Representation of SUSY Algebra

In summary, we discussed how states in the SUSY algebra have the same total spin despite having different spin projections, and how to determine whether fermions are Weyl or Majorana by looking at their transformation properties under CPT.
  • #1
karlzr
131
2
I have some questions about representations of SUSY algebra.
(1) Take ##N=1## as an example. Massive supermultiplet can be constructed in this way:
$$|\Omega>\\
Q_1^\dagger|\Omega>, Q_2^\dagger|\Omega>\\
Q_1^\dagger Q_2^\dagger|\Omega>$$ I understand the z-components ##s_z## of the last state and the first state are the same, but why do they also have the same total spin ##s##?

(2)How do we get to know whether the fermions are Weyl or majorana? For instance ##N=2## hypermultiplet
$$|\Omega_{-\frac{1}{2}}>: \chi_\alpha\\
Q^\dagger|\Omega_{-\frac{1}{2}}>: \phi\\
Q^\dagger Q^\dagger |\Omega_{-\frac{1}{2}}>: \psi^{\dagger \dot{\alpha}}$$ Is this representation CPT invariant? if so, I guess ##\chi## or ##\psi## should be majorana
Or we might need to supplement the states with their CPT conjugates when the two fermion fields are weyl?
 
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  • #2


Hello, thank you for your questions. Let me try to address them one by one.

(1) In SUSY algebra, the supercharges ##Q_1## and ##Q_2## have opposite spinor indices, which means they have different spin projections. However, when acting on the vacuum state ##|\Omega>##, they create states with the same total spin ##s##. This is because the supercharges are defined as a sum of fermionic and bosonic operators, and the overall spin of a state is determined by the number of fermions and bosons it contains. In this case, the states created by the supercharges have one fermion and one boson, giving them the same total spin.

(2) To determine whether the fermions in a representation are Weyl or Majorana, we need to look at the transformation properties under CPT. In the ##N=2## hypermultiplet example, the fermions transform as a Weyl spinor under CPT, which means they are Weyl fermions. This can also be seen from the fact that the fermions have only one spinor index, indicating that they are left- or right-handed. If the fermions were Majorana, they would have two spinor indices and would transform differently under CPT.

I hope this helps clarify your questions. If you have any further questions, please don't hesitate to ask.
 

1. What is SUSY algebra?

SUSY algebra, short for Supersymmetry algebra, is a mathematical framework that describes the relationship between particles with different spin values. It is a type of symmetry that predicts the existence of superpartners for each particle in the Standard Model of particle physics.

2. What is the significance of SUSY algebra in physics?

SUSY algebra is significant because it offers a solution to many issues in particle physics, such as the hierarchy problem and the stability of the Higgs boson. It also provides a possible explanation for dark matter and can potentially unify the fundamental forces of nature.

3. How is SUSY algebra represented mathematically?

SUSY algebra is represented mathematically using a set of operators that transform particles into their superpartners. These operators include the supersymmetry generators, which are fermionic, and the Poincaré generators, which are bosonic.

4. What is the role of SUSY algebra in string theory?

SUSY algebra plays a crucial role in string theory, a theoretical framework that attempts to unify all the fundamental forces of nature. In string theory, the supersymmetry generators are related to the vibrations of strings, and the algebra is used to describe the properties of these strings.

5. What are the current developments in the representation of SUSY algebra?

Currently, there are ongoing efforts to mathematically represent SUSY algebra in higher dimensions, which could provide a more complete understanding of the theory. There is also research being done to explore the implications of SUSY algebra in cosmology and the early universe.

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