2015
DOI: 10.1063/1.4935851
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A world-line framework for 1D topological conformal σ-models

Abstract: We use world-line methods for pseudo-supersymmetry to construct sl(2|1)-invariant actions for the (2, 2, 0) chiral and (1, 2, 1) real supermultiplets of the twisted D-module representations of the sl(2|1) superalgebra. The derived one-dimensional topological conformal σ-models are invariant under nilpotent operators. The actions are constructed for both parabolic and hyperbolic/trigonometric realizations (with extra potential terms in the latter case). The scaling dimension λ of the supermultiplets defines a c… Show more

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Cited by 3 publications
(3 citation statements)
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References 41 publications
(137 reference statements)
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“…The superalgebra ii) is the simplest example of superalgebra associated with the one-dimensional Supersymmetric Quantum Mechanics [24], where H is a Hamiltonian and Q is its (unique) square root supersymmetry operator. The superalgebra iii) enters the topological mechanics, with H playing the role of a scaling operator, see [26].…”
Section: The Minimal Z 2 -Graded Lie Superalgebrasmentioning
confidence: 99%
“…The superalgebra ii) is the simplest example of superalgebra associated with the one-dimensional Supersymmetric Quantum Mechanics [24], where H is a Hamiltonian and Q is its (unique) square root supersymmetry operator. The superalgebra iii) enters the topological mechanics, with H playing the role of a scaling operator, see [26].…”
Section: The Minimal Z 2 -Graded Lie Superalgebrasmentioning
confidence: 99%
“…In the presence of the oscillatorial term the action is also SL(2)-invariant, but the SL(2) field transformations are trigonometric and carry the dependence on the dimensional parameter (see [9,10] for details). The superconformal topological model [1] can be regarded as a topological twisted supersymmetric version, see [11], of the N = 2 superconformal mechanics introduced in [12].…”
Section: The Bosonic Part Of the Actionmentioning
confidence: 99%
“…Its N = 2 superconformal symmetry closes an sl(2|1) superalgebra, whose generators are the sl(2) subalgebra generators H, D, K, the supersymmetry operators Q 1 , Q 2 , its conformal superpartners Q 1 , Q 2 and a u(1) R-symmetry generator (see [11] for details).…”
Section: The Bosonic Part Of the Actionmentioning
confidence: 99%