Search for Anomalous Production of Multilepton Events in p-pbar Collisions at sqrt(s) = 1.96 TeV

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J. C. Pati and A. Salam, Phys. Rev. D 10
1974
Earlier work this paper cites.
R. D. Peccei and H.R. Quinn, Phys. Rev. Lett. 38
1978
Earlier work this paper cites.
R. N. Mohapatra and G. Senjanovic, Phys. Rev. D 11
1981
Earlier work this paper cites.
H. P. Nilles, Phys. Rep. 110
1984
Earlier work this paper cites.
H. E. Haber and G. I. Kane, Phys. Rep. 117
1985
Earlier work this paper cites.
W. Beenakker et al
1999
Earlier work this paper cites.

A. Sill et al
2000
Cited alongside, same era.
A. Heister et al
2001
Cited alongside, same era.
D. Acosta et al
2001
Cited alongside, same era.
T. Sjöstrand et al
2001
Cited alongside, same era.
M. Mühlleitner and M. Spira, Phys. Rev. D 68
2003
Cited alongside, same era.
T. Affolder et al
2004
Cited alongside, same era.
In this paper, the word “lepton” refers to electrons and muons
Cited in the paper.
V. Barger, P. Langacker, and H.-S. Lee, hep-ph/0508027
Cited in the paper.
In the CDF geometry, θ \theta is the polar angle with respect to the proton beam axis (positive z z direction), and ϕ \phi is the azimuthal angle. The pseudorapidity is η = − ln ⁡ [ tan ⁡ ( θ / 2 ) ] \eta=-\ln[\tan(\theta/2)] . The transverse energy, E T E_{\mathrm{T}} , of a shower or calorimeter tower is E sin ⁡ θ E\sin\theta , where E E is the energy deposited. The missing transverse energy is defined by ／ ⁡ E T \raisebox{1.29167pt}{$\not$}E_{\rm T}
Cited in the paper.
H. Baer et al
Cited in the paper.