Meaning of hypercharge in electroweak theory?

In summary, the physical meaning of hypercharge in electroweak theory is that it is a component of the SU(2) x U(1) gauge group that is broken via the Higgs mechanism. This results in a combination of three massive gauge fields, one massless U(1) gauge field, and one massive scalar. The leftover U(1) symmetry after breaking is not the same as the original U(1) of electric charge, but rather a linear combination of hypercharge and isospin. This explains why electric charge in everyday life is not the "natural" U(1) charge of electroweak theory.
  • #1
Mr. Apple
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Anybody knows what is the physical meaning of hypercharge in electroweak theory?
 
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  • #2


Electroweak theory uses an SU(2) x U(1) gauge group. However, the U(1) subgroup in this combination is NOT the U(1) of electric charge. It is a U(1) of hypercharge.

This SU(2) x U(1) gauge symmetry is broken via the Higgs mechanism, resulting in three massive gauge fields (W and Z bosons), one massless U(1) gauge field (photon), and one massive scalar (the Higgs particle). The trick is that the leftover U(1) after symmetry breaking is not the same as the U(1) before; instead, it is some linear combination of things. So in effect, the electric charge (and electrodynamics) we see in everyday life is not the "natural" U(1) charge of electroweak theory; it is some linear combination of things in SU(2) x U(1) that happen to have the symmetry U(1).

So basically, electric charge is some linear combination of hypercharge and isospin that has a remaining U(1) symmetry after symmetry breaking by the Higgs mechanism.
 
  • #3


Hypercharge is a fundamental property of particles in the electroweak theory, which describes the unification of the electromagnetic and weak nuclear forces. It is a conserved quantum number that determines the strength of a particle's interaction with the Higgs field, which gives particles their mass. In the electroweak theory, hypercharge is related to the electric charge and weak isospin of a particle through a mathematical relationship known as the Gell-Mann–Nishijima formula. This formula allows for the prediction of the electric charge of a particle based on its hypercharge and weak isospin, providing a deeper understanding of the underlying structure of matter. In summary, hypercharge plays a crucial role in the electroweak theory by connecting the fundamental forces and providing insight into the properties of particles.
 

1. What is hypercharge in the electroweak theory?

Hypercharge is a quantum number that is used to describe the electric charge of elementary particles in the electroweak theory. It is a combination of the electric charge and the third component of the weak isospin. It is denoted by the symbol Y and is conserved in all interactions.

2. How is hypercharge related to electric charge?

Hypercharge is related to electric charge through a mathematical equation, where Y = Q - (T3 + B3). Q represents the electric charge, T3 represents the third component of the weak isospin, and B3 represents the third component of the baryon number. This relationship helps to explain the conservation of hypercharge in interactions.

3. What is the significance of hypercharge in the electroweak theory?

Hypercharge is an important concept in the electroweak theory as it helps to explain the symmetry between particles and antiparticles. In this theory, particles with opposite hypercharge values cancel each other out, leading to the conservation of hypercharge. This plays a crucial role in the understanding of fundamental interactions between particles.

4. How does hypercharge affect particle interactions?

Hypercharge plays a significant role in particle interactions as it determines the strength and type of interaction between particles. Particles with the same hypercharge value interact with each other through the electromagnetic force, while particles with different hypercharge values interact through the weak nuclear force.

5. Can hypercharge change in interactions?

No, hypercharge is a conserved quantum number, meaning it does not change in interactions. This is due to the conservation laws of electric charge and weak isospin, which are components of hypercharge. However, in certain high-energy processes, particles can transform into different particles with different hypercharge values, but the total hypercharge of the system remains unchanged.

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