Abstract <p>Manganese oxides, especially birnessite-type <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\delta\)</EquationSource> </InlineEquation>-MnO<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>, are promising pseudocapacitive materials as electrodes in supercapacitors due to their layered structure and high specific capacitance. However, understanding how the nature of intercalated cations influences their structural evolution and charge storage mechanism remains an open challenge. In this work, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\delta\)</EquationSource> </InlineEquation>-MnO<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation> thin films were obtained through the electrochemical transformation of Mn<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(_x\)</EquationSource> </InlineEquation>O<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(_y\)</EquationSource> </InlineEquation> films deposited directly on stainless-steel current collectors by atmospheric pressure chemical vapor deposition (AP-CVD). The transformation was conducted in sulfate electrolytes containing K<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(^+\)</EquationSource> </InlineEquation>, Na<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(^+\)</EquationSource> </InlineEquation>, and Li<InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(^+\)</EquationSource> </InlineEquation> ions. After the transformation, the resulting <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\delta\)</EquationSource> </InlineEquation>-MnO<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation> electrodes were evaluated as supercapacitor electrode in different alkali sulfate electrolytes to assess the influence of the testing medium on their charge storage behavior. The results demonstrate that the electrolyte cation significantly determines the crystallinity, morphology, and pseudocapacitive response of the resulting birnessite films. <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\delta\)</EquationSource> </InlineEquation>-MnO<InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation> phases were successfully formed in K<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>SO<InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(_4\)</EquationSource> </InlineEquation> and Na<InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>SO<InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(_4\)</EquationSource> </InlineEquation>. K-<InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(\delta\)</EquationSource> </InlineEquation>-MnO<InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation> exhibited predominantly hexagonal structure with the coexistence of the monoclinic phase, while Na-<InlineEquation ID="IEq24"> <EquationSource Format="TEX">\(\delta\)</EquationSource> </InlineEquation>-MnO<InlineEquation ID="IEq25"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation> exhibited a monoclinic structure with well-defined nanowalls and the highest surface-controlled contribution to charge storage, achieving areal capacitances up to 6.5 mF cm<InlineEquation ID="IEq26"> <EquationSource Format="TEX">\(^{-2}\)</EquationSource> </InlineEquation> when evaluated in Li<InlineEquation ID="IEq27"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>SO<InlineEquation ID="IEq28"> <EquationSource Format="TEX">\(_4\)</EquationSource> </InlineEquation>, proving the monoclinic structure of <InlineEquation ID="IEq29"> <EquationSource Format="TEX">\(\delta\)</EquationSource> </InlineEquation>-MnO<InlineEquation ID="IEq30"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation> as the best for energy storage. These findings highlight the crucial role of cation species in tuning the intrinsic electrochemical behavior of <InlineEquation ID="IEq31"> <EquationSource Format="TEX">\(\delta\)</EquationSource> </InlineEquation>-MnO<InlineEquation ID="IEq32"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation> thin films and provide valuable insights for the rational design of high-performance birnessite-based electrodes for energy storage applications.</p> Graphical abstract <p></p>

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Electrochemical transformation of AP-CVD manganese oxide thin films into \(\delta\)-MnO\(_2\) in alkali sulfate electrolytes for supercapacitor applications

  • Perla Judith Pérez-Díaz,
  • Karime Carrera-Gutiérrez,
  • Yasmín Esqueda-Barrón,
  • Carolina Bohorquez-Martínez,
  • Próspero Acevedo Peña,
  • Daniella Esperanza Pacheco-Catalán,
  • Ana Karina Cuentas-Gallegos

摘要

Abstract

Manganese oxides, especially birnessite-type \(\delta\) -MnO \(_2\) , are promising pseudocapacitive materials as electrodes in supercapacitors due to their layered structure and high specific capacitance. However, understanding how the nature of intercalated cations influences their structural evolution and charge storage mechanism remains an open challenge. In this work, \(\delta\) -MnO \(_2\) thin films were obtained through the electrochemical transformation of Mn \(_x\) O \(_y\) films deposited directly on stainless-steel current collectors by atmospheric pressure chemical vapor deposition (AP-CVD). The transformation was conducted in sulfate electrolytes containing K \(^+\) , Na \(^+\) , and Li \(^+\) ions. After the transformation, the resulting \(\delta\) -MnO \(_2\) electrodes were evaluated as supercapacitor electrode in different alkali sulfate electrolytes to assess the influence of the testing medium on their charge storage behavior. The results demonstrate that the electrolyte cation significantly determines the crystallinity, morphology, and pseudocapacitive response of the resulting birnessite films. \(\delta\) -MnO \(_2\) phases were successfully formed in K \(_2\) SO \(_4\) and Na \(_2\) SO \(_4\) . K- \(\delta\) -MnO \(_2\) exhibited predominantly hexagonal structure with the coexistence of the monoclinic phase, while Na- \(\delta\) -MnO \(_2\) exhibited a monoclinic structure with well-defined nanowalls and the highest surface-controlled contribution to charge storage, achieving areal capacitances up to 6.5 mF cm \(^{-2}\) when evaluated in Li \(_2\) SO \(_4\) , proving the monoclinic structure of \(\delta\) -MnO \(_2\) as the best for energy storage. These findings highlight the crucial role of cation species in tuning the intrinsic electrochemical behavior of \(\delta\) -MnO \(_2\) thin films and provide valuable insights for the rational design of high-performance birnessite-based electrodes for energy storage applications.

Graphical abstract