Derivatives of a normalizable wavefunction

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Discussion Overview

The discussion revolves around the behavior of normalizable wavefunctions and their derivatives in the context of quantum mechanics, particularly as the spatial variables approach infinity. Participants explore whether all derivatives of a normalizable wavefunction also tend to zero under these conditions.

Discussion Character

  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants assert that a normalizable wavefunction approaches zero as spatial variables (r, x, y, z) tend to infinity, questioning if this holds for all derivatives as well.
  • One participant challenges the assumption that all derivatives must also approach zero, suggesting that the behavior of derivatives can differ from the wavefunction itself.
  • A participant references a specific example of a wavefunction, ##\psi (x) = \frac{\sin x^2}{x}##, noting that while it is normalizable, its derivative does not approach a limit as ##x \rightarrow \infty##.
  • Another participant cites Griffiths' Quantum Mechanics, stating that it claims both the wavefunction and its derivatives go to zero at infinity, but questions the universality of this statement by providing a counterexample involving a series of triangles.
  • There is a suggestion that while it may be reasonable to assume derivatives approach zero in practice, artificial examples exist that do not conform to this behavior.

Areas of Agreement / Disagreement

Participants express differing views on the behavior of derivatives of normalizable wavefunctions at infinity, with no consensus reached on whether all derivatives must tend to zero.

Contextual Notes

Participants highlight limitations in the assumptions made about wavefunctions and their derivatives, noting that specific examples can challenge general statements found in quantum mechanics literature.

dyn
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Hi.
In infinite volume a normalizable wavefunction → 0 as r or x,y,z→ 0 but do all the derivatives and higher derivatives → 0 as well ?
Thanks
 
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dyn said:
In infinite volume a normalizable wavefunction → 0 as r or x,y,z→ 0
What makes you think that ?
 
dyn said:
Hi.
In infinite volume a normalizable wavefunction → 0 as r or x,y,z→ 0 but do all the derivatives and higher derivatives → 0 as well ?
Thanks

Do you mean as ##x,y,z \rightarrow \infty##?
 
Sorry. Yes I meant r or x.y.z tend to infinity
 
Try to calculate the norm of ##\psi (x) = \frac{\sin x^2}{x}##, and draw a graph of its derivative with Wolfram Alpha... Function is normalizable but derivative doesn't approach any limit when ##x\rightarrow\infty##.
 
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I have just found the following in Griffiths QM " the wavefunction and all its derivatives go to zero at infinity"
 
dyn said:
I have just found the following in Griffiths QM " the wavefunction and all its derivatives go to zero at infinity"
Strictly speaking it's not true. Take the wavefunction that is a series of triangles, with the ##n##-th triangle centered on the integer ##n##, of height ##1## and of width ##\frac{1}{n}##, its square integral converges as it equals:
$$\sum_n \frac{1}{n^2}$$

However its magnitude doesn't tend to zero as you approach infinity..
 
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dyn said:
I have just found the following in Griffiths QM " the wavefunction and all its derivatives go to zero at infinity"

In practice you can probably assume so, but it's still possible to make artificial examples of wave functions that are not like that. I think it would be really difficult to solve the time evolution of that ##\frac{\sin x^2}{x}## function when used as the initial condition for a TDSE of a free particle, but it's likely that the time evolution would smooth it in no time to have ##\psi' (x)\rightarrow 0## when ##x \rightarrow \infty##.
 

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