Beam test possibilities at JINR and Fermilab V. Pronskikh Fermilab 02/15/2012.
ScECAL Fermilab Beam Test analysis
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1 ScECAL Fermilab Beam Test analysis ScECAL Group Meeting Kyungpook National University, Daegu, Republic of Korea, April 28 th , 2010 Adil Khan, Satoru Uozumi, DongHee Kim
description
ScECAL Fermilab Beam Test analysis. ScECAL Group Meeting Kyungpook National University, Daegu, Republic of Korea, April 28 th , 2010 Adil Khan, Satoru Uozumi, DongHee Kim. Energy Spectrum with out Temperature Correction. # of counts. Energy Deposit in ScECAL (MIPS). Mean. Energy(GeV). - PowerPoint PPT Presentation
Transcript of ScECAL Fermilab Beam Test analysis
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ScECAL Fermilab Beam Test analysis
ScECAL Group Meeting
Kyungpook National University, Daegu, Republic of Korea,April 28th , 2010
Adil Khan, Satoru Uozumi, DongHee Kim
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Energy Spectrum with out Temperature Correction
Energy Deposit in ScECAL (MIPS)
# of
co
unts
1/sqrt(E)
Energy(GeV)
Mean
Sig/E
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Energy Spectrum with Temperature Correction
Energy Deposit in ScECAL (MIPS)
# of
co
unts
1/sqrt(E)
Energy(GeV)
Mean
Sig/E
Esum += (slope*Nominal Temp+offset) / (Slope*HM3Temp+offset)*En
TNominal = 25C
After using Temperature Correction Factor, the result is almost same, No significant difference.
The quadratic function“Pol2” is used for fitting Energy Resolution.
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BACK UP
Esum += (slope*Nominal Temp+offset) / (Slope*HM3Temp+offset)*En
TNominal = 25C
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ScECAL Temp Vs HcalM3temp1
2 3 4
Splitted into 4 parts , in order to makethe Temp distribution for linear Fit
hCALM3Temp(C)
ScE
CA
LT
emp( C
)
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Mip Constant Vs Correlated Temp
Temperature=P0* hCALM3 + P1
MipConst and Temperature Obtained Run by Run
