Difference between revisions of "Mlr Summ TF"
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[[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. | ||
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===Photons Hits in R1=== | ===Photons Hits in R1=== | ||
[[File:S1_PhiThetaGammaHits.png | 400 px]] | [[File:S1_PhiThetaGammaHits.png | 400 px]] | ||
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| + | == 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
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.
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.
Moller Electron Events(1st hits)
Photons Hits in R1
