Perfect fluid equations with N=1,2 Schrodinger supersymmetry
Timofei Snegirev

TL;DR
This paper develops superconformal extensions of perfect fluid equations with N=1,2 Schrodinger supersymmetry, introducing anticommuting fields as superpartners for fluid variables and analyzing their conserved charges.
Contribution
It constructs superconformal fluid equations with N=1,2 Schrodinger supersymmetry using Hamiltonian and Lagrangian formalisms, including the interpretation of anticommuting variables as vorticity potentials.
Findings
Constructed superconformal fluid equations with N=1,2 supersymmetry.
Derived the full set of conserved charges for these supersymmetric fluids.
Interpreted anticommuting variables as fluid vorticity potentials.
Abstract
Superconformal extensions of the perfect fluid equations, which realize Schrodinger superalgebra, are constructed within the Hamiltonian formalism. They are built by introducing real (for ) or complex (for ) anticommuting field variables as superpartners for the density and velocity of a fluid. The full set of conserved charges associated with the Schrodinger superalgebra is constructed. Within the Lagrangian formalism, when the Clebsch decomposition for the velocity vector field is used, the anticommuting variables can be interpreted as potentials parameterizing fluid's vorticity.
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Taxonomy
TopicsNonlinear Waves and Solitons · Black Holes and Theoretical Physics · Quantum Mechanics and Non-Hermitian Physics
