A Trap for the Invisible ✛ ✎

Original: "Optimization and Underground Implementation of the KAPAE Phase II Detector for an Invisible New Particle Search in Positronium Decay"
arXiv:2609.10259v1 · 2026-09-09 · arXiv non-exclusive · independent analysis · 3 min
The KAPAE II detector sits a kilometer underground and is chilled to −37.5 °C to hear the silence of a decay that yields not a single photon.

Deep inside a mountain, where cosmic-ray muons are muffled by a thick layer of rock, stands a detector that catches not light but its absence. Positronium is a tiny atom in which an electron and its antiparticle, the positron, circle each other like a pair of dancers. Usually they come together and vanish in a flash of two or three gamma quanta. But sometimes, theorists suspect, instead of a flash something is born that carries energy away without a single trace. The KAPAE II detector was built to hear that silence.

Positronium is the lightest known atom: its mass is 2000 times smaller than that of a hydrogen atom. The lifetime of ortho-positronium in vacuum is about 142 nanoseconds.

The heart of the detector is an array of 25 BGO crystals (bismuth germanium oxide), each the size of a matchbox but 15 centimeters long. When a gamma quantum hits a crystal, the crystal flashes with blue light. The light is captured by silicon photomultipliers, devices that turn a faint flash into an electrical signal. To catch the positron before it annihilates, a thin PEN film as thick as a human hair is used; it acts like a starting pistol, giving the crystals their cue: "Watch closely."

But any detector on the Earth's surface drowns in background noise: cosmic muons pour down like rain, causing false coincidences. That is why KAPAE II was lowered into the underground Yemi laboratory to a depth of 1000 meters. There the muon flux is weakened by more than a factor of 330,000, which is like moving from a noisy street into a soundproof room. In addition, the detector was cooled to −37.5 °C: at that temperature the BGO crystals glow more brightly and for longer, allowing the flash energy to be measured more precisely.

Cooling to −37.5 °C improved the energy resolution from 14.8% to 11.7% at an energy of 511 keV. For comparison, the crystals in the ETH Zurich experiment had a resolution of about 15%.

The result exceeded expectations. The background coincidence rate fell from one event per second at the surface to less than one event per hour underground. That is a suppression by more than three orders of magnitude, as if the noise of a crowd turned into the whisper of a single person. After correcting for light leakage between neighboring crystals, the measured spectrum agrees well with computer simulations, confirming that the detector is ready for the main search.

Now KAPAE II will collect data for months, waiting for a rarest of events: positronium decays and no energy appears in the crystals. Such "silence" could mean the birth of a dark-sector particle, for example a dark photon or an axion-like particle. If no signal is found, the limit on the probability of an invisible decay will improve to 10⁻⁸, which is an order of magnitude stricter than before. The trap for the invisible is ready, and the silence inside it will be heard, even if it remains silence.

Positronium is the lightest known atom: its mass is 2000 times smaller than that of a hydrogen atom. The lifetime of ortho-positronium in vacuum is about 142 nanoseconds, but in the detector it annihilates faster because of interactions with matter.

The idea of invisible particles carrying away energy echoes the "dark matter" of science fiction, for example in Liu Cixin's novel The Three-Body Problem, where an invisible substance affects physical processes. In a real experiment, however, the goal is a rigorous search for specific candidates, not fictional substances.

\tau(T) = 493 \exp(-0.018T) \text{ нс}
The decay time of the BGO crystal grows exponentially as the temperature decreases: at −26 °C it reaches 789 ns, and at the operating temperature of −37.5 °C it is about 960 ns.
Concepts
besiii besiii detector neutrino detector cryogenic temperature neutrinoless double beta decay underground laboratory juno borexino neutrino detection liquid argon particle identification neutral pion xenonnt