Counting Light to Ten Thousand express

Original: "Generating Fock state exceeding 10000 excitations with near unit fidelity by adaptive generalized-parity measurement"
· Chen-yi Zhang, Jun Jing
arXiv:2606.01341 · 2026-05-31 · CC BY 4.0 · 3 min
Physicists have learned to gather photons into perfect bunches with a specified number of particles, almost without missing.

You're pouring water into a glass, but you want exactly one million drops — not approximately, but exactly. An ordinary faucet pours a stream where the number of drops always varies. In the quantum world, photons have the same problem: a laser emits light where the number of particles fluctuates like a crowd in a square. But for many tasks, from ultra-precise measurements to quantum computers, you need states with a perfectly defined number of photons, the so-called Fock states.

Previously, they were obtained in two ways. The first is to wait for a random event where the beam happens to contain the right number of photons. The second is to cleverly control the system, constantly tweaking parameters. Both paths are painful: either the success probability is minuscule, or the control is monstrously complex. The authors of the new work proposed a third path — an adaptive measurement protocol. The quantum system (light in a cavity) is coupled to a tiny sensor — an auxiliary qubit. A series of measurements is performed on the qubit, but not identical ones; instead, the interval between measurements depends on the previous result. This is like playing "hot and cold": after each step, we learn whether we're closer to the goal and adjust the next step.

The main difference from old methods is that here "failed" attempts are not discarded. In previous schemes, only one predetermined chain of measurement outcomes worked, and all others were thrown away, making the process extremely inefficient. In the new protocol, any measurement trajectory leads to the goal; the path just changes slightly.

In calculations on the Jaynes-Cummings model (light interacting with a qubit), a large coherent pulse (roughly speaking, a laser beam) almost certainly turns into a Fock state with ten thousand photons in just ten rounds of measurements. The average fidelity is about 87%. If you need fidelity above 99%, then with a probability of 35% you can obtain a state with a photon number from 20000 − √20000 to 20000 + √20000. This is a huge step forward compared to previous attempts.

The method proved robust: it doesn't break under moderate measurement errors and inaccuracies in system parameters. Even if the light is initially not perfectly pure but slightly "warm" (a so-called displaced thermal state), the protocol still works reliably.

The practical value is great. Large Fock states are a resource for quantum metrology: they can measure distances, fields, and forces with precision unattainable in classical physics. In quantum computing, such states serve as carriers of error-protected information. The new protocol doesn't require exotic equipment, just a cavity, a qubit, and standard measurements. This brings closer the day when quantum devices with macroscopic Fock states become a common tool.

So a light beam, like a disorderly crowd, turns into a handful of sand where every grain has been counted individually.

To feel the difference: in a bright laser beam, the number of photons per second is about $10^{16}$, but it is never exactly known. A Fock state with 10,000 photons is like a handful of sand where every grain has been counted individually.

In Arthur Koestler's novel "The Sleepwalkers," the protagonists strive for absolute knowledge but encounter uncertainty. Here, scientists do the opposite: they tame uncertainty, turning the probabilistic world of photons into a realm of exact numbers.

Scientists
Daniel GottesmanDavid DiVincenzoGilles BrassardIgnacio CiracJohn PreskillPeter Zoller
Concepts
Fock space fidelity Fermi's golden rule photon pair generation parameter fitting generalized uncertainty principle Born rule purity quantum measurement