What is the role of the Higgs in determining the mass of particles?

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Discussion Overview

The discussion centers on the role of the Higgs boson in determining the mass of particles, exploring concepts related to particle physics, the Higgs field, and the nature of mass in the context of the Standard Model. Participants raise questions about the relationship between the Higgs boson and protons, gauge bosons, and the underlying mechanisms that contribute to particle mass.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants express confusion about how the Higgs boson, which is said to have mass, can be part of a particle (like a proton) that is made up of massless components.
  • There is a discussion about the nature of gauge bosons, with some participants arguing that the Higgs is not a gauge boson due to its spin-0 nature, while others clarify that gauge bosons can interact with the forces they mediate.
  • Participants question why the Higgs boson has a mass parameter when other gauge bosons do not, suggesting that this could be a peculiarity of the Standard Model.
  • Some participants propose that a particle's mass parameter is determined by its interaction strength with the Higgs field, raising the "flavor problem" as an open question regarding why particles have different interaction strengths.
  • There is mention that the Higgs boson's mass parameter is considered a fundamental parameter in the Standard Model, which may be influenced by unknown underlying physics.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the nature of the Higgs boson, its role in mass generation, or the implications of its mass parameter. Multiple competing views and uncertainties remain throughout the discussion.

Contextual Notes

Limitations include unresolved questions about the fundamental nature of mass parameters, the interaction strengths of particles with the Higgs field, and the implications of gauge boson properties in the context of the Standard Model.

fanna
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Hi,

First time I've posted on this website.

I keep hearing & reading news stories that protons are made of sub-atomic particles, one of which is the Higgs-Boson. The story continue with how many times the Higgs weighs more than a proton.

I don't get that last bit.

How can the whole weigh less than a part?
 
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fanna said:
Hi,

First time I've posted on this website.

I keep hearing & reading news stories that protons are made of sub-atomic particles, one of which is the Higgs-Boson. The story continue with how many times the Higgs weighs more than a proton.

I don't get that last bit.

How can the whole weigh less than a part?

Bosons only mediate the forces they don't make up matter.
Protons are suppose to be made up of quarks, which have mass, but 95% of the mass of a proton is energy stored by via the strong force and EM force.
 
fanna said:
I keep hearing & reading news stories that protons are made of sub-atomic particles
Yes.

one of which is the Higgs-Boson.
No.

The story continue with how many times the Higgs weighs more than a proton.
Yes.
 
If the Higgs is the carrier boson of the Higgs field then I've always wondered why it has mass, because the other gauge bosons don't interact through the force they mediate, the photon has 0 electromagnetic charge, the gluon has no color charge and the hypothetical graviton has no mass, I don't know enough about weak isospin/hypercharge to comment about the W and Z bosons (never understood anything about the weak force). But this confuses me
 
Voltz said:
If the Higgs is the carrier boson of the Higgs field then I've always wondered why it has mass, because the other gauge bosons don't interact through the force they mediate, the photon has 0 electromagnetic charge, the gluon has no color charge and the hypothetical graviton has no mass, I don't know enough about weak isospin/hypercharge to comment about the W and Z bosons (never understood anything about the weak force). But this confuses me

1) Gauge bosons are the carriers of a force; and they are excited states of a field. It isn't meaningful to say that something is the "carrier of a field."

2) The Higgs is not a gauge boson. Gauge boson are necessarily spin-1 (or, if you include the graviton spin-2). To be a gauge boson it is necessary that at least one degree of freedom in the mathematical description actually be physically redundant. For spin-1 this isn't a problem. A spin-1 field has 4 components - 1 in each direction of spacetime - so, having one fewer be physically meaningful still leaves physical degrees of freedom. But, the Higgs is spin-0. This means it has 1 and only 1 component. So, there can't be a gauge-type redundancy.

3) Gauge bosons can, in fact, feel the forces they mediate. Gluons do carry color charge (in fact each gluon carries both a color charge and a color anti-charge), and the W triplet (in the unbroken phase of the electroweak force) carry weak isospin.

4) In quantum field theory, in general, it is not necessary that everything be fundamentally massless. It is only necessary that gauge bosons be massless and that fermion masses not violate any symmetries. The problem is that fermion mass terms require chiral symmetry and the isospin part of the weak force doesn't obey it. Because of this, fundamental masses for the fermions would actually break the symmetry of the weak force in a way that would make the theory inconsistent. The point here is that it's kind of a fluke that everything in the standard model has to get mass in a dynamical way.

This fluke, however, makes it seem odd that the Higgs field actually does have a fundamental mass parameter, when it really shouldn't be. The Higgs mass is really just a function of that mass parameter combined with the effects of the Higgs' interactions with itself.
 
Parlyne said:
The Higgs mass is really just a function of that mass parameter combined with the effects of the Higgs' interactions with itself.

What determines this mass parameter then?
 
gendou2 said:
A particle's mass parameter is set by its interaction-strength with the Higgs.
Why particles have different interaction-strengths is an open question.
It is sometimes called the "flavor problem".

http://profmattstrassler.com/articl...known-particles-if-the-higgs-field-were-zero/

This is not actually true of the Higgs itself, though. The Higgs, alone among standard model particles, actually has a mass parameter that is (so far as the standard model goes) a fundamental parameter. It's there in the theory to start with. It might come about from some underlying physics that we don't know about yet; but, from the point of view of standard model physics it's just a fundamental parameter. The mass of the physical Higgs is a function both of this parameter and of the strength of the Higgs' coupling to itself.
 

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