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diff --git a/content/know/concept/superdense-coding/index.pdc b/content/know/concept/superdense-coding/index.pdc new file mode 100644 index 0000000..e50be2b --- /dev/null +++ b/content/know/concept/superdense-coding/index.pdc @@ -0,0 +1,56 @@ +--- +title: "Superdense coding" +firstLetter: "S" +publishDate: 2021-03-07 +categories: +- Quantum information + +date: 2021-03-07T20:30:41+01:00 +draft: false +markup: pandoc +--- + +# Superdense coding + +In quantum information, **(super)dense coding** +is a protocol to enhance classical communication. +It uses a quantum communication channel and +[entanglement](/know/concept/quantum-entanglement/) +to send two bits of classical data with just one qubit. +It is conceptually similar to [quantum teleportation](/know/concept/quantum-teleportation/). + +Suppose that Alice wants to send two bits of classical data to Bob, +but she can only communicate with him over a quantum channel. +She could send a qubit, which has a larger state space than a classical bit, +but it can only be measured once, thereby yielding only one bit of data. + +However, they are already sharing an entangled pair of qubits +in the [Bell state](/know/concept/bell-state/) $\ket*{\Phi^{+}}_{AB}$, +where $A$ and $B$ are qubits belonging to Alice and Bob, respectively. + +Based on the values of the two classical bits $(a_1, a_2)$, +Alice performs the following operations on her side $A$ +of the Bell state: + +| $(a_1, a_2)$ | Operator $\qquad$ | Result | +|:--:|:--|:---------| +| $00$ | $\hat{I}$ | $\ket*{\Phi^{+}} = \frac{1}{\sqrt{2}} \Big(\ket{0}_A \ket{0}_B + \ket{1}_A \ket{1}_B \Big)$ | +| $01$ | $\hat{\sigma}_z$ | $\ket*{\Phi^{-}} = \frac{1}{\sqrt{2}} \Big(\ket{0}_A \ket{0}_B - \ket{1}_A \ket{1}_B \Big)$ | +| $10$ | $\hat{\sigma}_x$ | $\ket*{\Psi^{+}} = \frac{1}{\sqrt{2}} \Big(\ket{0}_A \ket{1}_B + \ket{1}_A \ket{0}_B \Big)$ | +| $11$ | $\hat{\sigma}_x \hat{\sigma}_z$ | $\ket*{\Psi^{-}} = \frac{1}{\sqrt{2}} \Big(\ket{0}_A \ket{1}_B - \ket{1}_A \ket{0}_B \Big)$ | + +Her actions affect the state on Bob's side $B$ due to entanglement. +Alice then sends her qubit $A$ to Bob over the quantum channel, +so he has both sides of the entangled pair. + +Finally, Bob performs a measurement of his pair in the Bell basis, +which will yield a Bell state that he can then look up in the table above +to recover the values of the bits $(a_1, a_2)$. +In the end, Alice only sent a single qubit, +and the rest of the information transfer was via entanglement. + + +## References +1. J.B. Brask, + *Quantum information: lecture notes*, + 2021, unpublished. |