How to Catch a Positron? ✛ ✎

Original: "Self-organized positron reorienting and pinching mechanism for the experimental detection of the linear Breit-Wheeler process"
arXiv:2609.07584v1 · 2026-09-07 · arXiv non-exclusive · independent analysis · 1 min
A laser hits foam, the plasma creates a magnetic funnel on its own, and it sends the newborn positrons back to where they are easier to spot.

If you aim a very powerful laser at a piece of foam, the light can give birth to a pair of particles: an electron and a positron. A positron is like an electron, but with a positive charge. Yet capturing that moment had long been elusive: the newborn particles got lost in the noise, like a whisper in a crowd.

It turns out that the plasma created by the laser helps on its own. Inside it, a magnetic field emerges, twisted like a funnel. This funnel catches the positrons and sends them back, toward the beam. Behind it, things are much quieter, making the particles easier to detect. The funnel also squeezes them into a narrow stream, like a hand gathering scattered beads.

Previously, the signal was sought ahead, where everything is flooded with light. Now they look backward, where it is nearly empty, and the positrons stand out clearly.

To produce more positrons, the target is made of two layers: first a low-density foam, then a dense one. In the sparse layer, the laser has time to create the funnel, while in the dense layer many pairs are born. Calculations show that the signal becomes hundreds of times stronger than before. Such an experiment can already be run on large laser facilities. If it works, scientists will for the first time see light directly turning into matter.

Positrons born in the plasma are turned 180 degrees and fly toward the laser beam, like swimmers carried back to shore by a current.

The idea of creating matter from light resembles science fiction plots, for example, in Arthur C. Clarke's novel 'The Light of Other Days', where light is used to create matter. In reality, the Breit-Wheeler process is the literal conversion of photon energy into particle mass.

\frac{d\mathbf{p}}{dt} = e\mathbf{E} + \frac{e}{\gamma mc}\mathbf{p}\times\mathbf{B}
The change in positron momentum is determined by the Lorentz force: the electric field accelerates, the magnetic field curves the trajectory.
\frac{d\theta}{dt} = -\frac{e}{\gamma mc}\frac{1}{|\mathbf{p}_\perp|}\left[p_\phi B_r - p_r B_\phi\right] - \frac{e}{p^2}\left[\frac{p_x}{|\mathbf{p}_\perp|}(p_r E_r + p_\phi E_\phi) - |\mathbf{p}_\perp| E_x\right]
The rate of change of the angle θ depends on the components of the magnetic and electric fields; the azimuthal magnetic field Bφ plays a key role in beam compression.
Concepts
positron emission tomography laser spectroscopy optical tweezers Weber–Fechner law positive feedback loop phase locking