
Emergence of ordered quantum states from chaotic or disordered systems.Quantum order from disorder refers to the surprising phenomenon where randomness or chaos in a quantum system can lead to the emergence of ordered, collective states. In classical physics, disorder usually destroys order, but in quantum mechanics, the interplay of interference, entanglement, and symmetry can turn a disordered system into a superfluid, a crystal, or a topological phase. This is a central theme in condensed matter physics, where materials with impurities or random interactions can still exhibit perfect conductivity or frictionless flow.
The concept of order from disorder was first explored in the context of spin glasses in the 1970s, but the quantum version gained prominence with the discovery of many-body localization in 2006 by Basko, Aleiner, and Altshuler. The idea that disorder can help create topological order was developed in the 2010s.
In a disordered quantum system, particles are localized (Anderson localization) if the disorder is strong. However, interactions between particles can break this localization and lead to a many-body localized phase or, under certain conditions, to a delocalized, ordered state. For example, in a system of ultracold atoms with random potentials, adding interactions can cause the atoms to form a superfluid, as the quantum fluctuations overcome the disorder. The article 'Когда хаос рождает сверхтекучесть' describes how this happens. Similarly, 'Квантовые узоры из хаоса' shows how disorder can create a rigid flow pattern.
This principle is used to design quantum memories in diamond (as in 'Беспорядок как союзник: квантовая память в алмазе'), where nitrogen-vacancy centers are randomly distributed but can be harnessed for coherent storage. It also informs the development of robust quantum simulators and superconducting materials.
In 2021, physicists observed that a disordered chain of atoms, when driven by a periodic pulse, spontaneously organized into a time-crystal—a phase that repeats in time, not space.
| r_n | variable | Level spacing ratio for adjacent energy levels — level spacing ratio |
| s_n | variable | Spacing between consecutive energy levels — energy level spacing joule |
| min | operator | Selects the smaller of the two arguments — minimum function |
| max | operator | Selects the larger of the two arguments — maximum function |
| \tau | variable | Order parameter (e.g., magnetization) — order parameter |
| \beta | variable | Inverse temperature (1/k_B T) — inverse temperature per joule |
| D_{\tau} | variable | Effective field (mean field) acting on the order parameter — effective field joule |
| \tanh | operator | Maps real numbers to (-1,1), typical for spin-1/2 systems — hyperbolic tangent |



















