Why Ultraviolet Light Is Brighter When the Gas Ends Abruptly ✛

Original: "Density-gradient effect in high-harmonic generation in gases"
arXiv:2608.28032v1 · 2026-08-28 · CC BY 4.0 · 1 min
The sharper the density gradient at the edges of a gas target, the brighter the ultraviolet emission.

When a laser beam passes through a gas, it generates ultraviolet light. But this light is very weak: out of a thousand laser photons, only one becomes ultraviolet. Scientists long wondered why so few, until they took a closer look at the edges of the gas cloud. It turned out that at the boundary, where the gas density smoothly changes from zero to maximum, many photons are lost. The smoother this transition, the greater the losses.

In the experiment at the Hungarian laser center ELI ALPS, they built a gas cell where the steepness of the density gradient could be varied. The sharper the gradient, the brighter the ultraviolet. For one of the emission colors, the energy increased from 20 to 150 femtojoules when the steepness was changed by a factor of a hundred.

Now it is clear what to do: make the gas boundary as sharp as possible. To do this, the holes in the cell can be drilled with a laser in a thin foil, so that the transition zone shrinks from 1.5 mm to 0.1 mm, and the efficiency increases almost 10 times. This can already be applied in existing setups to make ultraviolet sources brighter and more useful for microscopy and chip manufacturing.

The transition length of the gradient was determined by analogy with the rise time of a signal in electronics: between the 10% and 90% levels.

Concepts
second harmonic generation ultra high energy gamma ray hydrogen production frequency doubling hydrogen storage hot gas Hong–Ou–Mandel effect x ray imaging optimization gas density quantum light generation afterglow harmonic greenhouse effect particle creation germanium detector ultraviolet laser synchrotron radiation high speed imaging spectroscopy laser plasma acceleration helium burning