## 5 Interference Analysis
### Jammers Interference
The SE of the V2M connection with jammers is evaluated as  
\[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]2 \[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]3  
Plugging \(L_{I_{V}}(\bar{\mathbf{s}})\), \(L_{I_{V_{0}}}(\bar{\mathbf{s}})\), \(f_{M}(z)\), \(L_{I_{M}}(\bar{\mathbf{s}})\), \(L_{I_{L}}(\bar{\mathbf{s}})\), \(L_{I_{N}}(\bar{\mathbf{s}})\), \(L_{I_{J}}\) and \(f_{V}(z)\) in (59), the SE of the MBS connection with jammers is derived. The LOS-LAP's SE is determined if the acquired SIR of both the V2L and L2V links is greater than the limit and is provided as  
\[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]4 \[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]5  
where (a) is obtained by following a similar procedure to that which was derived in App. C. Plugging the values of \(L_{I_{V}}(\bar{\mathbf{s}})\), \(L_{I_{V_{0}}}(\bar{\mathbf{s}})\), \(f_{L}(z)\), \(L_{I_{M}}(\bar{\mathbf{s}})\), \(L_{I_{L}}(\bar{\mathbf{s}})\), \(L_{I_{N}}(\bar{\mathbf{s}})\) and \(f_{V}(z)\) in (60), LOS-LAP's SE without jammers is obtained. The SE of the LOS-LAP with jamming devices is evaluated as  
\[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]6 \[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]7  
Plugging \(L_{I_{V}}(\bar{\mathbf{s}})\), \(L_{I_{V_{0}}}(\bar{\mathbf{s}})\), \(f_{L}(z)\), \(L_{I_{M}}(\bar{\mathbf{s}})\), \(L_{I_{L}}(\bar{\mathbf{s}})\), \(L_{I_{N}}(\bar{\mathbf{s}})\), \(L_{I_{J}}\), and \(f_{V}(z)\) in (61), LOS-LAP's SE with jammers is obtained. The NLOS-LAP's SE is calculated whenever the SIR of the V2N as well as the N2V link exceeds the limit and is computed as  
\[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]8 \[\stackrel{{ b}}{{=}}\int_{0}^{\infty}\Pr\{g_{t}\geq \frac{\tau(I_{X})}{P_{t}\eta G_{t}G_{r}\|z_{r}-z_{t}\|^{-a_{r}}}\}f_{r}(z)dz \tag{41}\]9  
where (a) is obtained by following a similar procedure to that which was derived in App. C. The final expression for the SE of the NLOS-LAP connection without jammers is obtained by substituting the values of \(L_{I_{V}}(\bar{\mathbf{s}})\), \(L_{I_{V_{0}}}(\bar{\mathbf{s}})\), \(f_{N}(z)\), \(L_{I_{M}}(\bar{\mathbf{s}})\), \(L_{I_{L}}(\bar{\mathbf{s}})\), \(L_{I_{N}}(\bar{\mathbf{s}})\) and \(f_{V}(z)\) in (62). The SE of the V2N connection with jamming devices is evaluated as \[\stackrel{{ c}}{{=}}\int_{0}^{\infty}\exp\{-s(I_{X} )\}f_{r}(z)dz,\]0 \[\stackrel{{ c}}{{=}}\int_{0}^{\infty}\exp\{-s(I_{X} )\}f_{r}(z)dz,\]1  
Substituting \(L_{I_{V}}(\mathbf{\bar{s}})\), \(L_{I_{V_{0}}}(\mathbf{\bar{s}})\), \(f_{N}(\mathbf{z})\), \(L_{I_{M}}(\mathbf{\bar{s}})\), \(L_{I_{L}}(\mathbf{\bar{s}})\), \(L_{I_{N}}(\mathbf{\bar{s}})\), \(L_{N,I}\), and \(f_{V}(z)\) in (63), the SE of the V2N connection with jammers is obtained. The SE of the overall link, i.e., the V2X connection, is given as  
\[\stackrel{{ c}}{{=}}\int_{0}^{\infty}\exp\{-s(I_{X} )\}f_{r}(z)dz,\]2  
Plugging \(A_{V}\), \(SE_{V}\), \(A_{M}\), \(SE_{M}\), \(A_{L}\), \(SE_{L}\), \(A_{N}\), and \(SE_{N,I}\) in (64), the SE of the V2X link is derived. The SE of the overall link with jammers, i.e., V2X connection with jammers, is given as  
\[\stackrel{{ c}}{{=}}\int_{0}^{\infty}\exp\{-s(I_{X} )\}f_{r}(z)dz,\]3  
Plugging \(A_{V}\), \(SE_{V,J}\), \(A_{M}\), \(SE_{M,J}\), \(A_{L}\), \(SE_{L,J}\), \(A_{N}\) and \(SE_{N,J}\) in (65), the SE of the V2X link with jammers is derived.