Compton scattering in a general medium

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Homework Statement
In a medium of refractive index 𝑛, the wavelength of light 𝜆0 is related to its frequency 𝑓0 . Variables given: input photon frequency 𝑓, outgoing photon angle 𝜃, outgoing photon frequency 𝑓′, outgoing electron angle 𝜙, outgoing electron energy 𝐸 and outgoing electron momentum 𝒑. In this problem, the momenta of all particles, before and after, lie entirely in the plane of the paper.

Part 1: Write the energy conservation equation and the momentum conservation equations for Compton scattering for incident and outgoing photons in a medium of refractive index n

Part 2: Solve the equations to obtain the outgoing photon frequency 𝑓′ in the following form:
𝑓′ = [−𝐵 ± √(𝐵^2 − 4𝐴𝐶) ]/ (2𝐴) where you are to determine the unknowns 𝐴, 𝐵 and 𝐶 in terms of 𝑓, 𝑐, 𝑛, 𝜃, and electron rest mass 𝑚. You may use the fact that for general (relativistic) electrons, the dispersion relation is 𝐸 = √[(𝑝𝑐)^2 + (𝑚𝑐^2)^2]
Relevant Equations
𝜆0 = 𝑐/(𝑛𝑓0) where 𝑐 is the speed of light in vacuum
For part one, my energy conservation equation is nhf0 + mc2 = nhf' + E

my momentum conservation in x-axis is nhf0= nhf' cos(theta) + c𝒑 cos(fi)

My momentum conservation in y-axis is nhf' sin(theta) = c𝒑 sin(fi)

For part 2 I understand that I am supposed to get a qudratic equation in terms of f' but when I tried combining all three equations but all I did was derive Compton shift equation. Where did I go wrong?
 
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FAQ: Compton scattering in a general medium

What is Compton scattering?

Compton scattering is a quantum mechanical phenomenon that occurs when X-ray or gamma-ray photons collide with charged particles, typically electrons. During this interaction, the photon transfers some of its energy to the electron, resulting in a longer wavelength (lower energy) photon being emitted and the electron being ejected from its original position. This process illustrates the particle-like behavior of light and is a key concept in quantum mechanics.

How does Compton scattering differ in a general medium compared to a vacuum?

In a general medium, Compton scattering can be influenced by the presence of other particles, such as atoms or molecules, which can affect the scattering process. The density and type of the medium can alter the scattering cross-section, energy transfer, and angular distribution of the scattered photons. In a vacuum, the scattering is primarily between the photon and free electrons, whereas in a medium, interactions with bound electrons and other particles can complicate the scattering dynamics.

What factors affect the Compton scattering process in a medium?

Several factors can influence Compton scattering in a medium, including the energy of the incoming photon, the type of material (atomic number and density), the temperature of the medium, and the presence of other charged particles. The scattering angle also plays a significant role, as it determines the energy of the scattered photon and the direction of the ejected electron. Additionally, the electron binding energy in the medium can affect the scattering dynamics.

What are the applications of Compton scattering in a general medium?

Compton scattering has various applications in fields such as medical imaging (e.g., positron emission tomography), radiation therapy, material science (for characterizing materials), and astrophysics (for studying cosmic radiation). By analyzing the scattered photons, researchers can gain insights into the composition, structure, and properties of materials, as well as the behavior of high-energy photons in different environments.

How can Compton scattering be experimentally measured in a medium?

Compton scattering can be measured using detectors that capture the scattered photons and the recoiling electrons. Common experimental setups include using scintillation detectors, semiconductor detectors, or gas-filled detectors to measure the energy and angle of the scattered photons. By analyzing the energy spectrum of the detected photons and the scattering angles, researchers can extract information about the scattering process and the properties of the medium.

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