Abstract <p>We propose a simple model of two-dimensional <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal{N} = 2\)</EquationSource> <!--PhysPNLt2570164Krivonos-m1--> </InlineEquation> superconformal mechanics with a spin-orbit interaction term and demonstrate that it inherits the Galilean symmetry of the initial free-particle system. We then propose a quaternionic counterpart of this system, which describes the four-dimensional <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathcal{N} = 4\)</EquationSource> <!--PhysPNLt2570164Krivonos-m2--> </InlineEquation> superconformal mechanics <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(D(1,2{\kern 1pt} |{\kern 1pt} \alpha )\)</EquationSource> <!--PhysPNLt2570164Krivonos-m3--> </InlineEquation>. The bosonic part of the Hamiltonian describes a free particle on the cone, while the fermionic part necessarily includes the spin–orbit interaction term.</p>

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Note on Supersymmetric Mechanics with Spin–Orbit Interaction

  • S. Krivonos,
  • A. Nersessian

摘要

Abstract

We propose a simple model of two-dimensional \(\mathcal{N} = 2\) superconformal mechanics with a spin-orbit interaction term and demonstrate that it inherits the Galilean symmetry of the initial free-particle system. We then propose a quaternionic counterpart of this system, which describes the four-dimensional \(\mathcal{N} = 4\) superconformal mechanics \(D(1,2{\kern 1pt} |{\kern 1pt} \alpha )\) . The bosonic part of the Hamiltonian describes a free particle on the cone, while the fermionic part necessarily includes the spin–orbit interaction term.