Compton Scattering of a photon by a moving electron

AI Thread Summary
The discussion focuses on deriving the wavelength of a photon after Compton scattering with a moving electron, given the condition that the total energy of the electron is much greater than its rest mass energy. The initial attempt at the solution leads to an expression for the scattered wavelength, but the assumption E >> mc² needs to be applied to simplify the momentum term. The participants note that this approximation leads to the elimination of angular dependence and raises questions about the initial directions of the photon and electron. The final expression for the wavelength after scattering is confirmed to be λ' = (hc/E)(1 + (m²c⁴λ)/(4hcE)). This highlights the importance of correctly applying the energy-momentum relationship in high-energy scattering scenarios.
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Homework Statement


If the total energy of the electron E>>mc^{2}
Prove that the formula of wavelength would be
\lambda '=\frac{hc}{E}(1+\frac{m^{2}c^{4}\lambda}{4hcE})
where \lambda ' is the wavelenght after scattering
m is the mass of electron

Homework Equations





The Attempt at a Solution


I have proved that \lambda '=\frac{\lambda(E-Pc)+2hc}{E+Pc}
In my equation, P is the initial momentum of the electron.
I haven't use the given assumption E>>mc^{2}. So we must use it to eliminate P.

But if E>>mc^{2}\Rightarrow E\approxPc
this cannot get the answer
 
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There's no angular dependence? The problem seems a bit ambiguous to me. What are the directions of the photon and electron initially?
 
they are both along x axis, even after collision

The origin question should be
Consider Comton scattering of a photon by a moving electron. Before the collision the photon has wave length λ and is moving in the +x direction, and the electron is moving in the -x direction with total energy E. The photon and electron collide head-on. After the collision both are moving in the -x direction.
(a) Drive an expression for the wavelength λ' of the scattered photon.
(b) Show that for the case E>>mc^2, the result reduces to \lambda '=\frac{hc}{E}(1+\frac{m^{2}c^{4}\lambda}{4hcE}
 
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OK, you have
$$\lambda' = \frac{\lambda(E-Pc)+2hc}{E+Pc} = \frac{2hc}{E+Pc} + \lambda\frac{E-Pc}{E+Pc}$$Now multiply the second term by (E+Pc)/(E+Pc) and then use the approximation ##E\approx Pc##.
 
vela said:
OK, you have
$$\lambda' = \frac{\lambda(E-Pc)+2hc}{E+Pc} = \frac{2hc}{E+Pc} + \lambda\frac{E-Pc}{E+Pc}$$
The second term will become zero after using E=Pc, since the second term has the factor E-Pc.
 
That's not quite true. You need to multiply by (E+Pc)/(E+Pc) and simplify the numerator and then let E=pC.
 
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thx!
 
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