Energy conservation concerns in the weak interaction

In summary, the conversation discusses the concept of virtual particles and their role in physical processes. It is explained that virtual particles do not exist as isolated objects and are a mathematical tool used in perturbation theory to calculate approximations. The mass/energy shortfall in processes such as a proton turning into a neutron is made up by the binding energy of the particles involved. Virtual particles are compared to tunnelling and it is noted that they are not necessary for all calculation methods.
  • #1
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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  • #2
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.
 
  • #3
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.
 
  • #4
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.
 
  • #5
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.
 
  • #6
Thank you Snorkack!

If nobody contradicts, I may be onto something here.
 
  • #7
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.
 
  • #8
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?
 
  • #9
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.
 

1. What is the weak interaction?

The weak interaction is one of the four fundamental forces of nature, along with gravity, electromagnetism, and the strong interaction. It is responsible for radioactive decay and plays a key role in the synthesis of elements in stars.

2. How does energy conservation play a role in the weak interaction?

Energy conservation is a fundamental principle in the laws of physics, including the weak interaction. This means that energy cannot be created or destroyed, only transformed from one form to another. In the weak interaction, energy is conserved through processes such as beta decay, where a neutron decays into a proton, electron, and antineutrino while conserving energy.

3. Why is energy conservation important in the weak interaction?

Energy conservation is important because it helps to maintain the stability and balance of the universe. In the weak interaction, energy conservation ensures that the energy released from radioactive decay is not lost, but rather transformed into other forms of energy.

4. How do scientists study energy conservation in the weak interaction?

Scientists study energy conservation in the weak interaction through experiments and observations. They use particle accelerators to recreate the conditions of the early universe and observe the behavior of particles and energy during radioactive decay processes.

5. Are there any current concerns about energy conservation in the weak interaction?

There are ongoing studies and research to better understand the intricacies of energy conservation in the weak interaction. Some scientists are also exploring potential connections between the weak interaction and other fundamental forces, such as the Higgs field. Additionally, there is a focus on finding ways to harness energy from the weak interaction for practical applications.

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