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are constant on equivalenceclasses is rigorously reproduced on the reduced manifold with the reduced geometric structure and Hamiltonian The possibility of fulfilling these conditions is usually related to symmetries which leave a geometric structure and a Hamiltonian invariant For a more concrete construction, we start with a Poisson manifold P on which a Lie group G acts by canonical transformations; that is, the action leaves the Poisson bracket on P invariant We then decompose P into equivalence classes, where two elements are equivalent if they are mapped into each other by the action of some group element We assume that we can select a representative of each equivalence class in such a way that P r e d = P/G is a manifold, on which we can define a reduced Poisson structure.

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(A nonunisolvent element)

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For defining a Poisson bracket on F r e d , consider any two Ared ,B r e d E F ( P , e d ) Construct A, B E F(P) from A r e d , B r e d by mapping p E P to the value of Ared, B r e d on the equivalence class of p The function C = {A, B } is constant on equivalence because the bracket is invariant under group actions, and A, B are constant on equivalence classes We thus obtain a well-defined Poisson bracket {Ared, Bred}red on P r e d , which inherits all the defining properties from the Poisson bracket on P This construction of a Poisson structure is known as the Poisson Reduction Theorem [Marsden & Ratiu, p 3491 If a Hamiltonian H on P is invariant under 6.

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p where m u2 v2 . The OTF vanishes for m . A=ldi . The impulse response and MTF for a circular aperture are illustrated in Fig. 6.17. Compared with the corresponding plots for a coherent system a presented in Fig. 4.14, the support of the MTF is twice that of the coherent transfer function but the passband is no longer at. The MTF for an annular aperture, which was observed to produce a highpass coherent transfer function in 4, is shown in Fig. 6.18 for a lens with the center 0.9 radius component obscured. The MTF shows secondary peaks at high frequencies, but the maximum transfer function in the passband for incoherent systems is always at u 0, v 0.

In conclusion we have found the following bounds: X(K) 5 min max{E[Z] + DC, KD+}. (11.53)

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it must be constant on equivalence classes so that it defines a function H r e d on P r e d The Hamiltonian system given by H on P then reduces to that given by H r e d on P r e d The invariance of the Hamiltonian is indispensable for establishing the smaller space P r e d as an appropriate setting for reversible dynamics If we start from a symplectic manifold P on which a Lie group G acts canonically, that is, the action leaves the symplectic form on P invariant, we could try the above construction for Poisson manifolds because there exists a Poisson structure on any symplectic manifold However, a degeneracy problem arises so that one needs to select a symplectic leaf.

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This approach was usually referred to as creating a table in Datasheet view in previous versions of Microsoft Access. n

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