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| # Selective high-energy harmonic response in a weakly inhomogeneous field | |
| ## Background and research question | |
| In a periodic solid-state model, the high-energy part of a high-harmonic | |
| response can be much weaker than its lower-energy part, while simply raising | |
| the incident intensity may be incompatible with a material damage threshold. | |
| A weak spatial variation of the driving field offers a possible alternative, | |
| but a brighter spectrum alone does not show whether the useful response has | |
| been selectively changed or merely rescaled. | |
| For the model and field family below, determine whether weak spatial | |
| inhomogeneity can produce a selective and physically useful change of the | |
| high-energy harmonic response. If it can, establish the microscopic origin | |
| and decide whether the calculated evidence supports a change in the emission | |
| dynamics rather than only a common intensity rescaling. If it cannot, delimit | |
| the negative conclusion with equally strong evidence. | |
| Design the derivation, computation, evidence and scientific argument needed to | |
| answer this question. Do not assume the outcome in advance. | |
| ## Physical system | |
| Use atomic units unless stated otherwise. Treat one active electron in the | |
| one-dimensional periodic potential | |
| $$ | |
| V(x)=-V_0\left[1+\cos\left(\frac{2\pi x}{a_0}\right)\right], | |
| \qquad V_0=0.37, | |
| \qquad a_0=8. | |
| $$ | |
| The initial physical state is the field-free $k=0$ state at the top of the | |
| valence band, at the minimum band gap. Use the source-model length-gauge | |
| interaction | |
| $$ | |
| U_{\epsilon}(x,t)=xE(t)+\epsilon x^2E(t), | |
| $$ | |
| where $E(t)$ is a linearly polarized pulse. To close the source-unspecified | |
| carrier convention without selecting a numerical method, use the following | |
| task convention: | |
| $$ | |
| E(t)=E_0\cos^2\!\left(\frac{\pi t}{T}\right)\cos(\omega t), | |
| \qquad |t|\leq \frac{T}{2}, | |
| $$ | |
| and $E(t)=0$ outside that interval, with peak intensity | |
| $8.77\times10^{11}\ \mathrm{W\,cm^{-2}}$, wavelength $3200$ nm and | |
| $T=6(2\pi/\omega)$. Compare | |
| $$ | |
| \epsilon=0,\qquad 0.0002,\qquad 0.0005 | |
| $$ | |
| in the same atomic-unit coordinate convention. Use the same field, time origin | |
| and sign conventions in every compared case, and state the atomic-unit | |
| conversion used for $E_0$ and $\omega$. | |
| ## Research boundary | |
| Use a one-electron time-dependent Schrödinger treatment of the stated model. | |
| The representation, propagation method and scientific evidence package are | |
| your choices. Construct the emitted high-harmonic response from a physically | |
| consistent radiation observable. Any resolved or decomposed quantity used as | |
| evidence must be given a reconstructible mathematical definition; no | |
| particular decomposition is prescribed. | |
| Absolute harmonic yield is not a grading target. Declare any common | |
| normalization and representation conventions used in a comparison. You are | |
| responsible for ensuring that the evidence is sufficiently reliable and | |
| reproducible to support the claims made, but no grid, box, solver, absorber, | |
| window, transform, survey range or validation procedure is prescribed. | |
| ## Submission and resources | |
| Submit one self-contained scientific report and an offline reproduction | |
| package containing the producing code, the numerical data underlying 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. The organization of the report and the choice of evidence are | |
| yours. No fixed figure set, file tree, filename scheme or complete exploratory | |
| history is required. | |
| The available CPU allocation, candidate active deadline, node, network, | |
| memory and scratch limits are specified in the accompanying | |
| `resource_limits.json`. Complete the derivation, implementation, | |
| calculation, validation, interpretation and final-file preparation within these | |
| resource limits. More expensive modelling 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. | |