What contributes to proton mass besides quark mass?

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Discussion Overview

The discussion centers around the contributions to proton mass beyond quark mass, exploring the role of interaction energy among quarks and gluons within quantum chromodynamics (QCD). Participants examine theoretical implications, potential models, and the nature of mass in this context.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that a significant portion of proton mass arises from interaction energy rather than the mass of quarks themselves.
  • There is a discussion about whether mass refers to inertial mass or rest mass, with some clarifying it as standard rest mass.
  • Questions are raised regarding the possibility of negative energy states and the implications for bound state energies, with some arguing that bound states should have energies less than the sum of constituent masses.
  • Participants discuss the nature of the QCD potential, noting that it rises indefinitely and approximates a harmonic oscillator potential at large distances, while questioning the existence of a potential in QCD.
  • Some participants mention that the number of constituents in a proton is not fixed and depends on scale, leading to questions about how this affects the proton's mass.
  • There are references to the concept of asymptotic freedom and its implications for quark mass and binding energy.
  • Clarifications are made regarding the definition of potential in QCD, emphasizing that it is a derived quantity rather than an input parameter.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the nature of mass in protons, the role of interaction energy, and the implications of QCD. The discussion remains unresolved with no consensus reached on several key points.

Contextual Notes

Limitations include the dependence on definitions of mass and potential, as well as unresolved questions about the nature of bound states and the behavior of constituents at different scales.

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Hello all .

We know about 95 percent to 98 percent of proton mass is not contributed by quark mass. In truth, most proton mass is derived from interaction energy between the quarks .

MY question is how interact makes mass ?
the mass means inertial mass or relative mass ?
 
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It's standard rest mass; w/o using a particle collider or something like that you can't see that the mass is caused by interaction.

In quantum field theory you can in principle do the following: find an eigenstate |E,p=0> of the Hamiltonian H and the momentum operator P such that
H|E,p> = E|E,p>
P|E,p> = 0

b/c p=0, whenever E>0 this is due to interaction (kin. energy is zero)
 
tom.stoer said:
b/c p=0, whenever E>0 this is due to interaction (kin. energy is zero)

Can E<0?

Also I thought bound state energies are always negative, so if anything, shouldn't the proton mass be less than the sum of the quark masses?
 
E<0 is not reasonable for a particle mass, but E=0 is.

The idea of bound states which are lighter as their constituents makes some implicit assumptions which are no longer valid in QCD
- it means that one can identify a fixed, finite number of constituents (quarks, gluons)
- it means that one can add rest masses to get the mass of the bound state (- mass defect i.e. binding energy)
- it often starts with a potential and its energy levels

In QCD
- the number of constituents is not fixed; it has to be derived from the theory; and it turns out that it becomes scale dependent
- the kinetic energy of quarks and gluons dominates the total mass; so the quarks and gluons are highly relativistic
- there is no potential to start with

So having relativistic quarks and gluons it becomes clear the the proton rest mass is due to the energy of it's 'constituents'
 
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Can E<0? Also I thought bound state energies are always negative, so if anything, shouldn't the proton mass be less than the sum of the quark masses?
Not in this case. The QCD potential rises indefinitely at infinity, and approximates a harmonic oscillator potential (positive).
 
tom.stoer said:
In QCD
- the number of constituents is not fixed; it has to be derived from the theory; and it turns out that it becomes scale dependent
- the kinetic energy of quarks and gluons dominates the total mass; so the quarks and gluons are highly relativistic
- there is no potential to start with

There has to be a potential or else wouldn't the high kinetic energy of the quarks and gluons fly apart? You can estimate it with Δp ~ 1/Δx where Δx is the nuclear size?

Also, if the number of constituents is not fixed and depends on scale, but the mass of a proton is always the same, does this mean that the constituents always conspire to change their masses at each scale so that their total mass equals the proton mass?

Also, can you find the mass of a bound state via the propagator? Take the photon propagator. Technically, shouldn't there be an isolated pole at the bound state of an electron and positron? I don't ever recall seeing this though in the photon propagator.
 
Bill_K said:
Not in this case. The QCD potential rises indefinitely at infinity, and approximates a harmonic oscillator potential (positive).

O okay. The harmonic oscillator potential has positive energy. Actually, I don't ever recall a quantum system that has negative energy. Classically two particles attracted to each other can be very close and have negative energy.

So the QCD potential is a harmonic oscillator at large distances. But at short distances, isn't it free (asymptotic freedom)? Is there a transition zone?
 
Also, if the number of constituents is not fixed and depends on scale, but the mass of a proton is always the same...
"Not fixed" does not mean "changing in time." The proton wavefunction is an eigenfunction of H. It means "not sharply determined." The proton wavefunction is a superposition of parts which contain different number of partons.
 
geoduck said:
Actually, I don't ever recall a quantum system that has negative energy.
Chemical compounds such as a molecule of water, atomic nuclei such as 56Fe. A molecule of water has slightly less mass than the masses of its constituent parts (two atoms of hydrogen and an atom of oxygen), and a 56Fe nucleus weighs slightly less than the sum of the masses of 30 neutrons and 26 protons. Note the stark contrast to the situation where the mass of a proton vastly exceeds the sums of the masses of two up quarks and one down quark.
 
  • #10
geoduck said:
Can E<0?

Also I thought bound state energies are always negative, so if anything, shouldn't the proton mass be less than the sum of the quark masses?

There's no way to free a quark from a bound state, so the definition of a quark's mass comes from the idea of asymptotic freedom, which is to say that the strong force goes away at short distances. This is totally opposite of the electric force, which goes away at long distances.
If you could somehow get a lone quark, it's mass would be something like infinite, so the proton does indeed have less mass.
 
  • #11
Please be careful; there is no potential U(x) in QCD!

The linear potential is a derived quantity, a result, and expectation value, not an input like in Standard QM.

In QCD the interaction is due to a Coulomb gauge Hamiltonian (plus other terms); for a reference you may have a look at slide 4ff of http://www.ectstar.eu/meetings/ConfsWksAndCollMeetings/ConfWksDocument/2011/Talks/Binosi/Reinhardt.pdf
 
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  • #12
No one said the QCD potential was an input.
 
  • #13
And no one said it isn't; we should be clear about that
 

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