Figure
375 377 shows the principle of the determination of the interfering power. If f_ILT =f_ VLR then the interfering frequencies fall exactly in the receiving band of the victim link receiver (co-channel interference).
For simplification within the algorithms the mask function p_m_ILT is normalized normaliSed to 1 Hz reference bandwidth:
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| body | $emission\_re{{l}_{ILT}}=10\log \left\{ \int_{a}^{b}{P_{rel}^{linear}\left( \Delta f \right)d\Delta f} \right\}=10\log \left\{ \int_{a}^{b}{{{10}^{\frac{P_{rel}^{dBc}\left( \Delta f \right)}{10}}}d\Delta f} \right\}$ |
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(Eq. 113)
with 
denoting the normalized normaliSed user-defined mask in dBc/Hz.
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