Difference between revisions of "Mlr Summ TF"

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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.
  
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====With Magnet Components====
 
[[File:ChangingRates_S1_PhiThetaHits.png | 600 px]][[File:ChangingRates_S1_PhiThetaHits_Full.png | 600 px]]
 
[[File:ChangingRates_S1_PhiThetaHits.png | 600 px]][[File:ChangingRates_S1_PhiThetaHits_Full.png | 600 px]]
  
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[[File:ComparingOppositeFields_S1_PhiThetaHits.png | 800 px]]
  
[[File:ComparingOppositeFields_S1_PhiThetaHits.png | 800 px]]
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====Without Magnet Components====
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[[File:ComparingMagnetComponents_S1_PhiThetaHits.png]]
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=====With Only S1R1 DC======
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[[File:ComparingDCcomponents_S1_PhiThetaHits.png]]
  
 
===Moller Electron Events(1st hits)===
 
===Moller Electron Events(1st hits)===

Revision as of 01:54, 27 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]
Moller E -vs- Theta in lab


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.

Baseline

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.


With Magnet Components

ChangingRates S1 PhiThetaHits.pngChangingRates S1 PhiThetaHits Full.png


HitMakeUp.png


ComparingOppositeFields S1 PhiThetaHits.png

Without Magnet Components

ComparingMagnetComponents S1 PhiThetaHits.png

With Only S1R1 DC=

ComparingDCcomponents S1 PhiThetaHits.png

Moller Electron Events(1st hits)

S1 50nA PrimaryElectronSigmasWeightedRates.pngS1 50nA PrimaryElectronSigmasWeightedRates Full.png

Photons Hits in R1

S1 PhiThetaGammaHits.pngS1 PhiThetaGammaHits Full.png



Tomography (where are the photons coming from)

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