Difference between revisions of "Sadiq Thesis"

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= Intruduction =
+
= Introduction =
  
 
== Positron ==
 
== Positron ==
Line 17: Line 17:
  
  
 +
=Theory=
  
=HRRL Charecterization =
+
==positron creation from Bremsstrahlung=
  
== Emittance Measurement ==
+
=Apparatus=
  
== Energy Spread Measurement==
+
== HRRL Positron Beamline ==
  
== Other parameters==
+
==Beam properties==
  
= HRRL Positron Beamline =
+
=== Emittance Measurement ===
  
== Moving HRRL to New Location ==
+
=== Energy Spread Measurement===
  
===Radiation simulation ===
+
=== Current, rep-rate===
  
===Radiation experiment ===
+
===Radiation Footprint==
  
===Radiation Perdiction===
+
==Positron detection==
 +
===DAQ setup===
  
== HRRL==
+
=Data Analysis=
  
 +
==Signal extraction==
 +
==Background subraction==
  
 +
==Sources of Systematic Errors==
 +
 +
=Conclusion=
  
  

Revision as of 17:44, 20 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

HRRL Beamline for Positron Source

Theory

=positron creation from Bremsstrahlung

Apparatus

HRRL Positron Beamline

Beam properties

Emittance Measurement

Energy Spread Measurement

Current, rep-rate

=Radiation Footprint

Positron detection

DAQ setup

Data Analysis

Signal extraction

Background subraction

Sources of Systematic Errors

Conclusion

References

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