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Neutron emission in proton induced reactions

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Proton induced spallation reactions are proposed in current accelerator driven transmutation designs. Hence, new accurate measurements of neutron production using a proton beam are needed.

Barium fluoride is an efficient detector material for neutrons in a wide energy range [1,2]. The high acceptance BaFtex2html_wrap_inline5457 detector system TAPS is an effective tool for exclusive neutron measurements.

The beam of 190 MeV protons from AGOR was incident on thin W and Ni targets. Neutrons were detected by TAPS which was configured in 6 blocks of 64 BaFtex2html_wrap_inline5457 modules and positioned around the target to cover the polar angles tex2html_wrap_inline4837 from 60tex2html_wrap_inline6073 up to 170tex2html_wrap_inline6073.

 figure1043
Figure: The neutron efficiencies of the TAPS detectors for electron-equivalent amplitude threshold Ltex2html_wrap_inline6077 = 4 MeVtex2html_wrap_inline6079 (full line) and 10 MeVtex2html_wrap_inline6079 (dashed line).

The neutron detection efficiencies follow a simple exponential dependence on amplitude threshold tex2html_wrap_inline6083 for neutron energy tex2html_wrap_inline6085 lower than 20 MeV [1] and higher than 100 MeV up to 1.3 GeV [2]
equation1018
where tex2html_wrap_inline6087 is the efficiency in the limit of zero threshold and tex2html_wrap_inline6089 is the slope parameter.

Our new measurements show that this relation is valid also for the intermediate energy range from 20 to 100 MeV. Based on the available data it is possible to calculate the neutron detection efficiency for a given amplitude threshold, see figure 1.

 figure1050
Figure: The neutron production on the W target. The energy spectra for different angles (left side) and angular distributions for the low and high energy component (right side).

Preliminary results of the neutron production experiment with the tungsten target are shown in figure 2. The LAHET code was used to calculate the inclusive angular distribution of neutron production. The result of these calculations is in good agreement with the experiment.

a) NPI of ASCR Řež u Prahy, Czech Republic.
[1] T. Matulewitz et al., Nucl. Instr. and Meth. A274, 501 (1989).
[2] V. Wagner et al., Nucl. Instr. and Meth. A394, 332 (1997).


next up previous contents
Next: Mass dependence of neutral Up: Experimental Nuclear Physics: Reaction Previous: and subthreshold production

Johan Messchendorp
Sun Mar 29 20:24:28 GMT 1998