Answer on Question #46943, Physics, Quantum Mechanics
So we have three equations:
E g = E e 2 − m 2 c 4 c ⋅ cos φ + E g − E e c cos θ E e 2 − m 2 c 4 c ⋅ sin φ = E g − E e c sin θ E g − E g ′ = E e \begin{array}{l} E _ {g} = \frac {\sqrt {E _ {e} ^ {2} - m ^ {2} c ^ {4}}}{c} \cdot \cos \varphi + \frac {E _ {g} - E _ {e}}{c} \cos \theta \\ \frac {\sqrt {E _ {e} ^ {2} - m ^ {2} c ^ {4}}}{c} \cdot \sin \varphi = \frac {E _ {g} - E _ {e}}{c} \sin \theta \\ E _ {g} - E _ {g} ^ {\prime} = E _ {e} \\ \end{array} E g = c E e 2 − m 2 c 4 ⋅ cos φ + c E g − E e cos θ c E e 2 − m 2 c 4 ⋅ sin φ = c E g − E e sin θ E g − E g ′ = E e
We will introduce everything as functions of φ \varphi φ
E e = 1 4 E g ⋅ ( m 2 c 4 + 4 E g 2 ⋅ cos 2 ( φ ) ) E_{e} = \frac{1}{4 E_{g}} \cdot \left(m^{2} c^{4} + 4 E_{g}^{2} \cdot \cos^{2}(\varphi)\right) E e = 4 E g 1 ⋅ ( m 2 c 4 + 4 E g 2 ⋅ cos 2 ( φ ) ) - final energy of the electron
if φ = 0 ⇒ E e = m 2 c 4 4 E g \varphi = 0 \Rightarrow E_{e} = \frac{m^{2}c^{4}}{4E_{g}} φ = 0 ⇒ E e = 4 E g m 2 c 4 - this is minimal possible energy, that electron can obtain via Compton scattering.
E g ′ = E g − m 2 c 4 + 4 E g 2 ⋅ cos 2 ( φ ) 4 E g E _ {g} ^ {\prime} = E _ {g} - \frac {m ^ {2} c ^ {4} + 4 E _ {g} ^ {2} \cdot \cos^ {2} (\varphi)}{4 E _ {g}} E g ′ = E g − 4 E g m 2 c 4 + 4 E g 2 ⋅ cos 2 ( φ )
if φ = 0 ⇒ E g ′ = E g − m 2 c 4 4 E g \varphi = 0 \Rightarrow E_g' = E_g - \frac{m^2c^4}{4E_g} φ = 0 ⇒ E g ′ = E g − 4 E g m 2 c 4 - so we will have non zero energy, so non zero momentum along Y axis.
We can also calculate angle θ \theta θ
sin θ = E e 2 − m 2 c 4 E g ′ \sin \theta = \frac{\sqrt{E_e^2 - m^2c^4}}{E_g'} sin θ = E g ′ E e 2 − m 2 c 4 - also non zero angle.
Yes, θ \theta θ won't be equal to 90 degrees.
ANSWER:
Electron will get it's energy from the photon.
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