Difference between revisions of "Analysis"

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=Particle Identification=
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[[Particle Identification]]<br>
==Electron==
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[[Quality Checks]]<br>
  
=== Cuts ===
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[[EG1_Teleconferences_DeltaDoverD]]
  
==== Calorimeter based cuts====
+
[[http://wiki.iac.isu.edu/index.php/Delta_D_over_D Back to Delta_D_over_D]]
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.
 
  
  
 +
[[ phi angle in CM frame for different runs]]<br>
  
=====<math>EC_{tot}>0.2*p</math>=====
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[[some things]]
 
 
 
 
Without any cuts we have 181018 entries. After using the following cut <math>EC_{tot}>0.2*p</math> we are getting 127719 entries, which is about 70.55% of 181018. <br>
 
 
 
[[Image:Etotal_P_using_tot_cut.gif | 400 px|left]] [[Image:Einner_P_using_tot_cut.gif | 400 px|right]]<br>
 
 
 
 
 
 
 
 
 
=====<math>EC_{inner}>0.08*p</math>=====
 
 
 
 
 
After the cut on the energy deposited into inner part of electron calorimeter, number of entries decreases by 22%.<br>
 
 
 
[[Image:Etotal_P_using_inner_cut.gif | 400 px|left]] [[Image:Einner_P_using_inner_cut.gif | 400 px|right]]<br>
 
 
 
 
 
=====Both cuts <math>  EC_{tot}>0.2*p EC_{inner}>0.08*p  </math>=====
 
 
 
In case of using the cuts of the total deposited energy and the energy deposited into inner calorimeter number of entries decreases ~36% <br>
 
 
 
[[Image:Etotal_P_using_both_cuts.gif | 400 px|left]] [[Image:Einner_P_using_both_cuts.gif | 400 px|right]]<br>
 
 
 
 
 
====summary table====
 
 
 
 
 
{|border="2" colspan = "20"
 
!Beam Energy||Torus Current||Begin Run||End Run ||file used || cuts
 
|-
 
| || || || || || <math>EC_{tot}>0.2*p</math> || <math>EC_{inner}>0.08*p</math>|| <math>EC_{tot}>0.2*p </math> and <math> EC_{inner}>0.08*p</math>
 
|-
 
|1606||1500||25488||25559||dst25504_02.B00||64%||49.5%||78%
 
|-
 
|1606||1946||25560||25605
 
|-
 
|1606||1500||25669||25732||dst25669_02.B00||64%||49%||78%
 
|-
 
|1606||1500||25742||26221||dst25754_02.B00||21%||11%||24%
 
|-
 
|1606||-1500||26222||26359||dst26224_02.B00||4.6%||3%||6.6%
 
|-
 
|5764||-2250||26468||26722||dst26489_02.B00||12.2%||14.4%||19.1%
 
|-
 
|5764||0||26723||26775||dst26779_02.B00
 
|-
 
|5764||-2250||26776||26851
 
|-
 
|5735||-2250||26874||27068||dst26904_02.B00
 
|-
 
|5735||2250||27069||27198||dst27070_02.B00
 
|-
 
|2288||1500||27205||27351||dst27225_02.B00
 
|-
 
|5627||2250||27356||27364||dst27358_02.B00
 
|-
 
|5627||-2250||27366||27380||dst27368_02.B00
 
|-
 
|5627||2250||27386||27499||dst27388_02.B00
 
|-
 
|5627||965||27502||27617
 
|-
 
|1724||-1500||27644||27798||dst27649_02.B00
 
|-
 
|2562||-1500||27799||27924||dst27809_02.B00
 
|-
 
|2792||-1500||27936||27941||dst27937_02.B00
 
|-
 
|2562||-1500||27942||27995||dst27942_02.B00
 
|-
 
|2562||1500||28001||28069||dst28002_02.B00
 
|-
 
|4239||2250||28074||28277||dst28075_02.B00
 
|-
 
|4239||-2250||28280||28479||dst28281_02.B00
 
|-
 
|4239||2250||28482||28494
 
|-
 
|4239||-2250||28500||28505
 
|-
 
|4239||2250||28506||28510||dst28509_02.B00
 
|-
 
|1724||1500||28512||28526
 
|-
 
|1724||-1500||28527||28532
 
|-
 
|3210||-2250||28549||28570
 
|}
 
 
 
==Pion==
 
=Quality Checks=
 
==Rates==
 
==Asymmetries==
 

Latest revision as of 18:49, 13 January 2009