The inhomogeneous Helmholtz differential equation is
(1)
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where the Helmholtz operator is defined as . The Green's function is then defined by
(2)
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Define the basis functions as the solutions to the homogeneous Helmholtz differential equation
(3)
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The Green's function can then be expanded in terms of the s,
(4)
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and the delta function as
(5)
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Plugging (◇) and (◇) into (◇) gives
(6)
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Using (◇) gives
(7)
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(8)
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This equation must hold true for each , so
(9)
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(10)
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and (◇) can be written
(11)
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The general solution to (◇) is therefore
(12)
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(13)
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