Difference between revisions of "JB Analysis"

Latest revision as of 22:54, 3 September 2017

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 Go back [[2nCor_44]]
-=DU runs=
-==TDC spectrum==
-[[DTC]]
-==Target in vs. target out==
+[[Production_Analysis]]
-Gamma peak is revealed by comparing target in and target out runs.
-[[File:Gammas(2).jpg | 950 px]]
-==ToF==
-<math>Neutron TOF=\frac{PMT_{top}+PMT_{bottom}}{2}-t_{\gamma peak}+\gamma_{TOF}</math>
-[[Target_in_vs_target_out_ToF]]
-[[File:ToF.png| 1000 px]]
-==Energy==
-Neutron Energy:
-<math>\frac{1}{2}m_{n}\left(\frac{in}{ns}\right)^2=3.372\left(\frac{42}{t}\right)^2 MeV</math>
-Watt distribution:
-<math>Ce^{-aE^'}\sinh\left(\sqrt{bE^'}\right)=0.708 e^{-0.884 E^'}\sinh \left(\sqrt{E^'}\right)</math>
-[[File:Watt.jpg|1000 px]]
-==Second Hit==
-Odd TDC spectrum in the second hit:
-[[File:Snip20150815 28.png | 1110 px]]
-Applying cuts based on TDC difference could help:
-[[File:SecondHit.png|1000 px]]
-==Opening angles==
-Uncorrelated distribution from detectors 1-4:
-[[File:Snip20150729 3.png|750 px]]
-Analyzing 5653446 pulses from DU runs, I was able to find 349 two-neutron events in detectors 1-4.
-[[File:CorrOverUncorR.png| 750 px]]
-As a test I did the same for gamma events:
-[[File:Snip20150815 29.png| 500 px]]
+[[Past_work]]
 Go back [[2nCor_44]]