The First Nuclear Clocks Are Ticking, and One of Them Steers Itself
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For half a century, physicists dreamed of a clock that keeps time using the heart of an atom instead of its outer electrons. On 7 October 2026, that dream became hardware. Two papers in Nature described the first working nuclear clock prototypes, one built at TU Wien in Austria and one at Tsinghua University in Beijing. The Vienna clock went a step further: it stabilized itself, running for more than 24 hours without anyone touching it.
Atomic clocks vs nuclear clocks
Every clock needs something that ticks at a steady rate. In a grandfather clock it is a pendulum. In the atomic clocks behind GPS and internet timing, it is the frequency of light that makes an atom's electrons jump between energy levels.
A nuclear clock uses a jump inside the atomic nucleus instead. The nucleus is about 100,000 times smaller than the atom and is shielded by its electron cloud, so stray electric and magnetic fields disturb it far less. In principle, that makes a nuclear clock more stable and more precise than any atomic clock.
Why thorium-229 is special
Almost every nucleus needs huge energies, far beyond what lasers can supply, to change state. Thorium-229 is the famous exception. It has an unusually low-energy transition that an ultraviolet laser can reach.
The idea of using it was proposed in 2003 by Ekkehard Peik of PTB, Germany's national metrology institute. The breakthrough came in April 2024, when teams including TU Wien and PTB finally hit that transition with a laser. The 2026 papers turn that discovery into actual clocks.
How the Vienna clock steers itself
The core is a small calcium fluoride crystal with thorium-229 atoms built into it, produced at TU Wien. A laser shines through the crystal.
The trick is a feedback loop. The laser nudges the thorium nuclei into their excited state, and the way the nuclei absorb that light is used to keep correcting the laser's frequency. If the laser drifts, the nuclei pull it back. Physicist Thorsten Schumm summed up the idea simply: the laser changes the nuclei, and the nuclei stabilize the laser.
The result is a nuclear clock that runs on its own. Over a single day, it reached a precision of about one part in 10^15, roughly equivalent to losing one second in 30 million years. It was checked against a conventional ytterbium-ion optical clock throughout.
Is it the most accurate clock in the world?
Not yet. The best optical atomic clocks are still better. The Vienna team plans stronger lasers and higher-quality thorium crystals to close the gap. The point of this result is that the concept works as a self-running system, which is the step that turns a lab experiment into a technology.
Why the world needs better clocks
- Navigation and timing. Better clocks could improve satellite navigation, telecom networks and financial timestamps.
- New physics. A nuclear transition is sensitive to tiny changes in the fundamental forces. The Vienna team already used its data to rule out some models of ultralight dark matter.
- Portable precision. Because the thorium sits inside a solid crystal, nuclear clocks could eventually be more compact than atomic clocks that rely on trapped atoms.
Is a nuclear clock dangerous?
No. It has nothing to do with nuclear power or weapons and produces no nuclear energy. Thorium-229 is radioactive, but the clocks use tiny amounts sealed in a crystal, and the laser only lifts the nucleus into a slightly higher energy state.
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Frequently asked questions
What is a nuclear clock?
A clock that measures time using an energy transition inside an atomic nucleus, rather than in the atom's electrons.
Who built the first nuclear clocks?
Teams at TU Wien (with PTB) in Austria and Tsinghua University in China, both published in Nature on 7 October 2026.
How long did the Vienna clock run?
More than 24 hours without manual intervention.
Is a nuclear clock more accurate than an atomic clock?
Not yet, but nuclear clocks are expected to surpass them as the technology improves.
Why use thorium-229?
It is the only known nucleus with a transition low enough in energy to be driven by a laser.