JAEA-Conf 2011-002 - 日本原子力研究開発機構
JAEA-Conf 2011-002 - 日本原子力研究開発機構
JAEA-Conf 2011-002 - 日本原子力研究開発機構
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<strong>JAEA</strong>-<strong>Conf</strong> <strong>2011</strong>-<strong>002</strong><br />
3. Results and discussion<br />
3.1 Multi parameter MCA measurement<br />
A two dimensional spectrum of signals measured by the 3 He position sensitive proportional counter is shown in<br />
Fig.5. In the figure, the horizontal axis shows the sum of the two signals and the vertical axis shows one of the<br />
two signals. It was confirmed that the detection position information could successfully be extracted. The<br />
vertical axis value means the detection depth position from the detector edge. There are no cadmium collimators<br />
in the measurement, meaning that neutrons are entering the detector from the side surface uniformly. Full energy<br />
peaks marked with a red circle show the detection position distribution, y(r), in the detector by projecting on the<br />
y-axis. But, y(r) is not a clear detection position distribution as shown in the figure. In Fig.5, there is a zigzag<br />
curve formed with the full energy peaks and thus y(r) seems to be not a uniform distribution. One of the reasons<br />
is existence of the copper pipe of the detector. So we must make the identification system connecting between<br />
the two-dimensional figure and the detection depth spectrum. It means that it is necessary to make one-to-one<br />
correspondence between the position of the full energy peak in the figure and the real detection position in the<br />
detector. And it is quite important to fix the detectable reaction depth to define the measurable neutron energy<br />
range. For these requirements, in the next step, we carried out measurements with a cadmium collimator put<br />
around the detector.<br />
Fig.5 Two dimensional MCA result.<br />
3.2 Detection position identification<br />
For the collimator we used a cadmium cover, which has a large (n,γ) reaction cross section for thermal<br />
neutrons. Incident thermal neutrons are mostly blocked by the collimator and detected only from an open<br />
window of 1cm width. The schematic view for the test measurement is shown in the left figure in Fig.6. To<br />
establish the one-to-one correspondence, we have measured several tens times by moving the open window from<br />
one edge to another at every 1cm. Incident neutrons are perpendicular to the detector axis as shown in the figure.<br />
In the right figure, several cadmium collimators were rolled around the detector to demonstrate the position<br />
sensitive detector performance. The center positions of 7 open windows were 4cm, 9cm, 16cm, 25cm, 32cm,