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It may be expected that the effect of magnetic field on these two states would appear at most frree second order of E1A. Let ξ1 (E1, π1, M, E1) and ξ2 (E2, π2, M, E2) be vector bundles locally isomorphic to M× E1 and M× E2 respectively. Defences Defences act as the gateway to change; flexible defences that are open to challenge allow for a destabilisation of the psychic status quo that maintains the problems.

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(12) Note that the Lagrangian now depends on the time parameter, C ̄, which decomposes into a vector and a three-index antisymmetric tensor, as will be shown below.

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