The lithium-metal battery has long been regarded as the ultimate prize in rechargeable energy storage: lithium is exceptionally light, and a metallic lithium anode can store far more charge per unit mass than the graphite used in most commercial batteries. Replacing flammable liquid electrolytes with solid materials could also improve safety and enable batteries with greater energy density. Yet one of the most stubborn obstacles has remained hidden inside the battery interface itself. During charging and discharging, lithium can be removed unevenly from the metal electrode, leaving behind microscopic empty regions known as voids. Those gaps disrupt electrical contact, concentrate current into smaller areas and can eventually encourage needle-like lithium structures called dendrites. A study published in Nature Materials now reports a strategy for designing lithium anodes that resist this failure pathway, while identifying a quantitative rule that links void formation to both how much lithium is removed and how quickly it is extracted.
The researchers show that void formation is governed by the product of the lithium full-stripping areal capacity and the applied current density. They describe this combined quantity through a parameter called void suppression capability, or VSC. In practical terms, the metric captures a central trade-off in solid-state cells: stripping a large amount of lithium at a high current places a severe demand on the metal anode, because lithium atoms must move through the electrode quickly enough to replenish the interface as lithium ions migrate into the electrolyte. If the supply cannot keep pace with the electrochemical reaction, the interface begins to lose physical contact. Instead of remaining a uniform, electronically connected surface, it develops cavities where lithium has been depleted. The VSC framework provides a way to compare anodes according to how effectively their internal atomic transport can prevent that process.
At the heart of the problem is the difference between ionic and electronic transport in a solid-state battery. During discharge, lithium atoms in the metal anode give up electrons and become lithium ions, which travel through the solid electrolyte toward the cathode. During charging, lithium ions return and are reduced back to metallic lithium at the anode. For the reaction to remain stable, newly deposited lithium must spread across the interface, while lithium being stripped must be supplied from the bulk metal. In a liquid electrolyte, fluid motion and intimate wetting can help maintain contact, but a solid electrolyte does not readily flow into newly formed gaps. A void can therefore act like a growing crack in the electrochemical pathway. The local current then becomes concentrated around the remaining contact points, increasing the likelihood of uneven deposition and dendrite growth when the battery is charged again.
The study identifies two material properties that improve VSC: lithium self-diffusivity and the initial concentration of lithium atoms available to move through the metal. Self-diffusivity describes the thermally activated motion of lithium atoms within the anode. A higher value means that atoms can redistribute more rapidly in response to concentration gradients created during stripping. This redistribution can help replenish regions beneath the electrolyte interface before they become isolated and empty. The initial lithium atom concentration, meanwhile, affects how much mobile material is available to sustain the reaction. Together, these factors determine whether the anode can accommodate a demanding current without losing continuity. The finding shifts attention away from treating voids as an unavoidable consequence of solid-state operation and toward engineering the microscopic transport properties of the lithium itself.
To test that idea, the researchers introduced a small amount of magnesium and lanthanum into molten lithium. The resulting material, described as LiMgLa, contains magnesium with 1 weight percent lanthanum and was designed to refine the metal’s grain structure. Grain refinement changes the network of boundaries and pathways through which atoms move inside a polycrystalline metal. In the researchers’ experiments, the inoculant increased lithium self-diffusivity and improved the anode’s void suppression capability. The comparison was made with a LiMg anode, which contained magnesium but not the lanthanum addition. This type of alloying is significant because it does not depend solely on coating the electrode or modifying the solid electrolyte. Instead, it alters the transport behavior of the lithium electrode throughout its volume, potentially allowing the metal to respond more quickly as lithium is stripped from and plated back onto its surface.
The improvement was reflected in the critical operating limits of the anodes. For the LiMg material, the critical current density and areal capacity were reported as 1.2 milliamperes per square centimeter and 0.6 milliampere-hours per square centimeter, respectively. With the LiMgLa anode, those values increased to 2.2 milliamperes per square centimeter and 1.1 milliampere-hours per square centimeter. Critical current density indicates how rapidly charge can be transferred per unit area before unstable behavior emerges, while areal capacity describes how much charge is moved through a defined electrode area. These measures are especially important for practical batteries because increasing the active material loading and operating at higher power both raise the amount of lithium that must be transported through the interface. An anode that survives only gentle laboratory cycling may offer little advantage in a high-energy cell, whereas a wider operating window could make solid-state designs more relevant to electric vehicles and other demanding applications.
The LiMgLa electrodes also enabled stable lithium plating and stripping for more than 1,200 hours at room temperature under a current density of 0.7 milliamperes per square centimeter. Plating refers to the deposition of metallic lithium during charging, while stripping is the removal of lithium during discharge. Repeating these processes without rapid failure is difficult because each cycle can magnify small variations in contact, surface roughness and local current density. The reported endurance suggests that the refined alloy can maintain a more uniform electrochemical interface over long operation, although a laboratory symmetric-cell result is not equivalent to demonstrating a complete commercial battery. Full cells introduce additional complications, including cathode limitations, interfacial chemical reactions, mechanical pressure changes and the need to balance the amount of lithium against the cathode’s capacity. Even so, long-duration cycling at room temperature is an important demonstration that the material’s benefits are not limited to a single short experiment.
The researchers used phase-field modelling to examine how void formation and dendrite growth are connected. Phase-field models simulate the evolution of interfaces by representing transitions between different material states—such as lithium metal, solid electrolyte and empty space—through spatially varying fields. Rather than tracking every atom, the method calculates how thermodynamics, diffusion and electrochemical forces reshape the interface over time. The modelling indicates that the interfacial overpotential becomes larger than the electrolyte’s critical overpotential when the stripped capacity exceeds 70 percent of the full depletion capacity. Overpotential is the additional voltage required to drive an electrochemical reaction beyond its equilibrium condition. Once it passes the critical value, the interface can become unstable, favouring localized lithium deposition and dendritic structures. This 70 percent threshold offers a practical warning: operating too close to complete local lithium depletion may trigger failure even if the average current appears acceptable.
That threshold also helps explain why voids and dendrites should be treated as parts of the same failure sequence rather than as entirely separate problems. Stripping can first create a gap and reduce the area through which current flows. The remaining contact area then carries a larger fraction of the total current, increasing the local current density and interfacial overpotential. During the next charging step, lithium preferentially deposits at sites where the electrochemical conditions are most favorable, potentially producing protrusions that grow toward or through the solid electrolyte. Those dendrites can cause short circuits, while the mechanical stress associated with deposition can further damage the interface. By improving atomic self-diffusion, the LiMgLa alloy appears to reduce the likelihood that the initial void will form, thereby interrupting the chain of events before current focusing and unstable growth begin. The work therefore presents an anode-centered route to controlling a problem often attributed primarily to the solid electrolyte.
The findings provide a design rule for all-solid-state lithium-metal batteries: maximize the anode’s ability to redistribute lithium, and avoid operating conditions that strip the metal beyond the point where the interface can remain supplied. The proposed VSC concept could help researchers compare different lithium alloys, microstructures and processing methods using a common framework rather than relying only on trial-and-error cycling. It may also guide the selection of electrode thickness, applied current and usable lithium inventory in future cells. Important questions remain, including how the alloy behaves against different solid electrolytes, how it performs under practical stack pressures and whether the lanthanum-containing composition can be manufactured economically at large scale. Nevertheless, by connecting atomic motion to a measurable operating limit and demonstrating more than 1,200 hours of stable cycling, the study offers a concrete path toward lithium-metal batteries that combine high energy density with the mechanical and electrochemical stability required for real-world use.
Subject of Research: Void-suppressive lithium-metal anodes for all-solid-state batteries
Article Title: Void suppressive lithium anodes for all-solid-state batteries
Article References: Ji, X., Liu, Y., He, X. et al. “Void suppressive lithium anodes for all-solid-state batteries.” Nature Materials (2026). https://doi.org/10.1038/s41563-026-02729-w
Image Credits: AI Generated
DOI: 10.1038/s41563-026-02729-w
Keywords: all-solid-state batteries, lithium-metal anodes, void formation, dendrite growth, lithium self-diffusivity, void suppression capability, LiMgLa alloy, solid electrolytes
Tags: advanced lithium anode engineeringall-solid-state battery energy densitydendrite suppression in lithium batterieselectrode-electrolyte interface stabilityimproving lithium-metal battery lifespanlithium anode void formationlithium stripping and plating dynamicslithium-metal battery safetymitigation of lithium dendrite growthsolid electrolyte interface issuessolid-state battery failure mechanismsvoid suppression capability (VSC) in battery design
