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	<title>alkaline electrolyte &#8211; Science</title>
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	<title>alkaline electrolyte &#8211; Science</title>
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		<title>Copper doping supercharges nickel oxide catalysts for methanol fuel cells</title>
		<link>https://scienmag.com/copper-doping-supercharges-nickel-oxide-catalysts-for-methanol-fuel-cells/</link>
		
		<dc:creator><![CDATA[Victoria Harrison]]></dc:creator>
		<pubDate>Wed, 23 Sep 2026 23:25:28 +0000</pubDate>
				<category><![CDATA[Technology and Engineering]]></category>
		<category><![CDATA[alkaline electrolyte]]></category>
		<category><![CDATA[band gap engineering]]></category>
		<category><![CDATA[carbon monoxide tolerance]]></category>
		<category><![CDATA[co-sputtering deposition]]></category>
		<category><![CDATA[co-sputtering fabrication of catalytic thin films]]></category>
		<category><![CDATA[copper doping effects in catalyst performance]]></category>
		<category><![CDATA[Copper-doped nickel oxide catalysts for methanol oxidation]]></category>
		<category><![CDATA[Cu-doped NiO]]></category>
		<category><![CDATA[direct methanol fuel cells]]></category>
		<category><![CDATA[Electrocatalysis]]></category>
		<category><![CDATA[electrochemical impedance spectroscopy]]></category>
		<category><![CDATA[enhancement of methanol oxidation with copper and nickel oxide]]></category>
		<category><![CDATA[impact of copper content on electrochemical activity]]></category>
		<category><![CDATA[low onset potential in methanol oxidation catalysts]]></category>
		<category><![CDATA[low-cost catalysts for direct methanol fuel cells]]></category>
		<category><![CDATA[methanol oxidation reaction]]></category>
		<category><![CDATA[nanostructured catalysts]]></category>
		<category><![CDATA[nickel oxide]]></category>
		<category><![CDATA[nickel oxide thin films for fuel cell anodes]]></category>
		<category><![CDATA[overcoming platinum dependence in fuel cell catalysts]]></category>
		<category><![CDATA[Tafel analysis]]></category>
		<category><![CDATA[Tafel slope reduction in doped nickel oxide]]></category>
		<category><![CDATA[thin films]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=211218</guid>

					<description><![CDATA[Egyptian researchers have shown that doping sputtered nickel oxide thin films with 7 percent copper slashes the methanol oxidation onset potential, narrows the band gap by 0.4 electron volts, and preserves 94 percent of current over 12 hours, offering a platinum-free anode for alkaline direct methanol fuel cells.]]></description>
										<content:encoded><![CDATA[<p>Direct methanol fuel cells promise clean, portable electricity from one of the simplest liquid fuels available, but their commercial future has long been hostage to a stubborn materials problem: the anode reaction that strips electrons from methanol molecules is painfully slow, and the catalysts that speed it up are usually made of platinum, a precious metal that is expensive, scarce, and easily poisoned by the carbon monoxide fragments that accumulate during the reaction. Now a research team at Beni-Suef University in Egypt reports that a simple twist of composition can transform a cheap, abundant material into a serious contender for that job. By blending small amounts of copper into nickel oxide thin films grown by co-sputtering, the researchers found that the 7 percent copper-doped film achieved the lowest methanol oxidation onset potential in the study, 0.37 volts versus a silver-silver chloride reference, while cutting the characteristic Tafel slope by roughly a third compared with undoped nickel oxide.</p>
<p>The study, published in the Journal of Nanoparticle Research, was designed around a deceptively simple question: how does the copper fraction in a nickel oxide film change its ability to catalyze the methanol oxidation reaction in alkaline solution? The team deposited four compositions on fluorine-doped tin oxide glass, a transparent conducting substrate commonly used in photoelectrochemistry. A DC power source sputtered the nickel oxide target at a fixed 200 watts, while a separate radio-frequency power supply drove a copper target at 0, 40, 50, and 60 watts, corresponding to nominal copper contents of 0, 2.5, 4, and 7 percent. Everything else was held constant: a working pressure of 5 by 10 to the minus 3 torr, 400 seconds of deposition, 20 standard cubic centimeters per minute of argon, and a target-to-substrate distance of 14 centimeters. This kind of physical vapor deposition matters because it produces adherent, pinhole-free films whose composition and thickness can be dialled in precisely, unlike many solution-based routes where morphology is hard to reproduce.</p>
<p>Structural characterization showed that the copper was not forming a separate metallic phase. X-ray diffraction revealed only the cubic bunsenite phase of nickel oxide, with reflections from the (111), (200), and (220) crystal planes, and no peaks attributable to metallic copper. Instead, copper appeared to occupy interstitial and substitutional positions within the nickel oxide lattice, filling defects in the nonstoichiometric framework. The evidence was written into the peak shapes: the diffraction peaks broadened and weakened as copper content rose, and the average crystallite size, calculated with the Debye-Scherrer equation, shrank from 18.12 nanometers for pristine nickel oxide to 7.42 nanometers at 7 percent copper. Lattice strain climbed from 2.1 by 10 to the minus 4 to 5.31 by 10 to the minus 4, and the dislocation density rose nearly sevenfold, both signatures of a lattice that has been subtly disrupted by foreign atoms. Electron microscopy confirmed the trend, showing progressively rougher, more compact, and more agglomerated surfaces as the dopant level increased.</p>
<p>One consequence of the co-sputtering recipe deserves particular attention because it complicates the interpretation of catalytic data. Film thickness grew systematically with copper loading, from 53 nanometers for pristine nickel oxide to 90, 121, and 180 nanometers for the 2.5, 4, and 7 percent films. More material on the electrode naturally means more geometric current, so the researchers took the unusual and commendable step of normalizing their methanol oxidation currents in two additional ways: per unit of film thickness, and per unit of electrochemically active surface area estimated from double-layer capacitance measurements. The capacitance values rose from 0.226 to 0.44 millifarads per square centimeter across the composition series, yielding active surface areas between 5.65 and 11.12 square centimeters. Even after this careful normalization, the 7 percent copper film remained roughly 2.5 times more active than pristine nickel oxide, while the 2.5 and 4 percent films showed the highest currents per unit thickness and per active area respectively. The conclusion was nuanced: copper incorporation, enlarged active area, film growth, and improved interfacial kinetics all contributed, and no single factor explains the whole story.</p>
<p>Optical measurements pointed to a fundamental electronic reason for the improvement. Ultraviolet-visible spectroscopy combined with Tauc analysis showed that the optical band gap narrowed steadily as copper content increased, from 3.64 electron volts for pure nickel oxide to 3.24 electron volts at 7 percent doping. Band gap narrowing in doped nickel oxide is generally attributed to localized dopant states overlapping the band edges and to improved crystallization, and narrower gaps translate directly into better electronic conductivity through the film. For a p-type semiconductor like nickel oxide, which must shuttle holes and electrons between the current collector and the electrolyte interface during every catalytic cycle, that conductivity gain is not an academic nicety. It means less internal resistance, faster delivery of charge to surface reaction sites, and lower overpotentials, which is exactly what the electrochemical measurements went on to confirm.</p>
<p>Cyclic voltammetry in 1 molar sodium hydroxide exposed the redox machinery of the films. All four compositions showed anodic and cathodic peaks associated with the nickel(II) to nickel(III) and copper(I) to copper(II) couples, meaning that both metals contribute electroactive centers. Peak currents scaled linearly with the square root of the scan rate, indicating that hydroxide diffusion into the film pores, rather than some surface limitation, governed the redox process at the electrode-electrolyte boundary. When methanol was added, every film responded, but the doped films responded dramatically more, with anodic and cathodic current densities climbing in step with copper content. Onset potentials shifted to more negative values as methanol concentration rose from 0.25 to 3 molar, and the 7 percent copper film recorded the highest current density in 1 molar methanol, around 32 milliamperes per square centimeter.</p>
<p>Kinetic analysis tightened the picture. The team recorded linear sweep voltammograms at a deliberately slow scan rate of 5 millivolts per second, a quasi-steady condition that minimizes capacitive contributions from the nickel hydroxide to nickel oxyhydroxide transformation and yields Tafel slopes that reflect true faradaic kinetics. Pristine nickel oxide gave a slope of 178 millivolts per decade. Doping with just 2.5 percent copper dropped it to 127, and 7 percent copper brought it down to 120 millivolts per decade, a total reduction of about 32.5 percent. That final value corresponds to a charge-transfer coefficient of 0.5, consistent with the first electron transfer step dominating the reaction kinetics. Interestingly, the largest kinetic gain arrived at the lowest dopant loading, with the incremental benefit tapering off at 4 and 7 percent, suggesting the population of accessible surface redox sites begins to saturate. The authors attribute the enhancement to a bifunctional synergy: nickel centers cycle into the active nickel oxyhydroxide species that dehydrogenate methanol, while copper sites, present as mixed copper(I) and copper(II) states according to X-ray photoelectron spectroscopy, adsorb hydroxyl species at lower overpotentials and thereby strip carbonaceous intermediates from neighboring nickel sites before they can block them.</p>
<p>Electrochemical impedance spectroscopy, recorded at 0.6 volts in 1 molar sodium hydroxide with 1 molar methanol, backed this mechanism quantitatively. The fitted charge-transfer resistance decreased steadily with doping level, reflecting the greater density of redox-active nickel and copper sites on the film surfaces. A carbon monoxide stripping experiment delivered perhaps the most convincing evidence of poisoning resistance: the 7 percent copper film showed a clean stripping peak at 0.43 volts, and, strikingly, no reverse oxidation peak appeared during the backward scan, indicating negligible accumulation of adsorbed carbon monoxide intermediates. That absence of a backward peak is exactly the behavior fuel cell engineers want to see, because it means the catalyst surface stays clear and available for fresh fuel molecules rather than becoming choked with its own reaction byproducts.</p>
<p>Durability, the graveyard of many promising electrocatalysts, was tested on three fronts. Chronoamperometry at 0.6 volts for a full 12 hours showed only a 5.7 percent decline in current for the 7 percent copper film, with the small initial drop attributable to intermediate adsorption and local methanol depletion near the electrode surface. After 1000 cyclic voltammetry cycles the electrode retained 94.3 percent of its current, reaching 30.2 milliamperes per square centimeter, although the anodic oxidation feature shifted from roughly 0.40 to 0.49 volts. The authors interpret this shift not as degradation but as the gradual accumulation of adsorbed carbonaceous intermediates and reorganization of the surface oxyhydroxide layer, a reading supported by their post-mortem analyses. Inductively coupled plasma optical emission spectroscopy of the electrolyte after testing found nickel concentrations below the detection limit and copper at just 0.051 parts per million, and X-ray photoelectron spectra taken before and after operation showed the nickel and copper oxidation states essentially intact, confirming that the redox-active surface survives chemically.</p>
<p>What makes this work resonate beyond a single materials system is its recipe-like transferability. Rather than hunting for exotic compounds, the researchers demonstrated that a mainstream physical deposition technique, a cheap transition metal dopant, and careful normalization of electrochemical data can jointly push a simple nickel oxide film to performance levels that compete with far more elaborate catalysts. The band gap engineering, the bifunctional nickel-copper mechanism, and the documented poison tolerance together outline a practical roadmap for alkaline direct methanol fuel cells that sidestep platinum entirely. The authors point toward the logical next steps: integrating these optimized films into membrane electrode assemblies and testing them in full fuel cell stacks, where real operating conditions will judge whether laboratory elegance translates into engineered power. If it does, the humble nickel oxide lattice, nudged by a few percent of copper, may find itself at the heart of a new generation of liquid-fuel clean energy devices.</p>
<p><strong>Subject of Research:</strong> Copper-doped nickel oxide thin film electrocatalysts for the methanol oxidation reaction in direct methanol fuel cells</p>
<p><strong>Article Title:</strong> Tuning methanol oxidation activity: impact of Cu content on sputtered NiO thin film electrocatalysts</p>
<p><strong>Article References:</strong> Tuning methanol oxidation activity: impact of Cu content on sputtered NiO thin film electrocatalysts. (n.d.). <a href="https://doi.org/10.1007/s11051-026-06765-0" rel="noopener noreferrer">https://doi.org/10.1007/s11051-026-06765-0</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1007/s11051-026-06765-0" rel="noopener noreferrer">10.1007/s11051-026-06765-0</a></p>
<p><strong>Keywords:</strong> Cu-doped NiO, methanol oxidation reaction, direct methanol fuel cells, electrocatalysis, co-sputtering deposition, thin films, band gap engineering, Tafel analysis, alkaline electrolyte, nickel oxide, carbon monoxide tolerance, electrochemical impedance spectroscopy</p>
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		<post-id xmlns="com-wordpress:feed-additions:1">211218</post-id>	</item>
		<item>
		<title>Iron-tin dual-atom catalyst shields seawater batteries from chloride attack</title>
		<link>https://scienmag.com/iron-tin-dual-atom-catalyst-shields-seawater-batteries-from-chloride-attack/</link>
		
		<dc:creator><![CDATA[Bethany Barker]]></dc:creator>
		<pubDate>Tue, 22 Sep 2026 17:51:48 +0000</pubDate>
				<category><![CDATA[Marine]]></category>
		<category><![CDATA[advanced catalyst materials for seawater applications]]></category>
		<category><![CDATA[air cathode]]></category>
		<category><![CDATA[alkaline electrolyte]]></category>
		<category><![CDATA[atomic-scale catalyst design]]></category>
		<category><![CDATA[chloride corrosion]]></category>
		<category><![CDATA[chloride corrosion resistance]]></category>
		<category><![CDATA[chloride ion interference in electrochemistry]]></category>
		<category><![CDATA[corrosion prevention in seawater batteries]]></category>
		<category><![CDATA[density functional theory]]></category>
		<category><![CDATA[dual single-atom catalyst]]></category>
		<category><![CDATA[dual-atom iron-tin catalysts]]></category>
		<category><![CDATA[Electrocatalysis]]></category>
		<category><![CDATA[iron-tin catalyst]]></category>
		<category><![CDATA[marine energy device durability]]></category>
		<category><![CDATA[marine energy storage]]></category>
		<category><![CDATA[nitrogen-doped carbon]]></category>
		<category><![CDATA[oxygen reduction reaction]]></category>
		<category><![CDATA[oxygen reduction reaction in marine energy storage]]></category>
		<category><![CDATA[p-d orbital hybridization]]></category>
		<category><![CDATA[scalable marine energy storage solutions]]></category>
		<category><![CDATA[Seawater Batteries]]></category>
		<category><![CDATA[seawater battery cathode catalysts]]></category>
		<category><![CDATA[Seawater battery technology]]></category>
		<category><![CDATA[seawater electrolyte stability]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=207371</guid>

					<description><![CDATA[Researchers at Hainan University have designed an iron-tin dual single-atom catalyst that accelerates oxygen reduction in alkaline seawater while blocking chloride poisoning, enabling seawater batteries to deliver high power and stability for more than 500 hours.]]></description>
										<content:encoded><![CDATA[<p>Seawater batteries have long been celebrated as one of the most promising routes to safe, scalable marine energy storage. They rely on an electrolyte that is effectively inexhaustible, they avoid the flammable organic solvents that plague conventional lithium-ion cells, and their theoretical energy densities are attractive for powering buoys, underwater vehicles, desalination platforms and offshore sensors. Yet for all their promise, these devices have been held back by a stubborn electrochemical bottleneck at the air cathode, where the oxygen reduction reaction, the process that accepts electrons as the battery discharges, proceeds far too slowly on most available catalyst surfaces. Now a team at Hainan University reports an atomic-scale design that tackles both the sluggish kinetics and the corrosive chemistry of the sea at the same time.</p>
<p>The core of the problem is chloride. Seawater carries a high concentration of chloride ions, and at the cathode of a seawater air battery these ions behave as aggressive interlopers. They adsorb onto the very metal centers that are supposed to bind oxygen intermediates, blocking active sites, degrading catalytic performance and accelerating the corrosion of the catalyst layer itself. Iron-based single-atom catalysts, prized for their high intrinsic oxygen reduction activity in alkaline conditions, are particularly vulnerable. The result is a painful trade-off: catalysts that are highly active on the bench tend to lose their edge quickly in real seawater, while corrosion-resistant materials are often too sluggish to deliver competitive power.</p>
<p>The Hainan University group, led by corresponding author Peng Rao, approached this dilemma with a concept they describe as p-d orbital hybridization. Instead of leaving iron atoms to fend for themselves on a carbon support, the researchers paired each iron active site with an adjacent tin atom, creating what is known as a dual single-atom catalyst. Tin, a p-block element with its own distinct orbital character, does not simply sit nearby as a passive neighbor. Through overlap between its p orbitals and the d orbitals of iron, it reshapes the local electronic structure of the iron center, tuning how strongly the site binds oxygen-containing intermediates and how hospitably it treats chloride ions in the surrounding electrolyte.</p>
<p>This electronic engineering addresses a well-known limitation of conventional iron sites. In many iron-nitrogen-carbon catalysts, the binding of oxygen reduction intermediates is too strong, meaning that reaction intermediates such as hydroperoxyl species linger on the surface longer than they should and slow the overall turnover of the catalyst. The Fe-Sn interaction weakens this overly strong adsorption into a more favorable intermediate regime, while simultaneously creating a locally negatively charged interface around the iron site. Because chloride ions are negatively charged, that charged microenvironment electrostatically discourages them from approaching and poisoning the active center. In effect, the catalyst builds a nanoscale fence around its most valuable atom.</p>
<p>The design did not emerge by guesswork. The team first carried out density functional theory calculations, comparing several candidate pairings of iron with different p-block metals in dual-site configurations. Among the candidates, the iron-tin combination stood out with the best balance between oxygen reduction activity and chloride resistance, providing the theoretical justification for an ambitious synthesis. The researchers then produced the material using what they call a movable-type printing strategy, a modular approach that positions the two metal precursors with atomic precision on a nitrogen-doped carbon support before activation locks them into place.</p>
<p>Advanced characterization confirmed that the synthesis had achieved its goal. Microscopy and X-ray spectroscopy showed that both iron and tin were atomically dispersed across the carbon framework, stabilized as adjacent dual single-atom sites rather than clustering into nanoparticles. That atomic dispersion matters enormously. It maximizes the density of accessible active sites, ensures that every iron atom benefits from a tin neighbor, and prevents the formation of larger metal particles that could serve as initiation points for corrosion in the harsh chloride-rich environment.</p>
<p>Electrochemical testing in alkaline seawater electrolyte delivered striking results. The FeSn dual single-atom catalyst achieved a half-wave potential of 0.900 volts versus the reversible hydrogen electrode, outperforming both single-metal iron and tin catalysts prepared in the same way and beating commercial platinum-on-carbon, the traditional benchmark for oxygen reduction. The catalyst followed a near four-electron oxygen reduction pathway, the most efficient route that converts oxygen directly to hydroxide and delivers the maximum possible cell voltage. Equally important for real deployment, the material showed negligible activity decay after 30,000 accelerated durability test cycles, a punishing stress test that simulates years of charge-discharge operation.</p>
<p>Perhaps the most convincing evidence came from post-mortem analysis. After extended testing in the chloride-laden electrolyte, X-ray photoelectron spectroscopy revealed no observable iron-chloride signal on the catalyst surface, indicating that chloride adsorption on the iron active sites had been effectively suppressed throughout the testing period. This directly validates the design hypothesis: the negatively charged microenvironment generated by the Fe-Sn electronic interaction had done its job, keeping the poison away from the active center even as the catalyst worked hard for tens of thousands of cycles.</p>
<p>&#8220;For seawater batteries, activity alone is not enough,&#8221; said Peng Rao, the corresponding author of the study. &#8220;The catalyst also needs to drive oxygen conversion efficiently while resisting chloride-induced poisoning. The Fe-Sn dual-site structure gives us a way to combine these two functions at the atomic level.&#8221; The quote captures the central lesson of the work: in marine electrochemistry, selectivity against chloride is not an optional extra but a design requirement on par with activity itself.</p>
<p>The practical payoff was demonstrated when the catalyst was assembled into flow-type seawater air batteries. Devices built with the FeSn dual single-atom catalyst reached a peak power density of 255.6 milliwatts per square centimeter, higher than comparable cells based on platinum-on-carbon or the iron-only single-atom catalyst, and operated stably for more than 500 hours under the reported testing conditions. That combination of high power and long endurance in a realistic seawater-fed architecture suggests the material is ready to be taken seriously for marine energy systems rather than remaining a laboratory curiosity.</p>
<p>Beyond the immediate application, the study positions p-d orbital engineering as a general strategy for designing electrocatalysts that must simultaneously deliver high activity and resist chloride attack. Many reactions of interest in seawater electrochemistry, from oxygen evolution to chlorine-tolerant hydrogen production, face the same fundamental challenge of selective chemistry in an ionically aggressive medium. If pairing active transition-metal sites with judiciously chosen p-block partners proves general, the design principle demonstrated here could extend well beyond iron and tin, and well beyond oxygen reduction.</p>
<p>The research, published in Science Bulletin, arrives at a moment of growing investment in ocean-based energy infrastructure. Offshore wind farms, autonomous underwater systems and remote marine sensors all need durable storage, and seawater batteries are among the few options whose electrolyte comes free with the deployment site. By showing that a simple atomic partnership, one iron atom and one tin atom held in place on a carbon support, can defuse the corrosive chemistry of the ocean while accelerating the very reaction the battery depends on, the Hainan University team has moved the field a meaningful step closer to seawater batteries that survive, and thrive, in the environment they are built to harness.</p>
<p><strong>Subject of Research:</strong> Development of an iron-tin dual single-atom catalyst using p-d orbital hybridization to improve oxygen reduction activity and chloride resistance in seawater batteries</p>
<p><strong>Article Title:</strong> How can seawater batteries survive chloride corrosion?</p>
<p><strong>Article References:</strong> How can seawater batteries survive chloride corrosion?. (n.d.). <a href="https://www.eurekalert.org/news-releases/1144681" rel="noopener noreferrer">Original publication</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> Not provided</p>
<p><strong>Keywords:</strong> seawater batteries, oxygen reduction reaction, dual single-atom catalyst, chloride corrosion, p-d orbital hybridization, iron-tin catalyst, electrocatalysis, alkaline electrolyte, marine energy storage, density functional theory, nitrogen-doped carbon, air cathode</p>
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