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presented in Section 6.(vi)Finally, in Section 7, we present some remarks and conclusions. We use as a potential the well-known Woods-Saxon potential which can be written as 𝑉 𝑢 ( 𝑟 ) = 0 − 𝑢 1 + 𝑦 0 𝑦 𝑎 ( 1 + 𝑦 ) 2 ( 6 . 4 ) with 𝑦 = e x p
