Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents

被引:23
作者
Buchbinder, I. L. [1 ,2 ,3 ]
Gates, S. James, Jr. [4 ]
Koutrolikos, Konstantinos [5 ]
机构
[1] Tomsk State Pedag Univ, Dept Theoret Phys, Tomsk 634041, Russia
[2] Natl Res Tomsk State Univ, Lenina Ave, Tomsk 634050, Russia
[3] Univ Fed Juiz de Fora, Dept Fis, ICE, Campus Univ, BR-36036900 Juiz De Fora, MG, Brazil
[4] Brown Univ, Dept Phys, Box 1843,182 Hope St,Barus & Holley 545, Providence, RI 02912 USA
[5] Masaryk Univ, Inst Theoret Phys & Astrophys, CS-61137 Brno, Czech Republic
来源
JOURNAL OF HIGH ENERGY PHYSICS | 2018年 / 05期
关键词
Superspaces; Supersymmetric Effective Theories; CUBIC INTERACTION VERTICES; MASSLESS GAUGE SUPERFIELDS; POINCARE GROUP; INTERACTION TERMS; FIELDS; REPRESENTATIONS; CONSTRUCTION; SYMMETRIES;
D O I
10.1007/JHEP05(2018)204
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We consider a four dimensional generalized Wess-Zumino model formulated in terms of an arbitrary chiral potential K(Phi,(Phi) over bar) and an arbitrary chiral superpotential W(Phi). A general analysis is given to describe the possible interactions of this theory with external higher spin gauge superfields of the (s vertical bar 1, s vertical bar 1/2) supermultiplet via higher spin supercurrents. It is shown that such interactions do not exist beyond supergravity (s >= 2) for any K, and W. However, we find three exceptions, the theory of a free massless chiral, the theory of a free massive chiral and the theory of a free chiral with linear superpotential. For the first two, the higher spin supercurrents are known and for the third one we provide the explicit expressions. We also discuss the lower spin supercurrents. As expected, a coupling to (non -minimal) supergravity (s = 1) can always be found and we give the generating supercurrent and supertrace for arbitrary 1C and W. On the other hand, coupling to the vector supermultiplet (s = 0) is possible only if K = K((Phi) over bar Phi) and W = 0.
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页数:27
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