TY - JOUR
T1 - Universal time delays in the inelastic core level photoemission of metals
AU - Bae, Gimin
AU - Park, Hyosub
AU - Lee, J. D.
N1 - Publisher Copyright:
© 2021 American Physical Society.
PY - 2021/4/14
Y1 - 2021/4/14
N2 - Proposing a theoretical model of the core level photoemission of metals, we investigate the plasmon-driven inelastic photoemission delays based on a nonperturbative treatment of many-electron responses due to the long-range Coulomb potential. Being irrelevant to the plasmon coupling strength as well as the plasmon frequency, the emission delays Δτn of the nth-order plasmon satellites (n=1,2,3,...) are found to be universal order by order among the metals in the core level photoemission where the recoil-less approximation would be valid. In particular, for a main line with its weight e-γ, where γ quantifies the plasmon coupling strength, the average inelastic photoemission delay (Δτ) is found to be γ(1-e-γ)-1Δτ1 and thus is simply scaled by a universal time delay Δτ1. This finding is sharply contrasted with the emission delays under the localized potential, which indicates a fundamental difference in the emission process between extended and localized screenings.
AB - Proposing a theoretical model of the core level photoemission of metals, we investigate the plasmon-driven inelastic photoemission delays based on a nonperturbative treatment of many-electron responses due to the long-range Coulomb potential. Being irrelevant to the plasmon coupling strength as well as the plasmon frequency, the emission delays Δτn of the nth-order plasmon satellites (n=1,2,3,...) are found to be universal order by order among the metals in the core level photoemission where the recoil-less approximation would be valid. In particular, for a main line with its weight e-γ, where γ quantifies the plasmon coupling strength, the average inelastic photoemission delay (Δτ) is found to be γ(1-e-γ)-1Δτ1 and thus is simply scaled by a universal time delay Δτ1. This finding is sharply contrasted with the emission delays under the localized potential, which indicates a fundamental difference in the emission process between extended and localized screenings.
UR - http://www.scopus.com/inward/record.url?scp=85104442786&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.103.165413
DO - 10.1103/PhysRevB.103.165413
M3 - Article
AN - SCOPUS:85104442786
SN - 2469-9950
VL - 103
JO - Physical Review B
JF - Physical Review B
IS - 16
M1 - 165413
ER -