A problem with a Dirac delta function potential

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The discussion centers on the relationship between the potential height V0, the strength α of the Dirac delta function, and the width a of a rectangular barrier as the barrier approaches a delta function form. The participant expresses confusion about how the width influences the potential, noting that as the width approaches zero, the height must increase to maintain a constant area. It is emphasized that the Dirac delta function can be viewed as the limit of a square pulse where the area remains constant. The implication is that the area under the delta function must equal the area under the original rectangular barrier. This understanding is crucial for correctly relating V0, α, and a in the context of quantum mechanics.
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Homework Statement


An ideal particle of energy E is incident upon a rectangular barrier of width 2a and height V_{0}. Imagine adjusting the barrier width and height so that it approaches V(x)=\alpha \delta(x). What is the relationship between V0, alpha and a?

Homework Equations




The Attempt at a Solution


I must be thinking of this incorrectly because the only thing that occurs to me is that in this limit,
V(x) = \alpha \delta (x), x = 0;<br /> V(x) = 0, elsewhere
and so
V_{0} = V(0) = \alpha \delta (0)
My issue is that this doesn't include the width at all (but I'm not sure why it should since the width goes to zero). Any insights are greatly appreciated.
 
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You could think of the Dirac delta function as the limiting case of a square pulse as the width of that pulse goes to zero, but the height goes to infinity (in such a way that the product of the two, which is the area of the pulse, remains constant and is always equal to unity). Does that help? It implies that the area under the scaled Dirac delta function in your problem must be the same as the area under the original square pulse.
 

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