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Expand file tree Collapse file tree Original file line number Diff line number Diff line change 4040* <b>Model description:</b>
4141*
4242* The normalised Maxwellian distribution for moderated neutrons is defined by [1]
43+ * <div class="latex">
4344* $M(\lambda)=\frac{2a^2}{T^2\lambda^5}\exp\left(-\frac{a}{T\lambda^{2}}\right)$
45+ * </div>
4446* where
47+ * <div class="latex">
4548* $a=\left(\frac{h^2}{2m_{N}k_{B}}\right)$
49+ * </div>
4650* and the joining function for the under-moderated neutrons is given by [1]
51+ * <div class="latex">
4752* $M(\lambda)_{um}=\frac{1}{\lambda(1+\exp(\lambda\chi-\kappa))}$
53+ * </div>
4854*
4955* The normalised time structure of the long pulse is defined by [2]
56+ * <div class="latex">
5057* $N_{t<=t_p}=1-\exp\left(-\frac{t}{\tau/n}\right)$
58+ * </div>
59+ * <div class="latex">
5160* $N_{t>t_p}=\exp\left(-\frac{t-t_p}{\tau}\right)-\exp\left(-\frac{t}{\tau/n}\right)$
61+ * </div>
5262* where tp is the pulse period, tau is the pulse decay time constant, and n is the ratio of decay to ascend time constants.
5363*
5464* <b>Parameters for some sources:</b>
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