
Quantum decoherence is the loss of quantum coherence due to interaction with the environment, leading to classical behavior.Decoherence explains why we don't see superpositions of large objects: interaction with the environment (atoms, photons) extremely quickly converts the quantum state into a classical one. It is a process by which, from the possible states, only what looks like classical definiteness survives. The decoherence rate increases with the distance between superposed states and with the strength of interaction.
The quantum measurement paradox was illustrated by Erwin Schrödinger in 1935 (Schrödinger's cat). John Archibald Wheeler contributed to understanding the role of the observer and the informational aspect of quantum phenomena. The formal theory of decoherence was developed in the 1970s–80s, primarily by Hans Dieter Zeh and Wojciech Zurek, who showed that the inevitable interaction with a macroscopic environment destroys quantum interferences in an extremely short time.
The environment continuously 'measures' the position or other property of the system, entangling with it. In the density matrix, this is reflected by exponential decay of off-diagonal elements: |ρ_ij| ~ exp(-γ t (x_i - x_j)^2). Interference terms vanish, and effective classical behavior emerges. This process aligns with the second law of thermodynamics: information about coherence is dispersed into the environment, increasing entropy.
Key to understanding the transition from the quantum to the classical world; critical for building quantum computers, where decoherence must be suppressed.
Decoherence can occur even in a perfect vacuum — due to quantum fluctuations that act as a weak but inevitable noise.
| X | variable | a set — set |
| κ | variable | a cardinal number — cardinal number |
| |X| | operator | cardinality of the set X — cardinality |
| cf(κ) | operator | cofinality of the cardinal κ — cofinality |

















