Probability of quantum tunnelling

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Discussion Overview

The discussion revolves around the concept of quantum tunneling, particularly focusing on the conditions under which an electron can be said to have successfully tunneled through a barrier. Participants explore the implications of quantum mechanics, wavefunctions, and the role of probability in tunneling events, as well as the connection to real-world applications such as nuclear decay and fission bombs.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether an electron can be said to have definitely tunneled through a barrier or if it is merely a matter of probability, referencing the wavefunction and its potential collapse upon observation.
  • Another participant discusses the tunneling matrix element and the density of states as factors that govern the probability of tunneling, suggesting that tunneling is more common than often perceived.
  • A participant uses an analogy comparing an electron to a bullet encountering a wooden box, emphasizing the probabilistic nature of outcomes in both scenarios and the wave properties affecting tunneling.
  • There is a suggestion to simplify the discussion by using a common undergraduate quantum mechanics example of a free particle encountering a square potential barrier to clarify the concepts involved.
  • The original poster reiterates their focus on quantum mechanics by linking their question to the example of a fission bomb and its relation to quantum tunneling.

Areas of Agreement / Disagreement

Participants express differing views on the nature of quantum tunneling, particularly regarding the role of probability and the conditions for definitively stating that tunneling has occurred. There is no consensus on these points, and the discussion remains unresolved.

Contextual Notes

Participants highlight the complexity of quantum tunneling and its dependence on various factors, including the interpretation of quantum mechanics and the specifics of the systems being analyzed. There are unresolved aspects regarding the implications of tunneling in practical applications, such as nuclear decay.

Who May Find This Useful

This discussion may be of interest to those studying quantum mechanics, particularly in relation to tunneling phenomena, as well as individuals exploring the implications of quantum theory in practical applications like nuclear physics.

eehiram
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I'm continuing to read Jim Al-Khalili's book Quantum: A Guide for the Perplexed. I'm on page 190; today I just read a few paragraphs and page 176 about quantum tunnelling.

My question is this: what does it take to say that an electron, for example, has successfully and definitely tunnelled through a barrier? Or is there only the probability function of having done so?

Jim Al-Khalili explained quantum tunnelling in terms of the wavefunction. Does the wave function need to be collapsed by way of observation (a la Copenhagen interpretation) for the electron to definitely exist on the other side of the barrier?

I was thinking that if quantum tunnelling only occurs in terms of probability, then what happens after tunnelling becomes likely? Must we keep making our calculations using probability of quantum tunnelling to determine what the electron does on the other side of the barrier to interact with whatever is there? Is this to be added to and added to successively with each further interaction that takes place?

I would think perhaps not: One of the consequences of quantum tunnelling is decay of a nucleus, such as what happens in a fission bomb. Does the decay actually take place for sure, leading to the chain reaction that then detonates the fission bomb, or is it simply likely to occur? If so, then how does the fission bomb definitely detonate?

I bring this up because I know the fission bomb does really detonate -- for sure. (Of course, sometimes fission bombs are duds, which I think might have to do with the probability of nuclear decay.)
 
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My question is this: what does it take to say that an electron, for example, has successfully and definitely tunnelled through a barrier? Or is there only the probability function of having done so?

Jim Al-Khalili explained quantum tunnelling in terms of the wavefunction. Does the wave function need to be collapsed by way of observation (a la Copenhagen interpretation) for the electron to definitely exist on the other side of the barrier?

I was thinking that if quantum tunnelling only occurs in terms of probability, then what happens after tunnelling becomes likely? Must we keep making our calculations using probability of quantum tunnelling to determine what the electron does on the other side of the barrier to interact with whatever is there? Is this to be added to and added to successively with each further interaction that takes place?

These are quite confusing, and I have worked in tunneling!

Tunneling is described by (i) the tunneling matrix element that describes the probability of going from one state from one side of the barrier to the state on the other side of the barrier and (ii) the density of states of the initial state and the final state. Both of these factors govern the total probability of tunneling.

Note that tunneling isn't that exotic, and occurs more often than the examples you cited for nuclear processes. Tunneling is a diagnostic technique to study solids such as superconductors (I've highlighted an article on the progress in tunneling spectroscopy in superconductors in the Solid state forum). It is also use for imaging as in STM.

Zz.
 
as a simple example let's take in the place of the electron a bullet and in case of the barrier there is abox of wood... the bullet may just hit and fall on the box ...or it may hit and get into the box or hit the box and get through and be out ...there is probabilities for eeach case and the same with the electron... and because of the wave duality the barrier effect on its wave propereties that's why the wave decay when it tunnels till infinity...am i right?
 
moe_3_moe said:
as a simple example let's take in the place of the electron a bullet and in case of the barrier there is abox of wood... the bullet may just hit and fall on the box ...or it may hit and get into the box or hit the box and get through and be out ...there is probabilities for eeach case and the same with the electron... and because of the wave duality the barrier effect on its wave propereties that's why the wave decay when it tunnels till infinity...am i right?

Try something even simpler. Use the common example done in undergrad QM text - a free particle encountering a square potential barrier. Now, use that and ask your question.

Zz.
 
I used the example of an electron and a fission bomb

Therefore, my question is firmly placed in the realm of QM.

o| Hiram
 

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