B How does quantum tunneling occur without an observer?

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Quantum tunneling can occur without an observer, as it is a fundamental aspect of quantum mechanics where particles can pass through barriers due to their wave-like nature. The discussion highlights that while measurement can collapse a wave function, tunneling itself does not require observation; it is a probabilistic phenomenon described by the wave function's behavior. In the context of nuclear fusion in the Sun, tunneling plays a role because particles can interact and fuse even when their energy levels are insufficient for classical collision, due to quantum probabilities. The conversation also emphasizes that the concept of measurement in quantum mechanics is nuanced and may not directly relate to the physical act of observing. Ultimately, quantum tunneling remains a complex topic that intertwines with interpretations of quantum mechanics and the nature of reality.
  • #31
ITheir behavior transmits information. Other particles receive (observe), process, and react to this information.
When a photon strikes an object, it also collapses the wavefunction. Gravity is the physical result of an observable relationship between two objects. The difference is that humans can translate this relationship, while non-sentient objects can only respond physically and are not consciously "aware" of this relationship, but in the abstract they could still be called observers (receivers)..

Tunnelling indeed involves measurement. If we try to find the position of the electron a large number of times, most of the times it will be found inside the barrier meaning that the state of the quantum mechanical system has collapsed to a state corresponding to the position inside the barrier. Some times the electron will be found outside the barrier also (the number of such measurements depends on the probability given by quantum mechanics.) In this case the state has collapsed to a state corresponding to position outside the barrier. With regard to the sun, we indeed see the sun and experience its effect. This is indeed a measurement. It need not even be direct. For instance, the plants use the energy from the sun and we see the plants growing up. All these are measurements.

Well, that's what I thought in the first place, but everyone is giving me different answers...
 
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  • #32
Tunneling requires something which effectively can be interpreted as "wave function collapse". This means that tunneling requires decoherence, i.e. interaction with a large number of degrees of freedom. Decoherence can also be interpreted as "measurement", but such an interpretation is not essential for understanding of tunneling.
 
  • #33
Demystifier said:
Tunneling requires something which effectively can be interpreted as "wave function collapse". This means that tunneling requires decoherence, i.e. interaction with a large number of degrees of freedom. Decoherence can also be interpreted as "measurement", but such an interpretation is not essential for understanding of tunneling.
Do you have a reference for this linking of decoherence with tunnelling as a requirement? A technical treatment would be good. Thanks!
 
  • #34
e.bar.goum said:
Do you have a reference for this linking of decoherence with tunnelling as a requirement? A technical treatment would be good. Thanks!
I don't know a specific reference for tunneling, but there is a lot of technical literature linking decoherence with apparent "wave unction collapse". On the other hand, from general QM textbooks it should be clear than tunneling is linked with wave function collapse.
 
  • #35
Demystifier said:
I don't know a specific reference for tunneling, but there is a lot of technical literature linking decoherence with apparent "wave unction collapse". On the other hand, from general QM textbooks it should be clear than tunneling is linked with wave function collapse.
I'm very familiar with the former, it's the latter I'm struggling with. Naturally, my quantum texts are in my office, where I am not. If you had a specific reference, that'd be great.
 
  • #36
e.bar.goum said:
I'm very familiar with the former, it's the latter I'm struggling with. Naturally, my quantum texts are in my office, where I am not. If you had a specific reference, that'd be great.
If understood you correctly, it is not clear to you how tunneling is related to wave function collapse, am I right?
 
  • #37
Demystifier said:
If understood you correctly, it is not clear to you how tunneling is related to wave function collapse, am I right?
Right. I can write the Hamiltonian for a particle in a finite square well, isolated from any environment, and the solutions of the TDSE that I find will have portions of the wave function "outside" the barrier - this is what I would term tunnelling. No coupling to the environment is required for these solutions. Thus, I'm confused by your statement.
 
  • #38
e.bar.goum said:
Right. I can write the Hamiltonian for a particle in a finite square well, isolated from any environment, and the solutions of the TDSE that I find will have portions of the wave function "outside" the barrier - this is what I would term tunnelling. No coupling to the environment is required for these solutions. Thus, I'm confused by your statement.
The fact that a portion of the wave function is outside is not yet tunneling. It only means that there is certain probability for tunneling, but the actual tunneling itself may or may not happen. When (and if) the actual tunneling finally happens, then the whole wave function "jumps" outside, not only a portion of it. And how does this jump happen? Clearly, this "jump" must involve an effective "wave function collapse". But we know that "wave function collapse" is closely related to decoherence.
 
  • #39
Demystifier said:
The fact that a portion of the wave function is outside is not yet tunneling. It only means that there is certain probability for tunneling, but the actual tunneling itself may or may not happen. When (and if) the actual tunneling finally happens, then the whole wave function "jumps" outside, not only a portion of it. And how does this jump happen? Clearly, this "jump" must involve an effective "wave function collapse". But we know that "wave function collapse" is closely related to decoherence.
Then this is a terminology issue. To me, what you've said is "in order to know where a particle is, you've got to measure it's location" or "decoherence happens when decoherence happens" which is obvious, and not to me, the same thing at all as saying that decoherence is a requirement for tunneling to occur. I've looked at some literature, and the way I read it is tunneling is phenomenon allowing wave functions to "leak through" potential barriers. Whether or not you then measure that is a separate issue. This is why I asked for some other reference, clearly, I'm not reading what you are.
 
  • #40
The fact that a portion of the wave function is outside is not yet tunneling. It only means that there is certain probability for tunneling, but the actual tunneling itself may or may not happen. When (and if) the actual tunneling finally happens, then the whole wave function "jumps" outside, not only a portion of it. And how does this jump happen? Clearly, this "jump" must involve an effective "wave function collapse". But we know that "wave function collapse" is closely related to decoherence.

Finally...
 
  • #41
Demystifier said:
The fact that a portion of the wave function is outside is not yet tunneling. It only means that there is certain probability for tunneling, but the actual tunneling itself may or may not happen. When (and if) the actual tunneling finally happens, then the whole wave function "jumps" outside, not only a portion of it. And how does this jump happen? Clearly, this "jump" must involve an effective "wave function collapse". But we know that "wave function collapse" is closely related to decoherence.

This line of discussion is getting to be rather puzzling.

There is no "wave function collapse" in tunneling. You set up the schrodinger equation for each region, and all you do is match the boundary conditions. There is no collapse. The wavefunction may change form due to the change in the profile of the potential field, but that's about it. I could easily make the potential barrier into a potential well (i.e. change sign of "V") that the particle has to go through, and nothing would have changed other than the form of the wavefuction.

There is also no "jump". The particle did go through the barrier, not mysteriously appeared on the other side. I can, for instance, add magnetic impurities inside the barrier, which doesn't change the potential height, but merely interacts with the magnetic spins, and I could affect the tunneling current through the barrier (refer to inelastic tunneling in superconductors).

Zz.
 
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  • #42
e.bar.goum and Zapper Z, would you agree that it is standard to say that there is certain probability of tunneling? On the other hand, you seem to say that the presence of tunneling is merely a property of a certain solution of the Schrodinger equation. But I have to remind you that Schrodinger equation is deterministic, so with your definition of tunneling (if I understood your definition correctly), under appropriate initial conditions the tunneling would be a certain thing ocurring with probability equal to 1.
 
  • #43
Juraj said:
Finally...

Juraj: You seem to be giddy in trying to ONLY accept things that appeared (and that's the key word, because I don't believe you understand the physics behind even the ones you THINK agreed with your belief) to match what you like. I asked you to go look up the physics of tunneling, especially in calculating the Reflection and Transmission probabilities, but I don't think you have.

You really, REALLY need to learn the basic physics of tunneling FIRST before jumping into this, and before making any kind of conclusion. For example, look at the Page 2 of this link that shows exactly what I had asked for. Look at it carefully. Where, do you think, is there any "collapse" of anything in the physics?

You do not have to buy into what I say, but you owe it to yourself to learn something that is valid, not simply latch onto something that suits your needs, whatever those are. I spent 4 of the best years of my life in graduate school studying this phenomenon inside-out, AND also performed experiments on this. I'm no stinking amateur with respect to this physics.

This is the last time I will attempt to steer you into trying to make you understand why what you have stated is WRONG. I can only lead you to water, not force you to drink.

Zz.
 
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  • #44
Demystifier said:
e.bar.goum and Zapper Z, would you agree that it is standard to say that there is certain probability of tunneling? On the other hand, you seem to say that the presence of tunneling is merely a property of a certain solution of the Schrodinger equation. But I have to remind you that Schrodinger equation is deterministic, so with your definition of tunneling (if I understood your definition correctly), under appropriate initial conditions the tunneling would be a certain thing ocurring with probability equal to 1.

I don't understand this paragraph at all. Start from the very beginning with what we dealt with in intro QM. We have a square potential barrier. Why would the tunneling probability be 1? And what does the tunneling probability have anything to do with wavefunction collapse? And what value is being "collapsed"?

Zz.
 
  • #45
Demystifier said:
e.bar.goum and Zapper Z, would you agree that it is standard to say that there is certain probability of tunneling? On the other hand, you seem to say that the presence of tunneling is merely a property of a certain solution of the Schrodinger equation. But I have to remind you that Schrodinger equation is deterministic, so with your definition of tunneling (if I understood your definition correctly), under appropriate initial conditions the tunneling would be a certain thing ocurring with probability equal to 1.
1. Yes. 2. I don't see how that follows.
 
  • #46
ZapperZ said:
I don't understand this paragraph at all. Start from the very beginning with what we dealt with in intro QM. We have a square potential barrier. Why would the tunneling probability be 1? And what does the tunneling probability have anything to do with wavefunction collapse? And what value is being "collapsed"?
You are right that we have to start from the beginning with what we dealt with in intro QM. But before mentioning tunneling, a good introductory book will first tell you that psi-squared represents the probability for electron to be at a certain position. And perhaps it will also tell you that attending a definite position has something to do with the collapse of the wave function into a position eigenstate. I hope it answers your questions.
 
  • #47
Demystifier said:
You are right that we have to start from the beginning with what we dealt with in intro QM. But before mentioning tunneling, a good introductory book will first tell you that psi-squared represents the probability for electron to be at a certain position. And perhaps it will also tell you that attending a definite position has something to do with the collapse of the wave function into a position eigenstate. I hope it answers your questions.

No, it doesn't, because you didn't answer my question.

So psi-squared tells you that probability. But it doesn't tell you that a measurement has been made! It only tells you that IF you make a measurement, this is the chance you'll find the electron there! There is no such measurement done in tunneling experiments.

Now, how about you answer MY questions?

Zz.
 
  • #48
ZapperZ said:
So psi-squared tells you that probability. But it doesn't tell you that a measurement has been made! It only tells you that IF you make a measurement, this is the chance you'll find the electron there! There is no such measurement done in tunneling experiments.
Of course there is. In tunneling experiments there is an apparatus that detects the particle (otherwise how would an experimentalist know that tunneling happened?). This detector certainly detects the particle at some (more or less sharp) position.
 
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  • #49
Juraj said:
Finally...
I am glad that least the thread starter got the answer he wanted. :smile:
 
  • #50
Demystifier said:
Of course there is. In tunneling experiments there is an apparatus that detects the particle (otherwise how would an experimentalist know that tunneling happened?). This detector certainly detects the particle at some (more or less sharp) position.

But all you're saying there is that in order to make a measurement of location, you have to make a measurement of location. That's not telling you anything about the phenomenon.
 
  • #51
e.bar.goum said:
But all you're saying there is that in order to make a measurement of location, you have to make a measurement of location. That's not telling you anything about the phenomenon.
It looks as if you think that a particle attains its location (say outside) even if nothing measures it. But unless you accept the Bohmian interpretation of QM, it is wrong. In standard QM, the particle does not have a position if nothing measures it. In other words, the measurement is an essential part of the phenomenon. This is called contextuality of QM.
 
  • #52
Juraj: You seem to be giddy in trying to ONLY accept things that appeared (and that's the key word, because I don't believe you understand the physics behind even the ones you THINK agreed with your belief) to match what you like. I asked you to go look up the physics of tunneling, especially in calculating the Reflection and Transmission probabilities, but I don't think you have.

You really, REALLY need to learn the basic physics of tunneling FIRST before jumping into this, and before making any kind of conclusion. For example, look at the Page 2 of this link that shows exactly what I had asked for. Look at it carefully. Where, do you think, is there any "collapse" of anything in the physics?

You do not have to buy into what I say, but you owe it to yourself to learn something that is valid, not simply latch onto something that suits your needs, whatever those are. I spent 4 of the best years of my life in graduate school studying this phenomenon inside-out, AND also performed experiments on this. I'm no stinking amateur with respect to this physics.

This is the last time I will attempt to steer you into trying to make you understand why what you have stated is WRONG. I can only lead you to water, not force you to drink.

Zz.
The assumption you are making that I'm someone who will hold on my beliefs not matter what is entirely wrong. It seems you interpreted my words as provocative, but that was merely a way of saying that I'm relieved for not being alone with this understanding, right or wrong. And for the record, I will spend my couple of days reading about tunneling to fullfill and correct my understanding, because obviously, everyone here has different opinion, while science is defined by facts
 
  • #53
Demystifier said:
It looks as if you think that a particle attains its location (say outside) even if nothing measures it. But unless you accept the Bohmian interpretation of QM, it is wrong. In standard QM, the particle does not have a position if nothing measures it. In other words, the measurement is an essential part of the phenomenon. This is called contextuality of QM.
If that's your reading of my position, them we have failed to communicate. I've said nothing about the definite location of any particle.
 
  • #54
Demystifier said:
Of course there is. In tunneling experiments there is an apparatus that detects the particle (otherwise how would an experimentalist know that tunneling happened?). This detector certainly detects the particle at some (more or less sharp) position.

Can you show me where exactly in the physics where it shows a position measurement? Use the link I have earlier on the potential barrier.

Experimentalists (like me), measured no such thing, because we often measure the tunneling current. Nowhere in the physics, or in the data, is there ANY information about where the particle was along its longitudinal direction or transverse direction.

Zz.
 
  • #55
e.bar.goum said:
If that's your reading of my position, them we have failed to communicate. I've said nothing about the definite location of any particle.
So can you rephrase your position?
 
  • #56
ZapperZ said:
Experimentalists (like me), measured no such thing, because we often measure the tunneling current.
I am a theoretician, and I don't know how exactly you measure this current. But I am convinced that you measure the current at some position (e.g. the position where your ampermeter is connected with the wire conducting the current). Obviously, that position is also the position of the particles that carry this current.
 
  • #57
Demystifier said:
So can you rephrase your position?
I could, but I'm on my way to bed. ;) ZapperZ seems to be on the same wavelength as me, if this is still going in 9 hours or so, I'll jump back in.

In very few words- tunnelling is a phenomenon associated with ##\Psi##, not with <##x##>.
 
  • #58
Demystifier said:
I am a theoretician, and I don't know how exactly you measure this current. But I am convinced that you measure the current at some position. Obviously, that position is also the position of the particles that carry this current.

I measured the current using a large glob of electrode. If you think something the size of 2 mm by 2 mm as a "position" measurement, then you have a generous phase space for quantum effects. Besides, this is measured on the surface of the conductor, not at the tunnel junction. If you call this collapse, then the collapse happened OUTSIDE of it, not where all the action was taking place, i.e. at the tunnel junction.

Maybe you ought to get out of your office and see how experiments are done now and then to get some sense of reality.

Zz.
 
  • #59
e.bar.goum said:
In very few words- tunnelling is a phenomenon associated with Ψ
I agree. The crucial question is: does the change of Ψ involve a collapse?
 
  • #60
Demystifier said:
I agree. The crucial question is: does the change of Ψ involve a collapse?

And I've been asking you to show this from the very beginning.

I could start with a superposition of plane waves. They then go through the barrier. AFTER the barrier, I STILL get a superposition of those plane waves! The only thing that is different is the AMPLITUDE of the wave function. So where is the "collapse"?

Zz.
 

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