Difference between revisions of "Analysis"

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====summary table====
 
====summary table====
 +
{|border="3"
 +
!Beam Energy||Torus Current||Begin Run||End Run
 +
|-
 +
|1606||1500||25488||25559
 +
|-
 +
|1606||1946||25560||25609
 +
|-
 +
|1606||1500||25669||25732
 +
|
 +
}
  
 
==Pion==
 
==Pion==

Revision as of 23:55, 6 August 2007

Particle Identification

Electron

Cuts

Calorimeter based cuts

The distributions below represent two types of cuts applied to improve the electron particle identification (PID) using a 4 GeV electron beam incident on an NH3 target. The electron calorimeter is segmented into an inner[math]EC_{inner}[/math] and an outer[math]EC_{outer}[/math] region. The total energy absorbed by the calorimeter system is recorded in the variable [math]EC_{tot}[/math]. The momentum ([math]P[/math]) is calculated using the reconstructed track and the known torus magnetic field. The distributions of [math]EC_{tot}[/math] and [math]EC_{inner}[/math] are shown below where both have been divided by the electron momentum and no cuts have been applied.


[math]EC_{tot}\gt 0.2*p[/math]

Without any cuts we have 181018 entries. After using the following cut [math]EC_{tot}\gt 0.2*p[/math] we are getting 127719 entries, which is about 70.55% of 181018.

Etotal P using tot cut.gif
Einner P using tot cut.gif




[math]EC_{inner}\gt 0.08*p[/math]
Etotal P using inner cut.gif
Einner P using inner cut.gif



Etotal P using both cuts.gif
Einner P using both cuts.gif



After the cut on the energy deposited into inner part of electron calorimeter, number of entries decreases by 22%.
Einner over P using inner cut.gif

Both cuts are applied

Etotal over P using both cuts.gif

In case of using the cuts of the total deposited energy and the energy deposited into inner calorimeter number of entries decreases ~36%

Einner over P using both cuts.gif

summary table

Beam Energy Torus Current Begin Run End Run
1606 1500 25488 25559
1606 1946 25560 25609
1606 1500 25669 25732

}

Pion

Quality Checks

Rates

Asymmetries