<p>Pristine Bi<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>Se<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(_3\)</EquationSource> </InlineEquation> is a promising pseudocapacitive electrode material owing to its layered topological insulator structure and narrow band gap, but its moderate bulk conductivity (<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(10^{2}\)</EquationSource> </InlineEquation>–<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(10^{3}\)</EquationSource> </InlineEquation>&#xa0;S m<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(^{-1}\)</EquationSource> </InlineEquation>) and limited redox-active site density restrict its practical energy storage performance. While composite and multi-metal strategies have improved Bi<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>Se<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(_3\)</EquationSource> </InlineEquation>-based electrodes, the effect of systematic, lattice-level Co<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(^{2+}\)</EquationSource> </InlineEquation> substitution on the structural and electrochemical properties of Bi<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>Se<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(_3\)</EquationSource> </InlineEquation> is underexplored. Here, we synthesize a series of Co-doped Bi<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>Se<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(_3\)</EquationSource> </InlineEquation> nanostructures (0–20% Co) by hydrothermal method and establish a direct correlation between Co<InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(^{2+}\)</EquationSource> </InlineEquation> substitution at Bi<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> </InlineEquation> sites, Co–Se covalent bond formation confirmed by Fourier electron density mapping and XPS peak shifts, and enhanced pseudocapacitive performance. At the optimal 10% Co loading identified by the concurrent maximum in Fourier electron density (33.9&#xa0;e<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(^{-}\)</EquationSource> </InlineEquation>/Å<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(^{3}\)</EquationSource> </InlineEquation>), minimum charge-transfer resistance, and peak specific capacitance across the doping series, the specific capacitance reaches 856&#xa0;F g<InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(^{-1}\)</EquationSource> </InlineEquation> (a 2.1-fold increase over pristine Bi<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>Se<InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(_3\)</EquationSource> </InlineEquation>), with an energy density of 24.07&#xa0;Wh kg<InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(^{-1}\)</EquationSource> </InlineEquation>, coulombic efficiency of 98.7%, and 90.0% capacitance retention over 5000 cycles. Rietveld refinement confirms lattice contraction, while EIS reveals a minimised charge-transfer resistance of 2.21&#xa0;<InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(\Omega\)</EquationSource> </InlineEquation>. These results establish controlled Co doping as an effective and scalable strategy for engineering high-performance Bi<InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>Se<InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(_3\)</EquationSource> </InlineEquation>-based pseudocapacitive electrodes.</p>

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Enhanced electrochemical performance of cobalt-doped bismuth selenide for supercapacitor applications

  • Rumaisa Jan,
  • Seemin Rubab,
  • Sukanya Ghosh

摘要

Pristine Bi \(_2\) Se \(_3\) is a promising pseudocapacitive electrode material owing to its layered topological insulator structure and narrow band gap, but its moderate bulk conductivity ( \(10^{2}\) \(10^{3}\)  S m \(^{-1}\) ) and limited redox-active site density restrict its practical energy storage performance. While composite and multi-metal strategies have improved Bi \(_2\) Se \(_3\) -based electrodes, the effect of systematic, lattice-level Co \(^{2+}\) substitution on the structural and electrochemical properties of Bi \(_2\) Se \(_3\) is underexplored. Here, we synthesize a series of Co-doped Bi \(_2\) Se \(_3\) nanostructures (0–20% Co) by hydrothermal method and establish a direct correlation between Co \(^{2+}\) substitution at Bi \(^{3+}\) sites, Co–Se covalent bond formation confirmed by Fourier electron density mapping and XPS peak shifts, and enhanced pseudocapacitive performance. At the optimal 10% Co loading identified by the concurrent maximum in Fourier electron density (33.9 e \(^{-}\) \(^{3}\) ), minimum charge-transfer resistance, and peak specific capacitance across the doping series, the specific capacitance reaches 856 F g \(^{-1}\) (a 2.1-fold increase over pristine Bi \(_2\) Se \(_3\) ), with an energy density of 24.07 Wh kg \(^{-1}\) , coulombic efficiency of 98.7%, and 90.0% capacitance retention over 5000 cycles. Rietveld refinement confirms lattice contraction, while EIS reveals a minimised charge-transfer resistance of 2.21  \(\Omega\) . These results establish controlled Co doping as an effective and scalable strategy for engineering high-performance Bi \(_2\) Se \(_3\) -based pseudocapacitive electrodes.