Electrical charge deposition modulates carrier mobility in electronic devices and governs interfacial processes such as frictional energy dissipation and triboelectric power generation. Selective charge deposition on 2D materials enables logic and memory functions, but controlling charge transfer and trapping remains a challenge. Here, we report an unconventional contact electrification mechanism activated at a sliding structural superlubric interface between highly ordered pyrolytic graphite and h-BN. Spatially controlled charge deposition is achieved through mechanical manipulation at the sliding front in a reversible way, while face-to-face contact remains intact even under pressures exceeding the strength of most materials. First-principles calculations reveal that edge contact facilitates electron transfer, with charge deposition driven by a chemical potential difference across the graphite/h-BN interface and stabilized by surface adsorbates.
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http://dx.doi.org/10.1021/acsami.4c22073 | DOI Listing |
Biomed Phys Eng Express
March 2025
Department of Physics and Technology, University of Bergen, Allégaten 55, Bergen, Hordaland, 5007, NORWAY.
Monolithic active pixel sensors are used for charged particle tracking in many applications, from medical physics to astrophysics. The Bergen pCT collaboration designed a sampling calorimeter for proton computed tomography, based entirely on the ALICE PIxel DEtector (ALPIDE). The same telescope can be used for in-situ range verification in particle therapy.
View Article and Find Full Text PDFJ Phys Chem Lett
March 2025
Department of Chemistry and Biochemistry, North Dakota State University, Fargo, North Dakota 58102, United States.
The efficiency of silicon solar cells is affected by the light absorption and recombination losses of photoexcited charge carries. One possible way to improve the efficiency is through the deposition of transition metal nanoparticles on Si surfaces. Here, we first carry out density functional theory (DFT) calculations to obtain electronic structures for Ag ( = 1-7) monolayered clusters adsorbed on Si(111)/H surfaces.
View Article and Find Full Text PDFNanoscale
March 2025
The Russell Berrie Nanotechnology Institute, Technion-Israel Institute of Technology, Haifa 3200003, Israel.
The growth of ultrathin layers of oxides by atomic layer deposition (ALD) is well documented for oxide substrates such as SiO, BiO, AlO, in which oxygen is the only negatively charged atom. In contrast, the knowledge regarding ALD growth on substrates containing other negatively charged atoms, such as halogens, is quite limited. The commonly used bismuth oxyhalide (BiOX) family of materials are characterised by a low density of surface hydroxyls, required for the initiation of thermal ALD growth of oxides, thus hampering the ability to grow ultrathin layers of oxides on their surface.
View Article and Find Full Text PDFSmall Methods
March 2025
Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, Shenyang, 110016, China.
Lithium (Li) metal batteries hold great promise for next-generation energy storage due to their high energy density. However, their application is hindered by uncontrollable Li plating/stripping, leading to limited cycle life, especially under practical conditions with a low negative/positive (N/P) capacity ratio. Here, it is demonstrated that stable cycling of low N/P ratio Li metal batteries can be realized by harnessing hetero-interfacial redox chemistry to regulate Li nucleation and deposition behavior.
View Article and Find Full Text PDFACS Nano
March 2025
Department of Chemistry Education, Korea National University of Education (KNUE), Chungbuk 28173, Republic of Korea.
Hot carriers, generated through nonadiabatic energy dissipation during exothermic catalytic reactions, play a pivotal role in enhancing catalytic performance. Upon generation, hot electrons typically reside in the sp-band above the Fermi level, while hot holes are formed in the -band below the Fermi level, following the energy distribution of the metal's electronic structure. However, it has been technically challenging to simultaneously capture and understand the flow of these two opposite charges during chemical reactions.
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