Exercise 2.31#
Suppose \(V\) is a vector space with orthonormal basis \(\{|i\rangle_{V}\}\) and \(A:V\to V\) is a \(m\times m\) positive operator. Suppose \(W\) is a vector space with orthonormal basis \(\{|j\rangle_{W}\}\) and \(B:W\to W\) is a \(n\times n\) positive operator. Then the tensor product of \(A\) and \(B\) is an operator \(A\otimes B : V\otimes W\to V\otimes W\), and the basis in vector space \(V\otimes W\) is \(\{|i\rangle_{V}\otimes|j\rangle_{W}\}\). To prove operator \(A\otimes B\) is positive, we need to prove for arbitrary vector \(|\psi\rangle \in V\otimes W\), we have
We could compute \(\langle \psi|A\otimes B|\psi\rangle \) directly as
Note that \(A\) and \(B\) are positive operator, then for basis vector \(|i\rangle_{V}\) and \(|j\rangle_W\), we should always have \(\langle i|A|i\rangle\geq 0\) and \(\langle j|B|j\rangle\geq 0\). Also, since for any coefficient \(c_{ij}\), we have \(|c_{ij}|^2 \geq0\), for eq. (2) we should have
Then we could conclude that, \(\langle \psi|A\otimes B|\psi\rangle \geq 0 \) for arbitrary state \(|\psi\rangle \in V\otimes W\), and the tensor product of two positive operators is positive.