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In the region where two bulk phases meet, an intricate electric charge distribution arises due to charge transfer, ion adsorption, molecular orientation, and charge distortion. This complex distribution is commonly referred to as the electrical double layer.When a solid electrode interfaces with ions in an electrolyte solution, the speed of electron transfer dictates the rates of oxidation and reduction. The electrode acquires a charge through the escape of atoms into the solution as cations or...
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The electrode interacts with ions in the electrolyte solution at its interface. The rate of oxidation and reduction depends on the speed at which electrons can transfer through this interface. As ions attach to or leave the electrode surface, the electrode acquires a charge, and an electrical potential forms across the interface, making the process more difficult to reach equilibrium. The charge on the electrode affects the local ion concentrations in the solution, though thermal motion...
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The Debye-Hückel-Onsager equation is a cornerstone of physical chemistry, providing a method to determine the molar conductance (Λm) and molar conductance at infinite dilution (Λ°m) for uni-univalent electrolytes.Uni-univalent electrolytes are electrolytes that dissociate in solution to produce one cation with a +1 charge and one anion with a –1 charge per formula unit.This equation addresses two crucial phenomena: the asymmetry effect and the electrophoretic effect.
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Proton transfer through single-layer graphene is possible at room temperature via atomic defects. This process is selective for protons and involves a Grotthuss-type relay mechanism.

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Area of Science:

  • Materials Science
  • Physical Chemistry
  • Nanotechnology

Background:

  • Proton transfer across single-layer graphene typically has high energy barriers, limiting its feasibility at room temperature.
  • Previous research suggested that proton transfer requires modifications like holes, dopants, or external electrical bias.

Purpose of the Study:

  • To investigate the mechanism and feasibility of proton transfer across single-layer graphene under ambient conditions.
  • To identify the pathways and conditions that enable proton transport through graphene.

Main Methods:

  • Subjecting single-layer graphene on fused silica to cyclic high and low pH conditions.
  • Utilizing computer simulations to calculate energy barriers for proton transfer.
  • Analyzing proton transfer through atomic defects and comparing with other gas transfers.

Main Results:

  • Demonstrated reversible proton transfer across single-layer graphene through naturally occurring atomic defects.
  • Computed low energy barriers (0.61-0.75 eV) for proton transfer across hydroxyl-terminated atomic defects.
  • Identified that specific defect terminations (pyrylium-like ether) inhibit proton exchange, while others facilitate a Grotthuss-type relay.

Conclusions:

  • Proton transfer through single-layer graphene is achievable at room temperature via specific atomic defects.
  • The process is selective for aqueous protons and relies on hydroxyl-terminated defect sites.
  • Atomic defects in graphene can act as channels for proton transport, enabling acid-base chemistry with underlying materials.