2008
DOI: 10.1142/s0217732308023761
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Refining the Classification of the Irreps of the 1d N-Extended Supersymmetry

Abstract: The linear finite irreducible representations of the algebra of the 1D N -Extended Supersymmetric Quantum Mechanics are discussed in terms of their "connectivity" (a symbol encoding information on the graphs associated to the irreps). The classification of the irreducible representations with the same fields content and different connectivity is presented up to N ≤ 8.

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Cited by 41 publications
(94 citation statements)
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“…In this spirit, the authors of [9][10][11][12][13][14][15] developed a detailed classification of a huge class (∼ 10 12 for no more than 32 supersymmetries) of worldline supermultiplets wherein each supercharge maps each component field to precisely one other component field or its derivative, and which are faithfully represented by graphs called Adinkras; see also [16][17][18][19][20][21][22]. The subsequently intended dimensional extension has been addressed recently [7,8], and the purpose of the present note is to complement this effort and identify an easily verifiable obstruction to dimensional extension.…”
Section: Introduction Results and Summarymentioning
confidence: 99%
“…In this spirit, the authors of [9][10][11][12][13][14][15] developed a detailed classification of a huge class (∼ 10 12 for no more than 32 supersymmetries) of worldline supermultiplets wherein each supercharge maps each component field to precisely one other component field or its derivative, and which are faithfully represented by graphs called Adinkras; see also [16][17][18][19][20][21][22]. The subsequently intended dimensional extension has been addressed recently [7,8], and the purpose of the present note is to complement this effort and identify an easily verifiable obstruction to dimensional extension.…”
Section: Introduction Results and Summarymentioning
confidence: 99%
“…Let us consider a D-module irrep of a N -extended superconformal algebra (for our purposes N = 1, 2, 4, 8) acting on a (k, N , N − k) supermultiplet [29,30,31,32] (namely, k propagating bosons, N fermions and N − k bosonic auxiliary fields). In the linear basis the propagating bosons are labeled as x 1 , ..., x k , the fermions as ψ 1 , ..., ψ N and the auxiliary bosons as b 1 , ..., b N −k .…”
Section: Introductionmentioning
confidence: 99%
“…The former approach obviously will contain remnants of information about the symmetries of the higher dimensional spacetime. How are these data "downloaded" onto the theories constructed from a purely adinkra network-based [1,2,3,4,5,6,7,8,9,10] approach?…”
Section: Introductionmentioning
confidence: 99%