The reflection-one result describes a semi-infinite potential step, rather than a finite-width barrier. Define k=2mE/ℏ and κ=2m(V0−E)/ℏ. For E>0, takeThe growing exponential is excluded by boundedness as x→∞. Continuity of ϕ and ϕ′ at the finite step gives 1+r=c and ik(1−r)=−κc, henceThe probability current of the decaying tail is zero; the reflected and incident currents have equal magnitude. This agrees with the classical reflection coefficient even though the spatial wave function differs from a classical trajectory.
ϕ(x)={eikx+re−ikx,ce−κx,x<0,x>0.
r=k+iκk−iκ,c=k+iκ2k,R=∣r∣2=1.
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