Table 1 Values of |J₀(i^3/2αR)|, |P _S (i^3/2αR)|/|J₀(i^3/2αR)|, |P _Q (i^3/2αR)|/|J₀(i^3/2αR)| and θ _d = -θ _PQ + θ_{J 0}(in degrees).

αR

|J₀(i^3/2αR)|

|P _S (i^3/2αR)|

$\frac{\left|P_S\left(i^{3/2}\alpha R\right)\right|}{\left|J_0\left(i^{3/2}\alpha R\right)\right|}$

$\frac{\left|P_Q\left(i^{3/2}\alpha R\right)\right|}{\left|J_0\left(i^{3/2}\alpha R\right)\right|}$

-θ _PQ + θ_{J 0}