A question in four parts 4 supergravity by daniel z freedman and antoine van proeyen is quite excellent for illustrating clifford algebra techniques and calculations in the classical susy/sugra in general (in the component formalism) What are the main problems which supersymmetry purports to solve
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What would constitute lack of evidence for susy at the proposed lhc energy scales (e.g
In strathdeee's extended poincare supersymmetry, the first entry on page 16 lists the massless multiplets of 6d $\\mathcal{n} = (1,0)$ supersymmetry as $2^2 = (2,1
However, susy representations furnish reducible poincaré representations, so supermultiplets in general correspond to multiple particles having the same mass, which are related by supersymmetry transforms In this context, the broader term multiplet is used interchangeably with supermultiplet. I don't understand what this means I think i figured out the meaning of this after some research so, i am posting an answer to my own question
The answer is there is nothing called $\mathcal {n}= (1,1)$ superalgebra The superalgebra is always named by $\mathcal {n}$ with integers The $\mathcal {n}= (1,1)$ actually means a supergravity multiplet so my original question was wrong We get this multiplet as the massless level of.
However, the quadratically divergent corrections are still absent.
2 i am currently trying to read into susy and i am running into trouble with the van der waerden spinor notation for weyl spinors I am looking for resources that construct and justify the index notation given to the weyl spinors, especially van der waerden spinor notation.
