We report variational Monte Carlo calculations which give amplitudes and phases of the reflected and transmitted components of states representing scattering of helium atoms normally incident on a superfluid 4 He slab. The wave function describes a previously postulated condensate mediated process [J. W. Halley et al., Phys. Rev. Lett. 71, 2429(1993] and the results are consistent with uncertainty principle arguments suggesting that the transmission time for thin (but macroscopic) samples will be independent of slab thickness. [S0031-9007 (97)04554-7] PACS numbers: 67.40.DbWhile Bose condensation has been believed to be the fundamental reason for superfluidity in liquid helium four since London proposed it [1], direct experimental information concerning the nature of the condensate has remained sparse. Interpretation of deep inelastic scattering experiments [2,3] requires the impulse approximation, which in turn requires correction to account for final state interactions. Recently we proposed [4] an alternative experimental approach in which pulses of very low energy (ഠ1 K) helium atoms are to be fired at a suspended droplet or slab of superfluid helium. A model calculation suggested that transmission of a component of the incident beam through the slab would occur and that by measuring the dependence of the transmission on the area of the incident beam, one could experimentally confirm the existence of the condensate and extract information about it. The process by which this transmission would occur was envisioned to be the virtual excitation of the entire system into the ground state of the superfluid containing one extra particle, followed by reemission of the incident particle to form the final state. Crude estimates gave large rates for this process. However, a rigorous many-body calculation was required in order to study this possibility more fully. Here we report results of such a study which confirm several aspects of the previous work and provide estimates of transmission times and amplitudes.We consider the problem of transmission and reflection of an atomic beam incident normally on a slab of superfluid helium. Let the number of particles in the slab be N and consider the case of a single incident helium atom propagating along the z axis. We consider only elastic processes, normal incidence, and zero temperature here. Then the scattering states c must satisfy boundary conditions c ! ͑e ikz s 1 R e 2ikz s ͒ 3 c N ͑ r 1 2 r N cm , r 2 2 r N cm , . . . , r N 2 r N cm ͒ (1) as z s ! 2`for any s, and c ! Te ikz s c N ͑ r 1 2 r N cm , r 2 2 r N cm , . . . , r N 2 r N cm ͒ (2) as z s !`for any s. T jT je if and R jRje if 0 are transmission and reflection amplitudes. The condition jT j 2 1 jRj 2 1 is imposed by global current conservation. c N ͑ r 1 , . . . , r s21 , r s11 , . . . , r N11 ͒ is the N particle ground state wave function. We carry out a variational calculation of a steady state scattering wave function satisfying Eqs. (1) and (2) in which the amplitude jTj and phase f of T are obtained as a func...