## 5 Interference Analysis
### Jammers Interference
The coverage of the MBS with jammers can be evaluated as  
\[C_{M,J}=\int_{0}^{\infty}\Bigl{(}L_{I_{V}}(s)\times L_{I_{V_{0}}}(s)\times L_{ I_{J}}\Bigr{)}f_{M}(z)\times\int_{0}^{\infty}\Bigl{(}L_{I_{M}}(s)\times L_{I_{L}}(s) \times L_{I_{N}}(s)\times L_{I_{J}}\Bigr{  
\[C_{L,J} =\int_{0}^{\infty}\!\!\!\exp\!\left(-2\lambda_{R}\lambda_{V}\!\! \int_{0}^{\infty}\!\!\!\left(1-L_{I_{V}}^{z}(s)\right)\!\!\!H_{1}+\!\int_{z_{L} ^{2}}^{\infty}\!\!\!\left(1-L_{I_{V}}^{1}(s)\right)\!\!\!H_{2}\right)\!\!\exp \!\left(-2\lambda_{V}\!\!\int_{z_{L}}^{\infty}\!\!\!\left(1-\frac{1}{1+sP_{V} \eta G_{V,I}G_{L,r}b^{-\alpha_{L}}}\right)\!\!\!\right)\] \[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]0 \[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]1 \[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]2 \[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]3 \[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]4 \[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]5 \[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]6  
For the shared mode transmission using the NLOS-LAP, the connection of the NLOS-LAP is said to be in coverage if the SIR obtained for the V2N connection, as well as the N2V connection, is larger than the predefined values. This is given as  
\[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]7 \[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]8  
where (a) is obtained by following a similar procedure to (45). Substituting the values of \(L_{I_{V}}(s)\), \(L_{I_{V_{0}}}(s)\), \(f_{N}(z)\), \(L_{I_{M}}(s)\), \(L_{I_{L}}(s)\), \(L_{I_{N}}(s)\), and \(f_{V}(z)\) in (51), the NLOS-LAP's coverage is derived. The NLOS-LAP's coverage with jammers can be derived as  
\[\stackrel{{ a}}{{=}}\int_{0}^{\infty}\Pr\{\frac{P_{t} \eta g_{t}G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}{I_{X}}\geq\tau\}f_{r}(z)dz\]9  
Substituting \(L_{I_{V}}(s)\), \(L_{I_{V_{0}}}(s)\), \(f_{N}(z)\), \(L_{I_{M}}(s)\), \(L_{I_{L}}(s)\), \(L_{I_{N}}(s)\), \(L_{I_{J}}\), and \(f_{V}(z)\) in (52)  
The SE of the MBS link without jammers can be determined whenever the SIR of the V2M link and the M2V link is bigger than the specified limit. It is represented as  
\[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]0 \[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]1  
where (a) is obtained by following a similar procedure to that which was derived in App. C. Plugging the values of \(L_{I_{V}}(\bar{\mathbf{s}})\), \(L_{I_{V_{0}}}(\bar{\mathbf{s}})\), \(f_{M}(z)\), \(L_{I_{M}}(\bar{\mathbf{s}})\), \(L_{I_{L}}(\bar{\mathbf{s}})\), \(L_{I_{N}}(\bar{\mathbf{s}})\), and \(f_{V}(z)\) in (58), the SE of the MBS without jammers is derived.