Appendix E - Density Operator: Extensions

The following are somewhat standard conventions and those contained in Ref.~\cite{Byrd/Khaneja:03}. A density operator on an $N\,\!$-dimensional Hilbert space ${\mathcal {H}}_{N}\,\!$ will be represented using a set of traceless, Hermitan matrices $\{\lambda _{i}\}\,\!$, $i=1,2,...,N^{2}-1\,\!$ with the normalization condition ${\mbox{Tr}}(\lambda _{i}\lambda _{j})=2\delta _{ij}\,\!$. The commutation and anticommutation relations for this set of matrices are given by

	$[\lambda _{i},\lambda _{j}]=2ic_{ijk}\lambda _{k},\;\;\;\{\lambda _{i},\lambda _{j}\}={\frac {4}{N}}I\delta _{ij}+2d_{ijk}\lambda _{k},\,\!$	(E.1)

where the sum over repeated indices is to be understood unless otherwise stated. (In some cases the sum is displayed explicitly for emphasis.) These relations can be summarized using the trace, antisymmetric and symmetric combinations of the following equation

	$\lambda _{i}\lambda _{j}={\frac {2}{N}}I\delta _{ij}+d_{ijk}\lambda _{k}+ic_{ijk}\lambda _{k}.\,\!$	(E.2)

The density operator can now be written as

	$\rho ={\frac {1}{N}}\left(I+b{\vec {n}}\cdot {\vec {\lambda }}\right),\,\!$	(E.3)

where $b={\sqrt {(N(N-1)/2)}}\,\!$. The ``dot product is a sum over repeated indices,

	${\vec {a}}\cdot {\vec {b}}=a_{i}b_{i}=\sum _{i=1}^{N^{2}-1}a_{i}b_{i}.\,\!$	(E.4)

Any complete set of $N^{2}-1\,\!$ mutually trace-orthogonal, Hermitian matrices can serve as a basis and can be chosen to satisfy the conditions given here.

Pure states have the properties that

	${\vec {n}}\cdot {\vec {n}}=1,\;\;\;{\mbox{and}}\;\;\;{\vec {n}}\star {\vec {n}}={\vec {n}},\,\!$	(E.5)

where the "star" product is defined by

	$({\vec {a}}\star {\vec {b}})_{k}={\frac {1}{N-2}}{\sqrt {\frac {N(N-1)}{2}}}\;d_{ijk}a_{i}b_{j}.\,\!$	(E.6)

For later use, a "cross" product between two coherence vectors can also be defined by

	$({\vec {a}}\times {\vec {b}})_{k}=c_{ijk}a_{i}b_{j}.\,\!$	(E.7)