At the delta potential, the bound equation becomes ψ(x)=βψ(0)e−κ∣x∣/κ. A nonzero solution therefore requires κ=β, givingThere is one bound level. The transmission amplitude t(k) has its physical-sheet pole at k=iβ, which produces exactly this decaying state. The real-axis probability's rational continuation T(k)=k2/(k2+β2) has both +iβ and −iβ poles; the lower pole is not an additional bound state. It is essential to distinguish the analytic amplitude from an even continuation of its modulus squared.
Eb=−2ℏ2mα2,ψb(x)=βe−β∣x∣.
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