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Let us focus our attention on a detector located at some position . We close one of the slits and determine the probability of an electron arriving at . This is done by simply finding out the fraction of the total number of electrons that are emitted by the source are detected by the detector at . When is open, let this fraction be . Similarly, with closed but with open, we determine the corresponding fraction at the same position. If we open both the slits, we would expect the fraction to be , as every electron must pass either through or through . However, what one finds experimentally is that . |