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Electronic structure of liquid xenon in the context of light dark matter direct detection
by Riccardo Catena, Luca Marin, Marek Matas, Nicola A. Spaldin, Einar Urdshals
Submission summary
| Authors (as registered SciPost users): | Nicola Spaldin |
| Submission information | |
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| Preprint Link: | https://arxiv.org/abs/2502.02965v1 (pdf) |
| Data repository: | https://zenodo.org/records/14774056 |
| Date submitted: | April 1, 2025, 12:14 a.m. |
| Submitted by: | Spaldin, Nicola |
| Submitted to: | SciPost Physics |
| Ontological classification | |
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| Academic field: | Physics |
| Specialties: |
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| Approaches: | Theoretical, Computational |
Abstract
We present a description of the electronic structure of xenon within the density-functional theory formalism with the goal of accurately modeling dark matter-induced ionisation in liquid xenon detectors. We compare the calculated electronic structures of the atomic, liquid and crystalline solid phases, and find that the electronic charge density and its derivatives in momentum space are similar in the atom and the liquid, consistent with the weak interatomic van der Waals bonding. The only notable difference is a band broadening of the highest occupied $5p$ levels, reflected in the densities of states of the condensed phases, as a result of the inter-atomic interactions. We therefore use the calculated density of states of the liquid phase, combined with the standard literature approach for the isolated atom, to recompute ionisation rates and exclusion limit curves for the XENON10 and XENON1T experiments. We find that the broadening of the 5$p$ levels induced by the liquid phase is relevant only at low dark matter masses, where it increases the ionisation rate relative to that of the isolated atom. For most of the probable mass range the energies of the discrete 4$d$ and 5$s$ levels have the strongest effect on the rate. Our findings suggest a simple scheme for calculating dark matter-electron scattering rates in liquid noble gas detectors, using the calculated values for the atom weighted by the density of states of the condensed phase.
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