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Revealing a Pathway for Low-Temperature Recrystallization in Germanium

  • Gihan Velişa
  • , Eva Zarkadoula
  • , Decebal Iancu
  • , Maria D. Mihai
  • , Alexandre Boulle
  • , Yang Tong
  • , Da Chen
  • , Yanwen Zhang
  • , William J. Weber

Research output: Contribution to journalArticlepeer-review

Abstract

Thermally activated annealing in semiconductors faces inherent limitations, such as dopant diffusion. Here, a nonthermal pathway is demonstrated for a complete structural restoration in predamaged germanium via ionization-induced recovery. By combining experiments and modeling, this study reveals that the energy transfer of only 2.4 keV nm−1 from incident ions to target electrons can effectively annihilate pre-existing defects and restore the original crystalline structure at room temperature. Moreover, it is revealed that the irradiation-induced crystalline-to-amorphous (c/a) transformation in Ge is reversible, a phenomenon previously considered unattainable without additional thermal energy imposed during irradiation. For partially damaged Ge, the overall damage fraction decreases exponentially with increasing fluence. Surprisingly, the recovery process in preamorphized Ge starts with defect recovery outside the amorphous layer and a shrinkage of the amorphous thickness. After this initial stage, the remaining damage decreases slowly with increasing fluence, but full restoration of the pristine state is not achieved. These differences in recovery are interpreted in the framework of structural differences in the initial defective layers that affect recovery kinetics. This study provides new insights on reversing the c/a transformation in Ge using highly-ionizing irradiation and has broad implications across materials science, radiation damage mitigation, and fabrication of Ge-based devices.

Original languageEnglish
Article numbere07630
JournalAdvanced Science
Volume12
Issue number41
DOIs
StatePublished - Nov 6 2025

Funding

This work was supported by a grant of the Ministry of Research, Innovation and Digitization, CNCS – UEFISCDI, project number PN‐IV‐P1‐PCE‐2023–0567, within Planul Naţional de Cercetare‐Dezvoltare şi Inovare (PNCDI) IV. The contributions of D. Iancu and G. Velisa to this work were also supported by the CORE (Nucleu) PROGRAMME, project PN 23210201. Experiments were carried out at 3 MV Tandetron accelerator from “Horia Hulubei” National Institute for Physics and Nuclear Engineering (IFIN‐HH) and were supported by the Romanian Government Programme through the National Programme for Infrastructure of National Interest (IOSIN). This research used resources of the Compute and Data Environment for Science (CADES) at the Oak Ridge National Laboratory, which is supported by the Office of Science of the U.S. Department of Energy under Contract No. DE‐AC05–00OR22725″. E. Zarkadoula (theory and simulation works) was supported by the Center for Nanophase Materials Sciences, (CNMS), which is a US Department of Energy, Office of Science User Facility at Oak Ridge National Laboratory. The contribution of W.J. Weber was supported by the National Science Foundation under Grant No. DMR‐2104228. Y. Zhang was supported by the Canada Excellence Research Chairs Program (CERC). Y. Tong gratefully acknowledges the financial support by Taishan Scholars Program of Shandong Province (tsqn202103052), and Yantai city matching fund for Taishan Scholars Program of Shandong Province (122702). This work was supported by a grant of the Ministry of Research, Innovation and Digitization, CNCS – UEFISCDI, project number PN-IV-P1-PCE-2023–0567, within Planul Naţional de Cercetare-Dezvoltare şi Inovare (PNCDI) IV. The contributions of D. Iancu and G. Velisa to this work were also supported by the CORE (Nucleu) PROGRAMME, project PN 23210201. Experiments were carried out at 3 MV Tandetron accelerator from “Horia Hulubei” National Institute for Physics and Nuclear Engineering (IFIN-HH) and were supported by the Romanian Government Programme through the National Programme for Infrastructure of National Interest (IOSIN). This research used resources of the Compute and Data Environment for Science (CADES) at the Oak Ridge National Laboratory, which is supported by the Office of Science of the U.S. Department of Energy under Contract No. DE-AC05–00OR22725″. E. Zarkadoula (theory and simulation works) was supported by the Center for Nanophase Materials Sciences, (CNMS), which is a US Department of Energy, Office of Science User Facility at Oak Ridge National Laboratory. The contribution of W.J. Weber was supported by the National Science Foundation under Grant No. DMR-2104228. Y. Zhang was supported by the Canada Excellence Research Chairs Program (CERC). Y. Tong gratefully acknowledges the financial support by Taishan Scholars Program of Shandong Province (tsqn202103052), and Yantai city matching fund for Taishan Scholars Program of Shandong Province (122702). Open access publishing facilitated by Anelis Plus as part of the Wiley - Anelis Plus agreement.

Keywords

  • athermal recovery
  • complete damage annealing
  • defect analyses
  • defects simulation
  • germanium

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