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Mathinline
body$\sigma =\frac{1}{\sqrt{2\pi \ dens_{ILT}^{active}}}$
            (Eq. 182)

here:

           

Mathinline
body$den{{s}_{ILT}}^{active}=den{{s}_{ILT}}.{{p}_{ILT}}.activit{{y}_{ILT}}(time)$
          (Eq. 183)


For this mode, the path distance factor is fixed to a Rayleigh distribution and is not editable.

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