The no-cloning theorem states that an arbitrary unknown quantum state cannot be perfectly copied.The no-cloning theorem was proved in 1982 independently by William Wootters and Wojciech Zurek, and also by Dennis Dieks. It immediately explained why in the quantum world, communication through entanglement does not allow faster-than-light information transfer: the received signal is an unknown state that cannot be copied for repeated verification. The prohibition turned out to be a fundamental limitation born from the linearity of quantum mechanics. Thanks to it, quantum information is fundamentally different from classical information.
In 1982, William Wootters and Wojciech Zurek in a short note in Nature showed that cloning an unknown quantum state contradicts linearity. In the same year, Dennis Dieks published a similar result. The formulation quickly became a cornerstone of quantum information theory. Subsequently, the theorem was generalized to mixed states and entangled systems, and also formed the basis for proving the security of quantum cryptography protocols such as BB84.
The theorem is actively applied in quantum computing and quantum communication. It guarantees that an eavesdropper cannot undetectably intercept quantum keys, since any attempt to copy photons will introduce errors. In quantum computing, it prevents error correction by simple copying, forcing the use of sophisticated codes. Limits of applicability: the theorem holds for closed systems with unitary evolution; in open systems one can only talk about approximate cloning.
Protects quantum communication channels from eavesdropping: any intrusion leaves inevitable traces, making quantum cryptography absolutely secure.
Although perfect cloning is forbidden, one can build 'quantum copying machines' that create imperfect copies with a certain accuracy. They have almost reached the theoretical limit, but will never reach 100%.














