Difference between revisions of "DV Moller LH2"
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[[File:MolTheta.png|frame|center|alt=Moller Electron Angle Theta in Lab Frame|'''Figure 2b:''' The Moller electron scattering angle theta distribution for 4E7 incident 11 GeV electrons in the Lab frame of reference.]] | [[File:MolTheta.png|frame|center|alt=Moller Electron Angle Theta in Lab Frame|'''Figure 2b:''' The Moller electron scattering angle theta distribution for 4E7 incident 11 GeV electrons in the Lab frame of reference.]] | ||
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| + | Noting that the GEANT4 data included data for the Kinetic Energy and not the total energy, we can perform the substitution using | ||
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| + | <center><math>E^2=p^2+m^2</math></center> | ||
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| + | Performing [[DV_Calculations_of_4-momentum_components|the relativistic transformation]], we find for an incoming electron with momentum of 11GeV, we should find the momentum in the center of mass to be around '''53 MeV''' . | ||
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| + | [[File:FnlMomCM_new.png|frame|center|alt=Scattered Electron Momentum in Center of Mass Frame|'''Figure 3a:''' The scattered electron momentum distribution for 4E7 incident 11 GeV(Lab) electrons in the Center of Mass frame of reference.]] | ||
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| + | [[File:MolMomCM_new.png|frame|center|alt=Moller Electron Momentum in Center of Mass Frame|'''Figure 3b:''' The Moller electron momentum distribution for 4E7 incident 11 GeV(Lab) electrons in the Center of Mass frame of reference.]] | ||
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| + | [[File:FnlThetaCM.png|frame|center|alt=Scattered Electron Angle Theta in Center of Mass Frame|'''Figure 4a:''' The scattered electron scattering angle theta distribution for 4E7 incident 11 GeV(Lab) electrons in the Center of Mass frame of reference.]] | ||
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| + | [[File:MolThetaCM.png|frame|center|alt=Moller Electron Angle Theta in Center of Mass Frame Frame|'''Figure 4b:''' The Moller electron scattering angle theta distribution for 4E7 incident 11 GeV(Lab) electrons in the Center of Mass frame of reference.]] | ||
Latest revision as of 00:06, 15 April 2016
Figure 1a: The scattered electron momentum distribution for 4E7 incident 11 GeV electrons in the Lab frame of reference.
Figure 1b: The Moller electron momentum distribution for 4E7 incident 11 GeV electrons in the Lab frame of reference.
Figure 2a: The scattered electron scattering angle theta distribution for 4E7 incident 11 GeV electrons in the Lab frame of reference.
Figure 2b: The Moller electron scattering angle theta distribution for 4E7 incident 11 GeV electrons in the Lab frame of reference.
Noting that the GEANT4 data included data for the Kinetic Energy and not the total energy, we can perform the substitution using
Performing the relativistic transformation, we find for an incoming electron with momentum of 11GeV, we should find the momentum in the center of mass to be around 53 MeV .
Figure 3a: The scattered electron momentum distribution for 4E7 incident 11 GeV(Lab) electrons in the Center of Mass frame of reference.
Figure 3b: The Moller electron momentum distribution for 4E7 incident 11 GeV(Lab) electrons in the Center of Mass frame of reference.
Figure 4a: The scattered electron scattering angle theta distribution for 4E7 incident 11 GeV(Lab) electrons in the Center of Mass frame of reference.
Figure 4b: The Moller electron scattering angle theta distribution for 4E7 incident 11 GeV(Lab) electrons in the Center of Mass frame of reference.