Energy Reconstruction in Gamma Spectroscopy

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Discussion Overview

The discussion revolves around the topic of energy reconstruction in gamma spectroscopy, specifically focusing on the mathematical relationships used to derive the total energy from measurements taken by photo tubes in a crystal-scintillator detector. Participants explore the implications of using different equations for energy reconstruction and the factors influencing these calculations.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Exploratory

Main Points Raised

  • One participant questions why the reconstructed energy is given by the formula E_{T}^{\prime} = \sqrt{E_{1} \cdot E_{2}} instead of E_{T}^{\prime} = E_{1} + E_{2}, seeking a theoretical justification.
  • Another participant suggests that the multiplication of energies corresponds to an addition of the exponents in the exponential decay, implying that the first formula yields the correct result while the second does not.
  • A participant calculates the reconstructed energy and arrives at E_{T}^{\prime}=\widetilde{E}_{T} \cdot e^{-\alpha \cdot \frac{\ell}{2}}, expressing confusion about how this relates to the position of the incident gamma rays.
  • Some participants propose that the total energy reconstruction is independent of the position of the incident gammas relative to the PMTs, suggesting that the method yields consistent results regardless of the source's position.
  • There is a mention that the parameters α and l must be known for accurate energy reconstruction, highlighting the importance of calibration in the process.
  • One participant notes that α could vary with irradiation, suggesting that periodic recalibration may be necessary depending on the experimental setup.

Areas of Agreement / Disagreement

Participants generally agree on the independence of total energy from the position of the incident gammas relative to the PMTs, but there is no consensus on the implications of the mathematical derivations or the necessity of recalibration frequency.

Contextual Notes

Participants express uncertainty regarding the effects of varying parameters and the specific conditions under which the energy reconstruction formulas apply. The discussion does not resolve these uncertainties.

Cmertin
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I have a question about energy reconstruction. I'm writing up a paper, and I'm trying to understand why this is the reason, before putting it in my paper. I know from experimental evidence that it is the case, though I would like to know if there is a reason.

Let's say you have a sufficiently long crystal-scintillator detector, on the order of 50 cm or so. On each end of the crystal is one photo tube. Now, the energy that each photo tube receives can be written as the following formula (I know why, but I'd rather not explain if I don't have to)

E_{1}=\widetilde{E}_{T} \cdot e^{-x \cdot \alpha}
E_{2}=\widetilde{E}_{T} \cdot e^{-\alpha \cdot (\ell-x)}

Where E_{1,2} are the corresponding energies for each detector 1 and 2, \alpha is the light attenuation factor for said detector, \ell is the total length of the detector, x is the position of the incident photon before it interacts with the crystal, and \widetilde{E}_{T} is the theoretical value for the incident gamma - ie the total energy of the gamma.

Now, my question is, why when recreating the energy based off of the energy received from each detector is the equation

E_{T}^{\prime} = \sqrt{E_{1} \cdot E_{2}}

instead of

E_{T}^{\prime} = E_{1} + E_{2}

where E_{T}^{\prime} is the reconstructed energy based on the two PMT's​

Can anyone help me understand this?

Thanks in advanced.
 
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Just calculate both to see it. A multiplication of the energies corresponds to an addition of the exponents in the exponential. The first one gives the correct result, the second one does not.
 
mfb said:
Just calculate both to see it. A multiplication of the energies corresponds to an addition of the exponents in the exponential. The first one gives the correct result, the second one does not.

I've done that and got the following result, but I'm not sure how it reads as the total energy. What I get is

E_{T}^{\prime}=\widetilde{E}_{T} \cdot e^{-\alpha \cdot \frac{\ell}{2}}​

However, how I don't see how the relative positions to each photo tube take effect, since they cancel out when you work it out. Or, is this simply saying that the total energy is equal to when the source is at the center of the detector? But I can't follow that logic because it's been reconstructed at different positions.

Edit: I just had some brain food, a doughnut, and I think I came to the realization what this is saying. It's saying that the total energy is independent of the position of the incident gammas relative to the PMTs. Therefore, by using this relation, one always winds up with the same value that one were to have gotten if the source was in the center and the energy that each PMT "read" was equal. Yes? Sorry for the previous bit, I'm a bit tired.
 
Last edited:
It's saying that the total energy is independent of the position of the incident gammas relative to the PMTs. Therefore, by using this relation, one always winds up with the same value that one were to have gotten if the source was in the center and the energy that each PMT "read" was equal.
Right. The effect of x is cancelled, which is exactly what you want. α and l have to be known to reconstruct the energy afterwards.
 
mfb said:
Right. The effect of x is cancelled, which is exactly what you want. α and l have to be known to reconstruct the energy afterwards.


Awesome. Thank you. I kind of feel dumb for asking such a simple question now. And I understand that α and l have to be known to reconstruct the energy, you never forget the first time you calibrate detectors, do you?
 
α could change with irradiation, so it might be better to repeat the calibration from time to time. But that depends on the setup.
 

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