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Hence, a common set of eigenfunctions exists for both operators.
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The advantage of expressing a general function as a linear combination of a set of eigenfunctions is that it allows us to deduce the effect of an operator on a function that is not one of its own eigenfunctions.
A complete set of eigenfunctions for the total Hamiltonian H can be spanned in terms of products of periodic Bloch functions |J,J z 〉 near the L-point and envelope functions.
Suppose that for the ith individual sample we obtain the functional principal component score: (18) z i j (1 ) = ∫ T β j (t ) w i 1 (t ) d t, z i j (0 ) = ∫ T β j (t ) w i 0 (t ) d t, where w i 1 t) and w i 0 t) are the coefficient functions of the ODE for the ith individual sample and β j (t), j = 1,…, K, are a set of eigenfunctions (or principal component functions).
Consequently the set ({phi_{i}}) form an orthonormal set of eigenfunctions either for (mathfrak{F}) and (1 - 5).
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