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Projection-slice theorem
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== The FHA cycle == If the two-dimensional function ''f''('''r''') is circularly symmetric, it may be represented as ''f''(''r''), where ''r'' = |'''r'''|. In this case the projection onto any projection line will be the [[Abel transform]] of ''f''(''r''). The two-dimensional [[Fourier transform]] of ''f''('''r''') will be a circularly symmetric function given by the zeroth-order [[Hankel transform]] of ''f''(''r''), which will therefore also represent any slice through the origin. The projection-slice theorem then states that the Fourier transform of the projection equals the slice or : <math>F_1 A_1 = H,</math> where ''A''<sub>1</sub> represents the Abel-transform operator, projecting a two-dimensional circularly symmetric function onto a one-dimensional line, ''F''<sub>1</sub> represents the 1-D Fourier-transform operator, and ''H'' represents the zeroth-order Hankel-transform operator.
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