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N = 1 supersymmetry algebra in 1 + 1 dimensions

 
Wikipedia: N = 1 supersymmetry algebra in 1 + 1 dimensions

In 1 + 1 dimensions the N = 1 supersymmetry algebra (also known as \mathcal{N}=(1,1) because we have one left-moving SUSY generator and one right moving one) has the following generators:

supersymmetric charges: Q, \bar{Q}
supersymmetric central charge: Z\,
time translation generator: H\,
space translation generator: P\,
boost generator: N\,
fermionic parity: \Gamma\,
unit element: I\,

The following relations are satisfied by the generators:

\begin{align}
& \{ \Gamma,\Gamma \} =2I && \{ \Gamma, Q \} =0 && \{ \Gamma, \bar{Q} \} =0\\
&\{ Q,\bar{Q} \}=2Z && \{ Q, Q \}=2(H+P) && \{ \bar{Q}, \bar{Q} \} =2(H-P)  \\
& [N,Q]=\frac{1}{2} Q && [N,\bar{Q} ]=-\frac{1}{2} \bar{Q} && [N,\Gamma]=0 \\
& [N,H+P]=H+P && [N,H-P]=-(H-P) &&
\end{align}

Z\, is a central element.

The supersymmetry algebra admits a \mathbb{Z}_2-grading. The generators H, P, N, Z, I\,
are even (degree 0), the generators Q, \bar{Q}, \Gamma\, are odd (degree 1).

2(H − P) gives the left-moving momentum and 2(H + P) the right-moving momentum.

Basic representations of this algebra are the vacuum, kink and boson-fermion representations, which are relevant e.g. to the supersymmetric (quantum) sine-Gordon model.

References

  • K. Schoutens, Supersymmetry and factorized scattering, Nucl.Phys. B344, 665–695, 1990
  • T.J. Hollowood, E. Mavrikis, The N = 1 supersymmetric bootstrap and Lie algebras, Nucl. Phys. B484, 631–652, 1997, arXiv:hep-th/9606116

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