Verifications of running charge / running mass

In summary, the phenomenon of running charge predicted by QFT has been experimentally verified through physical measurements of an electron's charge varying with energy. While there have been canonical experiments confirming this, there has not been a similar experimental confirmation of the running mass, as mass behaves differently than coupling in this scenario. The pole mass, which is the mass of a free particle in its own frame, is not well-defined for quarks due to confinement. The running mass, which is the effective mass during interactions at a certain scale, is measured for the bottom quark in Z-boson decays and compared to measurements at lower scales. However, due to the ambiguity in defining the pole mass for quarks, pole mass values are not commonly seen
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metroplex021
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TL;DR Summary
Looking for citations of experimental confirmations of electronic running charge, and also running mass (if these exist).
Hi everyone,
I understand that the phenomenon of running charge predicted by QFT has been experimentally verified: the physical charge on an electron really does vary with the energy at which it is measured. I have two questions:
(1) Does anyone know what the canonical experiments confirming this are?
(2) Has there been a similar experimental confirmation of its 'running mass' (since formally mass behaves just like a coupling here)?
Any input most appreciated. Thanks!
 
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You can for example measure the running mass of the bottom quark from Z-boson decays and compare it to the running mass measured at lower scales:

https://arxiv.org/abs/hep-ph/9905495v2 states a value of
##m_b(m_Z)=2.56\pm 0.72(\rm{stat.})^{+0.28}_{-0.38}(\rm{syst.})^{+0.49}_{-1.48}(\rm{theor.})## GeV,
the PDG quotes
##m_b(m_b)=4.18^{+0.03}_{-0.02}## GeV.
 
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Orodruin said:
https://arxiv.org/abs/hep-ex/0507078
Mass is not the same as coupling. The physical mass is independent of the renormalisation scale. It refers to the pole of the propagator.
Thank you Orodruin. I thought the pole mass was just the mass of the *free* particle in its own frame -- which is why, given confinement, the pole mass isn't well-defined for quarks. And I thought that the 'running' mass of the particle was its effective mass when undergoing interactions at scale E. Is that not right?
 
  • #5
Reggid said:
You can for example measure the running mass of the bottom quark from Z-boson decays and compare it to the running mass measured at lower scales:

https://arxiv.org/abs/hep-ph/9905495v2 states a value of
##m_b(m_Z)=2.56\pm 0.72(\rm{stat.})^{+0.28}_{-0.38}(\rm{syst.})^{+0.49}_{-1.48}(\rm{theor.})## GeV,
the PDG quotes
##m_b(m_b)=4.18^{+0.03}_{-0.02}## GeV.
Thank you Reggid. Is this consistent with what Orodruin writes above - ie what we're measuring when we measure this 'running mass' is something different from the mass of bottom quark itself?
 
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Due to confinement the pole mass of a quark is not more a physical mass than any other mass scheme. The pole mass is only a strictly perturbative concept, since the full propagator of a quark does not have a pole due to non-perturbative effects.

This leads to an ambiguity in the definition of the pole mass of order ##\mathcal{O}(\Lambda_{\rm{QCD}})##, which is the reason why you will usually not see pole mass values for quarks very often. The only exception is the top quark, but also here this ambiguity might start to play a role when LHC takes more data and gains higher precision on top mass measurements, definitely with possible future lepton-colliders.
 
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1. What is a verification of running charge/running mass?

A verification of running charge/running mass is a process used in scientific experiments to ensure the accuracy and consistency of measurements over time. It involves taking multiple measurements of a particular variable and comparing the results to a known standard or control.

2. Why is a verification of running charge/running mass important?

A verification of running charge/running mass is important because it helps to identify any errors or inconsistencies in the measuring instrument or process. It also ensures that the measurements are reliable and can be trusted for further analysis and conclusions.

3. How is a verification of running charge/running mass performed?

A verification of running charge/running mass is performed by taking multiple measurements of the same variable over a period of time. The results are then compared to a known standard or control to determine if there are any variations or discrepancies. This process may be repeated multiple times to ensure accuracy.

4. What are the benefits of conducting a verification of running charge/running mass?

The benefits of conducting a verification of running charge/running mass include ensuring the accuracy and reliability of measurements, identifying any errors or inconsistencies, and providing confidence in the results of the experiment. It also allows for adjustments to be made to the measuring instrument or process if necessary.

5. Are there any limitations to a verification of running charge/running mass?

One limitation of a verification of running charge/running mass is that it may not identify all sources of error in the measuring instrument or process. It is also important to note that the results of a verification may vary depending on the conditions and settings of the experiment. Therefore, it is important to conduct multiple verifications to ensure consistency and accuracy.

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