Difference between revisions of "Theta Dependent Components"

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[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\vartriangleleft </math>]]
 
[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\vartriangleleft </math>]]
[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\triangle </math>]]
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[[VanWasshenova_Thesis#Weighted_Isotropic_Distribution_in_Lab_Frame|<math>\triangle </math>]]
 
[[CED_Verification_of_DC_Angle_Theta_and_Wire_Correspondance|<math>\vartriangleright </math>]]
 
[[CED_Verification_of_DC_Angle_Theta_and_Wire_Correspondance|<math>\vartriangleright </math>]]
  

Revision as of 14:32, 30 May 2017

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Xz lab.png
Figure 3: Definition of Moller electron variables in the CM Frame in the x-z plane.
Using \theta '_2=\arccos \left(\frac{p^'_{2(z)}}{p^'_{2}}\right)


\Longrightarrow {p^'_{2(z)}=p^'_{2}\cos(\theta '_2)}



Checking on the sign resulting from the cosine function, we are limited to:

90θ2180π2θ2πRadians

Since,

\frac{p^'_{2(z)}}{p^'_{2}}=cos(\theta '_2)


\Longrightarrow p^'_{2(z)}\ should\ always\ be\ negative


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