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where V'm(x) is a d-dimensional vector whose components are am(x)jax. Terms not shown may involve higher powers of m(x) and its derivatives. The external field H(x) enters only linearly, because we assume it is very weak. We have assumed for simplicity that m( x) is a single real field. More generally it could have many components, or be complex. The coefficient of 1V'm (x) 12 is chosen to be t, to fix the scale of m (x). All other coefficients are phenomenological parameters that may depend on the temperature and the cutoff. In practice we simply choose them to suit our purpose. However, there are constraints to be observed. For example, the term linear in m(x) must have H(x) as a coefficient for the order parameter to be correctly given by - aG j aH. The coefficient So for the cubic term must vanish for systems invariant under reversal of m(x) when H = 0, such as a ferromagnet. It is customary to assume that U o is independent of T, while .net pdf 417 reader Packages matching PDF417 - NuGet Gallery
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