One step of the block Jacobi method is needed to
diagonalize A.
Here a finite Hamiltonian matrix is obtained and one can
diagonalize it, find the smallest eigenvalue [E.sub.0] and its associated eigenfunction [T.sub.0].
The physical interpretation of Proposition 3 is that in order to
diagonalize the correlation matrix of the MIMO channel and at the same time to obtain the largest possible link power then the columns of the matrix T' [cross product] R should be chosen so that they equal the eigenvectors of the matrix [R.sub.m] corresponding its [M.sub.s] strongest and distinct eigenvalues.
Step 1
Diagonalize [S.sup.F] = [TT.sup.*] = U [[LAMBDA]U.sup.*], where [LAMBDA] = diag([[lambda].sub.i])i.
Humans love to take shortcuts; they love to
diagonalize.
Viable candidates include the Bohm theory which, selecting position as the preferred determinate observable, solves the measurement problem if measurement outcomes are without exception recorded in positions, and Modal Interpretations which, making the preferred determinate observable state-dependent, solve the measurement problem if measurement outcomes are without exception recorded in observables whose eigenbases
diagonalize the post-measurement reduced states of participant apparatus.
The eigenmodes
diagonalize the integral equation kernels and are independent of incident field [6].
Using 5 x 5 unitary matrices [64, 65], one can
diagonalize the neutrino mass matrix [M.sub.[nu]] in (5).
As mentioned, we
diagonalize the permeability tensor to obtain the principal permeability components and the principal directions [theta] and [mathematical expression not reproducible].
Let X = [[X.sub.1] [X.sub.2]] and [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] with [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] and [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] be non-singular matrices which simultaneously
diagonalize the Hermitian matrix pairs (H, M) and ([??], M) as in (2.2) and (2.4), where [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] are indefinite and [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] is positive definite.
As the permeability tensor in Equation (7) is symmetrical, we can always
diagonalize it [13].
For the evolution of the energy level, it is necessary to
diagonalize the Hamiltonian [[??].sub.l], which can be accomplished by introducing the vector Bose-operators [[??].sup.+.sub.[??]] and [[??].sub.[??]] [12]:
In fact, we only need the following bivariate special case of it (when we
diagonalize all [x.sub.i] = x and [y.sub.i] = y):