Digital Communication over Fading Channels

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You may use the ¯ non-relativistic equation for the energy. Mathematically, we can represent the superposition of these two waves as a generalization of equation (2.15): h = sin[−∆kx x + (ky + ∆ky )y − ωt] + sin[∆kx x + (ky − ∆ky )y − ωt]. (2.18) In this equation we have given the first wave vector a y component ky + ∆ky while the second wave vector has ky − ∆ky. Thus equivariance expresses the mutual compatibility, relative to ρψ, of the Schrödinger evolution of the wave function and the Bohmian motion of the configuration.

Pages: 936

Publisher: Wiley-IEEE Press; 2 edition (December 6, 2004)

ISBN: 0471649538

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