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These effects can be described by introducing an interference factor.
The concept of an interference factor [1] is used as a model of how much interference power will leak from adjacent channels.
An interference factor, f, defined by (1 − q shunt/q), the relative size of the thermal shunt between the loop segments, was employed as the modification required to properly model borehole thermal resistance.
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Figure 4 shows the spectral-efficiency versus SNR performance for a multicell system with an intercell interference factor α=0.5.
Let us introduce an average interference factor, defined as a ratio of the power loss due to the additional attenuation for a repeater r associated with the BS j.
The modifications of building responses from interference over a practical range of reduced velocities are represented by an envelope interference factor.
For an average interference factor of 1/7, the optical repeater-enhanced system shows a comparable improvement due to its ideal behavior, even outperforming the relay system with its orthogonal allocation.
Figure 8 Asymptotic spectral-efficiency versus system load-factor β for the multicell systems operated with SNR = dB and an intercell interference factor α = 0.5.
Figure 3 Spectral-efficiency versus the number of users per cell, when SNR = 10 dB, N = 4 and an intercell interference factor α = 0.5.
Figure 9 Asymptotic spectral-efficiency versus the number of receive antennas per BS for the multicell systems operated with SNR = dB and an intercell interference factor α = 0.5.
The authors [3] proposed a mutual interference factor that tended to leave when the host or parasite met.
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