Difference between revisions of "Experimental Sensitivity to Solenoidal Field"

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(References)
(Figure-of-Merit)
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* Sensitivity ~ time x luminosity / sqrt (time x luminosity x width) ~ sqrt (time x luminosity / width) ~  sqrt (time / (<math> R_{EM}</math> x width)   
 
* Sensitivity ~ time x luminosity / sqrt (time x luminosity x width) ~ sqrt (time x luminosity / width) ~  sqrt (time / (<math> R_{EM}</math> x width)   
 
* For constant sensitivity, the experimental run time ~ <math> R_{EM} </math> x width = 1/FOM.
 
* For constant sensitivity, the experimental run time ~ <math> R_{EM} </math> x width = 1/FOM.
We note that the calculated rates give <math> R_{EM} \sim 1/B^2 </math>, and  <math>\sigma_{\omega} \sim 1/B </math>, which leads to <math> FOM \sim 1/B^3 </math>. See figure below:
+
We note that the calculated rates give <math> R_{EM} \sim 1/B^2 </math>, and  <math>\sigma_{\omega} \sim 1/B </math>, which leads to <math> FOM \sim B^3 </math>. See figure below:
  
 
[[Image:Plot resolutions c5.png |thumb|left|300px|FOM ~ 1/(R_EM x omega width)]]
 
[[Image:Plot resolutions c5.png |thumb|left|300px|FOM ~ 1/(R_EM x omega width)]]

Revision as of 18:18, 27 April 2010

References

  • GlueX-doc-1425 Magnetic Field Studies Status
  • GlueX-doc-1471 Electromagnetic Background Rate Studies (for different solenoid magnet fields and FDC hole sizes)
  • GlueX-doc-1469 Studies of particle reconstruction for $\omega$ and X(2000) events

Figure-of-Merit

We construct a Figure-of-Merit (FOM) based on the calculated electromagnetic background rates in the detector and the resolution for reconstructing omega mesons. The validity for this FOM is based on the following argument:

  • Statistical sensitivity ~ signal/sqrt(background)
  • signal ~ time x luminosity
  • background ~ time x luminosity x width of signal peak

In addition, we assume that the luminosity is limited by the rates in the detectors, which is dominated by electromagnetic background. Therefore

  • luminosity ~ 1/R_{{EM}}, where R_{{EM}} is the rate in one of the inner detectors, either the start counter or the FDC. (We use the start counter rate)

Therefore,

  • Sensitivity ~ time x luminosity / sqrt (time x luminosity x width) ~ sqrt (time x luminosity / width) ~ sqrt (time / (R_{{EM}} x width)
  • For constant sensitivity, the experimental run time ~ R_{{EM}} x width = 1/FOM.

We note that the calculated rates give R_{{EM}}\sim 1/B^{2}, and \sigma _{{\omega }}\sim 1/B, which leads to FOM\sim B^{3}. See figure below:

FOM ~ 1/(R_EM x omega width)