What is charge? Why do fundamental particles possess it?

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Discussion Overview

The discussion revolves around the nature of electric charge in fundamental particles, questioning its origin and the reasons why certain particles possess charge while others do not. Participants explore theoretical implications, gauge theories, and the relationship between charge and other conserved quantities in physics.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants question the meaningfulness of asking what gives a particle its electric charge, suggesting it may relate to interactions with a charge field or gauge theories.
  • There are two distinct questions posed: why electric charge exists as a conserved quantity and why it is quantized.
  • One participant notes that electric charge is a fundamental force of nature, yet the deeper reasons for its existence and behavior are not well understood.
  • Another participant compares electric charge to mass, suggesting both are fundamental properties, but expresses confusion over why one can be probed further than the other.
  • Some participants discuss the mathematical similarities between gravitational and electric forces, hinting at deeper theoretical connections, including string theory.
  • A participant raises the question of whether electric charge arises from interactions with fields, similar to how mass is derived from the Higgs field.
  • There is mention of the Yukawa coupling and its implications for understanding the quantization of electric charge, alongside questions about anomalies in gauge theories.
  • Local Gauge Invariance (LGI) is introduced as a principle that relates to the existence of charge, with further inquiries into its necessity and implications.

Areas of Agreement / Disagreement

Participants express a range of views on the nature and origin of electric charge, with no consensus reached. The discussion remains open-ended, with multiple competing ideas and questions about the fundamental properties of charge.

Contextual Notes

Participants acknowledge limitations in understanding the deeper reasons behind the existence and quantization of electric charge, as well as the relationship between charge and other fundamental properties like mass.

logic smogic
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I attended a colloquium a few days ago concerning the LHC and the search for the Higgs Boson. After some thought, I have the following question.

Among other things, there are two measurable properties of all of the fundamental particles in the Standard Model: mass and charge. It is hypothesized that a particle gets its mass by interacting with the Higgs field (colloquially, by the tendency of local vacuum to 'cling' to it as it moves through space).

But what gives a particle its electric charge?

Is this a meaningful question? Is it by some interaction with some charge field - by interaction with the local EM field? No, for charge generates a local EM field, right? Is my question off the wall, unresearched, or being currently discussed? Is it only meaningful by way of discussing gauge theories? Essentially, what is charge, and why do some particles have it and others don't?
 
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There are really two different question: 1) Why does a preserved quantity such as electric charge exist? and 2) Why is it quantized?
 
It's one of the fundamental forces of nature [electric charge], it's a phenomenon we take for granted. People should be able to explain why [what happens] when one charged particle is attracted to another one, but to break it down further than that is not really known.

Not really sure if I am answering your question though...
 
arivero said:
There are really two different question: 1) Why does a preserved quantity such as electric charge exist? and 2) Why is it quantized?

...meaning we should just consider it as a conserved quantity of a system, similar to energy, momentum, etc. From that point of view, why is it considered special, and not just a dynamical symmetry? Because it is quantized and its greater applicability?

hxtasy said:
It's one of the fundamental forces of nature [electric charge], it's a phenomenon we take for granted. People should be able to explain why [what happens] when one charged particle is attracted to another one, but to break it down further than that is not really known.

Not really sure if I am answering your question though...

It would seem to me that mass would hold that status, too. That it is a fundamental property of nature, and that it's origin cannot be probed further - but that's seemingly incorrect. I guess why one can be probed further and the other not is the nature of my confusion.
 
Last edited:
logic smogic said:
...meaning we should just consider it as a conserved quantity of a system, similar to energy, momentum, etc. From that point of view, why is it considered special, and not just a dynamical symmetry? Because it is quantized and its greater applicability?



It would seem to me that mass would hold that status, too. That it is a fundamental property of nature, and that it's origin cannot be probed further - but that's seemingly incorrect. I guess why one can be probed further and the other not is the nature of my confusion.


Yeah gravity is also a fundamental force in nature, and it hasn't been probed further yet. Gravitational forces and electrical forces share similar mathematical properties, so uncanny that scientists are intriqued to find out why they behave in similar fashions. That is more getting into string theory though:

http://en.wikipedia.org/wiki/String_theory



But honestly I am still a little fuzzy on what you are asking?
 
… t3 + Y … ?

Is it fundamental … isn't it hypercharge plus t3?
 
hxtasy said:
Yeah gravity is also a fundamental force in nature, and it hasn't been probed further yet. Gravitational forces and electrical forces share similar mathematical properties, so uncanny that scientists are intriqued to find out why they behave in similar fashions. That is more getting into string theory though:

http://en.wikipedia.org/wiki/String_theory



But honestly I am still a little fuzzy on what you are asking?

Consider the Standard model (say, as it appears on the Wiki article http://en.wikipedia.org/wiki/Standard_Model). Each particle is listed in the left-most column, and to the right are listed the currently known values of its various observables (electric charge, weak isospin, weak hypercharge, color charge, mass).

So the positron has electric charge +1 and mass 511 keV.

A month ago, I would have thought it strange to ask, "Why does the positron have a mass of 511 keV?" Today, a particle physicist would likely answer, "Because it interacts with the Higgs field in such a way as to give it a 'mass' of 511 keV." That is, the positron's mass is defined by the strength of its interaction with the Higgs field.

My question is exactly this, "Why does the positron (or any other fundamental particle) have the charge it has." Is it because it interacts with some field that gives it its charge? This seems to me like a perfectly reasonable question that follows from our new understanding of mass and the Higgs field.
 
arivero said:
2) Why is it quantized?

Yes why ?
The yukawa coupling between higgs and fermions do not look really quantized.
Why electric charge is ? And why is it such that it cancels prefectly eg anomalies ?
Can it be explained in GUT theories ?
 
logic smogic said:
But what gives a particle its electric charge?
Charge (electric, weak or color) follows from the principle of Local Gauge Invariance (LGI) in quantum mechanics. If it is desired that the phase of a spinor wave function psi have no physical effect, then vector fields must be introduced with a psibar V psi interaction.
Why LGI is needed, and why e^2=1/137 are deeper questions.
 

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