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el.
eigenfunctions
for linear time-invariant systems
собственные функции линейных стационарных систем
(
ssn
)
Makarov.
in quantum mechanics, coherent states are often the
eigenfunctions
of the creation and annihilation operators
в квантовой механике когерентные состояния являются часто собственными функциями операторов построения и аннигиляции
math.
it is easy to establish that the
eigenfunctions
3
are orthogonal with the weight P
ортогональны с весом
(x, y)
math.
it is easy to establish that the
eigenfunctions
are orthogonal with the weight W
взаимно ортогональны
(x, y)
math.
it is required to construct the above set of
eigenfunctions
while the error estimates must be uniform with respect to n
причём оценка погрешности должна быть равномерной по n
math.
the Chebyshev polynomials are orthogonal in the interval
-1; 1
over a weight w
x
. it is easy to establish that these
eigenfunctions
are orthogonal with the weight p
ортогональны с весом
(x, y)
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