How does the electron mass run with energy?

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Discussion Overview

The discussion revolves around the running of electron mass with energy in the context of quantum electrodynamics (QED) and its implications at high energy scales, particularly near the Planck energy. Participants explore the calculations involved in determining how the electron mass changes with energy, the role of interactions, and the potential impact of other forces.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • François questions whether the physical electron mass increases or decreases with energy and mentions a reference suggesting a 16% change, seeking clarification.
  • One participant presents a calculation indicating that the electron mass increases in the ultraviolet (UV) limit, using the equation \(\frac{dm_e}{d\log\mu} = \left(\frac{3e^2}{8\pi^2}\right)m_e\) for one-loop QED.
  • Another participant argues that the weak interaction cannot be neglected in the UV, as QED is the infrared limit of electroweak theory.
  • A participant emphasizes that the initial calculation only applies to QED and is valid up to the muon mass, suggesting that a more comprehensive approach is needed to include other fermions and interactions for accurate results at the Planck scale.
  • François revisits the calculation, proposing that if the electron mass is measured at 511 keV, the mass at Planck energy could be only 2% higher, assuming neglect of weak and strong interactions.
  • Another participant cautions that the running should start at the electron mass (511 keV) rather than 1 eV and notes that the coupling constant \(e^2\) also runs, complicating the differential equation and potentially enhancing the mass change slightly.
  • Participants generally agree that the effect of running is small, with estimates suggesting a few percent increase, and highlight that the discussion is largely theoretical and simplified.
  • François shifts focus to neutrino mass, asking how it runs with energy and whether there are available numbers on neutrino mass renormalization at Planck energy, noting that neutrinos are not affected by QED in the same way as electrons.

Areas of Agreement / Disagreement

Participants express a range of views on the running of electron mass, with some calculations suggesting small increases while others emphasize the need for a more comprehensive approach. The discussion on neutrino mass introduces additional uncertainty, with no consensus on its behavior at high energies.

Contextual Notes

Participants acknowledge limitations in their calculations, including the neglect of weak and strong interactions and the assumption of a simplified universe with only electrons, positrons, and photons. The discussion remains exploratory, with various assumptions and conditions affecting the conclusions drawn.

franoisbelfor
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Renormalization in QED implies the running of charge and mass. But does the physical electron mass increase or decrease with energy? And what value is reached at the Planck energy? Somewhere I read that the mass change was 16%, but all books I on QED I searched do not give numbers. (Assuming the strong and weak interactions are neglected.)

Does anybody know a reference ?


François
 
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From a "straightforward" calculation (as straightforward as these calculations can be!):

\frac{dm_e}{d\log\mu} = \left(\frac{3e^2}{8\pi^2}\right)m_e

to one loop. So as you might expect from screening arguments, the mass increases in the UV.
 
To add, you cannot neglect the weak interaction in the UV, as QED is the IR limit of part of the electroweak theory.
 
quite right. the formula I gave is ONLY for QED at one loop - that means photon, electron and positron, NOTHING else. Strictly speaking, this is only correct in the UV up to the muon mass.

To get an accurate and correct number that describes the universe that we live in, of course you must go much further, including the other fermions (leptons and quarks), and then match to EW theory above the W boson mass, if you want to push the calculation up to the Planck scale (assuming that there's a desert from the weak to Planck scales).
 
blechman said:
From a "straightforward" calculation (as straightforward as these calculations can be!):

\frac{dm_e}{d\log\mu} = \left(\frac{3e^2}{8\pi^2}\right)m_e

to one loop. So as you might expect from screening arguments, the mass increases in the UV.

Ok, if one assumes hat the 511keV are measured at \mu= 1 eV, and uses \left(\frac{3e^2}{8\pi^2}\right)=2.7*10^{-4} one gets a electron mass at the Planck energy (10^28 eV) that is (10^28)^(2.7*10^-4)=1.018 times
higher than at 1 eV. Only 2% difference!

Is that correct? (This neglects weak and strong interaction effects, of course.)

François
 
you have to be more careful:

(1) nothing runs below the electron mass itself, so you don't want to start the running at 1 eV, but at m_e(m_e)=511 keV.

(2) you also have to take into account the (very important!) point that e^2 is not a constant but also runs, so the diffEQ is a little more complicated than what you naively wrote down. This will enhance the mass a bit.

But it is true that the effect is not very large... a few percent at most -- QED remains quite weak up to the Planck scale.

And of course, this is in a fictitious universe where there are no other forces or particles other than the electron, positron and photon. In other words, a homework problem, not a true physics result!
 
blechman said:
you have to be more careful:

(1) nothing runs below the electron mass itself, so you don't want to start the running at 1 eV, but at m_e(m_e)=511 keV.

(2) you also have to take into account the (very important!) point that e^2 is not a constant but also runs, so the diffEQ is a little more complicated than what you naively wrote down. This will enhance the mass a bit.

But it is true that the effect is not very large... a few percent at most -- QED remains quite weak up to the Planck scale.

And of course, this is in a fictitious universe where there are no other forces or particles other than the electron, positron and photon. In other words, a homework problem, not a true physics result!

Thank you very much! This was very illuminating. Even after recalculation, the effect
still is in the 2% range.

Thank you again!
François
 
How does the NEUTRINO mass run with energy?

In a separate thread I was told very clearly that even at Planck energy, the electron mass is renormalized (by QED alone) only by a few percent. The renormalization equation is quite simple.

Now, what happens to the *neutrino* mass at Planck energy? Obviously, being neutral, the neutrino mass is not normalized by QED (well, at least not at first order), but by the weak interaction.

Are there any numbers available on how neutrino masses run up to the Planck energy?
(Assuming, of course, that the standard model is valid throughout, i.e., no susy, no technicolor, etc.) Are the renormalization equations as simple as for QED? Are there any books/papers on the issue?

Thank you for any hint!

François
 

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