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Surface waves, continuum limit

Let us for a moment consider the three channel problem depicted in Fig. 20.1. We have just discussed the case in which Wt < 0 for all i, i.e. the region below the lowest limit. The quantum defect surface defined by Eq. (20.12) is a two dimensional surface inscribed in a cube of length Av, = 1 on a side. Now let us consider the region between the first and second ionization limits, where channel 1 is open. Since is a continuum wave the r — boundary condition does not... [Pg.419]


See other pages where Surface waves, continuum limit is mentioned: [Pg.223]    [Pg.265]    [Pg.367]    [Pg.280]    [Pg.212]    [Pg.34]    [Pg.113]    [Pg.81]    [Pg.483]    [Pg.95]   
See also in sourсe #XX -- [ Pg.223 ]




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