Difference between revisions of "Neutron Corr"

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[https://wiki.iac.isu.edu/index.php/HRRL Go Back]
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=Using the 44 MeV machine=
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=8/13/2012=
 
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http://www.hamamatsu.com/resources/pdf/etd/R580_TPMH1100E.pdf
 
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==First Results==
 
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[[File:G1L3966.png | 600 px]]
 
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[[File:G1L3967.png | 600 px]]
 
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=8/14/2012=
 
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==Gun/RF Tests==
 
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[[File:betterbeamtest.jpg | 600 px]]
 
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=8/15/2012=
 
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==Neutron Detector Layout==
 
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[[File:HRRL_LANDLO_8_15.jpg | 800px]]
 
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=8/16/2012=
 
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==Neutron Detector Layout(morning)==
 
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[[File:HRRL_LANDLO_8_16_am.jpg | 800px]]
 
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==Neutron Detector Layout(afternoon)==
 
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[[File:HRRL_LANDLO_8_16_pm.jpg | 800px]]
 
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=8/17/2012 - 8/24/2012=
 
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==Neutron Detector Layout==
 
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[[File:HRRL_LANDLO_8_20.jpg | 800px]]
 
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=August 2012 HRRL Data Analysis=
 
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The detector measurements used for this data analysis are illustrated in the schematic below:
 
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[[File:2ndetectormeas.jpeg | 800 px]]
 
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Using the index of refraction Oleksiy found:
 
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[[File:Slope_data.png]]
 
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When analyzing the data, all the runs in a particular day were added together for better statistics.  First, the raw data was used to determine where the neutrons cut would need to be placed for each run (or each day of runs if they were able to be combined).  Applying those neutron cuts to each TDC, coincidences were found.  The TDC spectra of the detectors that detected these coincidences were then analyzed to determine the spot on the detectors where each neutron hit.  Knowing the location of detection, the theta and phi angles between coincident neutrons were found.
 
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==8/17==
 
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Raw Data:
 
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[[File:TDC8_17.png | 800 px]]
 
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Coincidence Data:
 
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[[File:phi 8_17.png | 800 px]]
 
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[[File:theta 8_17.png | 800 px]]
 
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==8/20==
 
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Raw Data:
 
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[[File:TDC8_20.png | 800 px]]
 
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Coincidence Data:
 
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[[File:phi8_20.png | 800 px]]
 
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[[File:theta8_20.png | 800 px]]
 
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==8/21==
 
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Raw Data:
 
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[[File:TDC8_21.png | 800 px]]
 
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Here the multiple peak indicate that the timing in the beam was shifting, thus not allowing to combine.  Each run of this day is plotted below.
 
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===4143===
 
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[[File:TDC8_21_4143.png | 800 px]]
 
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===4144===
 
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[[File:TDC8_21_4144.png | 800 px]]
 
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===4145===
 
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[[File:TDC8_21_4145.png | 800 px]]
 
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===4146===
 
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[[File:TDC8_21_4146.png | 800 px]]
 
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==8/22==
 
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Raw Data:
 
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[[File:TDC8_22.png | 800 px]]
 
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Coincidence Data:
 
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[[File:phi8_22.png | 800 px]]
 
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[[File:theta8_22.png | 800 px]]
 
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==8/23==
 
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Raw Data:
 
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[[File:TDC_8_23.png | 800 px]]
 
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Coincidence Data:
 
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[[File:phi8_23.png | 800 px]]
 
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[[File:theta8_23.png | 800 px]]
 
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==8/24==
 
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Raw Data:
 
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[[File:TDC8_24.png | 800 px]]
 
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Coincidence Data:
 
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[[File:phi8_24.png | 800 px]]
 
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[[File:theta8_24.png | 800 px]]
 
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==8/17 - 8/20==
 
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[[File:TDC8_17_20.png | 800 px]]
 
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==8/17 - 8/21==
 
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[[File:TDC8_17_21.png | 800 px]]
 
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==8/17 - 8/22==
 
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[[File:TDC8_17_22.png | 800 px]]
 
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[[2nCor_44]]
  
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=Using the HRRL=
  
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[[nCorr_HRRL]]
  
 
[https://wiki.iac.isu.edu/index.php/HRRL Go Back]
 
[https://wiki.iac.isu.edu/index.php/HRRL Go Back]

Latest revision as of 17:12, 12 March 2015

Using the 44 MeV machine

2nCor_44

Using the HRRL

nCorr_HRRL

Go Back

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