Dirac Particle for the Position Dependent Mass in the Generalized Asymmetric Woods-Saxon Potential

Table 2

The abbreviations taking part in (26), (34), and (35).

---

𝑞𝛽=𝑝,𝑞𝛽=𝑝

𝐵₁=𝛽^−̃𝜁𝑒^{̃𝜁𝐿−𝑏}1−𝛽𝑒^{𝑏𝐿−𝜆}

𝐵₂=𝛽^𝜁𝑒^𝑎𝜁𝐿1−𝛽𝑒^𝑎𝐿𝜆

𝐵₃=𝛽^−𝜁𝑒^{−𝑎𝜁𝐿}1−𝛽𝑒^𝑎𝐿𝜆

𝐵₄=𝑏𝜁̃𝛽^−̃𝜁𝑒^{̃𝜁𝐿−𝑏}1−𝛽𝑒^{𝑏𝐿−𝜆}

𝐵₅=−𝑏𝜆𝛽^−̃𝜁+1𝑒^{̃−𝑏𝐿(𝜁−1)}1−𝛽𝑒^{𝑏𝐿−𝜆−1}

𝐵₆=−𝑏𝛽^−̃𝜁+1𝑒^{̃−𝑏𝐿(𝜁−1)}1−𝛽𝑒^{𝑏𝐿−𝜆}(−𝜁̃−𝜆+𝛾)(−𝜁̃−𝜆−𝛾)1−2𝜁̃

𝐵₇=𝑎𝜁𝛽^𝜁𝑒^𝑎𝜁𝐿1−𝛽𝑒^𝑎𝐿𝜆

𝐵₈=−𝑎𝜆𝛽^𝜁+1𝑒^{𝑎𝐿(𝜁+1)}1−𝛽𝑒^{𝑎𝐿𝜆−1}

𝐵₉=𝑎𝛽^𝜁+1𝑒^{𝑎𝐿(𝜁+1)}1−𝛽𝑒^𝑎𝐿𝜆(𝜁+𝜆+𝛾)(𝜁+𝜆−𝛾)1+2𝜁

𝐵₁₀=−𝑎𝜁𝛽^−𝜁𝑒^{−𝑎𝜁𝐿}1−𝛽𝑒^𝑎𝐿𝜆

𝐵₁₁=−𝑎𝜆𝛽^−𝜁+1𝑒^{−𝑎𝐿(𝜁−1)}1−𝛽𝑒^{𝑎𝐿𝜆−1}

𝐵₁₂=𝑎𝛽^−𝜁+1𝑒^{−𝑎𝐿(𝜁−1)}1−𝛽𝑒^𝑎𝐿𝜆(−𝜁+𝜈+𝛾)(−𝜁+𝜆−𝛾)1−2𝜁

𝐹₁=₂𝐹₁(−𝜁̃−𝜆+𝛾,−𝜁̃−𝜆−𝛾,1−2𝜁̃;𝛽𝑒^𝑏𝐿)

𝐹₂=₂𝐹₁(𝜁+𝜆+𝛾,𝜁+𝜆−𝛾,1+2𝜁;𝛽𝑒^𝑎𝐿)

𝐹₃=₂𝐹₁(−𝜁+𝜆+𝛾,−𝜁+𝜆−𝛾,1−2𝜁;𝛽𝑒^𝑎𝐿)

𝐹₄=₂𝐹₁(−𝜁̃−𝜆+𝛾+1,−𝜁̃−𝜆−𝛾+1,2−2𝜁̃;𝛽𝑒^𝑏𝐿)

𝐹₅=₂𝐹₁(𝜁+𝜆+𝛾+1,𝜁+𝜆−𝛾+1,2+2𝜁;𝛽𝑒^𝑎𝐿)

𝐹₆=₂𝐹₁(−𝜁+𝜆+𝛾+1,−𝜁+𝜆−𝛾+1,2−2𝜁;𝛽𝑒^𝑎𝐿)

𝐹₁=₂𝐹₁(−𝜆+𝛾_𝑐,−𝜆−𝛾_𝑐,1;𝛽𝑒^𝑏𝐿)

𝐹₂=₂𝐹₁(𝜆+𝛾_𝑐,𝜆−𝛾_𝑐,1;𝛽𝑒^𝑎𝐿)

𝐹₄=₂𝐹₁(−𝜆+𝛾_𝑐+1,−𝜆−𝛾_𝑐+1,2;𝛽𝑒^𝑏𝐿)

𝐹₅=₂𝐹₁(𝜆+𝛾_𝑐+1,𝜆−𝛾_𝑐+1,2;𝛽𝑒^𝑎𝐿)

---