Difference between revisions of "Final Lab Frame Moller Electron 4-momentum components in XZ Plane"

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=Final Lab Frame Moller Electron 4-momentum components in XZ Plane=
 
=Final Lab Frame Moller Electron 4-momentum components in XZ Plane=
 
<center>[[File:xz_lab.png | 400 px]]</center>
 
<center>[[File:xz_lab.png | 400 px]]</center>

Revision as of 22:15, 15 June 2017

[math]\textbf{\underline{Navigation}}[/math]

[math]\vartriangleleft [/math] [math]\triangle [/math] [math]\vartriangleright [/math]


Final Lab Frame Moller Electron 4-momentum components in XZ Plane

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


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



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

[math]0^\circ \le \theta '_2 \le 60^\circ \equiv 0 \le \theta '_2 \le 1.046\ Radians[/math]

Since,

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


[math]\Longrightarrow p^'_{2(z)}\ should\ always\ be\ positive[/math]