# Topological edge states in finite-chain high-harmonic generation ## Background In a finite dimerized chain, opposite structural phases can have different edge-state content even when both are insulating. High-harmonic emission is a coherent many-electron observable, so an edge state need not influence the total radiation in the same way that it changes a one-electron spectrum. ## Research problem Using the continuous-space finite-chain model below, determine whether and how the chain's dimerization topology is encoded in its low-energy high-harmonic response. Establish what role is played by edge-state occupation, and distinguish it from an explanation based only on the static gap, the structural distortion, or the time dependence of the self-consistent Kohn-Sham potential. The derivation, numerical construction, choice of discriminating evidence and organization of the argument are yours. Establish the mechanism from your calculation rather than assuming that the presence of an in-gap state is by itself sufficient. ## Physical inputs Use atomic units. The chain contains $N=100$ fixed singly charged ions and $N=100$ electrons in the spin-neutral configuration $N_\uparrow=N_\downarrow=50$. With $a=2$, define $$ x_i=\left(i-\frac{N+1}{2}\right)a, \qquad x_i'(\delta)=x_i-(-1)^i\delta, \qquad i=1,\ldots,N, $$ and $$ v_{\mathrm{ion}}(x)=-\sum_{i=1}^{N} \frac{1}{\sqrt{[x-x_i'(\delta)]^2+1}}. $$ Use the continuous-space, self-consistent x-only local-spin-density model with the same soft-core interaction in the Hartree and ion-ion terms and $$ v_{\mathrm{xc},\sigma}(x,t)=- \left[\frac{6}{\pi}n_\sigma(x,t)\right]^{1/3}. $$ Correlation is neglected. An SSH or other tight-binding Hamiltonian is not a substitute for this physical model. Investigate the following fixed geometries: | Task label | Dimerization shift | |---|---:| | M | $\delta=0$ | | D+ | $\delta=0.265$ | | D- | $\delta=-0.165$ | These shifts are prescribed structural inputs for the comparison; they are not stated here as numerical minima of a student-computed energy curve. Drive each geometry with $$ A(t)=A_0\sin^2\!\left(\frac{\omega t}{2n_{\mathrm{cyc}}}\right) \sin(\omega t), \qquad 0