Abstract. Various theories predict the possible existence of T-odd and P-odd shortrange forces between spin 1 2 fermions, proportional to S · r where S is the fermion spin and r is the separation between particles. We use ensembles of polarized nuclei and an un-polarized mass to search for such a force over sub-mm ranges. We established an improved upper bound on the product g s g n p of the scalar coupling to particles in the un-polarized mass and the pseudo-scalar coupling of polarized neutrons for force ranges from 10 −4 to 10 −2 m, corresponding to a mass range of 2 · 10 −3 to 2 · 10 −5 eV for the exchange boson [1].Possible short-range (mm-µm) forces between polarized spin 1 2 particles and un-polarized masses may exist beyond the Standard Model [2]. In particular a so-called monopole-dipole interaction would couple to fermions through scalar and pseudoscalar vertices by the exchange of spin-0 bosons [3]. This force has a Yukawa-type of interaction potential from one boson exchangewherer is the unit vector from the polarized particle to the unpolarized particle,σ is the spin of the polarized particle, m p is the mass of the polarized particle, g s g n p denotes the product of the couplings of the scalar vertex in the unpolarized mass and pseudoscalar vertex in the polarized mass and λ is the force range. Such a P-odd and T-odd interaction proportional to σ· r can cause a shift in the precession frequency of the polarized particle in the presence of an unpolarized mass [4,5]. This experiment presents improved laboratory limits on g s g n p in comparison to a previous work [6] for force ranges from 10 −4 to 10 −2 m. These results can be interpreted in terms of the pseudoscalar coupling g n p , since the spin of the polarized 3 He used in this work is dominated by the spin of its constituent neutron [7]. The pseudoscalar coupling constant from the polarized mass is spin dependent whereas the scalar coupling constant from the unpolarized mass is spin independent but fermion density dependent. This work also represents to our knowledge the most sensitive measurement done with 3 He at low energies for T and P odd interactions. a