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| # Spectral confinement of phase-matched slow electrons | |
| ## Background | |
| A free electron exchanging photons with a phase-matched optical mode occupies | |
| an energy ladder separated by the photon energy. Many descriptions developed | |
| for much faster electrons linearize the dispersion and treat this ladder as an | |
| effectively extended multilevel system. Whether that approximation remains | |
| adequate at low kinetic energy must be established rather than assumed. | |
| ## Research problem | |
| Determine whether and how a phase-matched optical field can confine the | |
| energy-domain evolution of a slow electron. Establish a quantitative physical | |
| distinction between Raman-Nath and Bragg dynamics, and assess whether the | |
| specified low-energy interaction can realize coherent control within a reduced | |
| energy-state manifold. | |
| The derivation, numerical construction, choice of discriminating evidence and | |
| organization of the argument are yours. Your conclusions must follow from your | |
| calculation rather than from an assumed regime label or a finite numerical | |
| basis. | |
| ## Physical model and inputs | |
| Use a one-dimensional relativistic minimal-coupling model along the electron | |
| propagation direction. Expand the field-free dispersion through quadratic | |
| order about the initial momentum $p_0$. Retain the symmetrized $Ap$ coupling | |
| and the $A^2$ interaction in the production model. Let $e>0$ denote the | |
| magnitude of the electron charge and use the monochromatic optical mode | |
| $$ | |
| A(z,t)=-\frac{E_f}{\omega} | |
| \sin(\omega t-k_z z+\phi_0). | |
| $$ | |
| Impose phase matching, $k_z=\omega/v_0$. Use a Floquet-Bloch sideband | |
| description with momenta $k_n=k_0+n k_z$ and energies separated by | |
| $\hbar\omega$. Derive the coupled dynamics needed for the research question; | |
| do not replace the production model by a linear nonrecoil model. A consistently | |
| transformed charge, phase or sideband-index convention is acceptable. | |
| Investigate both cases below with the same physical model: | |
| | Quantity | Case I | Case II | | |
| |---|---:|---:| | |
| | Phase-matched reference kinetic energy | $100\ \mathrm{eV}$ | $16\ \mathrm{eV}$ | | |
| | Initial state | single-energy $n=0$ state | $12\ \mathrm{eV}$ state, $n=-1$ | | |
| | Photon energy $\hbar\omega$ | $1.54\ \mathrm{eV}$ | $4\ \mathrm{eV}$ | | |
| | Electric-field amplitude $E_f$ | $0.5\ \mathrm{V\,nm^{-1}}$ | $0.1\ \mathrm{V\,nm^{-1}}$ | | |
| | Initial optical phase $\phi_0$ | $0$ | $0$ | | |
| Task unit-resolution convention for Case II: the field amplitude is | |
| $10^8\ \mathrm{V\,m^{-1}}=0.1\ \mathrm{V\,nm^{-1}}$. | |
| Construct the final electron-energy evidence from the sideband probabilities | |
| $|a_n(t)|^2$ with a declared energy mapping and normalization convention. | |
| Absolute probability is physically fixed by state normalization; colour, | |
| interpolation and display layout are not grading targets. | |
| ## Research boundary | |
| Use the stated one-dimensional Floquet-Bloch minimal-coupling model. A full | |
| Maxwell-field simulation, multidimensional electron propagation or an | |
| experimental device model is outside the required task. Analytical reductions | |
| may support the argument, but they do not replace the production calculation | |
| when omitted couplings change the physical object. | |
| All basis truncations, time sampling, propagation algorithms, plotting domains | |
| and diagnostic constructions not fixed above are yours. You are responsible | |
| for ensuring that the evidence is sufficiently reliable and reproducible for | |
| the claims made, but no grid, solver, truncation size, 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, reconstructible 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 and | |
| number of figures are yours. No fixed file tree, filename scheme, complete | |
| exploratory history or diagnostic prescribed by the evaluator 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 | |
| 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. | |