Components of Compton Spectrum

In summary, the Compton edge and the single and double escape peaks come from the maximum energy a photon can have before it escapes or is absorbed, respectively.
  • #1
droogie01
10
0
Hey can someone explain the significants of the different components of the Compton spectrum? I know that the Compton edge comes from the incident angle of the photon approaching 180 degrees and that its the maximum energy that can be transferred from the photon to the electron without reaching the photoelectric peak.

But what I'm not sure of is the significants of the single and double escape peaks ? Also at the photo electric peak is the photon absorbed and then remitted or just all of its momentum transferred to the electron?

Anyways I have an exam on this on monday and missed the lecture on it i guess.

Thanks!

Darren
 
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  • #2
droogie01 said:
Hey can someone explain the significants of the different components of the Compton spectrum? I know that the Compton edge comes from the incident angle of the photon approaching 180 degrees and that its the maximum energy that can be transferred from the photon to the electron without reaching the photoelectric peak.

But what I'm not sure of is the significants of the single and double escape peaks ? Also at the photo electric peak is the photon absorbed and then remitted or just all of its momentum transferred to the electron?
Is one asking about gamma spectroscopy in general.

The gamma spectrum depends on the energy levels of the initial gamma ray. When a gamma source produces a gamma ray with energy > 1.022 MeV, then it can produce electron-positron (e-e+) pairs. When a e-e+ is produced, the e+ eventually looses energy and is annihilated with an electron to produce to gamma rays, each of 0.511 MeV. Now on or both gamma rays can escape the scintillation detector. So in addition to a photopeak at E, there are peaks at E-0.511 and E-2(0.511) = E - 1.022 MeV.

There is also the Compton edge which is at E - Emax, where Emax is the maximum energy a gamma ray can loose by scattering 180°.
 
  • #3
so the single escape peak would just correspond to the energy of a photon that was produced by an electron-positron annihilation that has already happened? leftovers from the initial collision so to speak? and the double would just be the same thing happening again?
 
  • #4
ok i think i kinda got it now.

the single escape peak (E-.511) is just a photon that was created by the annihilation bouncing off another e- in the system right?

what does the double escape peak (E-(2*.511))correspond to though?
 
  • #5
droogie01 said:
ok i think i kinda got it now.

the single escape peak (E-.511) is just a photon that was created by the annihilation bouncing off another e- in the system right?
The single escape peak comes from the loss of the 0.511 MeV gamma (single gamma) that has escaped from the system, but the other one is caught. So the energy counted is total E minus the 0.511 MeV that escapes.

what does the double escape peak (E-(2*.511))correspond to though?
Two 0.511 MeV gammas have escaped, i.e. some of the energy is detected by the energy deposited by the electron-positron pair, but when the positron annihilates, it is possible that both 0.511 MeV gammas escape from the system.
 
  • #6
lol

so simple now:rolleyes:

thanks very much you probably just added 10% to my final exam mark !
 

Related to Components of Compton Spectrum

1. What is the Compton Effect?

The Compton Effect, also known as Compton Scattering, is a phenomenon in which a photon (particle of light) collides with an electron, causing the photon to lose energy and change direction. This effect was discovered by Arthur Compton in 1923, and it provided evidence for the particle nature of light.

2. What are the components of the Compton Spectrum?

The Compton Spectrum is made up of two components: the incident (incoming) photon and the scattered photon. The incident photon has a specific energy and wavelength, while the scattered photon has a lower energy and longer wavelength due to the collision with the electron.

3. How is the Compton Spectrum related to X-ray imaging?

X-ray imaging relies on the Compton Effect to create images of the inside of objects. When X-rays are directed at an object, some of the photons will be scattered, while others will pass through and create an image. The scattered photons create the Compton Spectrum, which can be used to identify the materials inside the object.

4. What is the significance of the Compton Spectrum in understanding the structure of matter?

The Compton Spectrum is significant in understanding the structure of matter because it provides information about the properties of electrons, such as their mass and energy. By studying the behavior of electrons in the Compton Effect, scientists can gain a better understanding of the subatomic particles that make up matter.

5. How does the Compton Spectrum demonstrate the wave-particle duality of light?

The Compton Effect is a clear demonstration of the wave-particle duality of light. The incident photon behaves like a particle, transferring energy and momentum to the electron, while the scattered photon behaves like a wave, changing direction and wavelength. This phenomenon is further evidence of the dual nature of light as both a particle and a wave.

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