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Nuclear Spectroscopy

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Figure 5.3. Spectrum for the β − decay of<br />

24 Na. Note the escape peaks from the<br />

2,754 keV gamma and the 511 keV<br />

gammas from the positron creation and<br />

annihilation.<br />

OBJECTIVE<br />

Observe the 511 keV gammas from positron annihilation<br />

and observe the escape peaks after pair production.<br />

SUPPLIES<br />

•NaI(Tl) detector with MCA<br />

•Radioactive sources: 22 Na, 65 Zn, 88 Y/ 88 Zr, 137 Cs,<br />

144<br />

Ce, 228 Th/ 232 Th<br />

SUGGESTED EXPERIMENTAL PROCEDURE<br />

1. Start the MCA and check the calibration using<br />

the 137 Cs source. Your energy scale must extend<br />

at least out to 2,800 keV.<br />

2. Place another source on the fourth shelf under<br />

the detector. Acquire a spectrum for a period<br />

long enough to observe the annihilation gammas<br />

and any escape peaks from the high-energy gammas.<br />

Record the energies of the observed<br />

photopeaks.<br />

DATA ANALYSIS<br />

The 22 Na, 65 Zn sources all have positron decay channels,<br />

while the 88 Y/ 88 Zr, 144 Ce, and Thorium sources<br />

emit high-energy gammas with energies greater then<br />

1,700 keV. What energies do you observe for the<br />

annihilation photons and the escape peaks? Do your<br />

results make good physical sense of the situation?<br />

Why are there no escape peaks visible in the 22 Na,<br />

spectrum? The answer lies in the cross section graph<br />

of Figure 6.2.<br />

18

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