1993
DOI: 10.1016/0030-4018(93)90591-r
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Spectral filtering within the Schawlow-Townes linewidth as a diagnostic tool for studying laser phase noise

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Cited by 14 publications
(12 citation statements)
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“…We shall refer to this correlation tendency to bunch when ω 1 ≈ ω 2 and is small (as compared to the relevant linewidths in the system) as indistinguishability bunching. This effect has been observed experimentally in the filtering of a single-mode laser [22].…”
Section: Theory Of One-and Two-photon Spectramentioning
confidence: 52%
See 1 more Smart Citation
“…We shall refer to this correlation tendency to bunch when ω 1 ≈ ω 2 and is small (as compared to the relevant linewidths in the system) as indistinguishability bunching. This effect has been observed experimentally in the filtering of a single-mode laser [22].…”
Section: Theory Of One-and Two-photon Spectramentioning
confidence: 52%
“…Their origin, as for the leapfrogs, stems from the uncertainty introduced by including the detector physics, which extends the interference appearing at the points ( ± , 0) and ( ± , ± ) to two circles. At the centre of these interference rings, ( ± /2, ± /2), two red spots of enhanced emission appear from the concentration of leapfrog outer lines in the Jaynes-Cummings model, equations (22). With a narrower detector, leapfrogs are enhanced due to the longer uncertainty in the time of two-photon emission, as shown in figures 6(g) and (h).…”
Section: Lasing and The Mollow Tripletmentioning
confidence: 90%
“…Experimentally, the two-photon spectrum corresponds to the usual Hanbury Brown-Twiss setup to measure second-order correlations through photon counting, with filters or monochromators being placed in front of the detectors to select two, in general different, frequency windows. The technique has been amply used in the laboratory [15,16,22,[42][43][44][45][46][47][48][49], but lacking hitherto a general theoretical description, the global picture provided here has not yet been achieved experimentally. Note finally that when considering correlations between equal frequencies, ω = ω 1 = ω 2 , the result is equivalent to placing a single filter before measuring the correlations of the outcoming photon stream [36] or embedding the quantum dot in a cavity and measuring the correlations from the emission of a weakly coupled cavity mode with frequency ω.…”
Section: Two-photon Spectrummentioning
confidence: 99%
“…However, in the limit Γ < γ, the additional effect of "indistinguishability bunching" [18] also becomes relevant. This phenomena originates in the quantum fluctuations of the light field [43,44] and has been observed to lead to photon bunching when filtering at less than the natural linewidth of a light source, even for a classical input state such as a laser [45]. In the case of the RF spectrum considered here, the filtering is narrow compared to the incoherent Rayleigh peak but still broad compared to the coherent component.…”
Section: Takedownmentioning
confidence: 94%