Difference between revisions of "Sadiq Thesis"

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===== hand calculation of error =====
 
===== hand calculation of error =====
  
<math>R = \frac{N_p}{N_e} = \frac{ 0.25 \pm 0.015}{ (1.365 \pm 0.0239) \times 10^{14} } = 1.83 10^{-15}</math>
+
<math>R = \frac{N_p}{N_e} = \frac{ 0.25 \pm 0.015}{ (3.90887 \pm 0.224963) \times 10^{13} } = 0.06395 \times 10^{-13}  = 6.395 \times 10^{-15}</math>
  
 
<math>R = 18.3 \times 10^{-16}</math>
 
<math>R = 18.3 \times 10^{-16}</math>

Revision as of 06:02, 24 September 2012

Introduction

Positron

Positron is the antimatter of electron. Positrons have same mass as electron ( [math]511~\frac{keV}{c^2}[/math]), carries positive charge, and it is noted as "[math]e^+[/math]".

Positrons predicted by Paul Dirac in 1928, <ref name="Dirac1928"> The Quantum Theory of the Electron, P. A. M. Dirac, Proc. R. Soc. Lond. A February 1, 1928 117 778 610-624;</ref>, and experimentally observed by Dmitri Skobeltsyn in 1929 and by Carl D. Anderson in 1932 <ref name="e+_discover"> General Chemistry, Taylor and Francis. p. 660. </ref>. Anderson also coined the term positron and he won the Nobel Prize for Physics in 1936.



<ref name="name"> BOOK_Gernal, Auther, Month_Year,issue,page </ref>

Positron Beamline History

Theory

positron creation from Bremsstrahlung

Positron rate prediction

Apparatus

HRRL Positron Beamline

Beam properties

Emittance Measurement

Energy Spread Measurement

Current, rep-rate

Radiation Footprint

Positron detection

DAQ setup

Data Analysis

Signal extraction

For 3 MeV and on detector show all the steps

  1. Raw counts target in and out (calibrated energy)
  2. Normalized counts
  3. background subtracted
  4. Integral (zoomed in and with error)

Example of error propagation for the above

Raw counts target in and out

The ingeral shown in read is from the background is subtracted spectrum.

run in run out NaI Left: image with cut NaI Right: image with cut 3735 3736 Hrrl pos 27jul2012 data ana with Cuts r3735 ove r3736 No Norm DL.png Hrrl pos 27jul2012 data ana with Cuts r3735 ove r3736 No Norm DR.png

Reprate = 300 Hz

Run time = 1002 s

Pulses = 301462

Events = 9045 (Hz)

e+ rate NaI Left = 256 +- 16 (Hz).

Normalized counts

The ingeral shown in read is from the background is subtracted spectrum.

3735 and 3736

Reprate = 300 Hz

Run time = 1002 s

Pulses = 301462

Events = 9045

Total number of electrons in this run = 3.91669e+016 +- 2.25412e+015

Total charge of electrons in this run = 0.00627523 +- 0.000361151 C

e- rate = 3.90887e+013 +- 2.24963e+012 (Hz)

e- current:I_e- =6.26271e-006+-3.6043e-007 (A).

e+ rate = 0.254997 +- 0.0159527 (Hz).

Ne+/Ne-=6.52353e-015+-4.0879e-016.

Ne+/I_e-=0.255 Hz e+ / 6.2627 [math]\mu[/math]A e-

hand calculation of error

[math]R = \frac{N_p}{N_e} = \frac{ 0.25 \pm 0.015}{ (3.90887 \pm 0.224963) \times 10^{13} } = 0.06395 \times 10^{-13} = 6.395 \times 10^{-15}[/math]

[math]R = 18.3 \times 10^{-16}[/math]

[math]\Delta R = \sqrt{\frac { \Delta N_p^{2} }{ N_e^{2} } + (- \frac{ N_p }{ N_e^{2} })^2 \Delta N_e^{2} } = \frac{\sqrt{ \Delta N_p^{2} + \frac{ N_p^{2} }{ N_e^{2} } \Delta N_e^{2} }}{ N_e}[/math]


[math]\Delta R = \frac{\sqrt{ 0.016^{2} + (\frac{ 0.25 }{ 3.909\times 10^{13} } 0.225 \times 10^{13})^{2} }}{ 3.909\times 10^{13}}[/math]

Background subraction

Sources of Systematic Errors

Efficiency measurement

acceptance, quad collection efficiency,

Conclusion

References

<references/>