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A Global Newton-like Method

All methods considered in the previous subsections rely on successive [Pg.71]

The object of this subsection consists in solving Eq.(3) by an associated differential equation. There are several ways to do this. [Pg.71]

The differential Eq.(54a) represents Newton s second law (with a dissipative force) and so the solution curves have a physically meaning within a semi classical framework. This question is discussed in detail in Ref.55. [Pg.72]

It is easy to verify that each stationary point x of E corresponds [Pg.72]

For a better understanding of the mathematical background method, a little excursion to the stability theory of differential equations is useful. To this end we consider the first order differential equation [Pg.72]


See other pages where A Global Newton-like Method is mentioned: [Pg.38]    [Pg.71]   


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