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International Reactor Dosimetry File 2002 - IAEA Publications

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more sensitive than volume effect devices to ionization radiation effects<br />

produced by either a neutron field or a mixed neutron–gamma field.<br />

The accepted methodology is to relate the damage caused by a specific<br />

fluence of a given neutron spectrum to an equivalent fluence from a monoenergetic<br />

spectrum at a reference energy that would produce the same level of<br />

damage. 1 MeV is the reference energy used by the semiconductor radiation<br />

effects community, and the ratio of the fluence from a specific neutron with<br />

energy E to the fluence of a reference 1 MeV neutron required to cause the<br />

same level of damage is referred to as the 1 MeV(Si) damage response<br />

function. IRDF-<strong>2002</strong> response functions include the results of the calculation<br />

of silicon displacement kerma factors (displacement kerma per unit neutron<br />

fluence) as a function of neutron energy over the range 10 –10 –20 MeV. The unit<br />

of the displacement kerma factor is megaelectronvolts times millibarns<br />

(MeV·mb). Each factor can be multiplied by 3.435 × 10 –13 to convert to<br />

rad(Si)·cm 2 , or by 3.435 × 10 –19 to convert to J·m 2 /kg or Gy(Si)·m 2 .<br />

An average value of the neutron displacement kerma factor near 1 MeV<br />

is difficult to determine because of sharp neutron cross-section resonances in<br />

that energy region. To avoid these difficulties, the semiconductor radiation<br />

effects community has defined the displacement kerma of a reference 1 MeV<br />

neutron to be exactly a reference displacement kerma level of 95 MeV·mb.<br />

Values for the silicon displacement kerma are determined by calculating the<br />

total kerma and then partitioning the data into ionization and displacement<br />

fractions [8.7]. The correlation of the displacement kerma with the measured<br />

damage in many neutron fields has been confirmed with integral uncertainties<br />

no larger than 10% [8.8]. Figure 8.2 shows the neutron energy dependent<br />

silicon displacement kerma.<br />

For any given neutron spectrum, a 1 MeV(Si) equivalent fluence is<br />

derived by convoluting the displacement kerma with the neutron spectrum and<br />

dividing by 95 MeV·mb. The uncertainty in the specification of the neutron<br />

spectrum should be propagated through this convolution and used to<br />

determine the uncertainty in the resulting 1 MeV(Si) equivalent fluence. Note<br />

that the displacement kerma is considered to be a radiation effects community<br />

specified exposure metric and has no uncertainty (i.e. it represents a specified<br />

response).<br />

8.3. GALLIUM ARSENIDE dpa (ELECTRONICS DAMAGE)<br />

The basis of the currently accepted protocol for the correlation of<br />

neutron damage effects to a neutron fluence in a GaAs semiconductor device is<br />

through the displacement kerma produced in bulk GaAs. However, this<br />

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