Difference between revisions of "DU data"

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(Created page with "==Beam DOWN configuration== Cumulative raw ToF spectra obteined for the case of D2O target and beam DOWN position are presented below: 800 px …")
 
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==Beam DOWN configuration==
 
==Beam DOWN configuration==
  
Cumulative raw ToF spectra obteined for the case of D2O target and beam DOWN position are presented below:
+
Cumulative raw ToF spectra obteined for the case of DU target and beam DOWN position are presented below:
  
 
[[File:DU_raw_cumul_DOWN.png | 800 px]]
 
[[File:DU_raw_cumul_DOWN.png | 800 px]]
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The width of the photon peak (sigma) shows the IAC linac pulse width at it was mentioned above it was around 2 ns.
 
The width of the photon peak (sigma) shows the IAC linac pulse width at it was mentioned above it was around 2 ns.
  
Neutron energy spectra reonstructed from the ToF spectra for the beam DOWN and D2O are shown below:
+
Neutron energy spectra reonstructed from the ToF spectra for the beam DOWN and DU are shown below:
  
 
[[File:DU_nene_cumul_DOWN.png | 800 px]]
 
[[File:DU_nene_cumul_DOWN.png | 800 px]]
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The uncertainty on the neutron energy depends mostly on the knowledge of the photon peak center position. The width of the photon peak gives an uncertainty in the neutron energy.
 
The uncertainty on the neutron energy depends mostly on the knowledge of the photon peak center position. The width of the photon peak gives an uncertainty in the neutron energy.
  
The energy uncertainty for the beam DOWN and D2O target are shown below:
+
The energy uncertainty for the beam DOWN and DU target are shown below:
  
 
[[File:DU_de_nene_cumul_DOWN.png | 800 px]]
 
[[File:DU_de_nene_cumul_DOWN.png | 800 px]]

Revision as of 15:29, 6 June 2013

Beam DOWN configuration

Cumulative raw ToF spectra obteined for the case of DU target and beam DOWN position are presented below:

DU raw cumul DOWN.png

The width of the photon peak (sigma) shows the IAC linac pulse width at it was mentioned above it was around 2 ns.

Neutron energy spectra reonstructed from the ToF spectra for the beam DOWN and DU are shown below:

DU nene cumul DOWN.png

The neutron detectors was placed azimuthally symmetric around the target so the distance was 135.5 cm from the center of the target to the face of each of the detector.

The uncertainty on the neutron energy depends mostly on the knowledge of the photon peak center position. The width of the photon peak gives an uncertainty in the neutron energy.

The energy uncertainty for the beam DOWN and DU target are shown below:

DU de nene cumul DOWN.png