In unreflected reactors, the probability of detecting chain-related counts is given by the well known Rossi-a expression as originally derived by Feynman [1-2] D k2C ..where C is the detector count rate, D is the adjoint-weighted neutron dispersion factor (i.e., D = gI'), F is the total fission reaction rate, k is the effective multiplication factor, r is the adjoint-weighted neutron removal lifetime, and [~x[ is the magnitude of the alpha-eigenvalue, defined by I a =-It -k0 -~)1 (2) T where B is the effective delayed neutron fraction. The integral of the correlated part of Eq. (1) is given by s -.rico -a) 2 ~._~... (3) zr 721o, i = Using the definition of alpha from Eq. (2) and using the &fruition of the magnitude of the reactivity of the system (in units of dollars), IOsl ffi ~. (4) Eq. (3) can also be written as ZF 02(1 + IosL) 2 (5) Solving for/3 in Eq. (5) yields the following expression [3]:We shall now demonstrate that this expression for/3 is equally applicable for a reflected system in which two alphas are experimentally observed. We begin by assuming the Rossi-ot solution for a simple reflected system as derived by Kistner [4]. That is, R(t)dt = Cdt + Ale-lC*,ltdt + A2e-I~'-Itdt (7) Institute of Physics and Power Engineering, Bondarenko sq., Obninsk, Kaluga Region, Russia. Los