Band-filling and relaxation effects in the transient dielectric function of Ge

C C. A. Armenta (Department of Physics, New Mexico State University 1 , MSC 3D, P. O. Box 30001, Las Cruces, New Mexico 88003-8001,) M M. Zahradník (ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,) M M. Rebarz (ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,) C C. Emminger (Department of Physics, New Mexico State University 1 , MSC 3D, P. O. Box 30001, Las Cruces, New Mexico 88003-8001,) S S. Espinoza (ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,) S S. Vazquez-Miranda (ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,) J J. Andreasson (ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,) S S. Zollner (Department of Physics, New Mexico State University 1 , MSC 3D, P. O. Box 30001, Las Cruces, New Mexico 88003-8001,)

Abstract

This study investigates the transient dielectric function of germanium at charge carrier densities of the order of 1020cm−3 using time-resolved spectroscopic ellipsometry. By employing a pump-probe technique, we explore the temporal evolution of the critical points E1 and E1+Δ1 after high-intensity laser excitation. Given the two-dimensional character of these critical points, the absorption of Ge is significantly enhanced by excitonic binding. Furthermore, at high carrier densities, intervalley scattering and band saturation play a significant role in the optical response of the material. To address these phenomena, we combined band-filling effects with a two-dimensional excitonic line shape to model the observed optical spectra. We also simulated the Fermi energies and electron temperatures governing the measurements using Fermi–Dirac statistics. Given the short timescales of the carrier relaxation and intervalley scattering, this analysis focuses exclusively on the first few picoseconds after excitation, with a minimum step size of 50 fs. The model successfully reproduces the main features of the experimental spectra, capturing the reduction in amplitude of the dielectric function and the redshift of the critical points due to bandgap renormalization. From these fits, we extract an energy relaxation rate of the order of 1.5meVfs−1 and provide a quantitative description of the ultrafast carrier dynamics in Ge.

Article Details

Volume / Issue Vol. 138, Issue 20
Published November 28, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (8)

C

C. A. Armenta

Department of Physics, New Mexico State University 1 , MSC 3D, P. O. Box 30001, Las Cruces, New Mexico 88003-8001,

M

M. Zahradník

ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,

M

M. Rebarz

ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,

C

C. Emminger

Department of Physics, New Mexico State University 1 , MSC 3D, P. O. Box 30001, Las Cruces, New Mexico 88003-8001,

S

S. Espinoza

ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,

S

S. Vazquez-Miranda

ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,

J

J. Andreasson

ELI Beamlines Facility, The Extreme Light Infrastructure ERIC 2 , Za Radnicí 835, 25241 Dolní Břežany,

S

S. Zollner

Department of Physics, New Mexico State University 1 , MSC 3D, P. O. Box 30001, Las Cruces, New Mexico 88003-8001,