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Atoms in a Row: A New Way to Control Light ⚡ экспресс

Original: "Programmable few-atom Bragg scattering and ground-state cooling in a cavity"
arXiv:2508.10748 · 2025-08-14 · CC BY · ⏱ 1 min · Quantum Physics Atomic Physics
Physicists arranged single atoms into a tidy chain, transforming them into a comb for light waves.
Abstract

By combining atomic traps (optical tweezers) with a ring resonator and chiral coupling, scientists obtained highly directional Bragg reflection from a chain of atoms. With each added atom, the reflected beam became sharper—like increasing the number of lines on a diffraction grating. This was achieved thanks to laser cooling to near the ground state (phonon numbers 0.17 and 3.4). The platform combines controlled atomic arrays with strong light-matter coupling, which is important for quantum computing and metrology.

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Light falling on a crystal reflects not like from a mirror, but in distinct narrow beams. This effect, discovered by William Lawrence Bragg, is called Bragg scattering and typically requires billions of atoms arranged by nature into a regular lattice. But physicists have managed to do the same with just a handful of individual atoms. Using laser tweezers—focused beams that act like invisible hands—they placed several atoms in a perfect line. The spacings were chosen so that the atoms act like the teeth of a comb for light waves: the incoming light gets "combed" and leaves as a single thin beam.

To achieve this, the atoms had to be cooled to near absolute zero—otherwise thermal jitter would blur the lineup. Adding atoms one by one, the scientists watched the reflected peak become sharper and sharper. The most striking thing: the effect appeared with a chain of just a handful of particles, not billions. Previously, such a thing had only been seen in bulky crystals.

Such an atomic "comb" promises optical circuits that can be tuned by changing the number and arrangement of elements. This paves the way for quantum computers, ultrasensitive sensors, and mirrors made of individual atoms.

🎯 Bragg scattering is typically seen in crystals with billions of atoms; here, for the first time, physicists observed it from a chain of just a few atoms, adding them one at a time.

2d \sin\theta = n\lambda
d — distance between atoms, θ — reflection angle, n — integer, λ — wavelength of light
Scientists
Christian DopplerD. B. McLaughlinDidier QuelozMichel MayorR. A. RossiterJames Clerk Maxwell
Tags
spectroscopy photometry
Laws
Doppler effectMaxwell's equationsPlanck's lawPlanck–Einstein relationWien's displacement lawStefan–Boltzmann law
Original: arXiv:2508.10748 · CC BY · bridge42worlds