A problem with a Dirac delta function potential

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SUMMARY

The discussion focuses on the relationship between the potential height \( V_0 \), the Dirac delta function coefficient \( \alpha \), and the width \( a \) of a rectangular barrier as it approaches a Dirac delta function potential \( V(x) = \alpha \delta(x) \). The key insight is that as the width of the barrier approaches zero, the height must increase such that the area under the potential remains constant. This leads to the conclusion that \( V_0 \) is equivalent to \( \alpha \delta(0) \), emphasizing the importance of maintaining the area under the potential in the limit.

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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.
 
Last edited:
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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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