Connection between the SU(2) group for the spin 1/2

In summary, there is no physical connection between the SU(2) group for spin 1/2 and the gauge group of weak interactions. They share the same group properties, but are used for different purposes in describing different physical phenomena. Similarly, the SU(3) group is used for two different purposes in describing the strong interaction and the flavour symmetry of quarks. While it is an approximative symmetry, it helps to explain the light hadron spectrum. It is important to note that the use of a mathematical tool, such as groups, does not imply a physical connection between the phenomena being described.
  • #1
captain
164
0
I wanted to ask if there is any connection between the SU(2) group for the spin 1/2 and the gauge group of weak interactions. I feel there isn't much of a connection other than the fact that they share the same group properties, but I am not sure. Thanks to anyone in advance that can clarify this for me.
 
Physics news on Phys.org
  • #2


A group is a mathematical "thing", SU(2) is the set of all unitary 2x2 matrices with determinant 1. So there is the same group describing both spin 1/2 and the gauge properties of the weak interactions. But there is no physical connection.

Another example is how we use SU(3), we use it as gauge group for the strong interactions (SU(3)_colour) and as an (approximative) symmetry of the strong interactions of the three lightest quarks (SU(3)_isospin)

In the strong interaction, a quark has three colours so the spinor is (q_red, q_blue, q_green), thus this spinor transform in colour space and from the requirement that the Lagrangian should be invariant under this transformation, we can derive the gluons and their interactions with themselves and the quarks by their colour charge. So we can say that the strong force is independent of colour, we can transform the quarks to any colour we want and still have the same end result.

In the flavour symmetry, we say that the force between quarks are flavour independent, i.e it does not matter what kinds of quarks that participate in the interaction. up-down is same as strange-up etc. Thus the spinor is (u,d,s), and by imposing this SU(3) symmetry, we end up with the light hadron spectrum.

As you can see, SU(3) is used for two different things. i) The transformations of what colour quarks have, and ii) the transformation on what flavour quarks have.

Now this second symmetry is first of all approximative, due to the quark mass differences. And more, there are more than 3 quarks. So this is just an approximative, but illuminating, symmetry.

So now the SU(2) case, the SU(2)_spin is rotation of a 2-spinor in spin-space, and SU(2)_weak is rotations in weak-isospin space. The spaces are different, but works in a similar manner.

I can describe the number of CD-records I have, and the number of books I have with the same mathematical tool (arithmetic), but that does not say that there is a connection between books and cd's. The mathematical tool can be used for anything that I expect it to be useful for. Same with groups.
 
  • #3


There is indeed a connection between the SU(2) group for spin 1/2 and the gauge group of weak interactions. In fact, the SU(2) group is a fundamental part of the Standard Model of particle physics, which describes the interactions between particles and the forces that govern them.

The SU(2) group is one of the three gauge groups in the Standard Model, along with the U(1) group for electromagnetism and the SU(3) group for strong interactions. Each of these groups is associated with a specific force, and the SU(2) group is responsible for the weak force.

The weak force is responsible for processes such as beta decay, where a neutron decays into a proton, electron, and anti-neutrino. This force is mediated by particles called W and Z bosons, which are described by the SU(2) group. The SU(2) group also plays a role in the Higgs mechanism, which gives particles their mass.

Additionally, the SU(2) group is related to spin in quantum mechanics. Spin is a fundamental property of particles and is described by the SU(2) group. This is why the SU(2) group is often referred to as the "spin group."

In summary, the SU(2) group for spin 1/2 and the gauge group of weak interactions are closely connected through their role in the Standard Model of particle physics. They share properties and play important roles in describing the fundamental forces and properties of particles.
 

1. What is the SU(2) group and what does it have to do with spin 1/2?

The SU(2) group, also known as the special unitary group, is a mathematical group that describes transformations in 2-dimensional complex vector spaces. It is used in quantum mechanics to describe the spin properties of particles, including particles with spin 1/2, which are fermions.

2. How does the SU(2) group relate to the Pauli matrices?

The Pauli matrices are a set of three 2x2 matrices that are used to represent the spin operators in quantum mechanics. These matrices are a basis for the SU(2) group, meaning that any SU(2) transformation can be represented as a combination of these matrices.

3. What is the significance of the Casimir operator in the SU(2) group?

The Casimir operator is a special operator in the SU(2) group that commutes with all other operators in the group. This means that it is a physically conserved quantity, and in the context of spin 1/2 particles, it represents the total spin angular momentum.

4. How does the SU(2) group relate to the concept of angular momentum in quantum mechanics?

In quantum mechanics, angular momentum is a property of particles that describes their rotational motion. The SU(2) group is used to mathematically describe this angular momentum, with the Pauli matrices representing the different possible spin states of particles.

5. Can the SU(2) group be extended to higher spin values?

Yes, the SU(2) group can be extended to higher spin values, including spin 1, spin 3/2, and so on. This leads to the concept of the SU(n) group, which describes transformations in n-dimensional complex vector spaces and is used to describe particles with higher spin values.

Similar threads

Replies
7
Views
813
Replies
2
Views
944
  • Quantum Physics
Replies
3
Views
1K
  • Quantum Physics
Replies
4
Views
660
Replies
4
Views
4K
Replies
1
Views
874
Replies
2
Views
2K
  • Quantum Physics
2
Replies
61
Views
1K
  • Quantum Physics
Replies
3
Views
1K
Replies
15
Views
1K
Back
Top