10.4 Investigation of the Transmission of High Energy Neutrons through Matter

magnified picture
Fig. 10-7 Quasi-monoenergetic, high energy neutron source device at the AVF cyclotron facility
Neutrons are generated by protons bombarding a 7Li-enriched target through the7Li(p,n)8Be reaction. An excellent low background is assured by (1) the separation between the neutron source part and the neutron measuring part, and (2) the bending of the proton beam into the beam dump by a bending magnet in the accelerator room. The use of a thin foil 7Li target serves to maintain a good quality monoenergetic neutron source with low background.

Fig. 10-8 Energy spectra of quasi-monoenergetic neutron source

Fig. 10-9 Comparison between measured and predicted values by calculation for a quasi-monoenergetic neutron source of 68 MeV protons
Good agreement is clearly observed between the experimental data and the improved prediction.


Recent rapid progress in accelerator technology has broadened its applications to varied and familiar areas in industry and medical care. The acceleration energy now extends from several MeV to several hundred MeV. However, increasing the thickness of the bulk shield becomes a major issue for the construction cost of the facility, because penetrable high energy neutrons are inevitably associated with high energy machines. To deal with this problem, JAERI has prepared a unique high energy neutron source device at the AVF cyclotron facility as shown in Fig. 10-7. It can provide quasi-monoenergetic neutrons of excellent quality with low background; that is achieved by separation between the neutron source and the measurement room by a thick shield wall (Fig. 10-8).
The transmission and energy change behavior of neutrons were measured on shielding media as iron and concrete of various thicknesses at this device. Based on the data obtained, examinations were made of the theoretical predictions by calculation. An example is shown in Fig. 10-9. As a result, it turned out that the theoretical predictions so far made gave larger values than the experi-mental ones, namely, they overestimated the transmission. The present experimental data leads to modification of the theoretical prediction resulting in remarkable improve-ment of the accuracy. Hence, it is expected that the optimization of the thickness of shielding reduces the construction cost, while keeping enough safety for the accelerator facility.


Reference
H. Nakamura et al., Transmission through Shields of Quasi-Monoenergetic Neutron Generated by 43- and 68-MeV Protons- I and - II, Nucl. Sci. Eng., 124, 228 (1996).

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