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f I F 2 = f I i I L center ∗ ⋯ ∗ f I i I L center ⏟ N − th order convolution (11).
Similarly, the conditional m th moment of Y can be calculated as E [ Y m L center ] = ∫ y m f Y ( y | L center ) dy = α m M 0 ( mβ, γ ) γ 2 R mβ (19).
As we know, the joint distribution functions shown in (28) can be calculated by P ( L center, k < K ) = P ( L center ) P ( k < K L center ) P ( L edge, k < K ) = P ( L edge ) P ( k < K L edge ) (29).
The distribution function of K can be expressed as P Set − B ( k < K ) = P ( L center, k < K ) + P ( L edge, k < K ) (28).
Figure 2 presents an example of a real trajectory matrix (left), the representations coefficients L (center), and the singular value distribution of the coefficients (right).
The interference from the interior UEs in a neighboring cell is I i =P t,0 X Y H, and its PDF is derived as f I i ( I L center ) = 1 P t, 0 ∫ 0 ∞ 1 h f H ( h ) ∫ 0 ∞ 1 x f X ( x ) f Y I / P t, 0 xh L center dxdh (10).
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Noon 11.
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