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| # Quantum-informed trajectory modelling of strong-field photoelectron spectra | |
| ## Background and physical system | |
| Semiclassical trajectory models provide an interpretable account of continuum | |
| electron motion, but their predictive value depends on how the outgoing | |
| wavepacket is represented as trajectory input. Investigate whether a | |
| quantum-informed trajectory description can give a quantitatively credible | |
| account of strong-field ionization while retaining a semiclassical description | |
| of continuum dynamics. | |
| Work in atomic units with the one-dimensional single-electron potential | |
| $$ | |
| V(x)=-\frac{1}{\sqrt{x^2+a^2}},\qquad a=1, | |
| $$ | |
| and initialize the electron in its field-free ground state. The laser field is | |
| defined by | |
| $$ | |
| A(t)=(-1)^{n+1}\frac{F_0}{\omega} | |
| \sin^2\!\left(\frac{\omega t}{2n}\right) | |
| \sin(\omega t+\phi), | |
| \qquad 0\leq t\leq t_f=\frac{2\pi n}{\omega}, | |
| $$ | |
| with $A(t)=0$ outside the pulse and $F(t)=-dA/dt$. Use | |
| $$ | |
| n=4,\qquad F_0=0.0757,\qquad \omega=0.057,\qquad \phi=0. | |
| $$ | |
| ## Research problem | |
| Assess whether a semiclassical two-step model with quantum input gives a | |
| defensible account of the final photoelectron momentum distribution for this | |
| target and pulse when judged against both a conventional one-dimensional | |
| semiclassical two-step (SCTS) calculation and an independently converged direct | |
| TDSE result. Determine which information carried by the quantum input is | |
| material to the agreement or disagreement you establish, and delimit the | |
| physical and numerical scope supported by your calculated evidence. | |
| How you derive the model, organize the comparisons and construct evidence for | |
| the final judgment is for you to decide. Base the conclusion on your own | |
| calculated final photoelectron signal; qualitative resemblance by itself does | |
| not establish model validity. | |
| ## Model identity and scope | |
| In the quantum-input model, the trajectory input is the **complex** | |
| position--momentum amplitude obtained from a Gaussian-window Gabor | |
| representation of the newly outgoing wavefunction removed by an absorbing | |
| boundary. Classical trajectories evolve in the stated laser and soft-core | |
| fields. Their asymptotic momentum contributions are combined coherently, with | |
| the task-specific semiclassical trajectory phase and the finite postpulse | |
| potential contribution retained. These conditions define the commissioned | |
| model; deriving a consistent computable realization remains part of the task. | |
| All discretization, TDSE extraction, absorbing-boundary, Gabor-window, | |
| sampling, propagation, asymptotic-matching, momentum-binning, normalization | |
| and display choices not fixed above are yours. State choices that materially | |
| affect your claims and provide evidence sufficiently reliable and | |
| reconstructible to support them. A declared common scale may be used; | |
| absolute yield is not a grading target unless independently established by | |
| your calculation. | |
| Do not add multielectron, three-dimensional, relativistic, focal-volume, | |
| macroscopic-propagation or detector-response physics to the required | |
| production model. Clearly separated extensions are permitted but cannot | |
| replace the stated commission. | |
| ## 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. | |