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| # Temporal control of solid-state high-harmonic emission with a shaped driver | |
| ## Physical setting | |
| Consider a one-dimensional crystal described in atomic units by the periodic | |
| single-electron potential | |
| $$ | |
| V(x)=-V_0\left[1+\cos\left(\frac{2\pi x}{d}\right)\right], | |
| \qquad V_0=0.37,\qquad d=8. | |
| $$ | |
| The crystal is driven along its periodic direction by a linearly polarized | |
| $3.2\ \mu\mathrm{m}$ pulse of duration $T=5\tau$, where | |
| $\tau=2\pi/\omega_0$. The peak-field scale $F_0$ corresponds to a peak | |
| intensity of $6.0\times10^{11}\ \mathrm{W\,cm^{-2}}$, and | |
| $$ | |
| f(t)=\sin^2\!\left(\frac{\pi t}{T}\right), | |
| \qquad 0\le t\le T. | |
| $$ | |
| Use the conventional reference field | |
| $$ | |
| \mathbf E_{\mathrm{ref}}(t)=F_0 f(t)\sin(\omega_0 t)\,\hat{\mathbf x} | |
| $$ | |
| and the delay-controlled shaped field | |
| $$ | |
| \mathbf E_{\mathrm{sh}}(t;t_d)=F_0 f(t) | |
| \left[ | |
| \frac{\sin\!\left(\omega_0(t-t_0-t_d)\right)} | |
| {\omega_0(t-t_0-t_d)} | |
| - | |
| \frac{\sin\!\left(\omega_0(t-t_0)\right)} | |
| {\omega_0(t-t_0)} | |
| \right]\hat{\mathbf x}, | |
| \qquad t_0=2.14\tau, | |
| $$ | |
| with each removable singularity understood by continuity. Use one consistent | |
| field-vector-potential convention throughout all comparisons. | |
| The central study is the coherent independent-electron response with the two | |
| lowest bands initially filled; these bands form the valence manifold for this | |
| task. Quantitative dephasing models are outside the required scope. A velocity- | |
| gauge Bloch-basis propagation or a demonstrably equivalent gauge representation | |
| may be used. The primary observable is the emitted high-harmonic response | |
| constructed from the total current over the occupied initial states and the | |
| Brillouin zone. A common normalization is acceptable; absolute spectral | |
| intensity is not a grading target. | |
| ## Research problem | |
| Determine whether the delay-controlled shaped driver provides genuine | |
| temporal control of the high-harmonic cutoff response of this crystal, rather | |
| than merely changing an overall signal scale. Establish the comparison with | |
| the conventional reference pulse, determine how the cutoff energy, its | |
| emission time, and a defensibly defined harmonic yield depend on $t_d$, and | |
| explain the observed behavior in terms of the field-driven band dynamics. | |
| Choose and justify a delay domain broad enough to support the dependence and | |
| scope you claim. Your evidence must make the physical cases and observable | |
| definitions auditable, but the derivation, numerical representation, cutoff | |
| and yield definitions, time-frequency or equivalent timing diagnostic, | |
| controls, reliability strategy, plotting choices, and report organization are | |
| for you to decide. If you infer a functional law, state how it was obtained and | |
| where the evidence supports or fails to support it. | |
| No particular number, order, or layout of figures is prescribed. Crystal- | |
| momentum sampling, basis or plane-wave truncation, time step, propagator, | |
| Fourier estimator or taper, time-frequency resolution, visibility threshold, | |
| interpolation, normalization, and plot range are student choices. State the | |
| choices material to your claims and submit reconstructible numerical data. | |
| ## 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. No fixed file tree, filename scheme, panel count, | |
| or complete exploration history is required. | |
| Resource limits are supplied exclusively by the accompanying | |
| `resource_limits.json`. Its fixed CPU allocation, candidate-active | |
| wall time, network boundary are binding. No separate aggregate CPU-hour limit applies. Greater computational expense | |
| receives no additional credit. | |
| ## Reference and integrity policy | |
| This examination is conducted without network access or live literature | |
| retrieval. You may rely on your existing general scientific knowledge and, if any are | |
| explicitly supplied with the examination, on those offline materials or | |
| software documentation. Record every such source actually consulted. For formulas, | |
| methods, constants, or conventions used from general knowledge rather than a | |
| consulted source, state enough of the method basis, definition, value, units, | |
| and convention to make the calculation auditable; do not invent a citation. | |
| You are not required to identify or prove a publication date or to retrieve | |
| literature during the examination. | |
| The hidden target article and its identifying metadata, figures or captions, | |
| supplementary material, author code or data, target-specific reproduction | |
| code, solution or scoring material, online solutions, and worked | |
| reproductions of this case must not be used. All submitted scientific figures | |
| and numerical data must be generated by your own implementation of the stated | |
| problem. | |
| See [submission requirements](../../submission_requirements.md) for the common submission entry points. | |