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.]] | ||
| − | == | + | ==DC hits -vs- Solenoid == |
With the Torus at zero Magnetic field the solenoid is changes to show how moller electrons move off the fact of R1 DC. | With the Torus at zero Magnetic field the solenoid is changes to show how moller electrons move off the fact of R1 DC. | ||
Revision as of 20:22, 8 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.
DC hits -vs- Solenoid
With the Torus at zero Magnetic field the solenoid is changes to show how moller electrons move off the fact of R1 DC.
Theta -vs- Phi
moller electron
Moller events per (112 x 12) wire [Hz]