Luis Aina, AlfredoSánchez Soto, Luis Lorenzo2023-06-202023-06-201998-11-09[1] S. M. Tan and D. F. Walls, Phys. Rev. A 47, 4663 (1993). [2] H. M. Wiseman, F. E. Harrison, M. J. Collet, S. M. Tan, D. F. Walls, and R. B. Killip, Phys. Rev. A 56, 55 (1997). [3] M. O. Scully, B.-G. Englert, and H. Walther, Nature (London) 351, 111 (1991). [4] P. Storey, S. Tan, M. Collet, and D. Walls, Nature (London) 367, 626 (1994); B.-G. Englert, M. O. Scully, and H. Walther, Nature (London) 375, 367 (1995); E. P. Storey, S. M. Tan, M. J. Collet, and D. F. Walls, Nature (London) 375, 368 (1995). [5] H. Wiseman and F. Harrison, Nature (London) 377, 584 (1995). [6] A. Lukš and V. Peřinová, Quantum Opt. 6, 125 (1994); R. Lynch, Phys. Rep. 256, 367 (1995); R. Tanaś, A. Miranowicz, and T. Gantsog, Prog. Opt. 36, 161 (1996). [7] M. Grabowski, Int. J. Theor. Phys. 28, 1215 (1989); A. Luis and L. L. Sánchez-Soto, Phys. Rev. A 56, 994 (1997). [8] J. M. Lévy-Leblond, Ann. Phys. (N.Y.) 101, 319 (1976); T. Opatrný, J. Phys. A 27, 7201 (1994). [9] A. Stern, Y. Aharonov, and Y. Imry, Phys. Rev. A 41, 3436 (1990).0031-900710.1103/PhysRevLett.81.4031https://hdl.handle.net/20.500.14352/59701© 1998 The American Physical SocietyQuantum phase difference is used to analyze which-path detectors in which the loss of interference predicted by complementarity cannot be attributed to classical momentum transfer between the interfering particle and the measuring apparatus. It is shown that the dynamics of the measurement disturbs the interference via random classical phase shifts.engComplementarity enforced by random classical phase kicksjournal articlehttp://dx.doi.org/10.1103/PhysRevLett.81.4031http://journals.aps.org/open access535UncertaintyÓptica (Física)2209.19 Óptica Física