Can virtual particles become real particles in experiments?

[PeterDonis]

Are the paths real at all given that only one could ever be observed?

No, no path is observed for virtual particles that are internal lines in Feynman diagrams.

 

[PeterDonis]

But they have a different kind of effects, let's call them virtual effects from virtual fields,(like say the line separation in the Lamb shift or the pressure in the Casimir effect), what makes these less real than clicks in a counter, or in the latter case the object that "causes" the click less of a math artifact?

The words "virtual" and "real" in this connection (i.e., referring to internal vs. external lines in Feynman diagrams) IMO are best viewed as technical terms; they're just labels attached to particular mathematical objects. No ontological claims are intended--or at least, using the terminology does not, IMO, require you to commit yourself to any ontological claims. If you don't like the words "virtual" and "real" because they seem to you to imply ontological claims, then just use different words (like "internal lines" vs. "external lines"). The math and the physical predictions are the same.

The distinction between types of effects IMO is a question of what types of effects are reasonably called "particle" effects. A track in a cloud chamber seems like an obvious case of a "particle" effect. A shift in a spectral line or a tiny force between uncharged plates, not so much. This distinction happens to correspond pretty closely with the distinction between internal and external lines in Feynman diagrams, which is why the terms "virtual particle" vs. "real particle" were originally chosen. But both types of effects are certainly real (in the ordinary ontological sense). It's just a question of what label you consider appropriate for the different types of effects.

 

[TrickyDicky]

Can you expand on this? Thanks.

Simply, since it's being claimed that internal lines of Feynman diagrams are mathematical artifacts I just showed a couple of elementary particles of the SM that are always internal lines and that are considered real indirectly by their effects(look up jets and hadronization). Why effects like electric repulsion, spectral line separation or Casimir force don't deserve the same treatment is what I was asking, but the best answerso far is by bhobba:just because.

 

[TrickyDicky]

The words "virtual" and "real" in this connection (i.e., referring to internal vs. external lines in Feynman diagrams) IMO are best viewed as technical terms; they're just labels attached to particular mathematical objects. No ontological claims are intended--or at least, using the terminology does not, IMO, require you to commit yourself to any ontological claims. If you don't like the words "virtual" and "real" because they seem to you to imply ontological claims, then just use different words (like "internal lines" vs. "external lines"). The math and the physical predictions are the same.

Hmmm, all the answers to the OP and ddd123 rest on the idea that something "doesn't exist", period. That looks pretty ontological to me. So your answer is reasonable but doesn't seem to correspond to what is being argued here by most. All the claims have been clearly ontological.

The distinction between types of effects IMO is a question of what types of effects are reasonably called "particle" effects. A track in a cloud chamber seems like an obvious case of a "particle" effect. A shift in a spectral line or a tiny force between uncharged plates, not so much.

That's why I used the word "virtual field", more appropriate to a theory of quantum fields. But honestly, I don't think this is about semantics, it seems to be about ontology.

 

[PeterDonis]

all the answers to the OP and ddd123 rest on the idea that something "doesn't exist", period

That's why I took the trouble to point out the difference in terminology; before you can even ask the ontological question, you have to first be sure what you are asking it about. It's perfectly reasonable to have different answers to the question "do virtual particles exist?" for different interpretations of the term "virtual particle"; for example, one could say that internal lines in Feynman diagrams don't exist (because they are artifacts of a particular model, perturbation theory) but quantum field modes that get excited and register in detectors do exist (because the detectors interact with them). But two people who have those two different viewpoints don't necessarily disagree with each other; they could both be right.

 

[ddd123]

But does this mean that the former camp also believes that quarks and gluons don't really exist?

 

[TrickyDicky]

But does this mean that the former camp also believes that quarks and gluons don't really exist?

Certainly not. But most, at least judging by the "official" position in this site will insist that any internal line in a Feynman diagram(other than those in the SM of elementary particles) doesn't really exist.

 

[PeterDonis]

That's why I used the word "virtual field", more appropriate to a theory of quantum fields.

But the fields are either never "virtual" or always "virtual", depending on how you look at it. They are never directly observable (so always "virtual" in that sense). The expansion in perturbation theory is an expansion of the amplitude in powers of the coupling constant, not powers of the field--the field doesn't even appear (so fields are never "virtual" in that sense).

 

[PeterDonis]

I just showed a couple of elementary particles of the SM that are always internal lines

This is not correct. The correct statement is that quarks and gluons are confined. But confinement does not prohibit you from looking at diagrams that have external quark or gluon lines. For example, the standard diagram for a weak interaction decay has external quark lines (the only internal line at lowest order is the W particle).

One could also argue that perturbation theory doesn't really work for the strong interaction anyway, because the coupling constant is large enough that the higher order terms are as large as the lower order terms. At higher energies, the coupling constant gets weaker, so this argument doesn't apply--but at higher energies, quarks and gluons are no longer confined.

 

[Jilang]

You misunderstand me. If all the paths contribute, but none except one are not observed, are not the unobserved paths virtual by this criterion?

 

[PeterDonis]

If all the paths contribute, but none except one are not observed

This doesn't happen. If all the paths contribute, it's because no path is observed; only the start and end points are observed. If you are actually observing every point along the path, then only that path contributes--just as if, in the double slit experiment, you measure which slit the particle goes through, there is no interference.

 

[TrickyDicky]

But the fields are either never "virtual" or always "virtual", depending on how you look at it. They are never directly observable (so always "virtual" in that sense).

I agree with this. I'm not arguing that "virtual particles" exist, rather that the distinction real vs virtual is basically arbitrary, so that if we decide the latter are mathematical artifacts this applies to the former too, and similarly if it is decided they have an ontological meaning.

The expansion in perturbation theory is an expansion of the amplitude in powers of the coupling constant, not powers of the field--the field doesn't even appear (so fields are never "virtual" in that sense).

I was actually referring to the appearance of the "virtual particles" effects when applying the name "virtual fields", in the sense that is not localized in the way dots in a screen are.
Note in any case that the coupling constant is related to the strength of the interaction, the EM force field in this case although this restricted sense of field is admittedly not the usual sense of field in QFT.

 

[TrickyDicky]

This is not correct. The correct statement is that quarks and gluons are confined. But confinement does not prohibit you from looking at diagrams that have external quark or gluon lines. For example, the standard diagram for a weak interaction decay has external quark lines (the only internal line at lowest order is the W particle).

You mean in the form of hadrons, I was obviously referring to single particles.
But I believe we are arguing the same, the distinction internal-external line is to a great extent arbitrary and with very little bearing on ontology, contrarily to the way is usually or often claimed.

 

[PeterDonis]

You mean in the form of hadrons

No; weak interaction decay diagrams don't show hadrons, they show quarks and leptons. The fact that the quarks involved are bound into hadrons is irrelevant to the diagram, because as far as the weak decay is concerned, the quarks do not behave like bound particles.

the distinction internal-external line is to a great extent arbitrary

Not really. An external line corresponds to a particle that is required to be on the mass shell. An internal line corresponds to a particle that can be off the mass shell--more precisely, it corresponds to an integral over a whole range of possible particles with momenta that are off shell.

 

[ddd123]

How is this interpreted wrt, say, a hydrogen atom? The bound electron doesn't really exchange photons with the proton since they are off shell and are thus only mathematical artifacts?

 

[TrickyDicky]

No; weak interaction decay diagrams don't show hadrons, they show quarks and leptons. The fact that the quarks involved are bound into hadrons is irrelevant to the diagram, because as far as the weak decay is concerned, the quarks do not behave like bound particles.

This only shows again how arbitrary and removed from what is observed can diagrams be drawn.

Not really. An external line corresponds to a particle that is required to be on the mass shell. An internal line corresponds to a particle that can be off the mass shell--more precisely, it corresponds to an integral over a whole range of possible particles with momenta that are off shell.

You probably know that the concept of on vs off the shell is not clear cut in many situations.

 

[PeterDonis]

You probably know that the concept of on vs off the shell is not clear cut in many situations.

Can you give an example?

 

[PeterDonis]

How is this interpreted wrt, say, a hydrogen atom? The bound electron doesn't really exchange photons with the proton since they are off shell and are thus only mathematical artifacts?

That's a possible interpretation, yes. But note carefully what it does not mean. It does not mean the electron is not really bound to the proton. It just means that our model of the binding interaction as being mediated by the exchange of virtual photons is not necessarily "true"; it's just the best we can do at this time. That's because we can't actually solve the equation that describes the binding interaction in closed form; we can only approximate it by a power series expansion in the coupling constant. Since the terms in this series get smaller for higher powers of the coupling constant (at least, they do for this particular interaction), we can compute answers accurately enough to compare with experiment. This is called "perturbation theory", and "virtual particles" are just particular mathematical factors that appear in the various terms of the expansion.

On the "virtual particles aren't real" interpretation, the virtual particles are therefore just artifacts of the particular model we are using; a better model would give us a way to solve the equations in closed form without having to do a power series expansion as an approximation. We know this is possible in principle because there are cases in which we can actually do it--i.e., where we can obtain non-perturbative closed-form solutions.

 

[TrickyDicky]

Can you give an example?

Sure, any "real" particle is always slightly off shell as it is in its way between interactions, in this sense free particles are the ones that "don't exist".
And viceversa you gave the example of how a virtual particle like a quark can be drawn as an external line(on mass as long as we consider them as pairs or triplets) even if it is always confined.

 

[Gerinski]

What about this? In minute 38:00 of his lecture, Krauss says that over 90% of the mass of the proton is due to virtual particles. Does this not make them a real thing?

 

[Vanadium 50]

And that's exactly the problem with trying to learn physics by taking a line here and a line there from different popularizers.

 

[PeterDonis]

any "real" particle is always slightly off shell

No, it isn't. Off shell means it violates the energy-momentum relation. No real particle that's ever been observed does that.

 

[PeterDonis]

In minute 38:00 of his lecture, Krauss says that over 90% of the mass of the proton is due to virtual particles.

He is using "virtual particles" in yet a third sense, not yet used in this thread. What he really means is that over 90% of the mass of the proton is not due to the rest masses of the valence quarks that compose it. "Virtual particles" here is just a label for "all the other stuff".

 

[Nick666]

He actually says "over 90% of the proton mass comes from fluctuations in empty space"

 

[bhobba]

He actually says "over 90% of the proton mass comes from fluctuations in empty space"

That isn't quite what's going on - its more complicated than that:


The trouble with popular explanations, including what I posted, is it is at best a half truth not to be taken literally. Although having seen that video its rather good.

Thanks
Bill

 

[TrickyDicky]

No, it isn't. Off shell means it violates the energy-momentum relation. No real particle that's ever been observed does that.

Apparently you are missing my point. My point is that off-shell and on-shell is a convention of the formalism, and in that sense yes, external lines are defined as on-mass, no in-between case of ever slightly off-shell, and this is a practical formalism as it leads to calculations that result in good approximations to what is observed. But if one is going to make any ontological comment to this, like if that makes them real, or if they really exist or are math artifacts, one has to realize that the on-shell particle of the formalism is not "real" at all, and to be observed it must be considered as off-shell to some degree. Because the completely on-shell particle that appears in the formalism is an idealized entity that comes from infinity and goes to infinity, and you'll admit that what we detect has a finite source, detection and route between source and detection. So we come full circle and conclude that "real" particles are the actual mathematical artifacts which only function is approximate what happens in reality and the "virtual particle" perturbative corrections are what allow us to describe the finite interactions.
So it is always about useful conventions or formalisms, certainly not a debate about virtual vs real, in any case about the contradictory concept of particle itself. It is more than likely that a future theory will completely give up the concept as fundamental.

 

[PeterDonis]

off-shell and on-shell is a convention of the formalism

Off-shell might be considered this way, in the sense that we only integrate over off-shell momenta for internal lines in Feynman diagrams, so if we're not using that formalism, we're not really considering off-shell particles.

But on-shell is not a convention of the formalism, because on-shell particles are actually observed. See below.

to be observed it must be considered as off-shell to some degree

Then please show me the experimental results that have observed off-shell particles.

the completely on-shell particle that appears in the formalism is an idealized entity that comes from infinity and goes to infinity

That doesn't mean actually observed particles are off-shell; it just means that, in this particular formalism, we only know how to extract answers if we let the limits of integration go to infinity. That is a limitation of the formalism that does not in any way correspond to a physical condition on observed particles. The theory most certainly does not say that a particle can only be on-shell if it comes in from minus infinity and goes out to plus infinity.

 

[TrickyDicky]

On-shell particles are defined by the formalism to be the ones we observe as dots,clicks, etc, if there can be anything more conventional you tell me.
Now, have you ever observed a photon on infinite route between asymptotic source and detector? I don't think so. See? We have two contexts here.
"The theory most certainly does not say that a particle can only be on-shell if it comes in from minus infinity and goes out to plus infinity."
We are talking about QFT, right? What does S-matrix say in relation to interacting particles then in your opinion?

 

[PeterDonis]

On-shell particles are defined by the formalism to be the ones we observe as dots,clicks, etc, if there can be anything more conventional you tell me.

So you think direct observables are "conventional"? That's a very...interesting...use of terminology.

have you ever observed a photon on infinite route between asymptotic source and detector?

Irrelevant. See the last paragraph of my post #87.

What does S-matrix say in relation to interacting particles then in your opinion?

See the last paragraph of my post #87. You don't appear to understand what an "approximation" is. S-matrix theory, in which we take the limits of integration to infinity in order to compute matrix elements, is an approximation. Nobody claims that it means particles are only on-shell "at infinity" or that they can only be observed "at infinity".

 

[TrickyDicky]

So you think direct observables are "conventional"? That's a very...interesting...use of terminology.

This would indeed lead to an interesting discussion. Not going to happen.

Irrelevant.

Hmmmm, you are basing your point on direct observability and when I point out to you that you are not actually observing what you are claiming you observe you find it irrelevant, that's amusing.

Nobody claims that it means particles are only on-shell "at infinity" or that they can only be observed "at infinity".

You do. You just don't realize it.
I