In a recent letter, Danan et al. [1] devised an elegant experiment investigating the past of photons inside two Mach-Zehnder interferometers, one inside the other-yet drew the wrong conclusions. Namely, that-based on weak measurements on pre-and post-selected states-some photons have been inside the inner interferometer but they never entered and never left. And, consequently, a "common sense" approach describing the past of a photon in terms of a trajectory, or a set of trajectories, for example [2][3][4], should be abandoned.But if weak measurements are carried out such that zero photons leave the inner interferometer-that is complete destructive interference is not disturbed, as should be the casethese measurements, which we show how to implement, do not find the photons to have been inside. Further, we argue that the story told by the two-state vector formulation (TSVF) that Danan et al. advocate is in fact contradictory.By vibrating the mirrors in their key setup of Figure (|A − i |B + |C ). The presence of detector peaks at the vibrational frequencies of mirrors A and B indicates that some photons have been near these mirrors. Now imagine that both mirrors A and B are made to vibrate at precisely the same frequency, such that whenever A is rotated by a small angle δθ, B is rotated by −δθ, i.e., in the opposite direction. By simple geometry, and provided that the distances from A and B to the beam-splitter on the way to F are equal, it is easy to see that complete destructive interference at F is not disturbed, as shown in our Figure 1.What happens to the detector peaks corresponding to mirrors A and B? The weak values of the projection operators at A and B are +1 and −1 respectively. The minus sign for mirror B corresponds, according to weak measurement theory, to an average vertical shift for the photons arriving at the detector that is in the opposite direction of that due to A-the two thus cancelling each other out. Classically, by electromagnetism, eliminating light leakage from the inner interferometer by restoring complete destructive interference means that the all-important detector peaks at the vibrational frequency of mirrors A and B now disappear!