Accessibility of doping ranges of semiconductors by terahertz spectroscopy

J J. Hennig (Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,) J J. Klier (Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,) S S. Duran (Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,) M M. Kutas (Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,) J J. Jonuscheit (Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,) G G. von Freymann (Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,) D D. Molter (Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,)

Abstract

While established semiconductor measurement techniques such as four-point probe or capacitance-voltage measurements require a physical contact to the material, terahertz spectroscopy is completely contact-free. Its capability to measure the doping of semiconductors is well known, yet the exact doping ranges that are accessible to terahertz spectroscopy are not obvious. Therefore, we introduce a sensitivity metric to clarify whether a semiconductor sample can be characterized, in principle, by reflection terahertz time-domain spectroscopy. This quantity takes into account the semiconductor material with a certain layer thickness, doping type, and doping level and is based on numerical simulations. In this work, we calculate this sensitivity value for relevant semiconductor materials (SiC, Si, and GaN) in realistic layer stacks with up to three layers. It is used to create meaningful heat maps depending on the thicknesses and charge carrier densities of the sample structures of interest. The plausibility of the sensitivity is validated by mapping a variety of measurements with terahertz techniques from us and from other groups onto these heat maps. Based on these, the accessible range of charge carrier densities for terahertz spectroscopy spans roughly from 1015 to 1020 cm−3 but with dependencies on material, doping type, and sample thickness. Furthermore, the sensitivity value allows for a substantiated assessment of the possible benefits that future improvements of photoconductive antennas and terahertz systems could have, which is demonstrated by simulations based on varied bandwidths.

Article Details

Volume / Issue Vol. 128, Issue 17
Published April 27, 2026
ISSN 0003-6951
Publisher American Institute of Physics

Journal Info

Applied Physics Letters

American Institute of Physics

ISSN: 0003-6951 Physical Sciences

Authors (7)

J

J. Hennig

Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,

J

J. Klier

Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,

S

S. Duran

Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,

M

M. Kutas

Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,

J

J. Jonuscheit

Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,

G

G. von Freymann

Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,

D

D. Molter

Fraunhofer Institute for Industrial Mathematics ITWM, Department Materials Characterization and Testing 1 , 67663 Kaiserslautern,