# Valley-resolved and Brillouin-zone-integrated topological high-harmonic emission ## Physical setting Work in atomic units. Consider a two-band Haldane model on a hexagonal lattice with two sites per unit cell. Let $$ \boldsymbol\delta_1=\frac{a}{2}(1,\sqrt{3}),\qquad \boldsymbol\delta_2=\frac{a}{2}(1,-\sqrt{3}),\qquad \boldsymbol\delta_3=-a(1,0), $$ and $$ \mathbf g_1=\mathbf a_1-\mathbf a_2,\qquad \mathbf g_2=-\mathbf a_1,\qquad \mathbf g_3=\mathbf a_2, $$ where $$ \mathbf a_1=\frac{a}{2}(3,\sqrt{3}),\qquad \mathbf a_2=\frac{a}{2}(3,-\sqrt{3}). $$ Use the Bloch Hamiltonian $$ H(\mathbf k)=\mathbf d(\mathbf k)\cdot\boldsymbol\sigma, $$ with $$ \begin{aligned} d_x(\mathbf k)&=t_1\sum_{n=1}^{3}\cos(\mathbf k\cdot\boldsymbol\delta_n),\\ d_y(\mathbf k)&=-t_1\sum_{n=1}^{3}\sin(\mathbf k\cdot\boldsymbol\delta_n),\\ d_z(\mathbf k)&=M+2\,\operatorname{Im}(t_2) \sum_{n=1}^{3}\sin(\mathbf k\cdot\mathbf g_n). \end{aligned} $$ The shared parameters are $$ a=2.683,\qquad M=0.026,\qquad t_1=-0.1. $$ Compare two physical cases, $t_2=-0.0013i$ and $t_2=-0.0087i$. Drive the system along the $\Gamma$-$M$ direction through the Peierls shift $\mathbf k\mapsto\mathbf k+\mathbf A(t)$, with $$ \mathbf A(t)=A_0\sin^2\!\left(\frac{\omega t}{2n_{\mathrm{cyc}}}\right) \sin(\omega t)\,\hat{\mathbf e}_{\parallel}, \qquad 0\le t\le\frac{2\pi n_{\mathrm{cyc}}}{\omega}, $$ and $\mathbf A(t)=0$ outside the pulse. Use $A_0=0.1$, $\omega=0.0075$, and $n_{\mathrm{cyc}}=5$. Treat the driven crystal within independent-electron dynamics of this two-band Bloch Hamiltonian, starting from its lower band. Characterize the emitted high-harmonic field through its complex components parallel and perpendicular to the driver. Use one consistent Fourier convention and a common normalization; absolute spectral intensity is not a grading target. ## Research problem Determine whether and how the change between the two Haldane-model cases affects the polarization and helicity of high-harmonic emission, and establish the relation between the valley-resolved response at the inequivalent $K$ and $K'$ points and the observable response of a completely occupied lower band. Use your computed harmonic yields and complex channel phases to decide whether the valley response follows one common rule at both valleys. Determine whether any polarization information remains in the integrated response, and state what that observable can and cannot establish about its microscopic crystal-momentum origin. Limit all conclusions to the bulk, independent-electron, two-band model specified above. Your evidence must keep the two model cases, the $K$ and $K'$ initial states, the fixed-valley and filled-band calculations, and the two response directions unambiguous. The derivation, numerical representation, Brillouin-zone sampling, propagator, time step, differentiation and Fourier procedures, treatment of weak components, reliability strategy, normalization, plotting choices, and report organization are for you to decide and justify. No particular number, order, or layout of figures is prescribed. ## Submission and resources Submit one self-contained scientific report and an auditable offline calculation package containing the task-specific derivation, code, numerical data underlying all material claims, a provenance note listing every offline source or software document actually consulted and the method basis for items supplied from general knowledge, and concise run and environment information. 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