PreprintCC BY 4.0arXiv
Photoemission from Semi-Infinite Crystals: First-Principles Scattering States and Quantitative Ag(111) Validation
Abstract
Photoemission is an escape problem, yet first-principles calculations usually trap the electron in a periodic box. We present a parameter-free \emph{ab initio} framework that removes this artificial boundary by constructing open scattering states for semi-infinite crystal-vacuum interfaces from Wannier Hamiltonians and Green-function embedding. The method gives continuum-normalized time-reversed LEED final states with microscopic quasiparticle attenuation. For Ag(111), it predicts absolute quantum efficiency, vectorial photoemission, and mean transverse energy on the experimental scale.
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BibTeX
@misc{wu2026photoemission,
title = {{Photoemission from Semi-Infinite Crystals: First-Principles Scattering States and Quantitative Ag(111) Validation}},
author = {Tyler Wu and Truman Idso and Siddharth Karkare and Tomás Arias},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2607.19551},
eprint = {2607.19551},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2607.19551},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Photoemission from Semi-Infinite Crystals: First-Principles Scattering States and Quantitative Ag(111) Validation
AU - Tyler Wu
AU - Truman Idso
AU - Siddharth Karkare
AU - Tomás Arias
PY - 2026
DA - 2026/09/02
PB - arXiv
DO - 10.48550/arxiv.2607.19551
UR - https://arxiv.org/abs/2607.19551
AB - Photoemission is an escape problem, yet first-principles calculations usually trap the electron in a periodic box. We present a parameter-free \emph{ab initio} framework that removes this artificial boundary by constructing open scattering states for semi-infinite crystal-vacuum interfaces from Wannier Hamiltonians and Green-function embedding. The method gives continuum-normalized time-reversed LEED final states with microscopic quasiparticle attenuation. For Ag(111), it predicts absolute quantum efficiency, vectorial photoemission, and mean transverse energy on the experimental scale.
ER -