Half-life using Schrodinger's wave equation

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SUMMARY

This discussion focuses on estimating half-life using Schrödinger's time-independent wave equation. The user explores dividing the energy barrier into smaller segments to improve tunneling probability approximations. The relevant equations include the wave function \(ψ = e^{-βx}\) and the parameter \(β = \frac {\sqrt {2m_α(U - E_α)}} {ħ}\). The user seeks assistance in solving the integral for \(ψ_{total} = e^{-2∫β(x)dx}\) to derive meaningful results.

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Hello guys!

I've been learning how to estimate half life using Schrödinger's time-independent wave equation. In class, we divided the energy barrier into five smaller segments just like this webpage http://hyperphysics.phy-astr.gsu.edu/hbase/Nuclear/alpdet.html#c1

I was wondering if we could divide the barrier into a large number of segments n to arrive at better approximations using calculus. In class, we used the following equation for the probability of tunneling

My work is shown below

$$ψ = e^{-βx}
\\β = \frac {\sqrt {2m_α(U - E_α)}} {ħ}
\\U = \frac {kq_1q_α} {x}
\\ψ^2 = e^{-2βx}
\\ψ_{total} = e^{-2∫β(x)dx}$$

I solved the integral and put a few numbers but didn't really get anything meaningful, so any help would be greatly appreciated
 
Last edited:
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Also, I have moved this post to the homework forum.
 

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