Difference between revisions of "Mlr Summ TF"

From New IAC Wiki
Jump to navigation Jump to search
Line 13: Line 13:
 
[[File:MolThetaCM_Theory.png |thumb | border | center |500 px |alt=Theory Frame Moller CM Frame |'''Figure 4a:''' A plot of the number of Moller scattering angle theta in the center of mass frame versus the theoretical differential cross section.  The width of the bins is 0.001 degrees for the angles in the center of mass frame corresponding to angles of 5 to 40 degrees in the lab frame.  A weight has been assigned for each value in theta which will give the theoretical differential cross section when applied.]][[File:MolThetaLab_Theory.png |thumb | border | center |500 px |alt=Theory Lab Frame Moller  Frame |'''Figure 4b:''' A plot of the number of Moller scattering angle theta in the lab frame versus the theoretical differential cross section.  The width of the bins is 0.5 degrees for the angles in the lab frame.  A weight has been assigned for each value in theta which will give the theoretical differential cross section when applied.]]
 
[[File:MolThetaCM_Theory.png |thumb | border | center |500 px |alt=Theory Frame Moller CM Frame |'''Figure 4a:''' A plot of the number of Moller scattering angle theta in the center of mass frame versus the theoretical differential cross section.  The width of the bins is 0.001 degrees for the angles in the center of mass frame corresponding to angles of 5 to 40 degrees in the lab frame.  A weight has been assigned for each value in theta which will give the theoretical differential cross section when applied.]][[File:MolThetaLab_Theory.png |thumb | border | center |500 px |alt=Theory Lab Frame Moller  Frame |'''Figure 4b:''' A plot of the number of Moller scattering angle theta in the lab frame versus the theoretical differential cross section.  The width of the bins is 0.5 degrees for the angles in the lab frame.  A weight has been assigned for each value in theta which will give the theoretical differential cross section when applied.]]
  
== Moller events using an lH2 target geometry==
+
== Moller events using an lH2 target geometry No Raster==
 
===DC hits -vs- Solenoid ===
 
===DC hits -vs- Solenoid ===
 
With the Torus at zero Magnetic field the solenoid is changes to show how moller electrons move off the faces of R1 DC.
 
With the Torus at zero Magnetic field the solenoid is changes to show how moller electrons move off the faces of R1 DC.
Line 25: Line 25:
 
===Photons Hits in R1===
 
===Photons Hits in R1===
 
[[File:S1_PhiThetaGammaHits.png | 400 px]]
 
[[File:S1_PhiThetaGammaHits.png | 400 px]]
 +
 +
 +
== Moller events using an dual polarized target geometry with Raster==
 +
 +
===Photon Hits in R1 when Raster size has radius of 0.2 cm===
  
 
=Latest Stuff=
 
=Latest Stuff=
  
 
[[VanWasshenova_Thesis#Mlr_Summ_TF]]
 
[[VanWasshenova_Thesis#Mlr_Summ_TF]]

Revision as of 20:20, 14 August 2018

VanWasshenova_Thesis#Mlr_Summ_TF

Moller Summary

Scattering Xsect

https://wiki.iac.isu.edu/index.php/Converting_to_barns


[math]\frac{d\sigma}{d\Omega}=\frac{ e^4 }{8E^2}\left \{\frac{1+cos^4\frac{\theta}{2}}{sin^4\frac{\theta}{2}}+\frac{1+sin^4\frac{\theta}{2}}{cos^4\frac{\theta}{2}}+\frac{2}{sin^2\frac{\theta}{2}cos^2\frac{\theta}{2}} \right \}[/math]
Theory Frame Moller CM Frame
Figure 4a: A plot of the number of Moller scattering angle theta in the center of mass frame versus the theoretical differential cross section. The width of the bins is 0.001 degrees for the angles in the center of mass frame corresponding to angles of 5 to 40 degrees in the lab frame. A weight has been assigned for each value in theta which will give the theoretical differential cross section when applied.
Theory Lab Frame Moller Frame
Figure 4b: A plot of the number of Moller scattering angle theta in the lab frame versus the theoretical differential cross section. The width of the bins is 0.5 degrees for the angles in the lab frame. A weight has been assigned for each value in theta which will give the theoretical differential cross section when applied.

Moller events using an lH2 target geometry No Raster

DC hits -vs- Solenoid

With the Torus at zero Magnetic field the solenoid is changes to show how moller electrons move off the faces of R1 DC.

ChangingRates S1 PhiThetaHits.png

Moller Electron Events(1st hits)

S1 50nA PrimaryElectronSigmasWeightedRates.png

Photons Hits in R1

S1 PhiThetaGammaHits.png


Moller events using an dual polarized target geometry with Raster

Photon Hits in R1 when Raster size has radius of 0.2 cm

Latest Stuff

VanWasshenova_Thesis#Mlr_Summ_TF