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The
production estimate
The estimate is based on
cross section for
production on proton target. Total luminosity for the 2000 run
is
, corresponding to
event rate and the total live time
. For
target
 |
(1) |
 |
(2) |
Total number of produced particles
in a given channel is
governed by the decay rate
.
The total number of reconstructed particles depends also on the acceptance
 |
(3) |
Rate of interest:
 |
(4) |
 |
(5) |
 |
(6) |
 |
(7) |
 |
(8) |
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Mihajlo Kornicer
2003-12-25