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Optimizing the second hyperpolarizability with minimally-parametrized potentials

The dimensionless zero-frequency intrinsic second hyperpolarizability γ_{int}=γ/4E_{10}^{-5}m^{-2}(e\hbar)^{4} was optimized for a single electron in a 1D well by adjusting the shape of the potential. Optimized potentials were found to have hyperpolarizabilities in the range -0.15\lessapproxγ_{int}\lessapprox0.60 ; potentials optimizing gamma were arbitrarily close to the lower bound and were within \sim0.5% of the upper bound. All optimal potentials posses parity symmetry. Analysis of the Hessian of γ_{int} around the maximum reveals that effectively only a single parameter, one of those chosen in the piecewise linear representation adopted, is important to obtaining an extremum. Prospects for designing new chromophores based on the design principle here elucidated are discussed.