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Helium incorporation induced direct-gap silicides

MetadataDetails
Publication Date2021-06-10
Journalnpj Computational Materials
AuthorsShicong Ding, Jingming Shi, Jiahao Xie, Wenwen Cui, Pan Zhang
InstitutionsJilin University, Jiangsu Normal University
Citations12
AnalysisFull AI Review Included

This research investigates a novel high-pressure synthesis route using Helium (He) to create direct-gap silicon (Si) compounds, aiming to overcome the inherent indirect band gap limitation of conventional Si for thin-film photovoltaics.

  • Core Value Proposition: He incorporation stabilizes four new Si2He host-guest structures, two of which exhibit direct band gaps near the optimal Shockley-Queisser limit (1.34 eV).
  • Key Candidates: The mC12-Si2He phase is the most promising, possessing a direct band gap of 1.34 eV and a dipole-allowed transition, indicating superior solar absorption capacity compared to cubic diamond Si (CD-Si).
  • Synthesis Pathway: He acts as a temporary intermediate. Due to weak Si-He interactions and low He migration barriers (as low as 0.01 eV), He atoms can be easily removed via thermal degassing.
  • Resulting Materials: The removal of He yields pure, metastable Si allotropes (oC24-Si, tP6-Si, mC8-Si), providing a viable chemical route for synthesizing these high-energy structures.
  • Structural Mechanism: The Si2He phases adopt channel-like Si frameworks filled with He guest atoms, with the Si framework potentially retained upon He removal to ambient pressure.
  • Stability: The oP36-Si2He phase is predicted to be the most energetically stable Si2He structure up to 18 GPa.
ParameterValueUnitContext
Optimal Band Gap (SQ Limit)1.34eVShockley-Queisser limit for maximum solar conversion efficiency (33.7%).
mC12-Si2He Band Gap1.34eVDirect, dipole-allowed transition; optimal for thin-film PV.
oP36-Si2He Band Gap1.24eVDirect band gap, high absorption capacity.
tP9-Si2He Band Gap2.18eVIndirect band gap (not suitable for PV).
mC8-Si Band Gap (Pure Si)0.84eVIndirect band gap of the pure Si allotrope resulting from mC12-Si2He degassing.
He Migration Barrier (tP9-Si2He)0.01eVLowest energy barrier, indicating easiest He removal via degassing.
He Migration Barrier (mC12-Si2He)0.37eVLow barrier, indicating comparative ease of He removal.
He Migration Barrier (mC18-Si2He)1.51eVHigh barrier, suggesting He is difficult to remove from this phase.
Si-He Charge Transfer0.03 to 0.09electronsSlight charge transfer from Si framework to He atoms (Bader analysis).
Pressure Stability (oP36-Si2He)0 to 18GPaEnergetically most stable phase in this pressure range (static-lattice).
MD Simulation Temperature300KUsed to confirm thermodynamic stability at ambient conditions.

The study relies entirely on first-principles calculations and structure prediction methods, focusing on computational materials design rather than experimental synthesis.

  1. Structure Prediction: Used the CALYPSO (Crystal structure Analysis by Particle Swarm Optimization) method to search for stable Si2He phases, primarily at 10 GPa, maximizing eight formula units per simulation cell.
  2. Structural Optimization: Employed Density Functional Theory (DFT) as implemented in VASP, utilizing the Perdew-Burke-Ernzerhof (PBE) generalized gradient approximation (GGA) functional.
  3. Electronic and Optical Property Calculation: The HSE06 (Heyd-Scuseria-Ernzerhof) hybrid functional was used to accurately calculate electronic band structures and band gaps, correcting the known underestimation by standard DFT functionals.
  4. Dynamic Stability Verification: Phonon dispersion calculations were performed using the supercell approach (PHONOPY code) to confirm the dynamic stability of the predicted Si2He phases at 0 and 10 GPa.
  5. He Removal Feasibility Assessment: The CI-NEB (Climbing Image Nudged Elastic Band) method was used to calculate the energy barriers for He migration along the Si channels, determining the feasibility of thermal degassing.
  6. Absorption Analysis: The imaginary part of the dielectric function (Δ2) and the square of the transition dipole moment (P2) were calculated to assess solar absorption capacity and confirm the dipole-allowed nature of the direct band gaps.

The successful computational design of direct-gap Si compounds opens pathways for significant advancements in energy and semiconductor technology.

  • Photovoltaic Energy Generation:
    • High-Efficiency Thin-Film Solar Cells: The primary application. Materials like mC12-Si2He (or the resulting mC8-Si allotrope) offer direct band gaps (1.34 eV) that are ideal for maximizing solar conversion efficiency, enabling the use of ultra-thin Si layers.
    • Flexible Electronics: Thin-film materials are crucial for flexible solar panels and integrated building photovoltaics (BIPV).
  • Advanced Semiconductor Materials:
    • Novel Si Allotrope Synthesis: The He incorporation/degassing method provides a practical, two-step chemical route to synthesize metastable Si allotropes (oC24-Si, tP6-Si, mC8-Si) that are otherwise difficult to obtain directly due to their high energy relative to CD-Si.
  • High-Pressure Materials Science:
    • Intermediate Synthesis Medium: Confirms the utility of inert noble gases (like He) under high pressure as a temporary “scaffolding” element to stabilize open-framework structures, a technique potentially transferable to synthesizing other novel functional materials.
View Original Abstract

Abstract The search of direct-gap Si-based semiconductors is of great interest due to the potential application in many technologically relevant fields. This work examines the incorporation of He as a possible route to form a direct band gap in Si. Structure predictions and first-principles calculations show that He and Si, at high pressure, form four dynamically stable phases of Si 2 He (oP36-Si 2 He, tP9-Si 2 He, mC18-Si 2 He, and mC12-Si 2 He). All phases adopt host-guest structures consisting of a channel-like Si host framework filled with He guest atoms. The Si frameworks in oP36-Si 2 He, tP9-Si 2 He, and mC12-Si 2 He could be retained to ambient pressure after removal of He, forming three pure Si allotropes. Among them, oP36-Si 2 He and mC12-Si 2 He exhibit direct band gaps of 1.24 and 1.34 eV, respectively, close to the optimal value (~1.3 eV) for solar cell applications. Analysis shows that mC12-Si 2 He with an electric dipole transition allowed band gap possesses higher absorption capacity than cubic diamond Si, which makes it to be a promising candidate material for thin-film solar cell.