Griffiths Problem 1.15: Understanding Complex Potential

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Discussion Overview

The discussion revolves around Griffiths Problem 1.15, which addresses the concept of complex potentials in quantum mechanics, particularly in relation to unstable particles and their decay. Participants explore the implications of using a complex potential, specifically the imaginary part associated with decay rates, and its physical significance.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants discuss the nature of complex potentials and the physical meaning of the imaginary part, \Gamma, which is proposed to represent the decay rate of unstable particles.
  • There is a suggestion that the complex potential indicates a probability of the particle "disappearing" over time, leading to an exponentially decreasing probability function.
  • One participant questions whether the advanced treatment in quantum field theory (QFT) would restore a real potential, implying that the complex potential might be a mathematical trick for describing unstable particles.
  • Another participant raises the issue of whether the formula \(\tau = \frac{\hbar}{2\Gamma}\) accounts for the nature of the particle, suggesting that it implies all particles in the potential have the same lifetime.
  • There is a discussion about the uniqueness of wavefunctions that satisfy the decay relation and whether different particles can be described within the same formalism.
  • Some participants express uncertainty about the implications of using complex potentials and the limitations of the current understanding, particularly regarding multiple particles and their decay processes.

Areas of Agreement / Disagreement

Participants generally express uncertainty and explore multiple competing views regarding the physical significance of complex potentials and their implications in quantum mechanics. There is no consensus on whether the complex potential is merely a mathematical tool or has deeper physical meaning.

Contextual Notes

Limitations include the dependence on definitions of decay rates and the potential's imaginary part, as well as unresolved questions about the treatment of multiple particles and the uniqueness of wavefunctions in this context.

neutrino
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Yet another question from question from Griffiths. This time I was able to do the problem, but I’m not able to understand what it means.

Chapter 1, problem 1.15

He talks about unstable particles for which the probability of finding it somewhere is not one, but an exponentially decreasing function of time.

[tex]\int_{-\infty}^{\infty}|\Psi(x,t)|^2dx = e^\frac{-t}{\tau}[/tex] ,

To arrive at this result (in a “crude” way), we assume that the potential energy function has an imaginary part, [itex]\Gamma[/itex].

[tex]V = V_0 - \imath\Gamma[/tex],

where [itex]V_0[/itex] is the true potential energy and [itex]\Gamma[/itex] a positive real constant.

What I don’t understand is the nature of this potential. What’s a complex potential, and does gamma have a physical meaning?
 
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neutrino said:
Yet another question from question from Griffiths. This time I was able to do the problem, but I’m not able to understand what it means.

Chapter 1, problem 1.15

He talks about unstable particles for which the probability of finding it somewhere is not one, but an exponentially decreasing function of time.

[tex]\int_{-\infty}^{\infty}|\Psi(x,t)|^2dx = e^\frac{-t}{\tau}[/tex] ,

To arrive at this result (in a “crude” way), we assume that the potential energy function has an imaginary part, [itex]\Gamma[/itex].

[tex]V = V_0 - \imath\Gamma[/tex],

where [itex]V_0[/itex] is the true potential energy and [itex]\Gamma[/itex] a positive real constant.

What I don’t understand is the nature of this potential. What’s a complex potential, and does gamma have a physical meaning?

have you related Gamma to the lifetime tau?
Gamma is bascially the decay rate of the particle. The complex part of the potential is related to the fact that the probability of observing the particle "decays" with time. Basically, that the particle has a probability of "disappearing". Of course, whatthis means is that a complex potential describes an *unstable* particle. At some point it will decay into *other particles* but since you have only an equation describing this particle, you must take this effect into account by introducing a complex part in the potential (a full treatment would have to include the other particles as well as a mean for the number of particles to change and would thus require a full-fledged quantum field theory).
 
Thanks for the reply. :smile:

nrqed said:
have you related Gamma to the lifetime tau?
Gamma is bascially the decay rate of the particle.
Yes, [tex]\tau = \frac{\hbar}{2\Gamma}[/tex]. Gamma, of course, has units of energy.

The complex part of the potential is related to the fact that the probability of observing the particle "decays" with time. Basically, that the particle has a probability of "disappearing". Of course, whatthis means is that a complex potential describes an *unstable* particle.
That part was clear, i.e. to describe a unstable particle you need a complex potential.

At some point it will decay into *other particles* but since you have only an equation describing this particle, you must take this effect into account by introducing a complex part in the potential (a full treatment would have to include the other particles as well as a mean for the number of particles to change and would thus require a full-fledged quantum field theory).
(A naïve question)So will this QFT treatment bring back the real (both physically and mathematically) potential?
 
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neutrino said:
That part was clear, i.e. to describe a unstable particle you need a complex potential.

Is that a generalization? Complex potentials have mathematical (functional) significance as entities in gaussian space, but can their real and imaginary parts be necessarily ascribed a physical signifiance?

(A naïve question)So will this QFT treatment bring back the real (both physically and mathematically) potential?

If this has something to do with renormalization (as an analogous mathematical step in procedure or even spirit) then I would be interested to know what you mean by "bring back".
 
maverick280857 said:
Is that a generalization? Complex potentials have mathematical (functional) significance as entities in gaussian space, but can their real and imaginary parts be necessarily ascribed a physical signifiance?
That's what I want to know. But my earlier statement was within the limits of the problem.

If this has something to do with renormalization (as an analogous mathematical step in procedure or even spirit) then I would be interested to know what you mean by "bring back".
I did say it was a naive question. To make it clear, will the advanced treatment make the complex potential a sort of "trick" to describe an unstable particle. Sorry, I'm unable to explain it any better, at the moment. :redface:
 
neutrino said:
I did say it was a naive question. To make it clear, will the advanced treatment make the complex potential a sort of "trick" to describe an unstable particle. Sorry, I'm unable to explain it any better, at the moment. :redface:

I am not exactly sure what this 'advanced treatment' actually does...perhaps we need to be directed to a paper/book where it is dealt with rigorously.

Given that the probability integral has an exponential time-dependance, it should be possible to get back a suitable wavefunction without resorting to the trick. If this is possible, it would be interesting to know whether such a wavefunction is unique (not in terms of complex amplitude for normalization) and if not, what class of wavefunctions satisfy such a relation.

My guess is that we need to look at the wavemechanics of radioactive decay...
 
One more question...

When we say, [tex]\tau = \frac{\hbar}{2\Gamma}[/tex], we don't actually take into consideration the nature of the particle. As per this formula, every particle in the given potential will have the same lifetime. Is that correct?
 
neutrino said:
One more question...

When we say, [tex]\tau = \frac{\hbar}{2\Gamma}[/tex], we don't actually take into consideration the nature of the particle. As per this formula, every particle in the given potential will have the same lifetime. Is that correct?

What if the "nature" is absorbed into [itex]\Gamma[/itex]?

EDIT: That's a wild guess.
 
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neutrino said:
One more question...

When we say, [tex]\tau = \frac{\hbar}{2\Gamma}[/tex], we don't actually take into consideration the nature of the particle. As per this formula, every particle in the given potential will have the same lifetime. Is that correct?

To answer one of your previous questions: yes, in a complete (QFT) treatment, the equivalent of th epotentials would be real and the decay of a certain particle would lead to the corresponding creation of other particles with the correct energies, quantum numbers, etc. That's the power of QFT.

For this question: I don't think there is a way in this formalism to describe two particles (even if they have the same decay rate). This is a trick which, (unless I am mistaken and someone else will correct me) will work only to describe one unstable particle. If you had two particles and an imaginary term in the potential, the combined wavefunction would be decaying and there is no way to untangle the decay of one particle vs the other. As far as I can see anyway.
 
  • #10
Messy, isn't it? And that kids, is why we use QFT :biggrin:
 
  • #11
nrqed said:
To answer one of your previous questions: yes, in a complete (QFT) treatment, the equivalent of th epotentials would be real and the decay of a certain particle would lead to the corresponding creation of other particles with the correct energies, quantum numbers, etc. That's the power of QFT.

For this question: I don't think there is a way in this formalism to describe two particles (even if they have the same decay rate). This is a trick which, (unless I am mistaken and someone else will correct me) will work only to describe one unstable particle. If you had two particles and an imaginary term in the potential, the combined wavefunction would be decaying and there is no way to untangle the decay of one particle vs the other. As far as I can see anyway.

Thanks for the clarification, nrqed.

Dimitri Terryn said:
Messy, isn't it? And that kids, is why we use QFT
More reasons to get to QFT ASAP. :biggrin:
 
  • #12
Neutrino, there's a post on QFT prereqs somewhere on the High Energy forum...check it out first.
 
  • #13
Yes, I've been following that for sometime now. But there is still a long way before I get to that point.
 
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Dimitri Terryn said:
Messy, isn't it? And that kids, is why we use QFT :biggrin:

Off Topic: Nice blog there mate. How did you type those equations? I want to put up equations on my blog too (but I am too lazy). Oh and I'm putting a link to your blog on my links page (http://spinor.sitesled.com/ ).
 
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