Scales for the Invisible: Weighing an Atom's Decay ✎ express

Original: "Precise determination of electron-capture $$Q$$ value of $$^{113}$$Sn decay related to electron neutrino mass measurements"
arXiv:2604.03410 · 2026-04-03 · arXiv non-exclusive · independent analysis · 1 min
Physicists have measured the decay energy of tin-113 with precision that paves the way for hunting the neutrino's mass.

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In the basement of a laboratory in Jyväskylä, a trap holds a single atom aloft, like a magician balancing a ball on a fingertip. The tin-113 atom is unstable: sooner or later it captures one of its own electrons and becomes indium-113, emitting an elusive particle — the neutrino. How much energy is released in the process was previously known only approximately.

Physicists measured this energy using a device that compares atomic masses by making them spin in a magnetic field. It turned out that tin-113 has two decay paths that release very little energy, as if a stone rolled down a gentle slope rather than falling off a cliff. One path is especially intriguing: in it, almost all the energy goes into the neutrino, not into other particles.

The neutrino is a ghostly particle: billions pass through us every second without touching a single atom. Its mass remains unknown.

Knowing the decay energy precisely is like having an accurate map before a hike. Future experiments can use this decay to catch neutrinos and, perhaps, finally weigh them. For now, tin-113 remains in its trap, patiently awaiting its transformation.

The energy released in one of tin-113's decays is less than that of a dental X-ray — about 15 thousand electronvolts.

Scientists
Christian DopplerD. B. McLaughlinDidier QuelozMichel MayorR. A. RossiterPaul Dirac
Concepts
electron mass electron capture neutron mass spectral line measurement gigaelectronvolt neutron capture kiloelectronvolt katrin ground state