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Dysprosium

Dysprosium is a chemical element with the atomic symbol Dy and atomic number 66, belonging to the lanthanide series of rare-earth metals. It appears as a soft, silvery-white metal at room temperature, exhibiting high thermal neutron absorption and strong magnetic susceptibility that distinguish it among elements. Discovered in 1886 by French chemist Paul-Émile Lecoq de Boisbaudran through fractional crystallization and spectroscopic separation from holmium oxide, its name derives from the Greek dysprositos, meaning "hard to get at," reflecting the challenges in its isolation. With an atomic mass of 162.50 u, dysprosium occurs naturally in minerals such as xenotime and monazite, though it constitutes a minor fraction of rare-earth deposits, complicating extraction. Dysprosium's defining properties include a high and resistance to demagnetization at elevated temperatures, enabling its alloying with in NdFeB permanent magnets for enhanced in applications like electric motors, generators, and devices. These magnets underpin technologies critical to and , where dysprosium doping improves performance under operational stresses. In , dysprosium's exceptional cross-section—among the highest for thermal neutrons—positions it as a key material for control rods in reactors, regulating fission without significant fission byproduct generation. Furthermore, dysprosium compounds find use in solid-state lasers and sources, leveraging their luminescent and radiative efficiencies for analytical and . Despite its scarcity and reliance on limited sources, primarily in , dysprosium remains indispensable for advancing high-performance materials in , , and clean sectors.

Properties

Physical properties

Dysprosium is a silvery-white rare earth metal with atomic number 66. Its density at is 8.55 g/cm³. The element melts at 1412 °C and boils at 2567 °C. Dysprosium exhibits a hexagonal close-packed in its stable form. At , it is paramagnetic, possessing a mass of 5.45 × 10⁻⁶ m³/. The metal demonstrates a Brinell of 500 and a Vickers of 540 . Dysprosium has one of the highest thermal neutron absorption cross-sections among elements, approximately 950 barns for key isotopes, enabling its role in neutron control applications. Its linear coefficient is 9.9 × 10⁻⁶ K⁻¹.
PropertyValueSource
(20 °C)8.55 g/cm³RSC Periodic Table
Melting point1412 °CRSC Periodic Table
Boiling point2567 °CRSC Periodic Table
Brinell 500 MPaWebElements
coeff.9.9 × 10⁻⁶ K⁻¹Engineering ToolBox

Chemical properties

Dysprosium exhibits the [Xe] 4f¹⁰ 6s², leading to a predominant +3 in its compounds, as the 4f electrons are shielded and the 6s electrons are readily lost. Less common +2 and +4 states occur under specific conditions, but +3 dominates due to the stability of the half-filled f-shell configuration and electronic trends. The Dy³⁺ , with an of approximately 0.912 Å in six-coordinate geometry, supports high coordination numbers (typically 7–9) in complexes, arising from its large size and preferences typical of early s despite effects. The metal displays moderate reactivity, tarnishing slowly in moist air via surface oxidation and igniting when heated to form the Dy₂O₃ via the reaction 4Dy + 3O₂ → 2Dy₂O₃. Dysprosium reacts slowly with cold water to generate Dy(OH)₃ and , accelerating with hot water, while it dissolves rapidly in dilute mineral acids (except , where insoluble DyF₃ passivates the surface). In aqueous media, Dy³⁺ remains stable as the aquo complex [Dy(H₂O)₈]³⁺ or similar, with minimal at neutral due to its intermediate positioning. Dysprosium forms trivalent halides such as DyF₃, DyCl₃, DyBr₃, and DyI₃, which are ionic solids with high melting points reflecting ionic character, and the pale yellow-green Dy₂O₃, sparingly soluble in but amphoteric. Organometallic derivatives like cyclopentadienyl complexes exist but are air-sensitive and less stable than those of lighter s. The progressively reduces ionic radii across the series (from ~1.03 Å for La³⁺ to 0.86 Å for Lu³⁺ in CN6), compressing Dy³⁺ bonds and enhancing field influences in compounds compared to non-f-block analogs.

Isotopes

Dysprosium consists of seven isotopes, ranging from 156Dy to 164Dy, with no radioactive isotopes contributing significantly to its natural abundance. The weighted average is 162.500(1) u, reflecting the relative abundances determined via . The isotopic abundances are as follows:
IsotopeRelative atomic mass (u)Natural abundance (atom %)
156Dy155.924 278 99(20)0.055 60(90)
158Dy157.924 404 8(20)0.095 0(20)
160Dy159.925 193 5(20)2.336(8)
161Dy160.926 934 6(20)18.90(2)
162Dy161.926 794 2(20)25.48(2)
163Dy162.928 728 4(20)24.87(2)
164Dy163.929 181 9(20)28.18(3)
164Dy is the most abundant, comprising approximately 28.18% of natural dysprosium. Dysprosium has 29 known radioactive , with masses ranging from 140Dy to 177Dy, characterized through experiments and decay studies. The longest-lived is 154Dy, with a of 3 × 106 years, decaying primarily via alpha emission. Another notable isotope is 159Dy, with a of 144.4 days, undergoing beta-minus decay. on stable isotopes, such as 164Dy(n,γ)165Dy, produces short-lived radioactive daughters like 165Dy ( ~2.3 hours), which can serve as precursors for isotopes via further reactions. Dysprosium isotopes exhibit exceptionally high thermal capture cross-sections, for example, ~2320 barns for 164Dy at 0.0334 eV, as measured in irradiation experiments. This occurs predominantly through (n,γ) reactions, leading to radiative capture without product generation, a property confirmed by nuclear data evaluations up to 20 MeV. Such characteristics stem from the even-odd nuclear structure of dysprosium, favoring over pathways observed in heavier actinides.

History

Discovery and isolation

Dysprosium oxide was first isolated in 1886 by French chemist through fractional crystallization of holmium oxide samples derived from yttrium preparations. Lecoq de Boisbaudran detected the presence of dysprosium via distinct spectroscopic lines observed in the spectrum of , which deviated from expected patterns and indicated an impurity requiring separation. He achieved this by dissolving the oxide in acid, followed by repeated precipitation and crystallization steps, requiring over 30 attempts to obtain a sufficient quantity of the new oxide. The isolation highlighted the challenges of separating chemically similar rare earth elements, as dysprosium co-occurred with and other lanthanides in mineral sources like yttria. While the oxide was obtained, the metallic form was not produced until 1906 by Georges Urbain, who reduced dysprosium compounds using or other metallothermic methods. Early samples remained impure due to limitations in separation techniques, with atomic weight determinations and spectral confirmations revealing persistent contaminants from neighboring elements. Significant advances in purification occurred only after , when ion-exchange chromatography enabled the production of dysprosium in relatively pure form by the 1950s, overcoming the inefficiencies of earlier fractional methods. This technique, developed for rare earth separations, allowed for precise elution based on differential affinities, yielding oxides and metals of high purity essential for subsequent characterization and applications.

Etymology and early research

The name dysprosium originates from the δυσπρόσιτος (dysprositos), meaning "hard to get at" or "difficult to access," a term chosen by to highlight the challenges in isolating the element from complex rare earth mixtures in and oxides. identified dysprosium oxide (dysprosia) in through spectroscopic analysis of oxide impurities, requiring over 30 attempts to separate spectral lines distinct from those of and , elements with which it was frequently conflated in early mineral analyses of and . This confusion stemmed from overlapping atomic spectra and chemical similarities among heavy lanthanides, delaying unambiguous identification until repeated purification efforts confirmed dysprosium's unique emission lines. Following Lecoq de Boisbaudran's announcement, early 20th-century emphasized verification of dysprosium's elemental status and basic properties via improved separation techniques. In 1906, French chemist Georges Urbain achieved a purer through fractional crystallization of rare earth double salts, enabling more precise characterization of its optical spectrum and . Initial studies revealed dysprosium's high , with susceptibility measurements adhering to the Curie-Weiss across paramagnetic phases, though scarcity limited extensive experimentation to spectroscopic and thermodynamic assessments rather than bulk applications. These investigations underscored dysprosium's potential as a strongly paramagnetic but highlighted purification barriers that confined to academic contexts until mid-century ion-exchange methods advanced yields.

Occurrence and Reserves

Abundance and distribution

Dysprosium exhibits an average crustal abundance of 5.2 to 6.2 parts per million (ppm) in the , positioning it as the 42nd most abundant overall. This places it within the heavy rare earth (HREE) subgroup, where it constitutes a minor but significant portion relative to lighter rare earths, with total rare earth crustal contents varying from at approximately 60 ppm to heavier elements like at 0.5 ppm. In , dysprosium concentrations are trace, typically around 0.9 to 1 nanogram per liter (ng/L), reflecting its low solubility and geochemical partitioning. Geochemically, dysprosium is predominantly associated with minerals such as ((Ce,La,Nd,Th)PO₄) and (YPO₄), the latter being particularly enriched in HREEs due to ionic radius similarities with and heavy lanthanides. It occurs in lesser amounts in fluorocarbonates like ((Ce,La)CO₃F), which favor light rare earth elements but contain trace HREEs. Dysprosium shows notable enrichment in ion-adsorption clays formed via of granitic rocks, where processes mobilize HREEs from primary minerals and adsorb them onto clay surfaces such as , preferentially retaining heavier elements due to stronger electrostatic interactions. Cosmically, dysprosium's abundance is estimated at approximately 0.28 in carbonaceous meteorites and lower in solar abundances (around 0.002 relative to ), primarily synthesized through rapid (r-process) in core-collapse supernovae and mergers, with contributions from slow (s-process) in stars. These nucleosynthesis pathways explain its relatively uniform distribution in primitive solar system materials, contrasting with differentiation-driven crustal enrichments on .

Major deposits

Global reserves of dysprosium are estimated at approximately 1.1 million metric tons of contained metal, with holding roughly 50% based on assessments of (REE) deposits enriched in heavy REEs such as dysprosium. , , and the follow as significant holders, though their shares are smaller and often tied to specific heavy REE-enriched sites rather than total REE volumes. China's major dysprosium deposits are primarily ionic adsorption clays in southern provinces including , , and , which uniquely concentrate heavy rare earth elements like dysprosium through weathering processes. These deposits supply the bulk of global dysprosium resources outside conventional hard-rock mining. The Bayan Obo site in , the world's largest REE deposit, contains dysprosium as a minor component within its vast and ores, contributing to China's overall reserves despite its predominance in light REEs. In , the Browns Range project in hosts xenotime-bearing deposits exceptionally rich in dysprosium and , with resource estimates highlighting its potential as a non-Chinese heavy REE source. The Mount Weld carbonatite deposit, operated by Rare Earths, includes dysprosium within its REE inventory, though at lower concentrations compared to Browns Range. Myanmar's ionic clay deposits in regions like have emerged as key heavy REE sources, analogous to China's, with empirical assays confirming elevated dysprosium levels amid recent exploration upticks. In the United States, the Fluorspar property in has verified neodymium-dysprosium enrichments through 2024–2025 fieldwork, indicating potential for domestic heavy REE recovery from unconventional sources.

Production

Extraction and separation processes

Dysprosium is extracted from (REE) ores, primarily , , and , via initial beneficiation to concentrate REE-bearing minerals. This involves crushing and grinding the ore, followed by using collectors such as fatty acids to separate REE phosphates or carbonates from materials like silica and iron oxides, yielding a concentrate with 30-70% total REE oxides. The concentrate undergoes hydrometallurgical processing, typically roasting at 200-300°C to convert insoluble REE phosphates to sulfates, followed by water or acid to solubilize over 90% of the REEs into as sulfates or chlorides; is also employed for certain ores like , achieving selective recovery of heavy REEs including dysprosium. Impurities such as and are removed via or solvent extraction prior to REE separation. Due to the chemical similarity of REEs, dysprosium isolation relies on multi-stage solvent extraction, where acidic organophosphorus extractants like di-(2-ethylhexyl)phosphoric acid (D2EHPA) in selectively partition dysprosium ions from nitric or feeds into the organic phase, exploiting differences in distribution coefficients (e.g., higher for heavy REEs like Dy over ). The process includes extraction, scrubbing with dilute acid to purify the loaded organic phase, and stripping with stronger acid to recover dysprosium, often requiring 100-200 stages for >99% purity; yield losses occur during heavy REE due to co-extraction of neighbors like and . The extracted dysprosium is precipitated as , filtered, and calcined to dysprosium (Dy₂O₃) at 800-1000°C. Dysprosium metal is obtained by metallothermic reduction of DyF₃ with calcium at 1200-1400°C under , producing crude metal that is vacuum-distilled to remove calcium and achieve >99.9% purity. of DyF₃ in molten salts (e.g., LiF-DyF₃ eutectic) at cathodes offers an alternative, with cathodic reduction of Dy³⁺ to Dy in a single three-electron step, though it is less common industrially due to corrosion and demands exceeding 10 kWh/kg. These reduction methods are highly energy-intensive, with overall process efficiencies limited by separation losses and thermal requirements.

Global production leaders

China dominates global dysprosium production, accounting for over 99% of processed dysprosium oxide as of 2025, with refined output concentrated in facilities controlled by state-backed enterprises like Northern Rare Earth Group and China Southern Rare Earth Group. Global production of dysprosium oxide exceeded 2,300 metric tons in 2024, primarily as rare earth oxide (REO) equivalent, driven by extraction from , , and ion-adsorption clay deposits, though nearly all separation and refining occurs within due to its technological and cost advantages in solvent extraction processes. This monopoly creates vulnerabilities, as disruptions in Chinese processing—such as export controls implemented in October 2025—can halt global availability of separated dysprosium despite mining in other regions. Non-Chinese production remains marginal, with Australia-based Rare Earths operating the Mount Weld mine and Malaysian processing facility yielding small volumes of separated dysprosium oxide, estimated at under 100 tonnes annually as of 2024. The ' , via its , focuses primarily on light rare earths but has initiated limited heavy rare earth separation including dysprosium, producing negligible quantities relative to in 2024. Myanmar contributes via ion-adsorption deposits exported largely to for processing, adding to feedstock but not refined output outside Chinese control. Recycling from end-of-life magnets and scrap represents less than 5% of supply, constrained by collection inefficiencies and technical challenges in recovering high-purity dysprosium. Production volumes have ramped up since , correlating with surging demand for dysprosium-doped neodymium-iron-boron magnets in electric vehicles and wind turbines, which require 1-2% dysprosium for thermal stability; global output tripled from under 1,000 tonnes REO equivalent in to current levels, yet diversification efforts by Western producers have failed to erode 's refining hegemony. This processing concentration amplifies geopolitical risks, as non-Chinese mined concentrates often ship to for final separation, linking output security to Beijing's policy decisions.

Applications

Industrial and technological uses

Dysprosium is incorporated as an additive in neodymium-iron-boron (NdFeB) permanent magnets at concentrations typically ranging from 1% to 5% by weight, where it substitutes for to form a core-shell structure that significantly enhances intrinsic and resistance to demagnetization at elevated temperatures. This improvement allows magnets to maintain performance in applications requiring thermal stability, such as motors operating at up to 150–180°C and direct-drive generators exposed to variable environmental conditions. The addition also elevates the effective range in these alloys, extending operational limits beyond those of undoped NdFeB, which has a base Curie point around 310–400°C but suffers loss at lower thresholds without dysprosium. In , dysprosium-enhanced NdFeB magnets are essential for the voice coil actuators in hard disk drives (HDDs), providing the high needed for reliable positioning in compact, high-speed mechanisms. Beyond magnets, dysprosium serves as a in materials, notably in dysprosium-doped yttrium aluminum (Dy:YAG) crystals, which enable efficient four-level operation in the , particularly yellow emissions around 577 nm suitable for medical and applications. Dysprosium ions (Dy³⁺) act as activators in phosphors for white light-emitting diodes (LEDs), where concentrations of 1–3 mol% produce complementary (480 nm) and (575 nm) emissions under near-UV excitation, achieving color temperatures around 5000–6500 K with quantum efficiencies exceeding 70% in optimized hosts like silicates or aluminates. In , dysprosium oxide-nickel cermets are employed in control rods for thermal reactors, leveraging dysprosium's high thermal cross-section (over 1000 barns) to absorb neutrons effectively without significant swelling or gas evolution under .

Military and strategic applications

Dysprosium enhances the performance of neodymium-iron-boron permanent magnets by increasing their intrinsic and , enabling reliable operation in high-temperature military environments where standard magnets would fail. These dysprosium-alloyed magnets are integral to actuators, sensors, and electric motors in platforms like the F-35 Lightning II fighter jet, which requires over 400 kilograms of rare earth elements including dysprosium to withstand operational stresses exceeding 150°C. Similarly, they support precision-guided munitions such as the (JDAM), where dysprosium contributes to the targeting and guidance systems' resilience under and vibration. In radar and avionics systems, dysprosium's role in heat-resistant magnets ensures and maintain accuracy during sustained high-power operations, as seen in advanced radar arrays. For naval applications, these magnets power propulsion and control systems in , where compact, high-torque performance is essential for and maneuverability. Dysprosium titanate serves as a neutron-absorbing material in control rods for thermal nuclear reactors, leveraging its high thermal cross-section (approximately 1,100 barns for Dy-164) and low swelling under , which supports reactivity control in compact naval reactor designs. The U.S. Department of Defense classifies dysprosium as a critical material for , with initiatives underway to establish stockpiles valued at up to $1 billion in rare earths to mitigate supply disruptions, as domestic reserves remain depleted and production lags behind defense demands.

Supply Chain and Geopolitics

Supply dependencies and risks

maintains near-total control over dysprosium , processing approximately 99.9% of global supply as of 2025, which exposes downstream industries to risks from unilateral policies. In April 2025, imposed restrictions on dysprosium and six other rare earth elements in response to U.S. tariffs, requiring special licenses that could delay or halt shipments to foreign buyers. Further controls announced on , 2025, targeted medium and heavy rare earths, intensifying supply concentration risks amid ongoing trade tensions. This dominance stems from 's integrated mining-to- infrastructure, where over 90% of heavy rare earth separation capacity resides, enabling rapid deployment of quotas or bans that historical precedents, such as 2010 restrictions, have shown can spike prices by over 500%. Myanmar's role as an emerging source for heavy rare earth ores, including dysprosium-bearing minerals, introduces additional geopolitical volatility due to ongoing following the coup. Rebel groups and ethnic armed organizations control key mining areas in northern regions like , where illicit operations supply up to 50% of China's heavy rare earth imports, but disruptions from fighting have already led to intermittent halts in 2025 exports. This instability amplifies supply risks, as Myanmar's ion-adsorption clay deposits are low-cost but unregulated, with no viable alternatives scaling quickly to offset potential shutdowns. Scenario analyses indicate that export bans or prolonged disruptions could severely constrain dysprosium availability, with demand alone projected to exceed historical supply levels by 2025 under moderate growth assumptions. Modeling from the and others forecasts three- to seven-fold increases in rare earth demand by 2040 for clean energy technologies, outpacing diversified mining capacity and leading to primary supply deficits unless processing bottlenecks are resolved. U.S. and EU diversification initiatives, including subsidies under the 2022 , have spurred investments in domestic separation facilities but remain nascent, with non-Chinese refining capacity under 10% of global needs as of 2025 and timelines extending beyond 2030 for meaningful scale-up. Recycling offers limited mitigation, with global rates for rare earth elements hovering below 1% and dysprosium efficiencies in end-of-life magnets typically under 50% due to technical challenges in separation and low e-waste collection yields. Projections estimate that even optimistic expansions would cover only 25-40% of demand gaps by 2040, failing to offset primary deficits driven by in magnet applications. Overreliance on concentrated sources thus perpetuates systemic vulnerabilities, as evidenced by price volatility exceeding 300% in response to prior controls, underscoring the need for accelerated, geopolitically resilient alternatives. Dysprosium prices exhibited significant volatility in 2024 and 2025, with dysprosium oxide trading as low as $220–270 per kg in December 2024 before surging to $780 per kg by mid-2025 amid supply constraints and heightened . This +121% year-to-date increase in 2025 reflected strategic stockpiling and controls rather than purely , though prices stabilized around $275 per kg by 2025 in . Global dysprosium market demand reached approximately $1 billion in 2024, driven primarily by its role in high-performance neodymium-iron-boron magnets for electric vehicles (EVs) and wind turbines, which account for over 70% of consumption. Projections indicate the market could expand to $1.75 billion by 2035 at a 5.2% CAGR, though aggressive clean energy deployment may triple magnetic rare earth needs to 176 kilotons annually by then, intensifying pressure on dysprosium supplies. Efforts to diversify supply included Rare Earths' August 2025 capital raise of A$750 million ($490 million) to expand operations at Mt Weld in and integrate new processing in , aiming to boost non-Chinese heavy rare earth output as part of its 2025 growth plan. In the United States, Energy Fuels achieved a milestone in August 2025 by producing the first high-purity (99.9%) dysprosium oxide domestically at its facility, with plans for scaled heavy rare earth separation potentially starting in 2027 pending investment decisions. Geopolitical tensions exacerbated supply risks, as —controlling over 90% of global dysprosium processing—imposed export controls in April 2025 on seven rare earth elements including dysprosium, followed by expanded licensing requirements in October 2025 effective November 8, targeting embedded products and equipment. These measures, linked to U.S. tariffs, have tightened chains and prompted Western diversification, though short-term disruptions persist. Supply-demand models highlight vulnerabilities in green transitions, with dysprosium reserves potentially depleting globally by 2045 under 1.5°C scenarios requiring massive and scaling, potentially creating shortfalls equivalent to 77 million or 3,040 of capacity. Such constraints challenge assumptions of seamless and deployment, as dysprosium's scarcity in high-temperature magnets cannot be easily substituted without performance losses, per analyses from the and others. and gains could mitigate up to 35% of by 2050, but primary supply gaps remain a feasibility barrier absent accelerated non-Chinese .

Safety and Environmental Impact

Health and handling precautions

Dysprosium and its compounds demonstrate low acute oral toxicity, with reported LD50 values exceeding 2,000 mg/kg in rats for dysprosium nitrate and greater than 5,000 mg/kg for dysprosium oxide. Soluble dysprosium salts are mildly toxic upon ingestion, while insoluble forms show negligible effects. Dysprosium has no known essential biological role in humans or other organisms. Inhalation of dysprosium fines or dust poses the primary health risk during handling, with potential for respiratory irritation and, upon chronic exposure, rare earth characterized by similar to effects observed with other rare earth elements. No specific permissible exposure limits (PELs) have been established by OSHA or NIOSH for dysprosium, necessitating reliance on general industrial hygiene practices. Handling precautions include such as local exhaust to minimize airborne dust, along with comprising NIOSH/MSHA-approved respirators for potential exposure exceedances, chemical-resistant gloves, protective clothing, and safety goggles to prevent skin or eye contact. For radioactive isotopes like dysprosium-166, used in medical or nuclear applications, additional handling must adhere to regulations from bodies such as the , incorporating shielding, dosimetry monitoring, and licensed personnel requirements.

Ecological and mining impacts

Dysprosium extraction, primarily as a byproduct of (REE) mining from and bastnasite ores, generates substantial laden with radioactive and decay products, posing long-term ecological risks through and sediment contamination. Processing these ores often results in , where from sulfide oxidation mobilizes and REEs into waterways, altering levels and impairing aquatic ecosystems. In -rich deposits, radioactivity exceeds background levels, with concentrations in waste ponds reaching thousands of becquerels per kilogram, necessitating isolation to prevent emanation and penetration. At China's Bayan Obo mine, the world's largest REE operation supplying much of global dysprosium, open-pit activities have caused widespread and chemical leaching into the basin, with documented and spikes in local sediments as of 2025. Lax regulatory enforcement has permitted untreated discharge, elevating REE concentrations in surrounding farmland soils by factors of 10-50 times natural baselines, compared to stricter containment standards in Western operations like those in . This disparity underscores causal pathways from unenforced to persistent hotspots, where alkaline neutralize acids but mobilize REEs via runoff during monsoons. REEs from mining effluents bioaccumulate in microbiota and , facilitating trophic transfer through agricultural , with dysprosium and other heavy REEs detected at elevated levels in root vegetables near extraction sites. Empirical sampling reveals mean REE contents in mine-adjacent crops 5-20 times higher than reference areas, driven by adsorption to clay particles and pH-dependent uptake, potentially amplifying concentrations up the despite observed biodilution in higher trophic levels. Such pathways highlight the indirect ecological costs of REE embedded in supply chains for low-carbon technologies, where unmitigated runoff undermines in contaminated watersheds. Efforts to mitigate impacts include REE recovery from tailings and recycling dysprosium from end-of-life magnets, which could offset up to 40% of primary demand by 2050 under optimized scenarios, reducing associated waste volumes. However, recycling scalability remains constrained by low collection efficiencies—currently below 1% globally for NdFeB sources—and energy-intensive separation processes that limit net environmental gains without widespread infrastructure. These limitations perpetuate reliance on high-impact mining, particularly in regions with weaker oversight, amplifying the causal footprint of dysprosium supply for "green" applications.