^ 1.01.11.21.31.41.5Dewan, Edmond M.; Beran, Michael J. Note on stress effects due to relativistic contraction. American Journal of Physics (American Association of Physics Teachers). March 20, 1959, 27 (7): 517–518. Bibcode:1959AmJPh..27..517D. doi:10.1119/1.1996214.
^ 4.04.1Moses Fayngold. Special Relativity and How it Works. John Wiley & Sons. 2009. ISBN 3527406077.: p. 407: "Note that the proper distance between two events is generally not the same as the proper length of an object whose end points happen to be respectively coincident with these events. Consider a solid rod of constant proper length l(0). If you are in the rest frame K0 of the rod, and you want to measure its length, you can do it by first marking its end-points. And it is not necessary that you mark them simultaneously in K0. You can mark one end now (at a moment t1) and the other end later (at a moment t2) in K0, and then quietly measure the distance between the marks. We can even consider such measurement as a possible operational definition of proper length. From the viewpoint of the experimental physics, the requirement that the marks be made simultaneously is redundant for a stationary object with constant shape and size, and can in this case be dropped from such definition. Since the rod is stationary in K0, the distance between the marks is the proper length of the rod regardless of the time lapse between the two markings. On the other hand, it is not the proper distance between the marking events if the marks are not made simultaneously in K0."