Excitons in solid molecular hydrogen from quantum Monte Carlo
Abstract
We use quantum Monte Carlo (QMC) methods to investigate the lowest neutral excitation of solid molecular hydrogen in phase-I under increasing compression, with emphasis on structural and response properties. We employ QMC wave functions for the excited state that feature only a single orbital substitution, or a multideterminant expansion including every single particle-hole transition, and compare the results with the Bethe-Salpeter equation (BSE) and time-dependent density-functional theory (TDDFT). We examine a number of nuclear configurations representing thermal and quantum fluctuations. The effect of the multideterminant expansion is marginal on the QMC excitation energies but crucial on the exciton localization and related quantities, irrespective of full optimization and imaginary time projection. In the strong insulating regime at low density, multideterminant QMC results match and in some cases surpass the degree of localization afforded by BSE. A similar trend is observed for transition dipole moments and excitation-induced forces, with generally good agreement between QMC and BSE but marked discrepancies for nuclear configurations where localization differs significantly. TDDFT generally gives a more extended exciton with correspondingly weaker transition dipole moments. These differences decrease upon compression, as the system approaches a semiconducting regime where multiple particle-hole transitions are less important.
Related
- Nuclear quantum effects in the thermal conductivity of solid hydrogen
- Momentum-Locked Edge Excitons in 2D Molecular Crystals
- Nonuniform Screening Reshapes Collective Excitons in Molecular Aggregates from Stochastic Bethe-Salpeter Theory
- Strong quantum interaction between excitons bound by cavity photon exchange
- Topological Frenkel excitons in 2D molecular crystals
BibTeX
@misc{borda2026excitons,
title = {{Excitons in solid molecular hydrogen from quantum Monte Carlo}},
author = {Edgar Josué Landinez Borda and Ravindra Shinde and Claudia Filippi and Markus Holzmann and Saverio Moroni},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.39894},
eprint = {2610.39894},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.39894},
}
RIS
TY - UNPB
TI - Excitons in solid molecular hydrogen from quantum Monte Carlo
AU - Edgar Josué Landinez Borda
AU - Ravindra Shinde
AU - Claudia Filippi
AU - Markus Holzmann
AU - Saverio Moroni
PY - 2026
DA - 2026/10/29
PB - arXiv
DO - 10.48550/arxiv.2610.39894
UR - https://arxiv.org/abs/2610.39894
AB - We use quantum Monte Carlo (QMC) methods to investigate the lowest neutral excitation of solid molecular hydrogen in phase-I under increasing compression, with emphasis on structural and response properties. We employ QMC wave functions for the excited state that feature only a single orbital substitution, or a multideterminant expansion including every single particle-hole transition, and compare the results with the Bethe-Salpeter equation (BSE) and time-dependent density-functional theory (TDDFT). We examine a number of nuclear configurations representing thermal and quantum fluctuations. The effect of the multideterminant expansion is marginal on the QMC excitation energies but crucial on the exciton localization and related quantities, irrespective of full optimization and imaginary time projection. In the strong insulating regime at low density, multideterminant QMC results match and in some cases surpass the degree of localization afforded by BSE. A similar trend is observed for transition dipole moments and excitation-induced forces, with generally good agreement between QMC and BSE but marked discrepancies for nuclear configurations where localization differs significantly. TDDFT generally gives a more extended exciton with correspondingly weaker transition dipole moments. These differences decrease upon compression, as the system approaches a semiconducting regime where multiple particle-hole transitions are less important.
ER -