How Does a Down Quark Emit a W- Boson During Decay Despite Mass Discrepancies?

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The discussion centers on the emission of a W- boson by a down quark during decay, despite the mass discrepancy between the quark and the boson. It is established that while the combined mass of the three quarks is approximately 10 MeV, the neutron's mass is around 939 MeV, leaving a significant mass gap. The W- boson, with a mass of about 80 GeV, is classified as a virtual particle in this context, which allows it to momentarily violate conservation of energy due to the uncertainty principle. The majority of the nucleon mass is attributed to virtual gluons binding the quarks, contributing around 90% of the mass as energy.

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Edi
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How can a down quark emit a W- when decaying if the boson is much heavier than the quark or even the whole neutron?

Actually, the three quarks together make ~10 MeV, but the neutron is said to be ~939 MeV, so there is 929 MeV missing, i though that W- bosons made it up, but then i realized that the bosons mass is said to be ~80 GeV, witch is much more than missing. And gluons are said to be massless.
 
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The W- is a virtual particle in this case. Virtual particles are "off the mass shell," that is, they don't satisfy the mass-energy-momentum relationship for real particles, E^2 = (pc)^2 + (mc^2)^2. Alternatively, people sometimes say that virtual particles can very briefly violate conservation of energy by "hiding" behind the uncertainty principle.
 
Edi said:
Actually, the three quarks together make ~10 MeV, but the neutron is said to be ~939 MeV, so there is 929 MeV missing
[...]
And gluons are said to be massless.
The W has nothing to do with the nucleon mass. The virtual gluons binding together the three quarks hold pretty much 90% of the nucleon mass in the form of energy. It is possible to describe the situation in a different manner : we can say that individual quarks whose bare mass (at high energy) is a few MeV dress up inside the hadrons to obtain a constituent mass around 350 MeV. This picture is supported by relativistic bound state equations, namely calculating the propagator using Dyson-Schwinger methods.
 

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