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arXiv:2610.08269

Boosting the photon bunching of classical light via a modified Fabry-Pérot cavity

Lu Zhang, Dongxu Zhou, Hongzhi Zhang, Guoquan Zhang

physics.opticsquant-phSubmitted Oct 6, 2026• Announced Oct 7, 2026• 0 citations
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Abstract

We proposed to boost the photon bunching effect of classical light via a modified Fabry-Pérot cavity with one of the cavity mirrors being replaced by a spatial light modulator, through which multiple independent transverse modulations, each was to encode independently spatially correlated phase on the wave front of the light field, was cascaded in sequence in the longitudinal propagation direction in the cavity. The two-photon bunching peak and the three-photon bunching peak of the generated superbunching light field were measured to be $36.9\pm2.0$ and $\rm (2.46\pm0.12)\times10^{3}$, respectively, which, as compared to those of thermal light, were improved by one-order and three-order of magnitude, respectively. Correspondingly, the ghost image visibility reconstructed with the superbunching light was demonstrated experimentally to be improved by $\sim 40$ times as compared to that with the pseudo-thermal light. Such classical superbunching light field is of essential importance not only for fundamental physics but also for potential applications such as correlated imaging, ghost interference and nonlinear optics.

Comments
12 pages, 8 figures

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We proposed to boost the photon bunching effect of classical light via a modified Fabry-Pérot cavity with one of the cavity mirrors being replaced by a spatial light modulator, through which multiple independent transverse modulations, each was to encode independently spatially correlated phase on the wave front of the light field, was cascaded in sequence in the longitudinal propagation direction in the cavity. The two-photon bunching peak and the three-photon bunching peak of the generated superbunching light field were measured to be 36.9±2.036.9\pm2.036.9±2.0 and (2.46±0.12)×103\rm (2.46\pm0.12)\times10^{3}(2.46±0.12)×103, respectively, which, as compared to those of thermal light, were improved by one-order and three-order of magnitude, respectively. Correspondingly, the ghost image visibility reconstructed with the superbunching light was demonstrated experimentally to be improved by ∼40\sim 40∼40 times as compared to that with the pseudo-thermal light. Such classical superbunching light field is of essential importance not only for fundamental physics but also for potential applications such as correlated imaging, ghost interference and nonlinear optics.
Superposition of multiple indistinguishable two-photon paths is introduced by means of a digital wave front encoding technique to design a spatially phase-correlated wave front of a light field, which could result in a superbunching effect with a bunching peak much larger than 2, the theoretical bunching peak of thermal light. Experimentally, we demonstrated a bunching peak of $11.72\ifmmode\pm\else\textpm\fi{}0.05$ with the digitally designed phase-correlated wave front of classical light, which can be improved further on. A significant improvement of the visibility of the second-order interference fringes and ghost imaging was also experimentally demonstrated. Our method provides a convenient digitally controllable way to implement superposition of multiple different but indistinguishable two-photon paths, and therefore to modify the optical coherence properties of photons. Such a superbunching effect may have potential applications in improving the visibility of correlation interference and imaging, and enhancing the efficiency of two-photon nonlinear effects such as two-photon absorption effect.
Thermal light by nature exhibits the well-known photon bunching effect with the zero-delay second-order correlation coefficient g(2){g}^{(2)}g(2) ideally equal to 2. The Photon extra-bunching effect, as a special class of the superbunching effect (g(2)>2{g}^{(2)}>2g(2)>2), describes the enhanced photon correlation (g(2)=3{g}^{(2)}=3g(2)=3) through the interference of bright twin beams produced in the spontaneous parametric down-conversion. In this work, we report that this effect can exist in classical beams and that g(2){g}^{(2)}g(2) can approach 4 in some extended extreme models. We experimentally demonstrate the nontrivial extra-bunching correlation ($\ensuremath{\sim}1.4\ifmmode\times\else\texttimes\fi{}$ gain) in pairwise-generated holographic thermal light beams with a Dove prism-embedded balanced Mach-Zehnder interferometer. The interaction of such a pair of conjugated thermal light beams can generate a pair of uncorrelated superthermal light beams, enabling ghost imaging and Young's intensity interference with enhanced visibility. The quantum-inspired interference-induced spatial extra-bunching effect provides novel insights into inducing superbunching correlation in classical light and holds the potential for application in the coherent two-photon Lidar system to enhance sensitivity.
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Two-photon bunching and superbunching are important to understanding the physics of ghost imaging and second-order interference of light. With the help of the recently proposed superbunching pseudothermal light, the physics of bunching and superbunching in superbunching pseudothermal light is studied in detail. A special two-photon coincidence count detection system is designed to measure the required two-photon coincidence counts. It is concluded that the two-photon superbunching effect cannot be observed without taking the intensity changing process into account. A similar conclusion holds for two-photon bunching of thermal light. The conclusions are helpful for understanding of the physics of two-photon bunching and superbunching in intensity or photon number fluctuation correlation theory.
We report on the two-photon superbunching effect of thermal light via constructive multiple two-photon path interference, showing the possibility of controlling the bunching property of thermal light in a linear optical system. By inserting nnn pairs of mutually first-order incoherent optical channels as a cascade into the traditional Hanbury Brown and Twiss (HBT) interferometer, the two-photon bunching peak-to-background ratio of thermal light can be increased by up to $2\ifmmode\times\else\texttimes\fi{}1.{5}^{n}$, surpassing the theoretical upper limit of 2 for a traditional HBT interferometer. Experimentally, the ratio was measured to be $2.4\ifmmode\pm\else\textpm\fi{}0.1$ when one pair of optical channels was inserted. Such a scheme can be viewed as a prototype of a two-photon grating.
Abstract Photon superbunching, with second-order coherence far beyond the Gaussian thermal limit, is a valuable resource for quantum optics and correlation-based imaging. However, existing sources often rely on fragile platforms, inefficient nonlinear conversion, or mechanically complex architectures. Here, we demonstrate the first highly stable, fully fiber-integrated superbunched random fiber laser that provides a broadly tunable source of giant photon bunching. We establish a cooperative linear–nonlinear mechanism in which Rayleigh-scattering-mediated diffusion provides distributed random feedback, while cascaded stimulated Brillouin scattering and quasi-phase-matched four-wave mixing amplify and redistribute stochastic intensity fluctuations across a spectral comb. This enables continuous tuning of g (2) (0) from approximately 1 to 28 via tailored modulation of linear diffusion strength and nonlinear coupling magnitude. Moreover, by combining photon-correlation measurements with Parisi-overlap analysis, we reveal an inverse correlation between disorder-induced photonic phase evolution and microscopic photon bunching, bridging macroscopic disordered-cavity dynamics and high-order photon statistics. Furthermore, we demonstrate that strongly superbunched light enables temporal ghost imaging with comparable reconstruction fidelity while requiring more than an order-of-magnitude fewer realizations than weakly bunched light. Together, these results establish a fiber-integrated route to engineering giant photon superbunching and high-order light statistics for correlation-based photonic technologies.