A Quiet Helper for Quantum Computers: How a DC Voltage Brings Order ✛

Original: "Engineering multi-photon dissipation with a dc-voltage-biased Josephson junction"
arXiv:2608.31154v1 · 2026-08-31 · CC BY 4.0 · 1 min
Scientists have learned to control photon losses in a superconducting circuit with a simple DC voltage, eliminating unwanted noise.

A courtroom interpreter must convey every word without being distracted by the noise in the room. In the quantum world, a superconducting resonator plays the role of such an interpreter: it must lose photons strictly on schedule, without being thrown off by extraneous effects. Previously, this was done with a microwave pump, but the pump itself created noise, as if the interpreter started shouting out the audience's remarks.

Now scientists have found a quieter way. Instead of a loud pump, they applied a DC voltage to the superconducting circuit. When a pair of electrons passes through the junction, it releases energy that can be precisely tuned so that two photons from the memory resonator are converted into one photon in the buffer resonator. The buffer resonator quickly loses that photon, and the system settles into the desired state.

The Kerr effect, which used to be a nuisance, is now suppressed by a factor of three thousand. It's as if the interpreter finally stopped hearing the noise in the room.

This approach opens the way to stabilizing cat-state qubits, which are needed for quantum error correction. Whereas previously the pump itself introduced errors, now the DC voltage works like a perfect interpreter: precise, quiet, and without unnecessary words.

A two-photon dissipation rate of 0.51 MHz means that a pair of photons leaves the resonator in 2 microseconds, which is comparable to the lifetime of a single photon in the same resonator (3.1 μs).

The idea of using dissipation to stabilize quantum states echoes the concept of a 'quantum Maxwell's demon': instead of fighting losses, they are channeled in the right direction, as in Greg Egan's novel 'Permutation City', where quantum states are maintained by actively managing the environment.

\kappa_n = \frac{4g_n^2}{\kappa_b}
The rate of losing n photons is proportional to the square of the exchange rate g_n and inversely proportional to the buffer decay rate κ_b.
Scientists
Leo EsakiSatyendra Nath BoseJohn BardeenFelix BlochGeorg OhmHendrik Casimir
Concepts
two photon absorption single photon source transmon qubit josephson current Josephson effect charge qubit photodetector spontaneous parametric down conversion silicon photomultiplier cavity qed heralded single photon generation d meson neutral pion aluminum oxide stimulated emission