Categories:
Physics,
Quantum information,
Quantum mechanics.
No-cloning theorem
In quantum mechanics, the no-cloning theorem states
there is no general way to make copies of an arbitrary quantum state ∣ψ⟩.
This has profound implications for quantum information.
To prove this theorem, let us pretend that a machine exists
that can do just that: copy arbitrary quantum states.
Given an input ∣ψ⟩ and a blank ∣?⟩,
this machines turns ∣?⟩ into ∣ψ⟩:
∣ψ⟩∣?⟩⟶∣ψ⟩∣ψ⟩
We can use this device to make copies of the basis vectors ∣0⟩ and ∣1⟩:
∣0⟩∣?⟩⟶∣0⟩∣0⟩∣1⟩∣?⟩⟶∣1⟩∣1⟩
If we feed this machine a superposition ∣ψ⟩=α∣0⟩+β∣1⟩,
we want the following behavior:
(α∣0⟩+β∣1⟩)∣?⟩⟶(α∣0⟩+β∣1⟩)(α∣0⟩+β∣1⟩)=(α2∣0⟩∣0⟩+αβ∣0⟩∣1⟩+αβ∣1⟩∣0⟩+β2∣1⟩∣1⟩)
Note the appearance of the cross-terms with a factor of αβ.
The problem is that the fundamental linearity of quantum mechanics
dictates different behaviour:
(α∣0⟩+β∣1⟩)∣?⟩=α∣0⟩∣?⟩+β∣1⟩∣?⟩⟶α∣0⟩∣0⟩+β∣1⟩∣1⟩
This is clearly not the same as before: we have a contradiction,
which implies that such a general cloning machine cannot exist.
References
- N. Brunner,
Quantum information theory: lecture notes,
2019, unpublished.
- J.B. Brask,
Quantum information: lecture notes,
2021, unpublished.