24.3.2010 Kamil Sedlak
New variable "timeToNextEvent" added in order to simulate time differences between subsequent events. 1) /gun/meanarrivaltime meanArrivalTime (defines the mean time difference betweent the subsequent events). 2) timeToNextEvent - new variable written out to the root tree. This new variable is needed for the pile-up studies
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@ -468,6 +468,12 @@ Three special volumes ``Target, M0, M1 and M2''.
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Set the primary particle type, if it is not positive muon. For example, the negative muons
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are specified by ``/gun/primaryparticle mu-''.
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\item{\bf /gun/meanarrivaltime \emph{meanArrivalTime}}\\
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(default: /gun/meanarrivaltime 33.33333 microsecond)\\
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Set mean arrival time difference between two subsequent muons (at continuos beam).
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The output variable ``timeToNextEvent'' is subsequently generated using
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the value of \emph{meanArrivalTime} and filled into the Root tree.
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\item{\bf /gun/vertex \emph{x0} \emph{y0} \emph{z0} \emph{unit}}\\
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(default: /gun/vertex 0 0 -100 mm) \\
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Set mean values of the $x$, $y$ and $z$ coordinates of the generated particles (muons).
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@ -827,6 +833,8 @@ The list of variables that can be stored in the Root tree:
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\begin{description}
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\item{\bf runID} (Int\_t) -- run ID number.
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\item{\bf eventID} (Int\_t) -- event ID number.
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\item{\bf timeToNextEvent} (Double\_t) -- time difference between two subsequent events (at continuous beam facility) (in $\mu$s).
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This time difference is generated randomly using the ``meanArrivalTime'' defined in ``/gun/meanarrivaltime meanArrivalTime''.
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\item{\bf weight} (Double\_t) -- event weight.
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\item{\bf BFieldAtDecay\_Bx, BFieldAtDecay\_By, BFieldAtDecay\_Bz, BFieldAtDecay\_B3, BFieldAtDecay\_B4, BFieldAtDecay\_B5} (Double\_t) --
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value of the 6 coordinates of the electromagnetic field at the position and time where and when the muon decayed.
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