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Anomalous bunching of nearly indistinguishable bosons
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Anomalous bunching of nearly indistinguishable bosons
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The commonly assumed straight link between boson bunching and particle indistinguishability in quantum interferometry has recently been challenged [Nat. Photon. 17, 702 (2023)]. Exploiting the connection between quantum optical interferences and matrix permanents, it appeared that bunching effects may arise that exceed the expected limit of fully indistinguishable particles by injecting peculiar polarization states of partially distinguishable photons in some interferometers. Surprisingly, all states giving rise to such an anomalous bunching were found to be far from the state of fully indistinguishable particles, raising the question of whether this intriguing phenomenon might even possibly exist with nearly indistinguishable particles. Here, we answer this question positively by relating it to a mathematical conjecture on matrix permanents dating from 1986, whose physical interpretation had not yet been unveiled. Using a recently found counterexample to this conjecture, we demonstrate that there is an optical interferometer involving 8 photons in 10 modes such that the probability that all photons bunch into two output modes can be enhanced by suitably perturbing the state of all photons having the same polarization. Such a finding reflects still another -- even less expected -- facet of anomalous boson bunching.
Forward citations
Cited by 3 Pith papers
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Loss-induced anomalous generalized bunching in multiphoton interference
Survival-conditioned loss makes three-photon generalized bunching anomalously maximized at partial distinguishability, a phenomenon forbidden for unconditioned bunching at N=3.
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A unified framework for anomalous boson bunching
Anomalous boson bunching is unified by defining total indistinguishability of postselected output states; the same permanent inequality yields new cases where added distinguishability enhances single-mode, multimode, ...
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Statistical-noise-enhanced multi-photon interference
In a symmetric three-photon Fourier interferometer, engineered super-Poissonian light with g(2)≈1.9 and g(3)≈3.6 maximizes visibility at ≈0.61, surpassing the magnitude of the single-photon value.
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