Exact(8)
Hence, inclusion of radiation interaction effects modifies Equation 3, and the polarizability of the electrical dipole is as follows [49, 50]: α i = α i CM 1 − 2 / 3 i k 3 α i CM.
The two major theories for CM kidney injury are as follows: (i) CM induced renal vasoconstriction that leads to medullary hypoxia and (ii) direct tubular injury produced by the concentrated CM within tubular fluid [ 3].
Hence, inclusion of radiation interaction effects modifies Eq. (2) and the polarizibilty of electrical dipole is [34]: α i = α i CM 1 − 2 / 3 i k 3 α i CM Open image in new window (3).
In Eq. (3), α i CM Open image in new window is Clausius-Mossotti polarizibility, and k is the wavenumber.
(b) SNR = 11 dB Figure 5 4 × 4 MIMO CM-AMI I CM and BICM-AMI I BICM vs. rotation angle θ for 16QAM over Rayleigh fading channels.
Since I(X Y|Λ)=I(C k ;Y|Λ), the I CM and I BICM are the same for BPSK.
Figure 4 4 × 4 MIMO CM-AMI I CM and BICM-AMI I BICM vs. rotation angle θ for QPSK over Rayleigh fading channels.
In Equation 4, α i CM Open image in new windowis the Clausius-Mossotti polarizability, and k is the wave number.
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