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Conventional quantum mechanics describes a pre- and post-selected system interms of virtual (Feynman) paths via which the final state can be reached. Inthe absence of probabilities, a weak measurement (WM) determines theprobability amplitudes for the paths involved. The weak values (VW) can beidentified with these amplitudes, or their linear combinations. This allows usto explain the "unusual" properties of the VW, and avoid the "paradoxes" oftenassociated with the WM.

Weak measurements measure probability amplitudes (and very little else)