Is the Higgs Boson Just a Force?

In summary, the conversation focuses on the function and existence of the Higgs boson, specifically whether it has mass or is purely a force. Theoretical and experimental evidence suggests that the Higgs boson has a non-zero mass and is responsible for imparting mass to other particles through the Higgs mechanism. There is also discussion about the relationship between the Higgs force and gravity, and the limitations of using standard terminology when discussing the Higgs boson.
  • #1
246ohms
14
2
Hello

I am trying to understand the function of the Higgs bosun which appears to lend mass to other particles. But what if it has no mass and is purely a force? Could the Higgs force be assimulated by another particle but at the same time it also imparts a reactional force - gravity.

If so it would seem to produce a 'mass' effect and it would be difficult to produce in the LHC.

Thanks - 246Ohms
 
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  • #2
246ohms said:
But what if it has no mass and is purely a force?

I don't know what this means, but the Higgs mass must be non-zero. Experimentally, we don't see a long-range force that behaves as the Higgs does, and the theoretical framework that makes a Higgs a Higgs has the relationship [tex]m/\lambda = 246~{\rm GeV}[/tex], where [tex]\lambda[/tex] is the Higgs self-coupling, which is non-zero.
 
  • #3
We have many old thread about this topic.
 
  • #4
If there is a higgs boson, it must have a mass. Even if you ignore the experimental evidence that we never saw it (maybe it decays in some super-bizarre way, which is why we didn't see it) there is still a lower bound on its mass coming from the stability of the vacuum. This bound is very weak (about 4 GeV), but it is definitely not zero.

Depending on how seriously you want to take the data, the higgs mass has experimentally been shown to be larger than 114 GeV (in the standard scenario) or more loosely 80-something GeV in more open-ended searches. Precision EW measurements also allow for the mass to be no bigger than around 250 GeV, and if you ignore that, other quantum effects enforce a stronger upper bound at around 2 TeV (to prevent the higgs from becoming strongly coupled, which would forbid it from doing its job in giving mass to the standard model particles).
 
  • #5
blechman said:
Even if you ignore the experimental evidence that we never saw it.

If Higgs is predicted by the SM and we argue its existence based on the model then it must exist as a mass. Some however are not so sure that the SM or even SS predict the Higgs field as a new one and others even propose it may be a quark or lepton field and if so it would be massless and as blechman says above the experimental evidence so far has not seen it.

My question is could Higgs be just a force that induces mass but also has a reactionary force - for instance gravity ie is the Higgs force connected to gravity. From a circular analysis gravity acts on mass and mass is supplied by the Higgs ... So what's the connection? Its an outside the box question.

Thanks 246ohms
 
  • #6
I still don't understand what you are talking about. "we argue its existence based on the model then it must exist as a mass" doesn't make sense, nor does "My question is could Higgs be just a force that induces mass but also has a reactionary force - for instance gravity ie is the Higgs force connected to gravity." Perhaps if you were to use standard terminology more people would understand what you write.

Nevertheless,

246ohms said:
and others even propose it may be a quark or lepton field and if so it would be massless

is clear. And it's not the case.

Do you understand the Higgs mechanism in the Standard Model? If so, it would help to pose your question in standard terminology. If not, I would suggest that the first step before declaring that it's wrong is to understand what it actually says.
 
  • #7
If all particles with mass are supposed to derive all of their mass from interactions with Higgs-particles, the logical conclusion would be that Higgs-particles have mass if and only if they interact with each other.

However, charged particles like the electron carry mass in their electromagnetic field. Some of their mass must therefore be due to something else than interactions with Higgs-particles. Unless, of course, their charge is also caused by interactions with Higgs-particles.
 
  • #8
If we are talking about a 'higgs particle' and 'higgs field' and 'higgs mechanism' that is not included in the electroweak SM, then it is pointless to even calle it Higgs, Just as Vanadium 50 is trying to tell you: Either relate the question and language to the higgs of the SM, or study it, or ask about alternative models for including mass to particles.

So, 246ohms: In the electroweak SM - Higgs mechanism is not a force, and is not there to explain the force of gravity either. The thing that higgs field does is to give mass to the quarks and leptons.

Almanzo: You reasoning about the electron mass is not based on based on physics but of some 'intuitive' feeling, not ok, back to school.
 
  • #9
malawi_glenn said:
Almanzo: You reasoning about the electron mass is not based on based on physics but of some 'intuitive' feeling, not ok, back to school.

Actually, it is based on The Feynman Lectures on Physics, part II, chapter 28.
 
  • #10
There is nothing about Higgs there..
Chapter 28.3 is about classical electrodynamics...which is not relevant so much in quantum field theories...
 
  • #11
I don't particularly care for that section in Feynman, largely because Feynman doesn't make it clear that this is generally regarded as a dead end. If you try and explain the electron's mass as purely electromagnetic in origin, you eventually get contradictions like [tex]m_e = \frac{4}{3} m_e[/tex]. This was known around the turn of the (last) century. But what really did this in was the discovery of the muon, a particle just like the electron but 200 times heavier.

Quantum mechanically, the situation is simpler. These effects are called "radiative corrections", and they get absorbed into the Higgs Yukawa coupling. So it's already included in the Higgs contribution.

Again, I think it's a very good idea that before declaring a theory to be wrong or incomplete that one spends some time understanding what the theory actually says.
 
  • #12
Sorry to have taken this long to reply; but I usually have time to visit once or twice a week only.

What Feynman seems to say, is this. Some (but definitely not all) of the electron's mass must be due to the electromagnetic field (and actually reside there, and not in the electron's "body"). Some other part of its mass must be due to "Poincaré stresses", that is: to whatever is preventing the electron from flying apart. And some of the mass may be due to something else.

What the Higgs theory seems to say (as presented by some post in this thread) is that all of the mass of every particle (including the electron) is due to interactions with Higgs-particles.

I do not pretend to know anything else about the Higgs theroy, but I am struck by an apparent contradiction. If some of the electron's mass is due to its having a charge, and all of its mass is due to interactions with Higgs particles, something has to give. Perhaps the Higgs particles are also responsible for the electron's charge? Then it could both be true. But there should be some explanation on how to reconcile the Higgs idea with, for
example, the formula for the electromagnetic energy density on top of page 146 in the Cambridge Handbook of Physical Formulas. It was published in 2000, so I don't think that it is obsolete.

And I think that this would be, generally, the explanation which 246ohms requested when he started this thread.
 
  • #13
Almanzo said:
What Feynman seems to say, is this. Some (but definitely not all) of the electron's mass must be due to the electromagnetic field (and actually reside there, and not in the electron's "body"). Some other part of its mass must be due to "Poincaré stresses", that is: to whatever is preventing the electron from flying apart. And some of the mass may be due to something else.

I don't think Feynman would agree with the "must". As I alluded to before, if you work out how much of the mass is carried in the self-interaction with the electric field, it works out to 133% of the mass. That's (one reason) why this line of thinking is essentially dead. Another is that this is a purely classical theory attempting to describe a quantum mechanical object.

Almanzo said:
What the Higgs theory seems to say (as presented by some post in this thread) is that all of the mass of every particle (including the electron) is due to interactions with Higgs-particles.

It does not say this. The only particles that the Higgs must give mass to are the W and Z bosons. Fermions can have a Dirac mass that has nothing to do with the Higgs. Alternatively, a completely different Higgs gives mass to the fermions.


Almanzo said:
I do not pretend to know anything else about the Higgs theroy(sic)

Again, I think it's a very good idea that before declaring a theory to be wrong or incomplete that one spends some time understanding what the theory actually says.
 
  • #14
I did not declare anything of the sort. I was asking for an explanation.
 
  • #15
Vanadium 50 said:
I don't think Feynman would agree with the "must". As I alluded to before, if you work out how much of the mass is carried in the self-interaction with the electric field, it works out to 133% of the mass. That's (one reason) why this line of thinking is essentially dead. Another is that this is a purely classical theory attempting to describe a quantum mechanical object.

I agree with this, but let me also expand on it. It is true that there is "self-energy" of the electron coming from its interactions with the electromagnetic field. Classically this doesn't work, as Vanadium_50 says. In QED, this effect is real. There is an (infinite) contribution to the electron's mass. To a QFT expert: an infinite mass correction implies that the electron mas RUNS, that is, the value of the mass you measure for the electron depends on the energy at which you measure it. I do not want to hijack the thread with a talk about renormalization group methods, but if you're interested, read up on that as well.

HOWEVER, even in this case, the Higgs field has to play a role, since an electron mass is not allowed by the symmetries of the SM without a Higgs (see below). So you see, even with these EM contributions, the Higgs is involved. To see how this works explicitly would require some knowledge of QFT, but if you actually compute the QED corrections and be careful, you find the Higgs is part of the picture, at least in the current version of the SM. For the experts: the loop requires a mass insertion to renormalize the mass.

Another way to see this (although a little more technical): In the classical theory, the EM mass of the electron is "linearly divergent". In the quantum theory, it is "LOG divergent". Dimensional analysis then says that there must be a mass scale for the electron to get a correction, and the only mass scale around is the Higgs vev. This emphasizes that there is a VITAL difference between the classical calculation and the QFT calculation (the latter being the correct one!). :wink:
It does not say this. The only particles that the Higgs must give mass to are the W and Z bosons. Fermions can have a Dirac mass that has nothing to do with the Higgs. Alternatively, a completely different Higgs gives mass to the fermions.

Well, it is certainly true that this COULD be the case. However, the "Standard Model" has the Higgs doing double-duty. The point being that you cannot write a Dirac mass for any of the fermions without somehow breaking the gauge symmetry. Minimally, the Higgs is what does that. Extensions of the SM are interesting, but we might not want to go that way here.
 

1. What is the Higgs Boson?

The Higgs Boson is a subatomic particle that is proposed to give mass to other particles in the universe. It was first theorized in the 1960s by Peter Higgs and has since been confirmed by experiments at the Large Hadron Collider.

2. Is the Higgs Boson just a force?

No, the Higgs Boson is not just a force. It is a particle that is responsible for the Higgs field, which is a fundamental force in the universe. The Higgs field interacts with other particles and gives them mass, but the Higgs Boson itself is not a force.

3. How was the Higgs Boson discovered?

The Higgs Boson was discovered in 2012 by scientists at the Large Hadron Collider. They observed a signal consistent with the predicted behavior of the Higgs Boson in proton-proton collisions at high energies.

4. Why is the discovery of the Higgs Boson important?

The discovery of the Higgs Boson confirmed the existence of the Higgs field and provided evidence for the Standard Model of particle physics. It also helps explain how particles acquire mass, which is a fundamental property of matter.

5. What are the implications of the Higgs Boson for future research?

The discovery of the Higgs Boson opens up new avenues for research in particle physics. Scientists can now study the properties of the Higgs Boson and its interactions with other particles, which can provide insights into the origins and workings of the universe.

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