Light That Bunches Up in Packs ✎ express

Original: "Superbunched random fiber laser"
arXiv:2603.22025 · 2026-03-23 · arXiv non-exclusive · independent analysis · 1 min
Scientists have learned how to make photons in an optical fiber bunch together more strongly than in ordinary light.

Ordinary light is like a crowd in a square: each photon moves on its own, bumping into others and scattering. But in some media, photons start running together like a pack of dogs: they bunch up. Scientists have built a random fiber laser where light particles gather into especially dense clusters. This effect is called superbunching of photons.

Inside the fiber, light scatters off imperfections, and under certain conditions photons stop being independent. By varying the pump power, the researchers controlled the degree of bunching — from nearly solitary photons to tight groups where a single pulse contained tens of times more photons than usual. This behavior is linked to phase transitions in the light field, just as water turns into ice, light shifts into a new state with different statistics.

Superbunching of photons resembles rush-hour crowds: instead of a steady flow, you get dense clumps that form and dissolve.

The practical payoff is in imaging. The scientists used superbunched light for 'ghost' imaging in time: instead of a regular picture, they reconstructed the shape of a light pulse by sending only a small fraction of photons to the detector. The stronger the bunching, the fewer measurements are needed for a clear result. This promises faster and more sensitive methods in optical sensing and quantum optics.

The degree of photon bunching in this laser reached 26—that's like having, on average, 26 people standing in a queue instead of one.

In M. John Harrison's novel 'Light', quantum effects warp reality — here, superbunching of light helps us see the invisible.

g^{(2)}(0) = \frac{\langle I^2 \rangle}{\langle I \rangle^2}
The parameter g(2)(0) indicates how likely photons are to arrive in pairs: g(2)(0)=1 for ordinary light, g(2)(0)>1 for bunched light (superbunching), and g(2)(0)<1 for antibunched light.
Scientists
Fritz ZwickyJeff KimbleLeonard MandelRoy GlauberAlbert EinsteinCharles Townes
Concepts
random laser second harmonic generation frequency doubling heralded single photon generation three photon entanglement raman scattering quantum photonics integration superradiant phase transition quantum light random number generator fiber optics superradiance free electron laser coherent light single photon detection quantum light networks photon pair generation greenberger horne zeilinger state strong lensing hard x ray