The Quantum Handshake by John G. Cramer

The Quantum Handshake by John G. Cramer

Author:John G. Cramer
Language: eng
Format: epub
Publisher: Springer International Publishing, Cham


Now suppose that we arrange for the light source L to emit only one photon within a given time period. Then, if we do the measurement with no opaque object on path A, we should detect the photon at 100 % of the time. If we perform the same measurement with the opaque object Obj blocking path A, we should detect a photon at 25 % of the time, a photon at 25 % of the time, and should detect no photon at all 50 % of the time (because it was removed by Obj in path A). In other words, the detection of a photon at guarantees that an opaque object is blocking path A, although no photon had actually interacted with object Obj. This is the essence of the Elitzur and Vaidmann interaction-free measurement.

Note that if a photon is detected at detector , the issue of whether an object blocks path A is unresolved. However, in that case another photon can be sent into the system, and this can be repeated until either a photon is detected at or absorbed by Obj. The net result of such a recursive procedure is that 66 % of the time a photon will strike the object, resulting in no detection signal, while 33 % of the time a photon will be detected at , indicating without interaction that an object blocks the A path. Thus, the EV procedure has an efficiency for non-interactive detection of 33 %.

As before, in analyzing interaction-free measurements with the Transactional Interpretation, we will explicitly indicate offer waves by a specification of the path in a Dirac ket state vector , and we will underline the symbols for optical elements at which a reflection has occurred. Confirmation waves will similarly be indicated by a Dirac bra state vector , and will indicate the path considered by listing the elements in the time-reversed path with reflections underlined.

Fig. 6.16Offer waves a ---- and b ----



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