Superpotential

In theoretical physics, the superpotential is a parameter in supersymmetric quantum mechanics. In theoretical physics, the superpotential is a parameter in supersymmetric quantum mechanics. Consider a one-dimensional, non-relativistic particle with a two state internal degree of freedom called 'spin'. (This is not quite the usual notion of spin encountered in nonrelativistic quantum mechanics, because 'real' spin applies only to particles in three-dimensional space.) Let b and its Hermitian adjoint b† signify operators which transform a 'spin up' particle into a 'spin down' particle and vice versa, respectively. Furthermore, take b and b† to be normalized such that the anticommutator {b,b†} equals 1, and take that b2 equals 0. Let p represent the momentum of the particle and x represent its position with =i, where we use natural units so that ℏ = 1 {displaystyle hbar =1} . Let W (the superpotential) represent an arbitrary differentiable function of x and define the supersymmetric operators Q1 and Q2 as Note that Q1 and Q2 seem self-adjoint. Let the Hamiltonian be where W' signifies the derivative of W. Also note that {Q1,Q2}=0. Under these circumstances, the above system is a toy model of N=2 supersymmetry. The spin down and spin up states are often referred to as the 'bosonic' and 'fermionic' states, respectively, in an analogy to quantum field theory. With these definitions, Q1 and Q2 map 'bosonic' states into 'fermionic' states and vice versa. Restricting to the bosonic or fermionic sectors gives two partner potentials determined by In supersymmetric quantum field theories with four spacetime dimensions, which might have some connection to nature, it turns out that scalar fields arise as the lowest component of a chiral superfield, which tends to automatically be complex valued. We may identify the complex conjugate of a chiral superfield as an anti-chiral superfield. There are two possible ways to obtain an action from a set of superfields: