A lossless beamsplitter has certain (complex-valued) probability amplitudes for sending an incoming photon into one of two possible directions. We use elementary laws of classical and quantum optics to obtain general relations among the magnitudes and phases of these probability amplitudes. Proceeding to examine a pair of (nearly) single-mode wavepackets in the number-states n 1 and n 2 that simultaneously arrive at the splitter's input ports, we find the distribution of photon-number states at the output ports using an argument inspired by Feynman's scattering analysis of indistinguishable Bose particles. The result thus obtained coincides with that of the standard quantum-optical treatment of beamsplitters via annihilation and creation operators a ̂ and a ̂ . A simple application of the Feynman method provides a form of justification for the Bose enhancement implicit in the well-known formulas a ̂ n = n n 1 and a ̂ n = n + 1 n + 1.

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10.
For there to be an arrival time and an exit time, the incoming electromagnetic fields must be in the form of multimode wavepackets with large cross-sectional areas and long durations to properly approximate single-mode photon-number states—hence our use of the qualifier “nearly” when referencing single-mode wavepackets. When discussing two packets that arrive simultaneously at the input ports 1 and 2 of a beamsplitter, we envision identical packets whose leading edges arrive simultaneously at the entrance ports. In a thought experiment, one may imagine packets as large as they need to be for the approximation to reach the desired level of accuracy. In practice, optical wavepackets with cross-sectional areas of about 1 c m 2 and durations of a few nanoseconds will probably suffice.
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The symmetry is not needed for our initial discussion, but will be invoked later, when we extend the argument to the case of incoming wavepackets with n 1 and n 2 photons simultaneously arriving at ports 1 and 2. Strictly speaking, even in the latter case, the symmetry of the splitter is merely convenient but not necessary for the validity of the argument.
14.
While the time interval Δ t in a practical setup might include the measurement time plus a photocell reset time (following each single-photon detection event), for the purposes of our thought experiment, the reset time is taken to be vanishingly small. We are also ignoring the possibility that two or more photons might arrive simultaneously within a single detection cell, since the available cells vastly outnumber the incoming photons. The ultimate justification for such assumptions is that our final results coincide with those obtained by the conventional methods of quantum optics, as demonstrated in Sec. IV.
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17.
Assigning a probability to stimulated emission when none of the incident photons participate in the process might seem questionable. Recall, however, that the quantum rule a ̂ 0 = 1 allows for the stimulation of the excited atom by vacuum fluctuations.
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