
The quantum mechanical analogue of entropy, describing the entanglement and inaccessibility of information in a quantum system.Quantum entropy, often called von Neumann entropy, is the quantum analogue of classical thermodynamic entropy. It measures the amount of uncertainty or missing information about the exact quantum state of a system. For a pure state, the entropy is zero, meaning the state is completely known; for a mixed state, it is positive, reflecting that the system is in a statistical mixture of possible pure states. In the context of entanglement, the entropy of a subsystem (like one particle of an entangled pair) quantifies how much information about that subsystem is inaccessible due to its correlations with the other subsystem.
The concept was introduced by John von Neumann in 1927, building on the work of Lev Landau and others, as a rigorous mathematical foundation for quantum statistical mechanics.
The von Neumann entropy is defined as S = -Tr(ρ ln ρ), where ρ is the density matrix of the system. For a bipartite system in a pure state, the entropy of one part equals the entropy of the other, and this common value is a measure of the entanglement between them. If the state is separable (not entangled), the entropy of each part is zero. The more entangled the state, the higher the entropy of each subsystem, indicating that the individual particles carry less definite information on their own.
Quantum entropy is used in quantum information theory to quantify entanglement resources, in quantum error correction to measure information loss, and in the study of black hole thermodynamics (Bekenstein-Hawking entropy).
For a maximally entangled pair of qubits, the entropy of each qubit is exactly 1 bit, meaning that each qubit individually contains no definite information, yet the pair as a whole contains 2 bits of information.



