Skip to content
DraconiticResearch
Search Sources API
203,203 studies31 sourcesUpdated 25 min ago
PreprintCC BY 4.0arXiv

Signature of Short-Range Order in Static Response of the Three-Dimensional Electron Gas

Abstract

The three-dimensional electron gas is a fundamental model in condensed matter physics and quantum chemistry, and the exchange-correlation energy derived from it serves as the starting point of \textit{ab initio} computations of materials. However, the wave-vector-dependent response, and hence the static local field factor G(q), has remained without accurate ground-state benchmark in the strongly coupled regime for three decades. Using diffusion Monte Carlo, we calculate the static density-density response function and G(q) across the liquid phase and find a pronounced structure in G(q) at intermediate wave vectors, already visible at metallic densities and growing with increasing interaction strength. We identify it as a fingerprint of short-range order by showing that it is required to reproduce the static structure factor. Our parametrization, valid in the entire liquid phase, predicts a low-energy resonant mode inside the particle-hole continuum.

Related

  1. Exchange self-energy and vertex corrections to static screening in the two-dimensional electron gas
    Sankar Das Sarma
    arXivPreprintarXiv licenceFull textCondensed matterarXiv
  2. Static Response of the Strongly Coupled Electron Gas from Diffusion Monte Carlo
    Muhammed H. Güneş, Yubo Yang, Vitaly Gorelov +4
    arXivPreprintCC BY 4.0Full textComputational physicsCondensed matterarXivHAL
  3. For any static interaction the self-energy and vertex corrections to the electron-gas polarizability combine exactly into one integrand free of the Coulomb singularity
    Carl A. Kukkonen
    arXivPreprintarXiv licenceFull textCondensed matterarXiv
  4. Static spin exchange-correlation kernel of the uniform electron gas at finite temperature
    Pengcheng Hou, Zhiyi Li, Youjin Deng +1
    arXivPreprintarXiv licenceFull textComputational physicsCondensed matterarXiv
  5. Static linear response of hot and dense QCD matter to electromagnetic fields: Leading hard and soft QCD corrections
    Osvaldo Ferreira, Eduardo S. Fraga, Tyler Gorda +3
    arXivPreprintCC BY 4.0Full textHigh-energy & particle physicsNuclear physicsarXiv
BibTeX
@misc{gunes2026signature,
  title = {{Signature of Short-Range Order in Static Response of the Three-Dimensional Electron Gas}},
  author = {Muhammed H. Güneş and Yubo Yang and Vitaly Gorelov and Miguel A. Morales and Matteo Gatti and Lucia Reining and Shiwei Zhang},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2609.10006},
  eprint = {2609.10006},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.10006},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Signature of Short-Range Order in Static Response of the Three-Dimensional Electron Gas
AU  - Muhammed H. Güneş
AU  - Yubo Yang
AU  - Vitaly Gorelov
AU  - Miguel A. Morales
AU  - Matteo Gatti
AU  - Lucia Reining
AU  - Shiwei Zhang
PY  - 2026
DA  - 2026/10/29
PB  - arXiv
DO  - 10.48550/arxiv.2609.10006
UR  - https://arxiv.org/abs/2609.10006
AB  - The three-dimensional electron gas is a fundamental model in condensed matter physics and quantum chemistry, and the exchange-correlation energy derived from it serves as the starting point of \textit{ab initio} computations of materials. However, the wave-vector-dependent response, and hence the static local field factor G(q), has remained without accurate ground-state benchmark in the strongly coupled regime for three decades. Using diffusion Monte Carlo, we calculate the static density-density response function and G(q) across the liquid phase and find a pronounced structure in G(q) at intermediate wave vectors, already visible at metallic densities and growing with increasing interaction strength. We identify it as a fingerprint of short-range order by showing that it is required to reproduce the static structure factor. Our parametrization, valid in the entire liquid phase, predicts a low-energy resonant mode inside the particle-hole continuum.
ER  -