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

Table 3

The constants given in (33) and (37).

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𝑞𝛽=𝑝,𝑞𝛽=𝑝

𝐷₁=𝛽^𝜁1𝑒^{𝑏𝜁1𝐿}1−𝛽𝑒^{𝑏𝐿−𝜆1}

𝐷₂=𝛽^𝜁1𝑒^{𝑎𝜁1𝐿}1−𝛽𝑒^{𝑎𝐿𝜆1}

𝐷₃=−𝑏𝜁₁𝛽^𝜁1𝑒^{𝑏𝜁1𝐿}1−𝛽𝑒^{𝑏𝐿−𝜆1}

𝐷₄=−𝑏𝜆₁𝛽^𝜁1+1𝑒^{𝑏𝜁𝐿(1+1)}1−𝛽𝑒^{𝑏𝐿−𝜆1−1}

𝐷₅=−𝑏𝛽^𝜁1+1𝑒^{𝑏𝜁𝐿(1+1)}1−𝛽𝑒^{𝑏𝐿−𝜆1}(𝜁₁−𝜆₁+𝛾₁)(𝜁₁−𝜆₁−𝛾₁)1+2𝜁₁

𝐷₆=𝑎𝜁₁𝛽^𝜁1𝑒^{𝑎𝜁1𝐿}1−𝛽𝑒^{𝑎𝐿𝜆1}

𝐷₇=−𝑎𝜆₁𝛽^𝜁1+1𝑒^{𝑎𝐿(𝜁1+1)}1−𝛽𝑒^{𝑎𝐿𝜆1−1}

𝐷₈=𝑎𝛽^𝜁1+1𝑒^{𝑎𝐿(𝜁1+1)}1−𝛽𝑒^{𝑎𝐿𝜆1}(𝜁₁+𝜆₁+𝛾₁)(𝜁₁+𝜆₁−𝛾₁)1+2𝜁₁

𝐹₇=₂𝐹₁(𝜁₁−𝜆₁+𝛾₁,𝜁₁−𝜆₁−𝛾₁,1+2𝜁₁;𝛽𝑒^𝑏𝐿)

𝐹₈=₂𝐹₁(𝜁₁+𝜆₁+𝛾₁,𝜁₁+𝜆₁−𝛾₁,1+2𝜁₁;𝛽𝑒^𝑎𝐿)

𝐹₉=₂𝐹₁(𝜁₁−𝜆₁+𝛾₁+1,𝜁₁−𝜆₁−𝛾₁+1,2+2𝜁₁;𝛽𝑒^𝑏𝐿)

𝐹₁₀=₂𝐹₁(𝜁₁+𝜆₁+𝛾₁+1,𝜁₁+𝜆₁−𝛾₁+1,2+2𝜁₁;𝛽𝑒^𝑎𝐿)

𝐹₇=₂𝐹₁(−𝜆₁+𝛾_𝑐,−𝜆₁−𝛾_𝑐,1;𝛽𝑒^𝑏𝐿)

𝐹₈=₂𝐹₁(𝜆₁+𝛾_𝑐,𝜆₁−𝛾_𝑐,1;𝛽𝑒^𝑎𝐿)

𝐹₉=₂𝐹₁(−𝜆₁+𝛾_𝑐+1,−𝜆₁−𝛾_𝑐+1,2;𝛽𝑒^𝑏𝐿)

𝐹₁₀=₂𝐹₁(𝜆₁+𝛾_𝑐+1,𝜆₁−𝛾_𝑐+1,2;𝛽𝑒^𝑎𝐿)

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