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| # When can a scattering model account for an attoclock offset? | |
| ## Background | |
| In an attoclock measurement, the maximum of the photoelectron momentum | |
| distribution is displaced from the direction expected from the laser vector | |
| potential at ionization. That displacement is often discussed as a timing | |
| observable, but the outgoing electron also scatters from the residual binding | |
| potential. | |
| ## Research problem | |
| For a short circularly polarized pulse, determine whether the intensity | |
| dependence of the offset angle can be accounted for by a post-release | |
| central-potential scattering model. Establish how far a conclusion obtained | |
| for an unscreened Coulomb target remains valid as the interaction is screened, | |
| and state what the resulting evidence does and does not establish about a | |
| universal interpretation of the attoclock offset. | |
| Choose the derivation, numerical evidence, comparisons and presentation needed | |
| to make that assessment scientifically convincing. The number and arrangement | |
| of figures are for you to decide. | |
| ## Physical inputs | |
| Work in atomic units. Use a circular driver of angular frequency | |
| $\omega=0.057$ and the intensity convention | |
| $$ | |
| I=2E_0^2,\qquad A_0=\frac{E_0}{\omega}, | |
| $$ | |
| where $E_0$ and $A_0$ are the peak electric-field and vector-potential | |
| amplitudes. Study a one-electron target with ionization potential | |
| $I_p=0.5$ under both | |
| $$ | |
| V_C(r)=-\frac{1}{r} | |
| $$ | |
| and the screened family | |
| $$ | |
| V_{\lambda}(r)=-\frac{Z_{\lambda}}{r}e^{-r/\lambda}. | |
| $$ | |
| For every finite $\lambda$, determine $Z_{\lambda}$ so that the field-free | |
| ground-state binding energy remains $I_p=0.5$. Include the Coulomb limit, the | |
| strong-screening case $\lambda=1$, and enough intermediate screening lengths | |
| of your choice to test whether an inference from either endpoint transfers | |
| across the family. | |
| ## Method and scope boundary | |
| Build the reduced model from the standard weak-field Keldysh exit scale, the | |
| stated vector-potential momentum scale, and the outgoing half of a | |
| central-potential scattering trajectory. Derive and declare the resulting | |
| angle convention. Standard Rutherford and screened central-potential | |
| scattering theory may be derived or cited. State the approximation level of | |
| the screened calculation you use. | |
| Choose an intensity domain that resolves the regimes needed for your claim | |
| while remaining consistent with the physical assumptions you invoke. Numerical | |
| grids, root solvers, quadrature, sampling, tolerances, plotting ranges and | |
| reliability tests are your choices. They are not grading targets in themselves; | |
| their consequences for the physical evidence are. | |
| High-cost TDSE/iSURF propagation and CTMC regeneration are outside the required | |
| task. They may be discussed as external tests, but neither is required and | |
| unsupported numerical data from those methods must not be presented as your | |
| own result. | |
| ## Submission and resources | |
| Submit one self-contained scientific report and an auditable offline | |
| calculation package. Include the task-specific derivation, code, 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 environment | |
| and run information. No fixed file tree, filename scheme, figure 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 and temporary-storage allowance are binding. | |
| No separate aggregate CPU-hour limit applies. | |
| Optional extensions must be clearly separated and do not earn extra credit | |
| merely by using more computation. | |
| ## Reference and integrity policy | |
| Complete this task without network access or live literature | |
| retrieval. You may rely on your existing general scientific knowledge and, if any are | |
| explicitly supplied with this task, 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 while completing this task. | |
| 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. | |