Energy conservation concerns in the weak interaction

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Discussion Overview

The discussion revolves around the weak interaction, specifically the transformation of quarks and the nature of virtual particles. Participants explore the implications of quark transitions, the role of carrier bosons, and the concept of virtual particles within quantum field theory.

Discussion Character

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

Main Points Raised

  • Some participants question whether a u quark can turn into a d quark via the weak interaction and how the mass/energy shortfall is accounted for.
  • There is a discussion on the nature of virtual particles, with some suggesting they are akin to a tunneling effect, while others argue they are mathematical constructs used in perturbation theory.
  • One participant asserts that in radioactive decays, only virtual W bosons are involved, not real particles.
  • Another participant emphasizes that quarks do not exist in isolation and that context, such as within a nucleon, is crucial for understanding these processes.
  • Some participants express uncertainty about the interpretation of virtual particles, with one stating that they are confusing buzzwords for propagators in Feynman diagrams.
  • There is a mention of alternative calculation methods that do not involve virtual particles, such as lattice calculations.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and disagreement, particularly regarding the nature of virtual particles and the mechanisms of quark transformation. No consensus is reached on these topics, and multiple competing views remain present.

Contextual Notes

Participants highlight limitations in understanding virtual particles and their role in calculations, as well as the dependence on specific contexts for quark interactions. The discussion reflects ongoing uncertainties and varying interpretations within the field.

Asgrrr
I have a few questions:

Can a u quark turn into a d quark (heavier) via the weak interaction? If so, how is the mass/energy shortfall made up?

How can the (supermassive) carrier bosons (W, Z) be called into being? Where does the energy come from? Or is the energy bill unpaid because they are virtual particles, on the verge of existence? Is it akin to a tunneling effect?

Thank you.
 
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Quarks don't exist as isolated objects. There is no u->d process without "context".
Asgrrr said:
How can the (supermassive) carrier bosons (W, Z) be called into being?
In radioactive decays: They don't. There are just virtual W, not real particles.
In particle accelerators: We give the particles enough energy.
 
mfb said:
Quarks don't exist as isolated objects. There is no u->d process without "context".

The context is within a nucleon in a nucleus, e.g. electron capture.
 
mfb said:
.In radioactive decays: They don't. There are just virtual W, not real particles.

Thank you. I already had that. I guess I could just write "they are not real" but that seems to me an unsatisfactory explanation. What is meant by a virtual particle? Is it just an arbitrary expedient, like when explaining lightning saying "Thor does it"? There has to be something more to be said.
 
Asgrrr said:
I have a few questions:

Can a u quark turn into a d quark (heavier) via the weak interaction? If so, how is the mass/energy shortfall made up?
A proton turning into neutron is caused by one u quark turning into d quark. And a neutron is heavier.
The mass/energy shortfall is made up by the (larger) binding energy of the neutron/d quark.
Asgrrr said:
How can the (supermassive) carrier bosons (W, Z) be called into being? Where does the energy come from? Or is the energy bill unpaid because they are virtual particles, on the verge of existence? Is it akin to a tunneling effect?
Yes, tunnelling is a good comparison for virtual particles.
 
Thank you Snorkack!

If nobody contradicts, I may be onto something here.
 
Asgrrr said:
What is meant by a virtual particle?
A mathematical concept in perturbation theory, which is a tool to calculate approximations to processes.
It is not "Thor does it", because we can calculate how often what happens.
Asgrrr said:
The context is within a nucleon in a nucleus, e.g. electron capture.
Then it can be possible, it depends on the nucleus and the binding energy of the initial and potential final nucleus.
 
I am not sure that
mfb said:
we can calculate how often what happens
For the simplest example of what a virtual particle is, consider virtual photon.
Electromagnetic field includes electromagnetic waves. They are freely propagating, carry energy, momentum and angular momentum independent of the source and eventual recipient.
They are also observably quantized into real photons.
But not all electromagnetic field is free waves.
Electromagnetic field also includes electrostatic and magnetostatic fields.
As well as evanescent waves. Oscillating electric fields exist in directions and volumes of space into which they are not freely propagating.
The concept of "virtual particle" is based on the idea of treating unfree fields as quantized like the freely propagating waves are.
If you look at the electrostatic field of a point charge, you can define the total strength of the field lines included. But can you break down the electrostatic field of a point charge into a countable number of virtual photons, the way you can in theory count the radio wave real photons emitted by an antenna?
 
snorkack said:
But can you break down the electrostatic field of a point charge into a countable number of virtual photons
No.

How is your post related to the part you quoted?
"How often what happens" is about physical processes, e. g. decays, cross sections and so on.
 
  • #10
mfb said:
No.

How is your post related to the part you quoted?
"How often what happens" is about physical processes, e. g. decays, cross sections and so on.
Ah, the real final outcome?
But do you need virtual particles for that?
 
  • #11
To make it very clear: "Virtual particles" is a confusing buzzword for propagators in Feynman diagrams, depicted there by internal lines. They are not interpretable as particles at all. That's only possible in the sense of asymptotic free states, and sometimes even those are not as simple as it looks in the standard procedure idealizing them to free plane-wave states. For a full understanding you have to study relativistic quantum field theory and deal with pretty mind-boggling conceptual problems, related to the definition of asymptotic states, LSZ reduction (named after Lehmann, Symanzik, and Zimmermann), and all that.
 
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  • #12
snorkack said:
But do you need virtual particles for that?
No, there are calculation methods that do not have virtual particles. Lattice calculations for example.
 

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