<p>Chemical vapor deposition (CVD) plays a crucial role in the fabrication of crystalline silicon (c-Si) solar cells. The structures, morphologies and properties of the silicon oxide (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\text {SiO}_x\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>SiO</mtext> <mi>x</mi> </msub> </math></EquationSource> </InlineEquation>) passivated contacts vary significantly with the specific CVD technique employed, including atmospheric-pressure (APCVD), low-pressure (LPCVD), and plasma-enhanced (PECVD) methods. This study demonstrates that, although APCVD offers the advantages of low cost and high deposition rate, the random motion of carrier gas molecules results in the non-uniform <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\text {SiO}_x\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>SiO</mtext> <mi>x</mi> </msub> </math></EquationSource> </InlineEquation> films with a high defect density. As a result, the TOPCon solar cells passivated with APCVD-SiO? exhibit the lowest open-circuit voltage (735.9 mV) and power conversion efficiency (24.9%). In contrast, the <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\text {SiO}_x\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>SiO</mtext> <mi>x</mi> </msub> </math></EquationSource> </InlineEquation> layers produced by LPCVD and PECVD are dense and uniform, providing superior surface passivation. The average open-circuit voltages of the LPCVD-<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\text {SiO}_x\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>SiO</mtext> <mi>x</mi> </msub> </math></EquationSource> </InlineEquation> and PECVD-<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\text {SiO}_x\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>SiO</mtext> <mi>x</mi> </msub> </math></EquationSource> </InlineEquation> passivated TOPCon solar cells reach 743.9 mV and 743.8 mV, respectively. Ultimately, the plasma-enhanced chemical activation of the reactant gases enables the PECVD-passivated TOPCon solar cells to achieve the highest short-circuit current density (41.43 <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\text {mA}\cdot \text {cm}^{-2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>mA</mtext> <mo>·</mo> <msup> <mtext>cm</mtext> <mrow> <mo>-</mo> <mn>2</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>) and an overall power conversion efficiency of 25.8%.</p>

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Silicon Oxide Passivated Contacts Manufactured by Chemical Vapor Deposition Processes for Crystalline Silicon Solar Cells

  • Han Wang,
  • Yuhe Zheng,
  • Xuying Duan,
  • Yonglin Ye,
  • Yang Li

摘要

Chemical vapor deposition (CVD) plays a crucial role in the fabrication of crystalline silicon (c-Si) solar cells. The structures, morphologies and properties of the silicon oxide ( \(\text {SiO}_x\) SiO x ) passivated contacts vary significantly with the specific CVD technique employed, including atmospheric-pressure (APCVD), low-pressure (LPCVD), and plasma-enhanced (PECVD) methods. This study demonstrates that, although APCVD offers the advantages of low cost and high deposition rate, the random motion of carrier gas molecules results in the non-uniform \(\text {SiO}_x\) SiO x films with a high defect density. As a result, the TOPCon solar cells passivated with APCVD-SiO? exhibit the lowest open-circuit voltage (735.9 mV) and power conversion efficiency (24.9%). In contrast, the \(\text {SiO}_x\) SiO x layers produced by LPCVD and PECVD are dense and uniform, providing superior surface passivation. The average open-circuit voltages of the LPCVD- \(\text {SiO}_x\) SiO x and PECVD- \(\text {SiO}_x\) SiO x passivated TOPCon solar cells reach 743.9 mV and 743.8 mV, respectively. Ultimately, the plasma-enhanced chemical activation of the reactant gases enables the PECVD-passivated TOPCon solar cells to achieve the highest short-circuit current density (41.43 \(\text {mA}\cdot \text {cm}^{-2}\) mA · cm - 2 ) and an overall power conversion efficiency of 25.8%.