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| # Quantum-statistical radiation pressure in strong-field ionization | |
| ## Physical setting | |
| Work in atomic units. The laser propagates along $+z$ and is circularly | |
| polarized in the $x$-$y$ plane. The measured longitudinal observable is the | |
| photoelectron momentum $p_z$. Treat direct ionization with a leading-order | |
| light-front nondipole strong-field approximation; rescattering is outside this | |
| problem. | |
| Compare two measurement regimes. | |
| For the photon-traced regime, consider H and Na driven either by bright | |
| squeezed vacuum (BSV) or by coherent light at the same mean incident | |
| intensity. Use wavelength $1580\,\mathrm{nm}$, a ten-cycle pulse, and an | |
| intensity domain within $10^{12}$--$10^{13}\,\mathrm{W\,cm^{-2}}$ broad | |
| enough to resolve the state-dependent intensity response. For BSV, define the | |
| amplitude width by | |
| $$ | |
| I=2\omega^2 A_{\rm rms}^2, | |
| $$ | |
| and use the bright-field limit. Standard, cited ionization potentials for H | |
| and Na may be used. | |
| For the photon-number-conditioned regime, consider Na at $400\,\mathrm{nm}$ | |
| with squeezing parameter $r=15$, mean incident intensity | |
| $10^{13}\,\mathrm{W\,cm^{-2}}$, mode-amplitude scale | |
| $\epsilon_V=3.2\times10^{-8}$ a.u., and a ten-cycle pulse. Study one | |
| neighboring pair of final photon-number channels in the low-effective-intensity | |
| regime near $10^{13}\,\mathrm{W\,cm^{-2}}$. The channel-conditioned field | |
| amplitude is to be evaluated by a bounded two-coherent-point approximation: | |
| the two points have phases separated by $\pi$ and use a common radius | |
| $$ | |
| \rho=\sqrt{\frac{n}{2-\tanh r}} | |
| $$ | |
| for the neighboring pair. At each point, evaluate the complete finite-pulse | |
| direct nondipole-SFA amplitude. Use the exact squeezed-vacuum/Fock overlaps and | |
| sum the two complex contributions before taking the modulus squared. | |
| If you use a matched incoherent control, it must differ only by removal of the | |
| cross term. Such a control is one optional diagnostic, not a required evidence | |
| route. Any alternative diagnostic used to distinguish coherent and | |
| incoherent explanations must preserve the same field points, overlaps, | |
| physical parameters, numerical domain, normalization relation, and final | |
| electron observable, so that it isolates the amplitude-level cross term rather | |
| than changing the physical problem. | |
| For finite-pulse calculations, the supplied reference convention is a | |
| $\cos^4$ vector-potential envelope with total duration $10T$. Handedness, | |
| axis, overall phase, normalization, and smooth-envelope conventions that are | |
| physically equivalent are acceptable when declared and when they do not alter | |
| the material conclusions. No particular momentum grid, time sampling, | |
| quadrature, binning, transform window, or display convention is prescribed. | |
| ## Research problem | |
| Determine how longitudinal radiation-pressure transfer depends on the quantum | |
| state of the driving field and on whether the outgoing photon state is traced | |
| or resolved into neighboring final-number channels. For the bounded | |
| conditioned case, determine what information, if any, the channel-resolved | |
| electron signal supports about the relation between alternative field | |
| pathways. Establish which similarities and differences between the two | |
| measurement regimes are supported by your own calculation, without assuming | |
| in advance that conditioning must reveal, preserve, or remove a particular | |
| kind of information. | |
| Distinguish conclusions supported by the bounded low-field conditioned case | |
| from claims requiring a larger channel or intensity survey. The detailed | |
| derivation, numerical realization, evidence package, controls, | |
| representations, plotting choices, and report organization are for you to | |
| choose and justify. The conclusion must remain within the direct-ionization, | |
| leading-order nondipole and stated target/field scope. | |
| ## Submission and resources | |
| Submit one self-contained scientific report and an auditable offline | |
| calculation package containing the task-specific derivation, code, underlying | |
| numerical data for every material claim, 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, figure | |
| count, output order, 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. | |