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All these achievements continuously showed us the computational potential of quantum<br />

computer over classic computer.<br />

Quantum information theory, like classical information theory, deals with information<br />

which can be transmitted by using quantum systems as carriers. Modern classical comput-<br />

ers guard against error largely by being digital instead of analog. At each time step the<br />

hardware corrects the bit to standard 0 and 1 (digital instead of analog). This prevents<br />

small errors from building up into large errors, which are therefore drastically reduced. The<br />

same technique cannot be used in a quantum computer, because measurement on a single<br />

qubit would destroy the entanglements that distinguish a quantum computer from a classical<br />

one. Unlike the classic digital circuits, quantum operations are fully linear and reversible<br />

and therefore will quickly accumulate noise. The no-cloning property makes it more difficult<br />

to implement a reliable quantum communication.<br />

Decoherence, the alteration of the quantum state as a result of the interaction with<br />

the environment, is probably the most challenging problem faced by quantum computation<br />

and quantum communication [Pre98]. Quantum error correcting codes, like classical error<br />

correcting codes, allow us to deal algorithmically with decoherence. Over time, researchers<br />

have come up with several codes: Peter Shor’s 9-qubit-code, also named the Shor code,<br />

encodes 1 logical qubit in 9 physical qubits and can correct for one bit flip and one phase<br />

flip error; Steane implemented the same code using 7 instead 9 qubits, named Steane code;<br />

In 1996, Robert Calderband, Peter Shor and Andrew Steane discovered an important class<br />

6

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