High Energy Muon scattering - 4-momentum

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Homework Help Overview

The discussion revolves around the concept of four-momentum transfer in the context of high-energy muon scattering. Participants explore the relationship between the four-momentum transfer and the scattering angle, specifically focusing on the approximation of \(q^2\) in terms of the initial and final energies of the muon.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the definition of four-momentum transfer and its implications in scattering processes. There are attempts to derive the expression for \(q^2\) using the properties of four-vectors and the conditions under which certain approximations hold, particularly the case where energy is much greater than mass.

Discussion Status

The discussion includes various attempts to clarify the calculation of the dot product of four-vectors and the implications of the approximation \(E \gg m\). Some participants have provided feedback on the calculations, indicating progress in understanding the relationships involved, but no consensus has been reached on the final expression.

Contextual Notes

Participants are working within the constraints of homework guidelines, which may limit the amount of direct assistance provided. The discussion reflects uncertainty regarding the correct application of four-momentum concepts and the necessary conditions for approximations.

Matt atkinson
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Homework Statement


Explain what the term "four-momentum transfer ##q##" is
Show that for a high energy muon scattering at an angle ##\theta##, the value of ##q^2## is given approximately by;
##q^2=2E_iE_f(1-cos(\theta))##
where ##E_i## and ##E_f## are the initial and final values of the muon's energy. State when this approximation is justified.

Homework Equations


##\vec{p}=(p_1,p_2,p_3,iE)##

The Attempt at a Solution


The first part, four momentum transfer is just the momentum and energy lost/gained in a scattering process by the scattered particle?

And the second part, i know the approximation should be that ##E>>m## but i can't seem to work with 4-momentum.

What i tried to do was;
##q^2=(p_i-p_f)^2=|p_i|^2+|p_f|^2-2p_i\cdot p_f=|p_i|^2+|p_f|^2-E_iE_fcos(\theta)##
and i assume somehow i need to get ##|p_i|^2+|p_f|^2=2E_iE_f## but I am not sure how.

Would it be because the ##E>>m## then the ##p \approx E## but then that would just mean ##q^2=E_i^2+E_f^2-E_iE_fcos(\theta)##
 
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What about the energy component in the dot product?
 
So,
##2p_i \cdot p_f=2((p_{i_x},p_{i_y},p_{i_z},iE_i) \cdot (p_{f_x},p_{f_y},p_{f_z},iE_f))=-2E_iE_f+2((p_{i_x},p_{i_y},p_{i_z}) \cdot (p_{f_x},p_{f_y},p_{f_z})##
actually my momentum transfer would be this then;
##q^2=|p_i|^2+|p_f|^2+2E_iE_f-2((p_{i_x},p_{i_y},p_{i_z}) \cdot (p_{f_x},p_{f_y},p_{f_z})##
##q^2=|p_i|^2+|p_f|^2+2E_iE_f-2|{}^3p_i||{}^3p_f|cos(\theta)##
The subscript before just to symbolize that they are three vectors not the 4 vectors? not sure how to show that.

then using my assumption that ##E \approx p## for ##E>>m##;

##q^2=|p_i|^2+|p_f|^2+2E_iE_f-2E_iE_fcos(\theta)##
 
Last edited:
You're not calculating the dot product of a 4-vector correctly. Try splitting the dot product into the energy component and the combined momentum components.

And remember that you're subtracting the two vectors and then taking the dot product of the result with itself.
 
I think i managed it, if you could just check my working!

##q^2=(p_i-p_f)\cdot(p_i-p_f)=(p_{i_x}-p_{f_x},p_{i_y}-p_{f_y},p_{i_z}-p_{f_z},i(E_i-E_f))\cdot(p_{i_x}-p_{f_x},p_{i_y}-p_{f_y},p_{i_z}-p_{f_z},i(E_i-E_f))##
##q^2=|p_i|^2+|p_f|^2-2p_i\cdot p_f-E_i^2-E_f^2+2E_iE_f##
Now using my condition that if, ##E>>m## then ##p\approx E##;
##q^2=2E_iE_f-2p_i\cdot p_f##
##q^2=2E_iE_f-2E_iE_fcos(\theta)##
 
Yes, you just needed to get the dot product sorted out.
 
Thank you!
 

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