2 research outputs found
Understanding the Effects of Cationic Dopants on α‑MnO<sub>2</sub> Oxygen Reduction Reaction Electrocatalysis
Nickel-doped
α-MnO<sub>2</sub> nanowires (Ni−α-MnO<sub>2</sub>) were prepared with 3.4% or 4.9% Ni using a hydrothermal
method. A comparison of the electrocatalytic data for the oxygen reduction
reaction (ORR) in alkaline electrolyte versus that obtained with α-MnO<sub>2</sub> or Cu−α-MnO<sub>2</sub> is provided. In general,
Ni-α-MnO<sub>2</sub> (e.g., Ni-4.9%) had higher <i>n</i> values (<i>n</i> = 3.6), faster kinetics (<i>k</i> = 0.015 cm s<sup>–1</sup>), and lower charge transfer resistance
(<i>R</i><sub>CT</sub> = 2264 Ω at half-wave) values
than MnO<sub>2</sub> (<i>n</i> = 3.0, <i>k</i> = 0.006 cm s<sup>–1</sup>, <i>R</i><sub>CT</sub> = 6104 Ω at half-wave) or Cu–α-MnO<sub>2</sub> (Cu-2.9%, <i>n</i> = 3.5, <i>k</i> = 0.015 cm
s<sup>–1</sup>, <i>R</i><sub>CT</sub> = 3412 Ω
at half-wave), and the overall activity for Ni−α-MnO<sub>2</sub> trended with increasing Ni content, i.e., Ni-4.9% > Ni-3.4%.
As observed for Cu−α-MnO<sub>2</sub>, the increase in
ORR activity correlates with the amount of Mn<sup>3+</sup> at the
surface of the Ni−α-MnO<sub>2</sub> nanowire. Examining
the activity for both Ni−α-MnO<sub>2</sub> and Cu−α-MnO<sub>2</sub> materials indicates that the Mn<sup>3+</sup> at the surface
of the electrocatalysts dictates the activity trends within the overall
series. Single nanowire resistance measurements conducted on 47 nanowire
devices (15 of α-MnO<sub>2</sub>, 16 of Cu−α-MnO<sub>2</sub>-2.9%, and 16 of Ni−α-MnO<sub>2</sub>-4.9%) demonstrated
that Cu-doping leads to a slightly lower resistance value than Ni-doping,
although both were considerably improved relative to the undoped α-MnO<sub>2</sub>. The data also suggest that the ORR charge transfer resistance
value, as determined by electrochemical impedance spectroscopy, is
a better indicator of the cation-doping effect on ORR catalysis than
the electrical resistance of the nanowire
Lithographically Defined Three-Dimensional Graphene Structures
A simple and facile method to fabricate 3D graphene architectures is presented. Pyrolyzed photoresist films (PPF) can easily be patterned into a variety of 2D and 3D structures. We demonstrate how prestructured PPF can be chemically converted into hollow, interconnected 3D multilayered graphene structures having pore sizes around 500 nm. Electrodes formed from these structures exhibit excellent electrochemical properties including high surface area and steady-state mass transport profiles due to a unique combination of 3D pore structure and the intrinsic advantages of electron transport in graphene, which makes this material a promising candidate for microbattery and sensing applications