- Let P represent the portion of the eigenvalue approximation circuit shown below.
.
.
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|ui
We consider the circuit for arbitrary unitary m-dimensional U, |ui Bm, and x {0,1}n (the eigenvalue estimation circuit took x = 0n and |ui to be an eigenvector).
Show that P |x,ui = |xi U[x] |ui, where [x] is the number with binary representation x and U[x] is matrix exponentiation.
- Let U be a unitary operator and suppose that |i and |i are eigenvectors with respective eigenvalues , C. Prove that if 6= then h | i = 0 (i.e. |i and |i are orthogonal).
- Let : {0,1} {0,1} be the identity function, defined by (x) = x. The function (x,y) = (x,x y) has the property that
(x,0) = (x,x),
meaning that it clones the bit x in the first register to the second register.
Let |i B be an arbitrary 1-qubit quantum state. Show that
.
That is, the quantum operator corresponding to the classical 1-bit cloning operator fails to clone |i unless |i is in a state corresponding to a classical bit.
- Let U be a (2n)-qubit operator that clones two n-qubit quantum states, |i,|i Bn, meaning
U(|i |0ni) = |i |i and U(|i |0ni) = |i |i.
Prove that U clones |i and |i if and only if |i = |i or h | i = 0. [Hint: take the inner product of the two equations.]
- Use the previous question to prove that a there are no quantum cloning operators that work for all pairs of states.
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