature-based search for long-lived charged massive particles (CHAMPs) produced in 1.0 $\rm{fb}^{-1}$ of $\bar{p}p$ collisions at $\sqrt{s}=1.96$ TeV, collected with the CDF II detector using a high transverse-momentum ($p_T$) muon trigger.
“R-hadron” refers to hadrons containing an R-parity-conserving supersymmetric particle. From G. R. Farrar and P. Fayet, Phys. Lett. B 76
1978
Earlier work this paper cites.
G. Ascoli et al
1988
Earlier work this paper cites.
M. Drees and X. Tata, Phys. Lett. B 252
1990
Earlier work this paper cites.
W. Beenakker et al
1999
Earlier work this paper cites.
J.L. Feng, T. Moroi, L. Randall, M. Strassler, and S. Su, Phys. Rev. Lett. 83
2000
Earlier work this paper cites.
A. Sill et al
2000
Earlier work this paper cites.
See R. Barbieri, L. J. Hall, and Y. Nomura, Phys. Rev. D 63
2001
Earlier work this paper cites.
A. Heister et al
2002
Cited alongside, same era.
P.F. Smith et al
2002
Cited alongside, same era.
F. Acosta et al
2003
Cited alongside, same era.
A.V. Kotwal, H.K. Gerberich, and C. Hays, Nucl. Instrum. Meth. A 506
2003
Cited alongside, same era.
T. Affolder et al
2004
Cited alongside, same era.
D. Acosta et al
2004
Cited alongside, same era.
LEP SUSY Working Group, ALEPH, DELPHI, L3 and OPAL collaborations, note LEPSUSYWG/02-05.1 (http://lepsusy.web.cern.ch/lepsusy/Welcome.html)
Cited in the paper.
See for instance P.H. Frampton and P.Q. Hung, Phys. Rev. D 58
2005
Later among the works it cites.
D. Acosta et al
2005
Later among the works it cites.
T. Sjöstrand, S. Mrenna, and P. Skands, J. High Energy Phys. 05 (2006) 026. See also http://home.thep.lu.se/ ∼ \sim torbjorn/Pythia.html
2006
Later among the works it cites.
M. Strassler and K. Zurek, Phys. Lett. B 651
2007
Later among the works it cites.
M. Fairbairn et al
2007
Later among the works it cites.
A. Abulencia et al
2007
Later among the works it cites.
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We use a coordinate system where ϕ \phi is the azimuthal angle around the beam axis and θ \theta is the polar angle measured with respect to the proton direction. The pseudo-rapidity, η \eta , is defined by η ≡ − log tan ( θ / 2 ) \eta\equiv-\log\tan(\theta/2) and Δ R ≡ Δ η 2 + Δ ϕ 2 \Delta R\equiv\sqrt{\Delta\eta^{2}+\Delta\phi^{2}}
Cited in the paper.
E. Barberio et al
Cited in the paper.
See http://www.ph/ed.ac.uk/ ∼ \sim tplehn/prospino
Cited in the paper.