Abstract
In the absence of gauge interactions the spontaneous breakdown of supersymmetry (Susy) is accompanied by a scalar field whose vacuum expectation value is not determined by the tree potential. Inclusion of the gauge interactions can fix this vev at the tree level. The situation is exemplified by a simpleSU(2)-model yielding nonvanishingF-andD-vevs.
Similar content being viewed by others
References
L. O'Raifeartaigh: Nucl. Phys.B96, 331 (1975)
P. Fayet, J. Iliopoulos: Phys. Lett.51B, 461 (1974)
B. Zumino: Lecture Notes in Physics, No. 160, p. 137. Berlin, Heidelberg, New York: Springer 1982; J. Wess: Supersymmetric gauge theories. The 1982 Trieste Proceedings. World Publishing Co. to be published
J. Wess, B. Zumino: Nucl. Phys.B70, 39 (1974); A. Salam, J. Strathdee: Nucl. Phys.B87, 85 (1975); Nucl. Phys.B97, 293 (1975); P. Fayet: Nucl. Phys.B90, 104 (1975)
S. Samuel, J. Wess: A Superfield formulation of the non-linear realization of supersymmetry and its coupling to Supergravity. Columbia Preprint CU-TP-258, Nov. 1982
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Dragon, N. Susy-breaking without sliding vev. Z. Phys. C - Particles and Fields 19, 115–117 (1983). https://doi.org/10.1007/BF01571771
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01571771