Massive gauge bosons in QFT in/out states

In summary, the conversation discusses the presence of massive gauge bosons (W and Z) in the external legs of Feynman diagrams and their existence as real particles. While it is possible to observe tracks of W and Z bosons in bubble or cloud chambers, their finite half-life and resonance nature make them restricted to internal legs of Feynman diagrams and not asymptotic in/out states. Additionally, the conversation touches on the difference between resonances and virtual particles, and the potential for particles to appear differently in different theories.
  • #1
Michael Price
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TL;DR Summary
Are the massive gauge bosons of electroweak theory (W, Z) permitted in the external legs of Feynman diagrams?
Because massive gauge bosons have a finite half life, are they excluded from the (infinitely, asymptotically remote?) in and out states of QFT? Or, to put it another way, are they restricted to the internal legs of Feynman diagrams, i.e. to being virtual only? We can see W and Z tracks in bubble or cloud chambers, is this sufficient to guarantee their "real" existence?
 
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  • #2
Michael Price said:
We can see W and Z tracks in bubble or cloud chambers, is this sufficient to guarantee their "real" existence?

For most people's definition of "real", this would seem to be sufficient, yes. :wink:
 
  • #3
Michael Price said:
We can see W and Z tracks in bubble or cloud chambers

I don't think we can.
 
  • #5
AFAIK they plotted "Lego diagrams" for electron-positron pairs from the decay of Z bosons using em. calorimeters. The Z-bosons are resonances and thus not asymptotic free states. You see them as peaks in invariant-mass plots of dileptons (electron-positron, or muon-antimuon pairs) in reactions like ##\text{hadrons} \rightarrow \ell^+ + \ell^- + X##.

For details on how the weak gauge bosons have been discovered, see Rubbia's Nobel lecture:

https://www.nobelprize.org/uploads/2018/06/rubbia-lecture.pdf
 
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  • #6
vanhees71 said:
AFAIK they plotted "Lego diagrams" for electron-positron pairs from the decay of Z bosons using em. calorimeters. The Z-bosons are resonances and thus not asymptotic free states. You see them as peaks in invariant-mass plots of dileptons (electron-positron, or muon-antimuon pairs) in reactions like ##\text{hadrons} \rightarrow \ell^+ + \ell^- + X##.

For details on how the weak gauge bosons have been discovered, see Rubbia's Nobel lecture:

https://www.nobelprize.org/uploads/2018/06/rubbia-lecture.pdf
I was thinking more of the charged W bosons. Being charged, should they not leave tracks?
 
  • #7
Hm, the W has a decay width of about ##\Gamma \simeq 2 \; \text{GeV}##. It's mean lifetime thus is ##1/\Gamma \simeq 0.2 \mathrm{GeV} \mathrm{fm}/(2 \mathrm{GeV}) =0.1 \text{fm}##. Thus it would leave a track of at most ##0.1 \; \text{fm} =10^{-16} \text{m}##, which is pretty hard to observe ;-)).
 
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  • #8
vanhees71 said:
Hm, the W has a decay width of about ##\Gamma \simeq 2 \; \text{GeV}##. It's mean lifetime thus is ##1/\Gamma \simeq 0.2 \mathrm{GeV} \mathrm{fm}/(2 \mathrm{GeV}) =0.1 \text{fm}##. Thus it would leave a track of at most ##0.1 \; \text{fm} =10^{-16} \text{m}##, which is pretty hard to observe ;-)).
Hah, I was about do the same calculation but you beat me to it. Yes, pretty hard to observe... in principle observable, though.
 
  • #9
Michael Price said:
... in principle observable, though.

Oh dear. This is going to be one of those threads.

Can we agree that a bubble or cloud chamber track can be no shorter than a single atom? What is the size of an atom compared to a track?
 
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  • #10
Vanadium 50 said:
Oh dear. This is going to be one of those threads.

Can we agree that a bubble or cloud chamber track can be no shorter than a single atom? What is the size of an atom compared to a track?
Well, let's put it back on track then; can W and Z states appear in the asymptotic in/out states in QFT? Seems to me they can. What do you think?
 
  • #11
No they can't since they are decaying! A resonance is a resonance is a resonance...
 
  • #12
Michael Price said:
Summary: Are the massive gauge bosons of electroweak theory (W, Z) permitted in the external legs of Feynman diagrams?

i.e. to being virtual only?
As has been said they won't because they are resonances. However being a resonance is not the same thing as a virtual particle. Resonances correspond to states in the Hilbert space, just not ones that survive to asymptotic infinity. Virtual lines however don't correspond to any element of the Hilbert space, they're purely part of a term in the perturbative expansion.
 
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  • #13
DarMM said:
As has been said they won't because they are resonances. However being a resonance is not the same thing as a virtual particle. Resonances correspond to states in the Hilbert space, just not ones that survive to asymptotic infinity. Virtual lines however don't correspond to any element of the Hilbert space, they're purely part of a term in the perturbative expansion.
Would a U238 atom appear in an in/out state? I presume yes, but how does that differ from a W boson?
 
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  • #14
Strictly speaking not ;-)). Of course, an U238 atom lives "a bit" longer than the W boson though...
 
  • #15
Michael Price said:
Would a U238 atom appear in an in/out state? I presume yes, but how does that differ from a W boson?
It wouldn't. Of course these things can be theory dependent. A particle could be stable in one theory, but a resonance in a more extensive theory that includes more of its interactions.
 
  • #16
So a U238 atom can't appear in an asymptotic in/out state?
Okay, I always suspected that the in/out states were mythical and that it is the virtual particles that comprise reality...
 
  • #17
Michael Price said:
So a U238 atom can't appear in an asymptotic in/out state?
Okay, I always suspected that the in/out states were mythical and that it is the virtual particles that comprise reality...
The in/out states aren't mythical, they're the particles that survive to asymptotic infinity.

Also U238 and the W bosons aren't virtual but resonances, that's the point I was making in #12. There's a difference between resonances and internal virtual lines in graphs.
 
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  • #18
Which difference? Do mean that resonances are discovered in s-channel contributions, when measuring invariant-mass spectra of "their decay products"?
 
  • #19
vanhees71 said:
Which difference? Do mean that resonances are discovered in s-channel contributions, when measuring invariant-mass spectra of "their decay products"?
Virtual lines are just terms in the perturbative expansion. Resonances are actual states in the Hilbert space. In other words resonances would appear in a non-perturbative formulation, virtual particles would not.
 
  • #20
Virtual particles do not correspond to states. See https://www.physicsforums.com/insights/physics-virtual-particles/, where the difference to unstable particles and resonances is explained.
DarMM said:
Resonances correspond to states in the Hilbert space, just not ones that survive to asymptotic infinity.
Small correction: Resonances do not correspond to states in the Hilbert space but to unnormalizable states in the dual of a nuclear space whose completion is the Hlbert space.
 
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  • #21
Michael Price said:
So a U238 atom can't appear in an asymptotic in/out state?
Not in the standard expansion. But one can analytically continue the standard expansion into asymptotic states (more precisely, the scalar product and the Möller operator). By deforming the integration contour in the scalar product (in a representation of the asymptotic space where the energy is diagonal) from the real line into the so-called unphysical sheet (of the Riemann surface associated with the resolvent), one gets an expansion in terms of long-living resonances.

If the half-life is very long (such as for U238), hardly any deformation is needed and one can approximate the contour by the real line, thus getting an approximate expansion in which the decay is neglected. But for short-lived resonances such as W or Z, the deformation of the contour is very substantial and the approximation bcomes ridiculously poor.

On the other hand, virtual particles can in no way be approximated in this sense.
 
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  • #22
A. Neumaier said:
Virtual particles do not correspond to states. See https://www.physicsforums.com/insights/physics-virtual-particles/, where the difference to unstable particles and resonances is explained.

Small correction: Resonances do not correspond to states in the Hilbert space but to unnormalizable states in the dual of a nuclear space whose completion is the Hlbert space.

As a reference for the second part, one just has to look for "Gamov vectors" (the Americans spell Gamow) and the work of Arno Böhm and his coworkers. The standard work on rigged Hilbert spaces (the PhD thesis of Rafael de la Madrid) has a chapter on Gamov vectors, as far as I remember.
 
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  • #23
A. Neumaier said:
Small correction: Resonances do not correspond to states in the Hilbert space but to unnormalizable states in the dual of a nuclear space whose completion is the Hlbert space.
I just want to understand this better. So if we take a reasonably long lived particle like a free neutron, ultimately it is still a resonance. What's going on during those ~15 minutes? Surely there is a state representing what is occurring in some manner. Or do you mean there is no state directly corresponding to the resonance pole on the second sheet of the S-matrix's analytic continuation.
 
  • #24
DarMM said:
Virtual lines are just terms in the perturbative expansion. Resonances are actual states in the Hilbert space. In other words resonances would appear in a non-perturbative formulation, virtual particles would not.
Resonances are indeed states in the continuous-spectrum part of the Hamiltonian. The most simple example from QM 1 is a particle moving in a finite-depth attractive potential pot in 1 dimension:

https://itp.uni-frankfurt.de/~hees/qm1-ss09/wavepack/node19.html

In QFT it's an internal line in a Feynman diagram (in the case that the corresponding "particles" are described as an elementary field in the Lagrangian). As such it's as "virtual" as any internal line in a Feynman diagram. More generally, it's a complex pole in the energy argument of some Green's function. E.g., in the pion-nucleon elastic scattering amplitude you have some prominent resonances like the Δ(1232)Δ(1232).

There's a lot of confusion about what a resonance really is, leading sometimes to long debates. E.g., "what's a ρρ meson"? According to the particle data group, it's a strong resonance state in the process e++e−→π++π−e++e−→π++π−. Then it has a well-defined mass and width of around 770MeV770MeV and 150MeV150MeV respectively. So looking at it in the point of view of hadron physics, you'd say "it's a two-pion resonance". Of course you see the corresponding peak also in the corresponding spin-isospin channel in elastic ππππ scattering. Now you build a model of pions, ρρ mesons and couple some baryons too. Now you can easily populate "ρρ-meson states" below the two-pion threshold in reactions like πN→ρNπN→ρN. There's a phenomenolgically quite well working model, where all couplings of leptons to hadrons go only through ligth vector mesons (it's by Sakurai from the 60ies and known as the vector-meson dominance model). Now building such a model for dielectron production, you all of a sudden see a "modified ρρ-meson lineshape" just from coupling the baryons on top of the pions to the ρρ meson. In other words: What's a ρρ meson is in some sense model dependent. You can as well use another effective model describing the hadron physics and take care of some dielectron production channels through other "mechanisms", which maybe work as well. What you can at the end only measure is how some incoming hadrons react somehow and produce a dielectron pair. Whether or not you identify certain structures in the dielectron-invariant-mass spectrum as a "##\rho##-meson" is a question of your interpretation in terms of some effective model. That's why it's in general not consistent to just mix "resonances" from different models into a new model. You have to carefully fit all the parameters (couplings, masses, etc.) to the model you are using since you can shuffle strength of the same scattering processes to run through different resonances, and there are tons of hadron resonances around, whose branching ratios to various decay channels are not well known. Thus there's a lot of freedom in modeling, and with new data from experiments it may well be that you have to refit your model!
 
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  • #25
vanhees71 said:
In QFT it's an internal line in a Feynman diagram (in the case that the corresponding "particles" are described as an elementary field in the Lagrangian). As such it's as "virtual" as any internal line in a Feynman diagram
I agree that's how it appears in the perturbative formalism. My point to @Michael Price was more that this is simply a perturbative representation and you shouldn't think of virtual particles actually flying about.
 
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  • #26
vanhees71 said:
Resonances are indeed states in the continuous-spectrum part of the Hamiltonian. [...]

In QFT it's an internal line in a Feynman diagram (in the case that the corresponding "particles" are described as an elementary field in the Lagrangian). As such it's as "virtual" as any internal line in a Feynman diagram.
No. Resonances are definitely not internal lines in a Feynmn diagram, since the latter have arbitrary real 4-momentum and no associated states, while resonances have complex 4-momentum and unnormalized states.

DarMM said:
I just want to understand this better. So if we take a reasonably long lived particle like a free neutron, ultimately it is still a resonance. What's going on during those ~15 minutes? Surely there is a state representing what is occurring in some manner. Or do you mean there is no state directly corresponding to the resonance pole on the second sheet of the S-matrix's analytic continuation.
There is no normalizable state directly corresponding to the resonance pole on the second sheet of the S-matrix's analytic continuation. But there are wave packets made from the energy eigenstates with energies in the region that approximate the resonance state. This shows in a modified short time behavior - unlike normalizable states, resonances decay purely exponentially at all times (which is impossible at times before preparation).
 
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  • #27
I didn't claim that there's a normalizable state for a resonance. Of course with "internal line" for a resonance you have to take a dressed line, i.e., you have to sum the Dyson equation for it, because otherwise you don't get a pole in the complex energy plane to begin with. Sorry that I forgot this detail ;-).
 
  • #28
DarMM said:
I agree that's how it appears in the perturbative formalism. My point to @Michael Price was more that this is simply a perturbative representation and you shouldn't think of virtual particles actually flying about.
Well, that is exactly how I do think of a virtual particle, namely as something flying about. If seems to me that it is the asymptotic in/out states that are fictions. Everything happens inside Feynman diagrams, not on the fictional asymptotic edges.
 
  • #29
Feynman diagrams are mathematical formulae in an ingeniously efficient notation, and their meaning in usual "vacuum QFT" is that they provide transition-matrix elements between asymptotic free in and out states.

Then there are also parts of such diagrams, which refer not directly to observable quantities but are building blocks to calculate systematically the transition-matrix elements. These are the proper vertex functions (one-particle-irreducible diagrams) which are evaluated, including renormalization and all that and then used finally in the diagrams describing S-matrix elements.

A "particle" interpretation however only the asymptotic free states have, and already in QED these are in fact quite complicated beasts due to the the long-range em. interaction!
 
  • #30
Michael Price said:
Well, that is exactly how I do think of a virtual particle, namely as something flying about. If seems to me that it is the asymptotic in/out states that are fictions. Everything happens inside Feynman diagrams, not on the fictional asymptotic edges.
This is untenable to me because the asymptotic particles are what actually registers in our detectors and virtual particles don't even appear in a non-perturbative formalism and depending on how you perform the perturbative expansion you get virtual particles with different properties.
 
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  • #31
DarMM said:
This is untenable to me because the asymptotic particles are what actually registers in our detectors and virtual particles don't even appear in a non-perturbative formalism and depending on how you perform the perturbative expansion you get virtual particles with different properties.
Particles also change with gauge transformations, but we have learned to get used to that. But to return to the asymptotic business. I can pick up a U238 atom and mail to someone on the other side of the world - clearly there is more to reality than asymptotic in/out states.
 
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  • #32
Michael Price said:
Particles also change with gauge transformations, but we have learned to get used to that. But to return to the asymptotic business. I can pick up a U238 atom and mail to someone on the other side of the world - clearly there is more to reality than asymptotic in/out states.
I never said there wasn't, I said:
  1. The asymptotic states are real, i.e. they're not fictions.
  2. Virtual particles are not part of reality as they only appear in the perturbative formalism.
What particles change with gauge transformations?
 
  • #33
Michael Price said:
Particles also change with gauge transformations, but we have learned to get used to that. But to return to the asymptotic business. I can pick up a U238 atom and mail to someone on the other side of the world - clearly there is more to reality than asymptotic in/out states.
No! Nothing changes with gauge transformations. To the contrary gauge transformations simply transform from one description of a situation to another complete equivalent one. That's why there's no spontaneous symmetry breaking possible for a local gauge symmetry, and that's why the ground state is not degenerate, and that's why in breaking a local gauge symmetry doesn't imply the existence of Goldstone modes.

What, in your opinion is a U238 atom else, in the quantum description, than an asymptotic free state?
 
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  • #34
vanhees71 said:
No! Nothing changes with gauge transformations. To the contrary gauge transformations simply transform from one description of a situation to another complete equivalent one. That's why there's no spontaneous symmetry breaking possible for a local gauge symmetry, and that's why the ground state is not degenerate, and that's why in breaking a local gauge symmetry doesn't imply the existence of Goldstone modes.

What, in your opinion is a U238 atom else, in the quantum description, than an asymptotic free state?
I agree, nothing measurable changes with a gauge transformation, but I don't want to get diverted off-topic here. To return to the U238 (or W boson) I got the distinct impression that some people are saying the U238 does not appear in an asymptotic state.
 
  • #35
Of course it does. Why shouldn't it? It's well observable after all!
 
<h2>1. What are massive gauge bosons in QFT in/out states?</h2><p>Massive gauge bosons in QFT (Quantum Field Theory) refer to particles that mediate the fundamental forces of nature, such as the electromagnetic force, strong nuclear force, and weak nuclear force. These particles have mass and carry a specific type of charge, such as electric charge or color charge. In/out states in QFT refer to the initial and final states of a particle interaction, where the particles are considered to be well-separated and free.</p><h2>2. How are massive gauge bosons described in QFT?</h2><p>In QFT, massive gauge bosons are described using the Standard Model, which is a mathematical framework that explains the interactions between particles and their properties. These particles are represented as excitations of their respective quantum fields, and their behavior is governed by the principles of quantum mechanics.</p><h2>3. What is the role of massive gauge bosons in the Standard Model?</h2><p>The Standard Model describes the interactions between particles through the exchange of gauge bosons. These particles are responsible for carrying the fundamental forces and are crucial in explaining the behavior of matter at the subatomic level. Without the inclusion of massive gauge bosons, the Standard Model would not accurately describe the behavior of particles.</p><h2>4. How are massive gauge bosons observed and measured?</h2><p>Massive gauge bosons can be observed and measured using high-energy particle accelerators, such as the Large Hadron Collider (LHC) at CERN. By colliding particles at high speeds, scientists can recreate the conditions of the early universe and study the behavior of particles, including massive gauge bosons. The properties of these particles, such as their mass and charge, can be measured through their interactions with other particles.</p><h2>5. What is the significance of studying massive gauge bosons in QFT?</h2><p>Studying massive gauge bosons in QFT is essential for understanding the fundamental forces of nature and the behavior of matter at the subatomic level. It also plays a crucial role in the development of new theories and models in physics, as well as in technological advancements, such as particle accelerators and medical imaging techniques. Additionally, studying massive gauge bosons can provide insights into the early universe and help us understand the origins of the universe.</p>

1. What are massive gauge bosons in QFT in/out states?

Massive gauge bosons in QFT (Quantum Field Theory) refer to particles that mediate the fundamental forces of nature, such as the electromagnetic force, strong nuclear force, and weak nuclear force. These particles have mass and carry a specific type of charge, such as electric charge or color charge. In/out states in QFT refer to the initial and final states of a particle interaction, where the particles are considered to be well-separated and free.

2. How are massive gauge bosons described in QFT?

In QFT, massive gauge bosons are described using the Standard Model, which is a mathematical framework that explains the interactions between particles and their properties. These particles are represented as excitations of their respective quantum fields, and their behavior is governed by the principles of quantum mechanics.

3. What is the role of massive gauge bosons in the Standard Model?

The Standard Model describes the interactions between particles through the exchange of gauge bosons. These particles are responsible for carrying the fundamental forces and are crucial in explaining the behavior of matter at the subatomic level. Without the inclusion of massive gauge bosons, the Standard Model would not accurately describe the behavior of particles.

4. How are massive gauge bosons observed and measured?

Massive gauge bosons can be observed and measured using high-energy particle accelerators, such as the Large Hadron Collider (LHC) at CERN. By colliding particles at high speeds, scientists can recreate the conditions of the early universe and study the behavior of particles, including massive gauge bosons. The properties of these particles, such as their mass and charge, can be measured through their interactions with other particles.

5. What is the significance of studying massive gauge bosons in QFT?

Studying massive gauge bosons in QFT is essential for understanding the fundamental forces of nature and the behavior of matter at the subatomic level. It also plays a crucial role in the development of new theories and models in physics, as well as in technological advancements, such as particle accelerators and medical imaging techniques. Additionally, studying massive gauge bosons can provide insights into the early universe and help us understand the origins of the universe.

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