While reading basic-mathematics of quantum mechanics I came across a statement –
"For every complex euclidean space $\cal X$ there exists spanning sets
of the space $L({\cal X})$ consisting of only density operators".
Here,
- $\cal X$ is euclidean space, say ${\mathbb C}^n$;
- $L({\cal X})$ correspond to linear operators over ${\cal X}$ which is just complex matrices of $n\times n$ size; and
- Density operators are just positive semi-definite matrices of trace one.
Now, I do not quite understand this that linear combination of positive semi-definite matrices should be at least a symmetric matrix, then how can span cover all the elements in $L({\cal X})$.
Any remarks will be of help. Thanks.
Best Answer
Given any $T\in L(\mathbb C^n)$, you can write $$ T=\frac{T+T^*}2+i\,\frac {T-T^*}{2i} $$ so $T$ is a linear combination of selfadjoints. And for each selfadjoint you have the Spectral Theorem saying that they are a linear combination of rank-one projections (which are positive semidefinite of trace one).
The result is even true when $\mathcal X$ is an infinite-dimensional Hilbert space, although it is not trivial in that case.