Dark States in Spin Chains express

Original: "Universal dynamics from a single-particle dark state"
arXiv:2605.16494 · 2026-05-15 · CC BY 4.0 · 1 min
Particles can freeze in a collective dance for a long time, barely losing energy.

In an orchestra, one musician plays so quietly that their sound is almost inaudible in the overall chorus. In the quantum world, such 'quiet' states are called dark: their energy barely escapes, like light in a darkened room. But if there are many musicians, their mutual influence can unexpectedly awaken even the most silent one.

In the new work, physicists considered a chain of spins (quantum 'tops') with a special type of dissipation acting on neighboring sites. In such a system, there exists a single-particle dark state with zero momentum: it, like a conductor, sets the rhythm but remains in the shadows. However, with a large number of particles, this state begins to slowly fade: its decay goes as [formula:decay]1/ln(t)[/formula], where t is time. It's like watching a candle flame not go out at once but smolder for a long time, obeying a tricky law.

Dark states are not just a curiosity. They could become the basis for storing quantum information, where data lives longer without being destroyed by noise.

The most surprising thing is that the system's behavior turned out to be universal. The distribution of particles over velocities (momenta) is described by a single form depending on [formula:scaling]k√t[/formula], and the total particle density falls as [formula:density]1/(√t * ln(t))[/formula]. This resembles the pattern left on sand after the tide: no matter what the tide was like, the lines remain similar. The results were confirmed by numerical simulation, and even with weak particle interactions the picture does not change — nature seems to insist on this scenario.

Similar dark states occur in optics: if atoms are placed at distances smaller than the wavelength of light, they can stop emitting, forming a 'silent' lattice.

In Greg Egan's novel 'The Permutation City', dark states of quantum systems allow the creation of virtual worlds that consume almost no energy.

\sim \frac{1}{\ln t}
Decay law of the dark state: inversely proportional to the logarithm of time.
k\sqrt{t}
Universal scaling variable for the momentum distribution.
\frac{1}{\sqrt{t}\ln t}
Decay law of the total particle density.
Scientists
Niels BohrPascual JordanWerner HeisenbergDavid DeutschErwin SchrödingerJohn Stewart Bell
Concepts
dark state open quantum system quantum collective phenomena false vacuum ground state complex system dynamics law of conservation of momentum energy dissipation universality dark matter ultra low temperature condensed matter physics collective effect backreaction principle of least action uncertainty principle false vacuum decay hidden particle decay condensate relaxation