Question about limit of wave function as x goes to infinity

vincent_vega
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So I understand why the limit of the wave function as x goes to infinity is 0. But on pg 14 of Griffiths 2nd ed. qm for example, why does he call lim x\rightarrow\infty ψ*\frac{dψ}{dx} = 0? How can you assume that \frac{dψ}{dx} doesn't blow up at x = ∞
 
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Hello, vincent.

You have a good question there. It is possible to construct functions ψ(x) that go to zero at infinity but such that ψ*(x)ψ'(x) is not defined at infinity. For example ψ = sin(x^4)/\sqrt{1+x^2}

Griffiths wants to argue that the combination ψ*(x)ψ'(x) - ψ(x)ψ*'(x) goes to zero at infinity so that the normalization of the wavefunction is time independent. For any real wavefunction, you can see that this combination is identically zero for all x. However, it is possible to construct complex valued functions ψ for which the combination does not go to zero at infinity even though ψ goes to zero at infinity. For example ψ = e^{ix^4}/\sqrt{1+x^2}. But this wavefunction is "pathological". For example, the expectation value of the kinetic energy operator is undefined for this function.

So, maybe the allowable wavefunctions are restricted to exclude these pathological functions. I don't know.
 
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Interesting example - I'm guessing the class of allowed wavefunctions is pretty close to the class of functions for which an inverse Fourier transform exists. Probably this one fails the bounded variation test.
 
TSny said:
Hello, vincent.

You have a good question there. It is possible to construct functions ψ(x) that go to zero at infinity but such that ψ*(x)ψ'(x) is not defined at infinity. For example ψ = sin(x^4)/\sqrt{1+x^2}

Griffiths wants to argue that the combination ψ*(x)ψ'(x) - ψ(x)ψ*'(x) goes to zero at infinity so that the normalization of the wavefunction is time independent. For any real wavefunction, you can see that this combination is identically zero for all x. However, it is possible to construct complex valued functions ψ for which the combination does not go to zero at infinity even though ψ goes to zero at infinity. For example ψ = e^{ix^4}/\sqrt{1+x^2}. But this wavefunction is "pathological". For example, the expectation value of the kinetic energy operator is undefined for this function.

So, maybe the allowable wavefunctions are restricted to exclude these pathological functions. I don't know.

thanks that makes sense.

do you have any idea why x*ψ(x)*ψ'(x) is defined to be zero at x = infinity? this also occurred in the example by griffiths. I am thrown off by the x in front of the expression
 
vincent_vega said:
thanks that makes sense.

do you have any idea why x*ψ(x)*ψ'(x) is defined to be zero at x = infinity? this also occurred in the example by griffiths. I am thrown off by the x in front of the expression

I don't know. It seems that Griffiths is making an assumption about the behavior of the wavefunction and its derivative at infinity.
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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