Difference between revisions of "BCal Beam Test Plots, January 3, 2007"

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From suggestions from Alex and others I wrote a piece of code that plots z finds sigma and then adjusts the PMT gain correction factors until the sigma of the gaussian fit is at it's minimum. Z is defined as
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From suggestions from Alex and others I wrote a piece of code that runs in ROOT that plots z finds sigma and then adjusts the PMT gain correction factors until the sigma of the gaussian fit is at it's minimum. Z is defined as
  
 
: <math> z = \frac{E_{cal} - E_{beam}}{E_{beam}} </math>  
 
: <math> z = \frac{E_{cal} - E_{beam}}{E_{beam}} </math>  
  
You can find the [[peakfit.C]] code here.  
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You can find the [[peakfit.C]] code here. ( in ROOT > .x peakfit.C )
  
 
The code goes through and adjusts each parameter by an amount epsilon until sigma is minimal. Of course the ADC conversion factor (E_beam/E_cal) has to be calculated each time too. Doing this shows a good improvement in the "floor term" and the energy dependent is still approximately 5%.
 
The code goes through and adjusts each parameter by an amount epsilon until sigma is minimal. Of course the ADC conversion factor (E_beam/E_cal) has to be calculated each time too. Doing this shows a good improvement in the "floor term" and the energy dependent is still approximately 5%.
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The fit is using <math> \sigma_{z} = \frac{a}{\sqrt{E(GeV)}} + b </math> in the package xmgrace.
  
 
[[Image:Bcalres.gif]]
 
[[Image:Bcalres.gif]]

Revision as of 16:29, 3 January 2007

From suggestions from Alex and others I wrote a piece of code that runs in ROOT that plots z finds sigma and then adjusts the PMT gain correction factors until the sigma of the gaussian fit is at it's minimum. Z is defined as

z={\frac  {E_{{cal}}-E_{{beam}}}{E_{{beam}}}}

You can find the peakfit.C code here. ( in ROOT > .x peakfit.C )

The code goes through and adjusts each parameter by an amount epsilon until sigma is minimal. Of course the ADC conversion factor (E_beam/E_cal) has to be calculated each time too. Doing this shows a good improvement in the "floor term" and the energy dependent is still approximately 5%.

The fit is using \sigma _{{z}}={\frac  {a}{{\sqrt  {E(GeV)}}}}+b in the package xmgrace.

Bcalres.gif