bimetallic films
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Nanomaterials ◽  
2021 ◽  
Vol 12 (1) ◽  
pp. 118
Author(s):  
Jingyuan Bai ◽  
Jin Zhang ◽  
Konrad Eiler ◽  
Zhou Yang ◽  
Longyi Fan ◽  
...  

Ni-based bimetallic films with 20 at.% and 45 at.% Cu and mesostructured surfaces were prepared by electrodeposition from an aqueous solution containing micelles of P123 triblock copolymer serving as a structure-directing agent. The pH value of the electrolytic solution had a key effect on both the resulting Cu/Ni ratio and the surface topology. The catalytic activity of the CuNi films toward hydrogen evolution reaction was investigated by cyclic voltammetry (CV) in 1 M KOH electrolyte at room temperature. The Cu45Ni55 film showed the highest activity (even higher than that of a non-mesostructured pure Ni film), which was attributed to the Ni content at the utmost surface, as demonstrated by CV studies, as well as the presence of a highly corrugated surface.


2021 ◽  
Vol 418 ◽  
pp. 129493
Author(s):  
Hongjing Wang ◽  
Qiqi Mao ◽  
Hongjie Yu ◽  
Shengqi Wang ◽  
You Xu ◽  
...  

2021 ◽  
Author(s):  
Maheswari Pandaram ◽  
Subanya Santhanakumar ◽  
Ravi Veeran ◽  
Rajesh Karuppaiya Balasundaram ◽  
Rajan Jha ◽  
...  

Abstract Highly sensitivity Surface Plasmon resonance (SPR) sensor consisting of Ag-Pt bimetallic films sandwiched with 2D materials Black Phosphorus (BP) and Graphene over Pt layer in Kretschmann configuration is analyzed theoretically using the Transfer Matrix Method. Numerical results shows that upon suitable optimization of thickness of Ag-Pt and number of layers of BP & graphene, sensitivity as high as 412º/RIU can be achieved for p-polarized light of wavelength 633 nm. This performance can be tuned and controlled by changing the number of layers of BP and graphene. Further, the addition of graphene and heterostructures of black phosphorus not only improved the sensitivity of the sensor but keep the FWHM of the resonance curve much smaller than the conventional sensor utilizing Au as plasmon metal and hence improved the resolution to a significant extent. We expect that this new proposed design will be useful for medical diagnosis, biomolecular detection and chemical examination.


Micromachines ◽  
2020 ◽  
Vol 11 (4) ◽  
pp. 410
Author(s):  
Francesco Ruffino ◽  
Maria Censabella ◽  
Giovanni Piccitto ◽  
Maria Grimaldi

Bimetallic Au/Pd nanoscale-thick films were sputter-deposited at room temperature on a silicon carbide (SiC) surface, and the surface-morphology evolution of the films versus thickness was studied with scanning electron microscopy. This study allowed to elucidate the Au/Pd growth mechanism by identifying characteristic growth regimes, and to quantify the characteristic parameters of the growth process. In particular, we observed that the Au/Pd film initially grew as three-dimensional clusters; then, increasing Au/Pd film thickness, film morphology evolved from isolated clusters to partially coalesced wormlike structures, followed by percolation morphology, and, finally, into a continuous rough film. The application of the interrupted coalescence model allowed us to evaluate a critical mean cluster diameter for partial coalescence, and the application of Vincent’s model allowed us to quantify the critical Au/Pd coverage for percolation transition.


2020 ◽  
Vol 52 (1) ◽  
pp. 235-262 ◽  
Author(s):  
Lou Kondic ◽  
Alejandro G. González ◽  
Javier A. Diez ◽  
Jason D. Fowlkes ◽  
Philip Rack

Metal films of nanoscale thickness, deposited on substrates and exposed to laser heating, provide systems that involve several interesting multiphysics effects. In addition to fluid mechanical aspects associated with a free boundary setup, other relevant physical effects include phase change, thermal flow, and liquid–solid interactions. Such films are challenging to model, in particular because inertial effects may be relevant, and large contact angles require care when considering the long-wave formulation. Applications of nanoscale metal films are numerous, and the materials science community is actively pursuing more complex setups involving templated films and substrates, bimetallic films and alloys, and a variety of elemental film geometries. The goal of this review is to discuss our current understanding of thin metal film systems, while also providing an overview of the challenges in this research area, which stands at the intersection of fluid mechanics, materials science, and thermal physics.


Coatings ◽  
2019 ◽  
Vol 9 (5) ◽  
pp. 337 ◽  
Author(s):  
Manuela Proença ◽  
Marco S. Rodrigues ◽  
Joel Borges ◽  
Filipe Vaz

Magnetron sputtered nanocomposite thin films composed of monometallic Au and Ag, and bimetallic Au-Ag nanoparticles, dispersed in a CuO matrix, were prepared, characterized, and tested, which aimed to find suitable nano-plasmonic platforms capable of detecting the presence of gas molecules. The Localized Surface Plasmon Resonance phenomenon, LSPR, induced by the morphological changes of the nanoparticles (size, shape, and distribution), and promoted by the thermal annealing of the films, was used to tailor the sensitivity to the gas molecules. Results showed that the monometallic films, Au:CuO and Ag:CuO, present LSPR bands at ~719 and ~393 nm, respectively, while the bimetallic Au-Ag:CuO film has two LSPR bands, which suggests the presence of two noble metal phases. Through transmittance-LSPR measurements, the bimetallic films revealed to have the highest sensitivity to the refractive index changes, as well as high signal-to-noise ratios, respond consistently to the presence of a test gas.


2018 ◽  
Vol 20 (3) ◽  
pp. 1524-1530 ◽  
Author(s):  
Edvin Fako ◽  
Ana S. Dobrota ◽  
Igor A. Pašti ◽  
Núria López ◽  
Slavko V. Mentus ◽  
...  

Surface properties of supported bimetallic films can be predicted from the lattice mismatch between the overlayer and the support already there for trilayers.


2017 ◽  
Vol 81 (12) ◽  
pp. 1387-1390
Author(s):  
M. N. Gerke ◽  
A. V. Istratov ◽  
D. N. Bukharov ◽  
O. A. Novikova ◽  
I. O. Skryabin ◽  
...  

2016 ◽  
Vol 121 (5) ◽  
pp. 765-768 ◽  
Author(s):  
A. Antipov ◽  
S. Arakelian ◽  
T. Vartanyan ◽  
M. Gerke ◽  
A. Istratov ◽  
...  

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