1992
DOI: 10.1016/0003-4916(92)90350-u
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Extended superconformal Galilean symmetry in Chern-Simons matter systems

Abstract: We study the nonrelativistic limit of the N = 2 supersymmetric Chern-Simons matter system. We show that in addition to Galilean invariance the model admits a set of symmetries generated by fermionic charges, which can be interpreted as an extended Galilean supersymmetry . The system also possesses a hidden conformal invariance and then the full group of symmetries is the extended superconformal Galilean group. We also show that imposing extended superconformal Galilean symmetry determines the values of the cou… Show more

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Cited by 83 publications
(192 citation statements)
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“…To answer this question, it is first necessary to understand and further explore the notion of "non-relativistic supersymmetry" itself. While specific examples of non-relativistic supersymmetric field theories have been constructed previously [22][23][24], many aspects of this subject still remain unexplored.…”
Section: Jhep06(2016)028mentioning
confidence: 99%
“…To answer this question, it is first necessary to understand and further explore the notion of "non-relativistic supersymmetry" itself. While specific examples of non-relativistic supersymmetric field theories have been constructed previously [22][23][24], many aspects of this subject still remain unexplored.…”
Section: Jhep06(2016)028mentioning
confidence: 99%
“…The Galilean invariance as well as non-relativistic conformal invariance (known as Schrödinger invariance [3,7,18,19]) can be implemented by directly taking the non-relativistic limit of relativistic Chern-Simons-matter theory in the same dimension [10,11]. The construction can be applied to the supersymmetric Chern-Simons-matter theory as well [12], and explicit examples of non-relativistic superconformal field theories have been constructed in this way [14,16]. As a particular example, various non-relativistic limits of the M2-brane gauge theory were scrutinized in [15], 1 which may admit the explicit gravity solution that can be studied in the context of non-relativistic AdS/CFT correspondence.…”
Section: Introductionmentioning
confidence: 99%
“…[10]. Notice that terms of the potential proportional to λ 2 and λ 3 would be equivalent to each other in ordinary space and that the term proportional to λ 4 would be identically zero due to the anticommuting character of the fermion fields.…”
mentioning
confidence: 99%
“…Notice that terms of the potential proportional to λ 2 and λ 3 would be equivalent to each other in ordinary space and that the term proportional to λ 4 would be identically zero due to the anticommuting character of the fermion fields. We have chosen a particular sign for the Pauli interaction (corresponding to a "down" spinor) which coincides with the one in [10].…”
mentioning
confidence: 99%
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