-
1
-
-
85038316128
-
-
ATLAS: Detector and physics performance technical design report, CERN-LHCC-99-14.
-
ATLAS: Detector and physics performance technical design report, CERN-LHCC-99-14.
-
-
-
-
2
-
-
0542400790
-
-
See references in H. P. Nilles, Phys. Rep. 110, 1 (1984).
-
(1984)
Phys. Rep.
, vol.110
, pp. 1
-
-
Nilles, H.P.1
-
13
-
-
0036871466
-
-
Phys. Rev. DT. Kobayashi, H. Nakano, T. Noguchi, and H. Terao, 66, 095011 (2002);
-
(2002)
Phys. Rev. D
, vol.66
, pp. 95011
-
-
Kobayashi, T.1
Nakano, H.2
Noguchi, T.3
Terao, H.4
-
20
-
-
85038326575
-
-
I. Hinchliffe, F. E. Paige, E. Nagy, M. D. Shapiro, J. Soderqvist, and W. Yao, LBNL-40954.
-
I. Hinchliffe, F. E. Paige, E. Nagy, M. D. Shapiro, J. Soderqvist, and W. Yao, LBNL-40954.
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-
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21
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85038316900
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We assume for simplicity that the SUSY (Formula presented)-violating phases are vanishing. The end point is determined by only the SUSY particle masses, not coupling constants. Thus the dependence on the (Formula presented)-violating phases appears through the SUSY particle masses.
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We assume for simplicity that the SUSY (Formula presented)-violating phases are vanishing. The end point is determined by only the SUSY particle masses, not coupling constants. Thus the dependence on the (Formula presented)-violating phases appears through the SUSY particle masses.
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22
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85038318568
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hep-ph/0001086
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H. Baer, F. E. Paige, S. D. Protopopescu, and X. Tata, “ISAJET 7.48: a Monte Carlo event generator for (Formula presented) (Formula presented) and (Formula presented) reactions,” hep-ph/0001086.
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-
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Baer, H.1
Paige, F.E.2
Protopopescu, S.D.3
Tata, X.4
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24
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85038308297
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E. Richter-Was et al. ATLFAST2.21, ATLAS Internal Note PHYS-NO-079.
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E. Richter-Was et al., ATLFAST2.21, ATLAS Internal Note PHYS-NO-079.
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25
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85038305714
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For the results shown in this paper, we simply reject events with visible leptons; (Formula presented) and (Formula presented) However for point C in Table I, events with leptons with (Formula presented) are rejected.
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For the results shown in this paper, we simply reject events with visible leptons; (Formula presented) and (Formula presented) However for point C in Table I, events with leptons with (Formula presented) are rejected.
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26
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85038299852
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Strictly speaking the lower bound of the integral is slightly above (Formula presented) However, as we use a limited (Formula presented) range around the (upper) end point for the fit, this formula gives good approximation.
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Strictly speaking the lower bound of the integral is slightly above (Formula presented) However, as we use a limited (Formula presented) range around the (upper) end point for the fit, this formula gives good approximation.
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27
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85038347428
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these sets, the SUSY particles decay into two bodies dominantly. If the relevant two-body decays of gluino or top squarks are closed, the distribution of (Formula presented) at the end point does not have an edge and the significance is worse.
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In these sets, the SUSY particles decay into two bodies dominantly. If the relevant two-body decays of gluino or top squarks are closed, the distribution of (Formula presented) at the end point does not have an edge and the significance is worse.
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29
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85038285363
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The detail of the parameter sets in Table I will be shown in a future publication
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The detail of the parameter sets in Table I will be shown in a future publication 18.
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85038335022
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J. Hisano, K. Kawagoe, R. Kitano, and M. M. Nojiri (in preparation).
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J. Hisano, K. Kawagoe, R. Kitano, and M. M. Nojiri (in preparation).
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85038287505
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For events with (Formula presented) the gluino decay into (Formula presented) starts to contribute.
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For events with (Formula presented) the gluino decay into (Formula presented) starts to contribute.
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