Metal borides (transition-metal diborides and boride layers) TM borides
MB2 for ZrB2, HfB2, NbB2 and TaB2 (AlB2-type hexagonal) · CAS 12045-64-6 (ZrB2); 12007-23-7 (HfB2); 12007-35-1 (TaB2); 12007-09-9 (WB, as listed on PubChem); 12006-84-7 (FeB) · hexagonal, P6/mmm (ZrB2 and TaB2, AlB2 prototype)
This family profile covers the transition-metal borides that are not yet profiled on their own: zirconium diboride (ZrB2), hafnium diboride (HfB2), niobium diboride (NbB2), tantalum diboride (TaB2), tungsten boride (WB), cobalt borides (Co2B and CoB) and the iron borides (FeB and Fe2B) that form on steel during boriding.
Evidence level
2 of 5
Lab-measured
- 0Predicted only. No one has made it, or no measurement exists.
- 1Calculated. Only calculated or predicted values from sources.
- 2Lab-measured. Measured properties with their conditions stated.
- 3Space-relevant tests. Measured in conditions relevant to space, such as vacuum or atomic oxygen.
- 4Ground-qualified. Qualified for an application on the ground.
- 5Flown or field-proven. Flight or field results exist.
Density
6.119 g/cm3
Heat resistance
3245 degC
Hardness
23 GPa
Stiffness
539 GPa
Recipe, share of the weight
- B not statedBoron
- Zr not statedZirconium
- Ta not statedTantalum
Best for
Hard, high-melting diboride parts and coatings where ZrB2 or TaB2 is needed, and boride layers that give steel a hard, wear-resistant surface (Fe2B)
Weakest at
Brittleness and few measured bulk values for most borides (only ZrB2, TaB2 and NbB2 have sourced bulk values here, and FeB fractures easily under load)
Risk at a glance
- People None found. Irritant or harmful; GHS data are partial
- If it fails Moderate. Brittle fracture of dense NbB2 ceramic
- Corrosion No data. No corrosion data recorded
Quick facts: TM borides
| Property | Value | Basis |
|---|---|---|
| Density | 5.56 to 12.6 g/cm³ | 4 sourced values across conditions |
| Young's modulus | 248 to 489 GPa | 2 sourced values across conditions |
| Thermal conductivity | 16 to 60 W/(m·K) | 2 sourced values across conditions |
| Thermal expansion (CTE) | 5.9 to 8.2 ppm/K | 2 sourced values across conditions |
| Melting point | 3,037 to 3,245 °C | 2 sourced values across conditions |
What is the density of Metal borides (TM borides)?
Metal borides (TM borides) has a density of 5.56 to 12.6 g/cm³. The range covers 4 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is the thermal conductivity of Metal borides (TM borides)?
Metal borides (TM borides) has a thermal conductivity of 16 to 60 W/(m·K). The range covers 2 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is the coefficient of thermal expansion of Metal borides (TM borides)?
Metal borides (TM borides) has a coefficient of thermal expansion of 5.9 to 8.2 ppm/K. The range covers 2 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is the melting point of Metal borides (TM borides)?
Metal borides (TM borides) has a melting point of 3,037 to 3,245 °C. The range covers 2 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is the Young's modulus of Metal borides (TM borides)?
Metal borides (TM borides) has a Young's modulus of 248 to 489 GPa. The range covers 2 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is Metal borides (TM borides) used for?
Uses recorded in the sources include Thermal protection system material for sharp leading edges; Solar thermal absorber for concentrating solar power; Boride layer on low-carbon steel for hard, wear-resistant surfaces.
Why it exists
Transition-metal borides are hard, high-melting ceramics or layers. Dense ZrB2 has a melting temperature of 3245 degC and a hardness of 23 GPa (Sani 2016), and dense NbB2 has a hardness of 20.25 GPa and an elastic modulus of 539 GPa (Sairam 2014). Steel boriding gives a surface boride layer of about 16 GPa microhardness. The sourced uses are heat shields for launch vehicles (NASA), solar absorbers (Sani) and wear layers on steel (Kartal).
Where it's used
Heat-shield material for sharp leading edges
NASA Ames lists hot-pressed ZrB2 with 20 vol percent SiC for thermal protection, such as sharp leading edges on next-generation reusable launch vehicles.
Solar thermal absorbers
Sani et al. studied dense ZrB2 and TaB2 for the first time as solar absorbers that work at very high temperature.
Wear-resistant boride layers on steel
A single-phase Fe2B layer of 75 micrometres, grown by electrochemical boriding at 950 degC, has a microhardness of about 16 GPa (Kartal 2011).
Recipe
MB2 for ZrB2, HfB2, NbB2 and TaB2 (AlB2-type hexagonal); WB; Co2B and CoB; FeB and Fe2B (boride layers on steel)
These are hexagonal metal borides. ZrB2 and TaB2 take the AlB2-type structure (space group P6/mmm, Sani 2016 Table 1). Sani et al. made dense ZrB2 and TaB2 by reactive spark plasma sintering from metal and amorphous boron, or by spark plasma sintering of powders first made by self-propagating high-temperature synthesis. Sairam et al. made dense NbB2 (97.7 percent) from elemental niobium and boron, synthesised at 1200 degC and then densified at 1700 to 1900 degC by reaction spark plasma sintering. The iron borides form as layers on steel during electrochemical boriding in a borax electrolyte at 950 degC (Kartal 2011).
| Ingredient | Share of the weight | What it does |
|---|---|---|
| Boron B | not stated | Forms the boron layers in the hexagonal structure. In Sani et al., amorphous boron of at least 95 percent purity was used as one reactant. |
| Zirconium Zr | not stated | Metal in ZrB2, the most-studied diboride in this family; Sani et al. used Zr powder below 44 micrometres. |
| Tantalum Ta | not stated | Metal in TaB2, which is denser than ZrB2 (12.568 g/cm3 against 6.119 g/cm3). |
Weight shares are as printed in the sources.
What it can do
Density
6.119 g/cm3
measured
Dense ZrB2 has a density of 6.119 g/cm3, and TaB2 is much denser at 12.568 g/cm3 (Sani 2016).
Heat resistance
3245 degC
measured
The melting temperature is 3245 degC for ZrB2 and 3037 degC for TaB2 (Sani 2016).
Hardness
23 GPa
measured
ZrB2 has a hardness of 23 GPa and TaB2 19.6 GPa (Sani 2016). NbB2 is 20.25 GPa at 97.7 percent density (Sairam 2014).
Stiffness
539 GPa
measured
NbB2 has an elastic modulus of 539 GPa (Sairam 2014). ZrB2 is 489 GPa and TaB2 248.2 GPa (Sani 2016).
How it compares
Within this family, ZrB2 is the lightest and hardest of the diborides with sourced bulk values: 6.119 g/cm3, 23 GPa and a melting temperature of 3245 degC. TaB2 is about twice as dense and has a lower melting point (3037 degC), hardness (19.6 GPa) and modulus (248.2 GPa). NbB2 has a hardness of 20.25 GPa and a modulus of 539 GPa at 97.7 percent density, so its stiffness is the highest of the sourced diborides. Hafnium diboride, tungsten boride and the cobalt and iron borides lack sourced bulk values here.
The same measurements for each material, so you can compare them. Each row names the key condition under the value; the full conditions and methods are in the numbered notes under Technical details. Other materials are shown beside it; each was measured under its own conditions, so open its page before comparing closely. Compare every grade in the family.
| Measurement | TM borides | CrB2 | LaB6 | MoSi2 | TiB2 | MSi2 |
|---|---|---|---|---|---|---|
| Capacity and energy | ||||||
| Heat capacity at 25 degC, ZrB2 | 48.2 J/(mol·K)7 | no data | no data | no data | no data | no data |
| Heat capacity at 25 degC, TaB2 | 33.92 J/(mol·K)16 | no data | no data | no data | no data | no data |
| Thermal behavior and safety | ||||||
| Melting temperature, zirconium diboride (ZrB2) | 3245 °C2 | 1850 °C | 2528 K | no data | 3225 °C | 2160 °C |
| Thermal conductivity, ZrB2 | 60 W/(m·K)4 | no data | 47 W/mK | 30 W/m·K | 96 W/m·K | no data |
| Melting temperature, tantalum diboride (TaB2) | 3037 °C11 | 1850 °C | 2528 K | no data | 3225 °C | 2160 °C |
| Thermal conductivity, TaB2 | 16 W/(m·K)13 | no data | 47 W/mK | 30 W/m·K | 96 W/m·K | no data |
| Physical and electrical | ||||||
| Density, zirconium diboride (ZrB2) | 6.119 g/cm³1 | 5.15 g/cc | 4.72 g/cm³ | 5.6 g/cm³ | 4.5 g/cm³ | 9.3 g/cm³ |
| Hardness, ZrB2Hardness row of Table 1 in Sani et al. 2016 | 23 GPa | 9.72 GPa | 20 GPa | 9 GPa | 25 GPa | no data |
| Density, tantalum diboride (TaB2) | 12.57 g/cm³10 | 5.15 g/cc | 4.72 g/cm³ | 5.6 g/cm³ | 4.5 g/cm³ | 9.3 g/cm³ |
| Hardness, TaB2Hardness row of Table 1 in Sani et al. 2016 | 19.6 GPa | 9.72 GPa | 20 GPa | 9 GPa | 25 GPa | no data |
| Density, ZrB2 with 20 volume percent SiC (composite, not pure ZrB2) | 5.56 g/cm³19 | 5.15 g/cc | 4.72 g/cm³ | 5.6 g/cm³ | 4.5 g/cm³ | 9.3 g/cm³ |
| Hardness, NbB2 (reaction SPS, 97.7 percent dense) | 20.25 GPa20 | 9.72 GPa | 20 GPa | 9 GPa | 25 GPa | no data |
| Relative density, NbB2 after reaction SPS at 1900 degC | 97.7 %22 | no data | 85.1 % | no data | no data | no data |
| Density, Co2B nanocrystals (specific density, measured) | 7.61 to 7.78 g/cm³23 | 5.15 g/cc | 4.72 g/cm³ | 5.6 g/cm³ | 4.5 g/cm³ | 9.3 g/cm³ |
| Hardness, Fe2B single-phase layer on low-carbon steel (electrochemical boriding)Microhardness value stated in the abstract | 16 GPa | 9.72 GPa | 20 GPa | 9 GPa | 25 GPa | no data |
| Boride layer thickness, single-phase Fe2B after phase homogenisation | 75 µm25 | no data | no data | no data | no data | no data |
| Hardness, WB3 (predicted structure, DFT, not WB) | 38.3 GPa26 | 9.72 GPa | 20 GPa | 9 GPa | 25 GPa | no data |
| Other measurements | ||||||
| Coefficient of thermal expansion, ZrB2 | 5.9 10-6/K3 | 11.1 10-6/K | 6.2 10-6/K | 7 to 8 10-6/K | 7.4 10-6/K | no data |
| Young's modulus, ZrB2 | 489 GPa5 | no data | no data | 59 psi x 10^6 | 565 GPa | no data |
| Enthalpy of formation at 25 degC, ZrB2 | -322.6 kJ/mol6 | no data | no data | no data | no data | no data |
| Lattice parameter a, ZrB2 | 3.17 Å8 | no data | no data | no data | no data | no data |
| Lattice parameter c, ZrB2 | 3.53 Å9 | no data | no data | no data | no data | no data |
| Coefficient of thermal expansion, TaB2 | 8.2 10-6/K12 | 11.1 10-6/K | 6.2 10-6/K | 7 to 8 10-6/K | 7.4 10-6/K | no data |
| Young's modulus, TaB2 | 248.2 GPa14 | no data | no data | 59 psi x 10^6 | 565 GPa | no data |
| Enthalpy of formation at 25 degC, TaB2 | -209.2 kJ/mol15 | no data | no data | no data | no data | no data |
| Lattice parameter a, TaB2 | 3.088 Å17 | no data | no data | no data | no data | no data |
| Lattice parameter c, TaB2 | 3.241 Å18 | no data | no data | no data | no data | no data |
| Elastic modulus, NbB2 (reaction SPS, 97.7 percent dense)Elastic modulus stated in the abstract | 539 GPa | no data | no data | 59 psi x 10^6 | 565 GPa | no data |
| Indentation fracture toughness, NbB2 (reaction SPS) | 4 MPa·m1/221 | no data | 3.02 MPa m1/2 | 3 to 4 MPa·m1/2 | 6.2 MPa·m1/2 | no data |
| Saturation magnetization, Co2B nanocrystals | 35 to 50 emu/g24 | no data | no data | no data | no data | no data |
Why choose it, and why not
Good for
- Hard, stiff parts made from ZrB2 or NbB2. The sourced values are 23 GPa for ZrB2 and 20.25 GPa and 539 GPa for NbB2.
- Hard wear layers on steel from boriding, with a single-phase Fe2B layer of about 16 GPa microhardness.
Watch out for
- Brittleness: NbB2 has an indentation fracture toughness of 4 MPa·m1/2 (Sairam 2014). FeB fractures easily under high load (Kartal 2011).
- Thin data: hafnium diboride and tungsten boride have no sourced density or hardness here, and Co and Fe boride bulk values are missing.
- Mixed basis: the ZrB2 density 6.119 g/cm3 is for pure ZrB2, while the NASA ZrB2 density of 5.56 g/cm3 is for a SiC composite.
The sourced family is a set of hard, high-melting ceramics and steel boride layers. ZrB2 and NbB2 have the best bulk values here, TaB2 is much denser, and the cobalt, iron, hafnium and tungsten borides still need measured data before they can be compared properly.
Technical details
For scientists and researchers. Everything above comes from the record below: every number with its method, its conditions and its source.
Notes
The method, full conditions and any caveat for the numbered rows above.
| # | Measurement | Method | Conditions | Caveat |
|---|---|---|---|---|
| 1 | Density, zirconium diboride (ZrB2) | Density (g/cm3) row of Table 1 in Sani et al. 2016 | basis Table 1 literature value for ZrB2 (cited to ref. 6 in the paper); not the paper's own samplesprocess Sani et al. section 2 used Zr powder below 44 micrometres (98.5 percent purity) and amorphous boron of at least 95 percent purity | — |
| 2 | Melting temperature, zirconium diboride (ZrB2) | Melting Temperature row of Table 1 in Sani et al. 2016 | basis Table 1 literature value (ref. 6 in the paper) | — |
| 3 | Coefficient of thermal expansion, ZrB2 | Coefficient of Thermal Expansion row of Table 1 (printed as 5.9 x 10-6 K-1) | basis Table 1 literature value; temperature not stated in the table | — |
| 4 | Thermal conductivity, ZrB2 | Thermal conductivity row of Table 1 in Sani et al. 2016 | basis Table 1 literature value; temperature not stated in the table | — |
| 5 | Young's modulus, ZrB2 | Young's Modulus row of Table 1 in Sani et al. 2016 | basis Table 1 literature value; temperature not stated in the table | — |
| 6 | Enthalpy of formation at 25 degC, ZrB2 | Enthalpy of Formation row of Table 1 in Sani et al. 2016 (custom property name, not in the canon file) | temperature 25 °C | — |
| 7 | Heat capacity at 25 degC, ZrB2 | Heat Capacity row of Table 1 in Sani et al. 2016 (molar basis as printed; custom property name) | temperature 25 °C | — |
| 8 | Lattice parameter a, ZrB2 | a (Å) row of Table 1 in Sani et al. 2016 (custom property name) | basis hexagonal P6/mmm cell, as printed in Table 1 | — |
| 9 | Lattice parameter c, ZrB2 | c (Å) row of Table 1 in Sani et al. 2016 (custom property name) | basis hexagonal P6/mmm cell, as printed in Table 1 | — |
| 10 | Density, tantalum diboride (TaB2) | Density (g/cm3) row of Table 1 in Sani et al. 2016 | basis Table 1 literature value for TaB2 (cited to ref. 6 in the paper); not the paper's own samples | — |
| 11 | Melting temperature, tantalum diboride (TaB2) | Melting Temperature row of Table 1 in Sani et al. 2016 | basis Table 1 literature value (ref. 6 in the paper) | — |
| 12 | Coefficient of thermal expansion, TaB2 | Coefficient of Thermal Expansion row of Table 1 (printed as 8.2 x 10-6 K-1) | basis Table 1 literature value; temperature not stated in the table | — |
| 13 | Thermal conductivity, TaB2 | Thermal conductivity row of Table 1 in Sani et al. 2016 | basis Table 1 literature value; temperature not stated in the table | — |
| 14 | Young's modulus, TaB2 | Young's Modulus row of Table 1 in Sani et al. 2016 | basis Table 1 literature value; temperature not stated in the table | — |
| 15 | Enthalpy of formation at 25 degC, TaB2 | Enthalpy of Formation row of Table 1 in Sani et al. 2016 (printed as -209.200; custom property name) | temperature 25 °C | — |
| 16 | Heat capacity at 25 degC, TaB2 | Heat Capacity row of Table 1 in Sani et al. 2016 (molar basis as printed; custom property name) | temperature 25 °C | — |
| 17 | Lattice parameter a, TaB2 | a (Å) row of Table 1 in Sani et al. 2016 (custom property name) | basis hexagonal P6/mmm cell, as printed in Table 1 (3.0880) | — |
| 18 | Lattice parameter c, TaB2 | c (Å) row of Table 1 in Sani et al. 2016 (custom property name) | basis hexagonal P6/mmm cell, as printed in Table 1 (3.2410) | — |
| 19 | Density, ZrB2 with 20 volume percent SiC (composite, not pure ZrB2) | Density row of the Properties at Standard Conditions table; converted from kg/m3 to g/cm3 here. The composite is not pure ZrB2, so it is not compared with the 6.119 value. | basis hot-pressed ZrB2 plus 20 vol percent SiC particulate, above 98 percent of theoretical density (NASA TPSX description)unit in source kg/m3, SI column of the NASA table (5.56 x 10^3 kg/m3) | — |
| 20 | Hardness, NbB2 (reaction SPS, 97.7 percent dense) | Hardness value stated in the abstract (test method and load not stated in the abstract) | temperature room temperature (not stated)basis dense NbB2 at 97.7 percent of theoretical density, reaction spark plasma sintering at 1900 °C for 15 min | — |
| 21 | Indentation fracture toughness, NbB2 (reaction SPS) | Indentation fracture toughness stated in the abstract (custom property name) | basis dense NbB2 at 97.7 percent of theoretical density; indentation method | — |
| 22 | Relative density, NbB2 after reaction SPS at 1900 degC | Abstract, reaction spark plasma sintering from elemental Nb and B (two-stage heat treatment, 1200 degC synthesis, 1700 to 1900 degC densification) | temperature 1900 °Ctime 15 min holding periodbasis percent of theoretical density (the abstract prints it as about 97.7 percent of rho-th) | — |
| 23 | Density, Co2B nanocrystals (specific density, measured) | Specific density range printed in the abstract of the 2016 Bulletin of Materials Science paper | basis Co2B nanocrystals from mechanochemical synthesis, not bulk Co2B | — |
| 24 | Saturation magnetization, Co2B nanocrystals | Saturation magnetization range printed in the abstract (custom property name) | basis Co2B nanocrystals from mechanochemical synthesis | — |
| 25 | Boride layer thickness, single-phase Fe2B after phase homogenisation | Thickness stated in the abstract (custom property name) | basis electrochemical boriding at 950 °C, 15 min, then 45 min at rest without polarisation | — |
| 26 | Hardness, WB3 (predicted structure, DFT, not WB) | Vickers hardness stated in the abstract as a property of the predicted structure (calculated, not measured) | basis hP24-WB3 structure predicted by density functional theory; a different phase from WB | Predicted for WB3, not for tungsten boride (WB). Shown only as the one tungsten boride hardness read in this run. |
Corrosion and compatibility
What happens when it meets other materials and environments.
| Environment | Concern | What happens |
|---|---|---|
| Oxidising air at high temperature (ZrB2 with 20 volume percent SiC, hot pressed) | not rated | NASA TPSX says SiC improves the oxidation resistance of the composite compared with pure ZrB2. No numbers are given.1 |
| # | Environment | Details | Test conditions |
|---|---|---|---|
| 1 | Oxidising air at high temperature (ZrB2 with 20 volume percent SiC, hot pressed) | The NASA Ames TPS database says studies indicate that the SiC particulate improves the oxidation resistance of ZrB2 compared with pure ZrB2. The page gives no oxidation rate, scale thickness or temperature limit, so the rating is left as unknown. | form hot-pressed composite, ZrB2 plus 20 vol percent SiCbasis qualitative statement in the Description |
Risks and side effects
Hazards to people, what happens when a cell overheats, and how the material is handled and stored.
For people
PubChem aggregated notifications give harmful-category codes (H302, H312, H332) for ZrB2 and irritation codes (H315, H319, H335) for HfB2 and TaB2. Most reports agree, but a small share say the material is not classified. No supplier SDS was read for these borides.
- Dust
- Control dust when handling powders of any boride. PubChem lists irritation of skin, eyes and the respiratory tract for HfB2 and TaB2.
- Ingestion and skin
- PubChem lists H302, H312 and H332 (harmful if swallowed, in contact with skin or inhaled) for ZrB2 in 85.2 percent of its 54 reports.
If a part fails
These are the numbers read for dense material at room temperature.
- Brittleness
- Dense NbB2 has an indentation fracture toughness of 4 MPa·m1/2, so a flaw can start a crack well below the hardness limit.
- Boride layer
- The FeB layer is much harder than Fe2B but fractures or delaminates easily under high load (Kartal 2011).
Test details
The original wording and numbers from the sources, for readers who want them.
Failure risks
| Failure | Trigger and consequence |
|---|---|
| Brittle fracture of dense NbB2 ceramicmoderate severity | Tensile or bending load on a flawIndentation fracture toughness of 4 MPa·m1/2 for dense NbB2 (reaction SPS, 97.7 percent dense), so a flaw can grow at a stress well below the hardness limit |
| Delamination or fracture of FeB-rich boride layermoderate severity | High normal or tangential load on the boride layer on steelFeB is much harder than Fe2B but has very poor fracture toughness, so it can fracture or delaminate easily under high normal or tangential loading (Kartal et al.) |
Handling and storage
- Powder of HfB2 and TaB2: PubChem lists H315, H319 and H335, so avoid skin and eye contact and do not breathe the dust.
- Zirconium and tantalum borides are hard to consolidate by pressure-assisted sintering, so spark plasma sintering or reactive sintering is used (Sani et al. 2016, introduction).
Supply and geography
How common the raw materials are and where they come from.
Boron (common to all the diborides and the boride layers)
USGS: borates occur in volcanic and arid deposits. The 2025 world total is withheld (XX). 2025 production by country, in thousand metric tons and as printed: Turkey 1,500 (refined borates), Bolivia 380 (ulexite), Chile 300 (ulexite), China 230 (boric oxide equivalent), Peru 220 (crude borates), Argentina 170 (crude ore), Russia 80 (datolite ore), Germany 40 (compounds).
- Critical mineral lists
- US: listed, EU: listed
- Recycling
- USGS: insignificant.
- Substitutes
- USGS: substitution is possible in detergents, enamels, insulation and soaps. No substitute for boron in a boride is discussed.
Iron (the metal in FeB and Fe2B)
USGS: the only source of primary iron is iron ore. World usable ore production was 2,600,000 thousand metric tons in 2024 and an estimated 2,600,000 in 2025, with an iron content of 1,600,000 thousand metric tons in both years. 2025 usable ore by country, in thousand metric tons: Australia 980,000, Brazil 420,000, India 310,000, China 290,000.
- Critical mineral lists
- EU: not listed
- Recycling
- USGS: none for iron ore; see the iron and steel scrap chapter (not read).
- Substitutes
- USGS: the only source of primary iron is iron ore, used directly as direct-shipping ore or converted to pig iron.
Zirconium (the metal in ZrB2)
USGS: world mine production of zirconium mineral concentrates was about 1,200 thousand metric tons gross weight in 2025 (1,300 in 2024). 2025 by country, in thousand metric tons: Australia 400, South Africa 270, Mozambique 160, Senegal 70, China 100, Indonesia 52, Madagascar 26, Sierra Leone 25. Zirconium reserves are more than 70,000 thousand metric tons ZrO2 content.
- Critical mineral lists
- EU: not listed
- Recycling
- USGS: companies in Oregon and Utah recycled zirconium from new scrap and from post-commercial old scrap; foundry mould cores and spent zirconia refractories are often recycled but cannot be quantified.
- Substitutes
- USGS: chromite and olivine can substitute for zircon in some foundry applications, and niobium, stainless steel and tantalum in some nuclear applications.
Hafnium (the metal in HfB2)
USGS: world primary hafnium production data and quantitative hafnium reserve estimates were not available. Germany supplied 54 percent of unwrought hafnium imports in 2021 to 2024 (USGS import sources); the leading global exporters of unwrought hafnium were China and Germany.
- Critical mineral lists
- EU: listed
- Recycling
- USGS: hafnium metal recycling was minimal.
Niobium (the metal in NbB2)
USGS: world mine production of niobium was 112,000 t in 2024 and 2025 (rounded total). Brazil produced 104,000 t in 2024 and 2025e, and Canada 6,900 t in 2024 and 6,000 t in 2025e. U.S. net import reliance was 100 percent.
- Top producers (2025)
- Brazil 93%, Canada 5%
- Critical mineral lists
- EU: listed
- Recycling
- USGS: niobium was recycled with niobium-bearing steels and superalloys, but scrap recovery specifically for niobium content was negligible.
- Substitutes
- USGS: ceramic matrix composites, molybdenum, tantalum and tungsten in superalloys, and molybdenum, tantalum and titanium as alloying elements in steels, can substitute with a performance loss or higher cost.
Tantalum (the metal in TaB2)
USGS: tantalum has not been mined in the United States since 1959, and U.S. net import reliance was 100 percent. World mine production was 2,500 t in 2024 and 2025e (rounded). Congo (Kinshasa) produced 1,270 t in 2024 and 1,300 t in 2025e, Rwanda 374 t and 400 t, Nigeria 390 t in both years.
- Critical mineral lists
- EU: listed
- Recycling
- USGS: tantalum was recycled mostly from new scrap of tantalum electronic components and from cemented carbide and superalloy scrap; recycling may account for as much as 30 percent of consumption by domestic primary processors.
- Substitutes
- USGS: niobium and tungsten in carbides; aluminium, ceramics and niobium in capacitors; hafnium, iridium, molybdenum, niobium, rhenium and tungsten in high-temperature applications.
Tungsten (the metal in WB)
USGS: tungsten has not been mined commercially in the United States since 2015. World mine production was 82,000 t in 2024 and 85,000 t in 2025 (rounded). China produced 67,000 t in both years. U.S. net import reliance was more than 50 percent.
- Critical mineral lists
- EU: listed
- Recycling
- USGS: the quantity of secondary tungsten and the amount consumed from secondary sources were withheld to protect company data.
- Substitutes
- USGS: molybdenum carbide, niobium carbide or titanium carbide cemented carbides, ceramics, cermets and tool steels can substitute for cemented tungsten carbide, but most of these reduce rather than replace the tungsten used.
Cobalt (the metal in Co2B and CoB)
USGS: Congo (Kinshasa) was the world's leading source of mined cobalt, with an estimated 73 percent of the 2025 world total, followed by Indonesia with 14 percent. World mine production was 302,000 t in 2024 and 310,000 t in 2025 (rounded). U.S. net import reliance was 79 percent in 2025e.
- Top producers (2025)
- Congo (Kinshasa) 73%, Indonesia 14%
- Critical mineral lists
- EU: listed
- Recycling
- USGS: cobalt content of purchased scrap represented 25 percent of estimated U.S. cobalt consumption in 2025.
- Substitutes
- USGS: barium or strontium ferrites, neodymium-iron-boron alloys, nickel-iron alloys in magnets; iron, nickel, cermets or ceramics in cutting and wear-resistant materials.
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spore: profile
id: metal-borides
spore_version: 0.2
family: carbide-nitride-boride-ceramics
name: Metal borides (transition-metal diborides and boride layers)
abbreviation: TM borides
role: 'family of hard transition-metal borides: ZrB2, HfB2, NbB2, TaB2, WB, Co2B/CoB and the FeB/Fe2B boride layers on steel'
category: ceramics
type: ultra-high-temperature-ceramics
summary: |
This family profile covers the transition-metal borides that are not yet profiled on their own: zirconium diboride (ZrB2), hafnium diboride (HfB2), niobium diboride (NbB2), tantalum diboride (TaB2), tungsten boride (WB), cobalt borides (Co2B and CoB) and the iron borides (FeB and Fe2B) that form on steel during boriding. Sani et al. (2016) give the best sourced set: dense ZrB2 has a density of 6.119 g/cm3, a melting temperature of 3245 degC, a Young's modulus of 489 GPa and a hardness of 23 GPa, while dense TaB2 is much denser (12.568 g/cm3), melts at 3037 degC and is softer (hardness 19.6 GPa, modulus 248.2 GPa). Birmingham's reaction spark plasma sintering study gives NbB2 a hardness of 20.25 GPa, an elastic modulus of 539 GPa and a fracture toughness of 4 MPa m1/2 at 97.7 percent of theoretical density. For the iron borides, a 2011 electrochemical boriding study grew a single-phase Fe2B layer of 75 micrometres with a microhardness of about 16 GPa, and reports that FeB is harder but fractures more easily. Hafnium diboride and tungsten boride have no measured density, hardness or modulus in a source read for this profile, and the cobalt borides have only a nanocrystal density (7.61 to 7.78 g/cm3, Co2B).
best_for: Hard, high-melting diboride parts and coatings where ZrB2 or TaB2 is needed, and boride layers that give steel a hard, wear-resistant surface (Fe2B)
weakest_at: Brittleness and few measured bulk values for most borides (only ZrB2, TaB2 and NbB2 have sourced bulk values here, and FeB fractures easily under load)
identity:
formula: MB2 for ZrB2, HfB2, NbB2 and TaB2 (AlB2-type hexagonal); WB; Co2B and CoB; FeB and Fe2B (boride layers on steel)
cas: 12045-64-6 (ZrB2); 12007-23-7 (HfB2); 12007-35-1 (TaB2); 12007-09-9 (WB, as listed on PubChem); 12006-84-7 (FeB)
crystal_system: hexagonal (ZrB2, TaB2, AlB2-type)
space_group: P6/mmm (ZrB2 and TaB2, AlB2 prototype)
source: sani-2016
where: Table 1 of Sani et al. 2016 (crystal system, space group and AlB2 prototype rows); CAS numbers from the PubChem records listed under documents
tags:
environments: []
stresses:
- extreme-heat
applications:
- heat-shields
- thermal-control
- mechanisms
properties:
- benchmark: density
label: Density, zirconium diboride (ZrB2)
value: 6.119
unit: g/cm3
scope: material
conditions:
basis: Table 1 literature value for ZrB2 (cited to ref. 6 in the paper); not the paper's own samples
process: Sani et al. section 2 used Zr powder below 44 micrometres (98.5 percent purity) and amorphous boron of at least 95 percent purity
method: Density (g/cm3) row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Density row, ZrB2 column
- benchmark: melting_point
label: Melting temperature, zirconium diboride (ZrB2)
value: 3245
unit: degC
scope: material
conditions:
basis: Table 1 literature value (ref. 6 in the paper)
method: Melting Temperature row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Melting Temperature row, ZrB2 column
- benchmark: cte
label: Coefficient of thermal expansion, ZrB2
value: 5.9
unit: 10-6/K
scope: material
conditions:
basis: Table 1 literature value; temperature not stated in the table
method: Coefficient of Thermal Expansion row of Table 1 (printed as 5.9 x 10-6 K-1)
status: ground
source: sani-2016
where: Table 1, Coefficient of Thermal Expansion row, ZrB2 column
- benchmark: thermal_conductivity
label: Thermal conductivity, ZrB2
value: 60
unit: W/(m·K)
scope: material
conditions:
basis: Table 1 literature value; temperature not stated in the table
method: Thermal conductivity row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Thermal conductivity row, ZrB2 column
- benchmark: elastic_modulus
label: Young's modulus, ZrB2
value: 489
unit: GPa
scope: material
conditions:
basis: Table 1 literature value; temperature not stated in the table
method: Young's Modulus row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Young's Modulus row, ZrB2 column
- benchmark: hardness
label: Hardness, ZrB2
value: 23
unit: GPa
scope: material
conditions:
basis: Table 1 literature value; test method and load not stated in the table
method: Hardness row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Hardness row, ZrB2 column
- benchmark: enthalpy_of_formation
label: Enthalpy of formation at 25 degC, ZrB2
value: -322.6
unit: kJ/mol
scope: material
conditions:
temperature: 25 degC
method: Enthalpy of Formation row of Table 1 in Sani et al. 2016 (custom property name, not in the canon file)
status: ground
source: sani-2016
where: Table 1, Enthalpy of Formation at 25 degC row, ZrB2 column
- benchmark: molar_heat_capacity
label: Heat capacity at 25 degC, ZrB2
value: 48.2
unit: J/(mol·K)
scope: material
conditions:
temperature: 25 degC
method: Heat Capacity row of Table 1 in Sani et al. 2016 (molar basis as printed; custom property name)
status: ground
source: sani-2016
where: Table 1, Heat Capacity at 25 degC row, ZrB2 column
- benchmark: lattice_parameter_a
label: Lattice parameter a, ZrB2
value: 3.17
unit: Å
scope: material
conditions:
basis: hexagonal P6/mmm cell, as printed in Table 1
method: a (Å) row of Table 1 in Sani et al. 2016 (custom property name)
status: ground
source: sani-2016
where: Table 1, a (Å) row, ZrB2 column
- benchmark: lattice_parameter_c
label: Lattice parameter c, ZrB2
value: 3.53
unit: Å
scope: material
conditions:
basis: hexagonal P6/mmm cell, as printed in Table 1
method: c (Å) row of Table 1 in Sani et al. 2016 (custom property name)
status: ground
source: sani-2016
where: Table 1, c (Å) row, ZrB2 column
- benchmark: density
label: Density, tantalum diboride (TaB2)
value: 12.568
unit: g/cm3
scope: material
conditions:
basis: Table 1 literature value for TaB2 (cited to ref. 6 in the paper); not the paper's own samples
method: Density (g/cm3) row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Density row, TaB2 column
- benchmark: melting_point
label: Melting temperature, tantalum diboride (TaB2)
value: 3037
unit: degC
scope: material
conditions:
basis: Table 1 literature value (ref. 6 in the paper)
method: Melting Temperature row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Melting Temperature row, TaB2 column
- benchmark: cte
label: Coefficient of thermal expansion, TaB2
value: 8.2
unit: 10-6/K
scope: material
conditions:
basis: Table 1 literature value; temperature not stated in the table
method: Coefficient of Thermal Expansion row of Table 1 (printed as 8.2 x 10-6 K-1)
status: ground
source: sani-2016
where: Table 1, Coefficient of Thermal Expansion row, TaB2 column
- benchmark: thermal_conductivity
label: Thermal conductivity, TaB2
value: 16
unit: W/(m·K)
scope: material
conditions:
basis: Table 1 literature value; temperature not stated in the table
method: Thermal conductivity row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Thermal conductivity row, TaB2 column
- benchmark: elastic_modulus
label: Young's modulus, TaB2
value: 248.2
unit: GPa
scope: material
conditions:
basis: Table 1 literature value; temperature not stated in the table
method: Young's Modulus row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Young's Modulus row, TaB2 column
- benchmark: hardness
label: Hardness, TaB2
value: 19.6
unit: GPa
scope: material
conditions:
basis: Table 1 literature value; test method and load not stated in the table
method: Hardness row of Table 1 in Sani et al. 2016
status: ground
source: sani-2016
where: Table 1, Hardness row, TaB2 column
- benchmark: enthalpy_of_formation
label: Enthalpy of formation at 25 degC, TaB2
value: -209.2
unit: kJ/mol
scope: material
conditions:
temperature: 25 degC
method: Enthalpy of Formation row of Table 1 in Sani et al. 2016 (printed as -209.200; custom property name)
status: ground
source: sani-2016
where: Table 1, Enthalpy of Formation at 25 degC row, TaB2 column
- benchmark: molar_heat_capacity
label: Heat capacity at 25 degC, TaB2
value: 33.92
unit: J/(mol·K)
scope: material
conditions:
temperature: 25 degC
method: Heat Capacity row of Table 1 in Sani et al. 2016 (molar basis as printed; custom property name)
status: ground
source: sani-2016
where: Table 1, Heat Capacity at 25 degC row, TaB2 column
- benchmark: lattice_parameter_a
label: Lattice parameter a, TaB2
value: 3.088
unit: Å
scope: material
conditions:
basis: hexagonal P6/mmm cell, as printed in Table 1 (3.0880)
method: a (Å) row of Table 1 in Sani et al. 2016 (custom property name)
status: ground
source: sani-2016
where: Table 1, a (Å) row, TaB2 column
- benchmark: lattice_parameter_c
label: Lattice parameter c, TaB2
value: 3.241
unit: Å
scope: material
conditions:
basis: hexagonal P6/mmm cell, as printed in Table 1 (3.2410)
method: c (Å) row of Table 1 in Sani et al. 2016 (custom property name)
status: ground
source: sani-2016
where: Table 1, c (Å) row, TaB2 column
- benchmark: density
label: Density, ZrB2 with 20 volume percent SiC (composite, not pure ZrB2)
value: 5.56
unit: g/cm3
scope: material
conditions:
basis: hot-pressed ZrB2 plus 20 vol percent SiC particulate, above 98 percent of theoretical density (NASA TPSX description)
unit_in_source: kg/m3, SI column of the NASA table (5.56 x 10^3 kg/m3)
method: Density row of the Properties at Standard Conditions table; converted from kg/m3 to g/cm3 here. The composite is not pure ZrB2, so it is not compared with the 6.119 value.
status: ground
source: nasa-tpsx-zrb2
where: Properties at Standard Conditions table, Density row (SI units); Description
- benchmark: hardness
label: Hardness, NbB2 (reaction SPS, 97.7 percent dense)
value: 20.25
unit: GPa
scope: material
conditions:
temperature: room temperature (not stated)
basis: dense NbB2 at 97.7 percent of theoretical density, reaction spark plasma sintering at 1900 degC for 15 min
method: Hardness value stated in the abstract (test method and load not stated in the abstract)
status: ground
source: sairam-nbb2-2014
where: Abstract, final sentence
- benchmark: elastic_modulus
label: Elastic modulus, NbB2 (reaction SPS, 97.7 percent dense)
value: 539
unit: GPa
scope: material
conditions:
basis: dense NbB2 at 97.7 percent of theoretical density, reaction spark plasma sintering at 1900 degC for 15 min
method: Elastic modulus stated in the abstract
status: ground
source: sairam-nbb2-2014
where: Abstract, final sentence
- benchmark: fracture_toughness
label: Indentation fracture toughness, NbB2 (reaction SPS)
value: 4
unit: MPa·m1/2
scope: material
conditions:
basis: dense NbB2 at 97.7 percent of theoretical density; indentation method
method: Indentation fracture toughness stated in the abstract (custom property name)
status: ground
source: sairam-nbb2-2014
where: Abstract, final sentence
- benchmark: relative_density
label: Relative density, NbB2 after reaction SPS at 1900 degC
value: 97.7
unit: '%'
scope: material
conditions:
temperature: 1900 degC
time: 15 min holding period
basis: percent of theoretical density (the abstract prints it as about 97.7 percent of rho-th)
method: Abstract, reaction spark plasma sintering from elemental Nb and B (two-stage heat treatment, 1200 degC synthesis, 1700 to 1900 degC densification)
status: ground
source: sairam-nbb2-2014
where: Abstract, second sentence
- benchmark: density
label: Density, Co2B nanocrystals (specific density, measured)
value: 7.61
value_high: 7.78
bound: range
unit: g/cm3
scope: material
conditions:
basis: Co2B nanocrystals from mechanochemical synthesis, not bulk Co2B
method: Specific density range printed in the abstract of the 2016 Bulletin of Materials Science paper
status: ground
source: co2b-2016
where: Abstract, sentence on specific density
- benchmark: saturation_magnetization
label: Saturation magnetization, Co2B nanocrystals
value: 35
value_high: 50
bound: range
unit: emu/g
scope: material
conditions:
basis: Co2B nanocrystals from mechanochemical synthesis
method: Saturation magnetization range printed in the abstract (custom property name)
status: ground
source: co2b-2016
where: Abstract, sentence on saturation magnetization
- benchmark: hardness
label: Hardness, Fe2B single-phase layer on low-carbon steel (electrochemical boriding)
value: 16
unit: GPa
scope: material
conditions:
basis: single-phase Fe2B layer of 75 micrometres after 15 min boriding in a borax electrolyte at 950 degC plus 45 min homogenisation at rest
test: microhardness, load not stated in the abstract
method: Microhardness value stated in the abstract
status: ground
source: kartal-2011
where: Abstract, final part (microhardness of about 16GPa)
- benchmark: layer_thickness
label: Boride layer thickness, single-phase Fe2B after phase homogenisation
value: 75
unit: micrometre
scope: material
conditions:
basis: electrochemical boriding at 950 degC, 15 min, then 45 min at rest without polarisation
method: Thickness stated in the abstract (custom property name)
status: ground
source: kartal-2011
where: Abstract, second half (thickness increased to 75 micrometres)
- benchmark: hardness
label: Hardness, WB3 (predicted structure, DFT, not WB)
value: 38.3
unit: GPa
scope: material
conditions:
basis: hP24-WB3 structure predicted by density functional theory; a different phase from WB
method: Vickers hardness stated in the abstract as a property of the predicted structure (calculated, not measured)
status: calculated
note: Predicted for WB3, not for tungsten boride (WB). Shown only as the one tungsten boride hardness read in this run.
source: wb3-2012
where: Abstract, first paragraph
corrosion:
- environment: Oxidising air at high temperature (ZrB2 with 20 volume percent SiC, hot pressed)
headline: NASA TPSX says SiC improves the oxidation resistance of the composite compared with pure ZrB2. No numbers are given.
effect: The NASA Ames TPS database says studies indicate that the SiC particulate improves the oxidation resistance of ZrB2 compared with pure ZrB2. The page gives no oxidation rate, scale thickness or temperature limit, so the rating is left as unknown.
rating: unknown
conditions:
form: hot-pressed composite, ZrB2 plus 20 vol percent SiC
basis: qualitative statement in the Description
source: nasa-tpsx-zrb2
where: Description paragraph of the Zirconium Diboride (ZrB2/SiC) entry
risks:
hazards:
- text: 'PubChem aggregated GHS for zirconium diboride (CID 9812765, signal word Warning): H302 harmful if swallowed, H312 harmful in contact with skin and H332 harmful if inhaled, each in 85.2 percent of the 54 company reports. 7.4 percent (4 of 54) of reports say it does not meet GHS hazard criteria.'
ghs:
- H302
- H312
- H332
source: pubchem-zrb2
where: Safety and Hazards, GHS Classification
- text: 'PubChem aggregated GHS for hafnium diboride (CID 6336857, signal word Warning): H315 causes skin irritation, H319 causes serious eye irritation and H335 may cause respiratory irritation, each in 98.6 percent of 212 reports. 1.4 percent (3 of 212) of reports say it does not meet GHS hazard criteria.'
ghs:
- H315
- H319
- H335
source: pubchem-hfb2
where: Safety and Hazards, GHS Classification
- text: 'PubChem aggregated GHS for tantalum diboride (CID 9815613, signal word Warning): H315, H319 and H335 in 99.5 percent of 210 reports. 0.5 percent (1 of 210) of reports say it does not meet GHS hazard criteria.'
ghs:
- H315
- H319
- H335
source: pubchem-tab2
where: Safety and Hazards, GHS Classification
- text: PubChem lists tungsten boride (CID 82793) as Not Classified, reported as not meeting GHS hazard criteria by 1 of 1 company. This is one notification, so it is weak evidence.
ghs: []
source: pubchem-wb
where: Safety and Hazards, GHS Classification
- text: PubChem lists iron boride (FeB, CID 82789) as not meeting GHS hazard criteria for 100 percent (5 of 5) of reports. No supplier safety data sheet for any boride in this family was read in this run.
ghs: []
source: pubchem-feb
where: Safety and Hazards, GHS Classification
failure_risks:
- mode: Brittle fracture of dense NbB2 ceramic
trigger: Tensile or bending load on a flaw
consequence: Indentation fracture toughness of 4 MPa·m1/2 for dense NbB2 (reaction SPS, 97.7 percent dense), so a flaw can grow at a stress well below the hardness limit
severity: moderate
source: sairam-nbb2-2014
where: Abstract, final sentence
- mode: Delamination or fracture of FeB-rich boride layer
trigger: High normal or tangential load on the boride layer on steel
consequence: FeB is much harder than Fe2B but has very poor fracture toughness, so it can fracture or delaminate easily under high normal or tangential loading (Kartal et al.)
severity: moderate
source: kartal-2011
where: Abstract, opening sentences
side_effects: []
handling:
- text: 'Powder of HfB2 and TaB2: PubChem lists H315, H319 and H335, so avoid skin and eye contact and do not breathe the dust.'
source: pubchem-hfb2
where: Safety and Hazards, GHS Classification
- text: Zirconium and tantalum borides are hard to consolidate by pressure-assisted sintering, so spark plasma sintering or reactive sintering is used (Sani et al. 2016, introduction).
source: sani-2016
where: Introduction, paragraph on consolidation
mitigations: []
uses:
- application: heat-shields
device: Thermal protection system material for sharp leading edges
example: NASA Ames lists hot-pressed ZrB2 with 20 volume percent SiC for thermal protection, such as sharp leading edges on next-generation reusable launch vehicles, and notes that the material can be machined by EDM.
source: nasa-tpsx-zrb2
where: Description paragraph of the Zirconium Diboride (ZrB2/SiC) entry
- application: thermal-control
device: Solar thermal absorber for concentrating solar power
example: Sani et al. studied the optical properties of dense monophasic ZrB2 and TaB2 for the first time, because they may suit solar absorbers that work at very high temperature.
source: sani-2016
where: Abstract and Introduction
- application: mechanisms
device: Boride layer on low-carbon steel for hard, wear-resistant surfaces
example: Electrochemical boriding at 950 degC for 15 min in a borax electrolyte gives a boride layer, and a further 45 min at rest turns it into a single-phase Fe2B layer with a microhardness of about 16 GPa (Kartal et al.).
source: kartal-2011
where: Abstract
supply:
- subject: Boron (common to all the diborides and the boride layers)
abundance: 'USGS: borates occur in volcanic and arid deposits. The 2025 world total is withheld (XX). 2025 production by country, in thousand metric tons and as printed: Turkey 1,500 (refined borates), Bolivia 380 (ulexite), Chile 300 (ulexite), China 230 (boric oxide equivalent), Peru 220 (crude borates), Argentina 170 (crude ore), Russia 80 (datolite ore), Germany 40 (compounds).'
producers: []
critical_lists:
- list: USGS 2025 Final List of Critical Minerals (boron added in 2025, per the USGS boron chapter)
listed: true
- list: EU critical raw materials list (Boron/Borate)
listed: true
recycling: 'USGS: insignificant.'
substitutes:
- 'USGS: substitution is possible in detergents, enamels, insulation and soaps. No substitute for boron in a boride is discussed.'
source: usgs-mcs2026-boron
where: World Production and Reserves table, 2025 column (world total XX); Events, Trends and Issues (critical list paragraph); Recycling; Substitutes
- subject: Iron (the metal in FeB and Fe2B)
abundance: 'USGS: the only source of primary iron is iron ore. World usable ore production was 2,600,000 thousand metric tons in 2024 and an estimated 2,600,000 in 2025, with an iron content of 1,600,000 thousand metric tons in both years. 2025 usable ore by country, in thousand metric tons: Australia 980,000, Brazil 420,000, India 310,000, China 290,000.'
producers: []
critical_lists:
- list: EU critical raw materials list (iron is not named)
listed: false
recycling: 'USGS: none for iron ore; see the iron and steel scrap chapter (not read).'
substitutes:
- 'USGS: the only source of primary iron is iron ore, used directly as direct-shipping ore or converted to pig iron.'
source: usgs-mcs2026-iron
where: World Mine Production and Reserves table (usable ore, 2025e column); Substitutes; the critical list paragraph in Events, Trends and Issues
- subject: Zirconium (the metal in ZrB2)
abundance: 'USGS: world mine production of zirconium mineral concentrates was about 1,200 thousand metric tons gross weight in 2025 (1,300 in 2024). 2025 by country, in thousand metric tons: Australia 400, South Africa 270, Mozambique 160, Senegal 70, China 100, Indonesia 52, Madagascar 26, Sierra Leone 25. Zirconium reserves are more than 70,000 thousand metric tons ZrO2 content.'
producers: []
critical_lists:
- list: EU critical raw materials list (zirconium is not named)
listed: false
recycling: 'USGS: companies in Oregon and Utah recycled zirconium from new scrap and from post-commercial old scrap; foundry mould cores and spent zirconia refractories are often recycled but cannot be quantified.'
substitutes:
- 'USGS: chromite and olivine can substitute for zircon in some foundry applications, and niobium, stainless steel and tantalum in some nuclear applications.'
source: usgs-mcs2026-zirconium-hafnium
where: World Mine Production and Reserves table; Recycling; Substitutes
- subject: Hafnium (the metal in HfB2)
abundance: 'USGS: world primary hafnium production data and quantitative hafnium reserve estimates were not available. Germany supplied 54 percent of unwrought hafnium imports in 2021 to 2024 (USGS import sources); the leading global exporters of unwrought hafnium were China and Germany.'
producers: []
critical_lists:
- list: EU critical raw materials list (hafnium is named)
listed: true
recycling: 'USGS: hafnium metal recycling was minimal.'
substitutes: []
source: usgs-mcs2026-zirconium-hafnium
where: World Mine Production and Reserves text; Import Sources (2021 to 2024); Recycling
- subject: Niobium (the metal in NbB2)
abundance: 'USGS: world mine production of niobium was 112,000 t in 2024 and 2025 (rounded total). Brazil produced 104,000 t in 2024 and 2025e, and Canada 6,900 t in 2024 and 6,000 t in 2025e. U.S. net import reliance was 100 percent.'
producers:
- country: Brazil
share_percent: 93
year: 2025
- country: Canada
share_percent: 5
year: 2025
critical_lists:
- list: EU critical raw materials list (Niobium)
listed: true
recycling: 'USGS: niobium was recycled with niobium-bearing steels and superalloys, but scrap recovery specifically for niobium content was negligible.'
substitutes:
- 'USGS: ceramic matrix composites, molybdenum, tantalum and tungsten in superalloys, and molybdenum, tantalum and titanium as alloying elements in steels, can substitute with a performance loss or higher cost.'
source: usgs-mcs2026-niobium
where: Events, Trends and Issues (Brazil about 93 percent, Canada 5 percent); World Mine Production and Reserves table; Salient Statistics (net import reliance); Substitutes
- subject: Tantalum (the metal in TaB2)
abundance: 'USGS: tantalum has not been mined in the United States since 1959, and U.S. net import reliance was 100 percent. World mine production was 2,500 t in 2024 and 2025e (rounded). Congo (Kinshasa) produced 1,270 t in 2024 and 1,300 t in 2025e, Rwanda 374 t and 400 t, Nigeria 390 t in both years.'
producers: []
critical_lists:
- list: EU critical raw materials list (Tantalum)
listed: true
recycling: 'USGS: tantalum was recycled mostly from new scrap of tantalum electronic components and from cemented carbide and superalloy scrap; recycling may account for as much as 30 percent of consumption by domestic primary processors.'
substitutes:
- 'USGS: niobium and tungsten in carbides; aluminium, ceramics and niobium in capacitors; hafnium, iridium, molybdenum, niobium, rhenium and tungsten in high-temperature applications.'
source: usgs-mcs2026-tantalum
where: Salient Statistics (net import reliance); World Mine Production and Reserves table; Recycling; Substitutes
- subject: Tungsten (the metal in WB)
abundance: 'USGS: tungsten has not been mined commercially in the United States since 2015. World mine production was 82,000 t in 2024 and 85,000 t in 2025 (rounded). China produced 67,000 t in both years. U.S. net import reliance was more than 50 percent.'
producers: []
critical_lists:
- list: EU critical raw materials list (Tungsten)
listed: true
recycling: 'USGS: the quantity of secondary tungsten and the amount consumed from secondary sources were withheld to protect company data.'
substitutes:
- 'USGS: molybdenum carbide, niobium carbide or titanium carbide cemented carbides, ceramics, cermets and tool steels can substitute for cemented tungsten carbide, but most of these reduce rather than replace the tungsten used.'
source: usgs-mcs2026-tungsten
where: Domestic Production and Use; Salient Statistics (net import reliance); World Mine Production and Reserves table; Substitutes
- subject: Cobalt (the metal in Co2B and CoB)
abundance: 'USGS: Congo (Kinshasa) was the world''s leading source of mined cobalt, with an estimated 73 percent of the 2025 world total, followed by Indonesia with 14 percent. World mine production was 302,000 t in 2024 and 310,000 t in 2025 (rounded). U.S. net import reliance was 79 percent in 2025e.'
producers:
- country: Congo (Kinshasa)
share_percent: 73
year: 2025
- country: Indonesia
share_percent: 14
year: 2025
critical_lists:
- list: EU critical raw materials list (Cobalt)
listed: true
recycling: 'USGS: cobalt content of purchased scrap represented 25 percent of estimated U.S. cobalt consumption in 2025.'
substitutes:
- 'USGS: barium or strontium ferrites, neodymium-iron-boron alloys, nickel-iron alloys in magnets; iron, nickel, cermets or ceramics in cutting and wear-resistant materials.'
source: usgs-mcs2026-cobalt
where: Events, Trends and Issues (Congo 73 percent, Indonesia 14 percent); World Mine Production and Reserves table; Salient Statistics; Recycling; Substitutes
media: []
documents:
- title: Sani E. et al. 2016, Optical properties of dense zirconium and tantalum diborides for solar thermal absorbers, Renewable Energy 91, 340-346 (arXiv preprint copy read)
type: paper
url: https://arxiv.org/pdf/1803.06528
year: 2016
- title: Sairam K. et al. 2014, Reaction spark plasma sintering of niobium diboride, Int. J. Refract. Met. Hard Mater. 43, 259-262 (abstract read)
type: paper
url: https://research.birmingham.ac.uk/en/publications/reaction-spark-plasma-sintering-of-niobium-diboride/
year: 2014
- title: Kartal G. et al. 2011, The growth of single Fe2B phase on low carbon steel via phase homogenization in electrochemical boriding (PHEB), Surface and Coatings Technology 206(7), 2005-2011 (abstract read)
type: paper
url: https://research.itu.edu.tr/en/publications/the-growth-of-single-fesub2subb-phase-on-low-carbon-steel-via-pha/
year: 2011
- title: Mechanochemical synthesis and characterization of pure Co2B nanocrystals, Bulletin of Materials Science 39(4), 1119-1126 (2016), abstract read
type: paper
url: https://avesis.hacettepe.edu.tr/yayin/8d53ea59-7ba3-464f-9afa-322edb325d5c/mechanochemical-synthesis-and-characterization-of-pure-co2b-nanocrystals
year: 2016
- title: Liang Y. et al., Novel Tungsten Triboride (arXiv 1210.3777, DFT prediction of WB3)
type: paper
url: https://arxiv.org/pdf/1210.3777
year: 2012
- title: NASA Ames Thermal Protection Materials Database, Zirconium Diboride (ZrB2/SiC)
type: report
url: https://tpsx.arc.nasa.gov/Material?id=28
year: 2001
- title: PubChem compound record CID 9812765, Zirconium diboride (GHS classification and melting point)
type: database
url: https://pubchem.ncbi.nlm.nih.gov/compound/9812765
year: 2026
- title: PubChem compound record CID 6336857, Hafnium boride (HfB2) (GHS classification)
type: database
url: https://pubchem.ncbi.nlm.nih.gov/compound/6336857
year: 2026
- title: PubChem compound record CID 9815613, Tantalum boride (TaB2) (GHS classification)
type: database
url: https://pubchem.ncbi.nlm.nih.gov/compound/9815613
year: 2026
- title: PubChem compound record CID 82793, Tungsten boride (GHS classification)
type: database
url: https://pubchem.ncbi.nlm.nih.gov/compound/82793
year: 2026
- title: PubChem compound record CID 82789, Iron boride (FeB) (GHS classification)
type: database
url: https://pubchem.ncbi.nlm.nih.gov/compound/82789
year: 2026
- title: USGS Mineral Commodity Summaries 2026, Niobium (Columbium)
type: report
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-niobium.pdf
year: 2026
- title: USGS Mineral Commodity Summaries 2026, Tantalum
type: report
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-tantalum.pdf
year: 2026
- title: USGS Mineral Commodity Summaries 2026, Tungsten
type: report
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-tungsten.pdf
year: 2026
- title: USGS Mineral Commodity Summaries 2026, Cobalt
type: report
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-cobalt.pdf
year: 2026
- title: USGS Mineral Commodity Summaries 2026, Zirconium and Hafnium
type: report
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-zirconium-hafnium.pdf
year: 2026
- title: USGS Mineral Commodity Summaries 2026, Iron Ore
type: report
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-iron-ore.pdf
year: 2026
- title: USGS Mineral Commodity Summaries 2026, Boron
type: report
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-boron.pdf
year: 2026
- title: European Commission, Critical raw materials list (Regulation (EU) 2024/1252)
type: standard
url: https://single-market-economy.ec.europa.eu/sectors/raw-materials/areas-specific-interest/critical-raw-materials_en
year: 2024
gaps:
- 'Hafnium diboride: no density, melting point, hardness or modulus was read in a source for this run. The Gurcan (ITU/Anadolu) and Akcamli SPS papers were unreachable or gave only search snippets, and the HfB2 values in Wikipedia and vendor pages are not used.'
- 'Niobium diboride: no density or melting point was read in a source for this run (the Wikipedia and webqc values were not read on a primary page). Only the Birmingham abstract (hardness, modulus, fracture toughness, relative density) is used.'
- 'Tungsten boride (WB): no measured density, hardness or modulus was read. PubChem''s density (15.2 at 25 degC) has no source stated and is not used. The WB3 hardness is a DFT prediction for a different phase and is not a WB value. W2B5 identity is disputed in the literature (USPEX 2018 snippet), so it is not profiled.'
- 'Cobalt boride: CoB has no value, and the Henschel 2019 Dalton paper on Co2B and CoB layers was blocked by a browser challenge. The PubChem record for cobalt boride (CID 121233614) has a malformed formula and was not used. No GHS entry for Co2B or CoB was read.'
- Iron boride density (Fe2B and FeB) was not found. The MDPI Coatings 2023 paper returned HTTP 403, and only search snippets gave hardness (about 1600 HV Fe2B, about 2000 HV FeB) which are not used as values. FeB hardness as a number was not read in a fetched page.
- 'Oxidation or corrosion data for NbB2, TaB2, HfB2, WB, Co borides and Fe borides: none read in this run. The only corrosion entry is NASA''s qualitative statement for ZrB2 with SiC.'
- 'Space use: the only space-related source is NASA TPSX (ZrB2 with SiC for thermal protection of sharp leading edges, ground-test material). No flight or lunar source for any boride in this family was read.'
- 'U.S. 2025 Final List of Critical Minerals status: the boron chapter confirms boron was added, but the niobium, tantalum, tungsten, cobalt, zirconium and hafnium chapters do not state their list status. Only the EU list is recorded for those metals.'
- 'Designations (UNS, EN, DIN, JIS, AISI and similar codes) for any boride in this family: none printed in a source read in this run.'
- 'Custom property names used because they are not in spores/property-canon.yaml: hardness, fracture_toughness, relative_density, enthalpy_of_formation, molar_heat_capacity, lattice_parameter_a, lattice_parameter_c, layer_thickness, saturation_magnetization.'
- Sani et al. electrical conductivity values (printed as 1.0 x 10^7 and 3.03 x 10^6 S/m) are left out because the exponent is not printed in plain form. The molar heat capacities are kept in J/(mol·K) as printed.
- Hardness test method and load for ZrB2, TaB2 and NbB2 are not stated in the Table 1 or abstract that gives them, so the values are reported without a method.
- 'Source disagreement: ZrB2 density is 6.119 g/cm3 for dense pure ZrB2 (Sani) and 5.56 g/cm3 for a ZrB2 plus 20 vol percent SiC composite (NASA). They are different materials and are not compared as one value.'
- 'Story compare paragraph: the comparison is inside this family only. No family or industry comparison set is sourced for HfB2, NbB2 or the cobalt and iron borides.'
sources:
sani-2016:
title: Sani E. et al., Optical properties of dense zirconium and tantalum diborides for solar thermal absorbers, Renewable Energy 91 (2016) 340-346, doi 10.1016/j.renene.2016.01.068 (arXiv preprint 1803.06528)
url: https://arxiv.org/pdf/1803.06528
kind: paper
license: arXiv preprint, read for its Table 1 values
sairam-nbb2-2014:
title: Sairam K. et al., Reaction spark plasma sintering of niobium diboride, Int. J. Refract. Met. Hard Mater. 43 (2014) 259-262, doi 10.1016/j.ijrmhm.2013.12.011
url: https://research.birmingham.ac.uk/en/publications/reaction-spark-plasma-sintering-of-niobium-diboride/
kind: paper
license: University of Birmingham repository page (abstract)
kartal-2011:
title: Kartal G. et al., The growth of single Fe2B phase on low carbon steel via phase homogenization in electrochemical boriding (PHEB), Surface and Coatings Technology 206(7) (2011) 2005-2011, doi 10.1016/j.surfcoat.2011.08.049
url: https://research.itu.edu.tr/en/publications/the-growth-of-single-fesub2subb-phase-on-low-carbon-steel-via-pha/
kind: paper
license: Istanbul Technical University repository page (abstract)
co2b-2016:
title: Mechanochemical synthesis and characterization of pure Co2B nanocrystals, Bulletin of Materials Science 39(4) (2016) 1119-1126, doi 10.1007/s12034-016-1231-x
url: https://avesis.hacettepe.edu.tr/yayin/8d53ea59-7ba3-464f-9afa-322edb325d5c/mechanochemical-synthesis-and-characterization-of-pure-co2b-nanocrystals
kind: paper
license: repository listing (abstract)
wb3-2012:
title: Liang Y. et al., Novel Tungsten Triboride (arXiv 1210.3777), density functional theory prediction of hP24-WB3
url: https://arxiv.org/pdf/1210.3777
kind: paper
license: arXiv
nasa-tpsx-zrb2:
title: NASA Ames Thermal Protection Materials Database, Zirconium Diboride (ZrB2/SiC) entry
url: https://tpsx.arc.nasa.gov/Material?id=28
kind: database
license: NASA public domain
pubchem-zrb2:
title: PubChem compound CID 9812765, Zirconium diboride (GHS aggregated notifications, melting point)
url: https://pubchem.ncbi.nlm.nih.gov/compound/9812765
kind: database
license: PubChem public database
pubchem-hfb2:
title: PubChem compound CID 6336857, Hafnium boride (HfB2), GHS aggregated notifications
url: https://pubchem.ncbi.nlm.nih.gov/compound/6336857
kind: database
license: PubChem public database
pubchem-tab2:
title: PubChem compound CID 9815613, Tantalum boride (TaB2), GHS aggregated notifications
url: https://pubchem.ncbi.nlm.nih.gov/compound/9815613
kind: database
license: PubChem public database
pubchem-wb:
title: PubChem compound CID 82793, Tungsten boride, GHS classification
url: https://pubchem.ncbi.nlm.nih.gov/compound/82793
kind: database
license: PubChem public database
pubchem-feb:
title: PubChem compound CID 82789, Iron boride (FeB), GHS classification
url: https://pubchem.ncbi.nlm.nih.gov/compound/82789
kind: database
license: PubChem public database
usgs-mcs2026-boron:
title: USGS Mineral Commodity Summaries 2026, Boron
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-boron.pdf
kind: report
license: US government work, public domain
usgs-mcs2026-iron:
title: USGS Mineral Commodity Summaries 2026, Iron Ore
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-iron-ore.pdf
kind: report
license: US government work, public domain
usgs-mcs2026-zirconium-hafnium:
title: USGS Mineral Commodity Summaries 2026, Zirconium and Hafnium
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-zirconium-hafnium.pdf
kind: report
license: US government work, public domain
usgs-mcs2026-niobium:
title: USGS Mineral Commodity Summaries 2026, Niobium (Columbium)
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-niobium.pdf
kind: report
license: US government work, public domain
usgs-mcs2026-tantalum:
title: USGS Mineral Commodity Summaries 2026, Tantalum
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-tantalum.pdf
kind: report
license: US government work, public domain
usgs-mcs2026-tungsten:
title: USGS Mineral Commodity Summaries 2026, Tungsten
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-tungsten.pdf
kind: report
license: US government work, public domain
usgs-mcs2026-cobalt:
title: USGS Mineral Commodity Summaries 2026, Cobalt
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-cobalt.pdf
kind: report
license: US government work, public domain
ec-crm:
title: European Commission, Critical raw materials (list under Regulation (EU) 2024/1252)
url: https://single-market-economy.ec.europa.eu/sectors/raw-materials/areas-specific-interest/critical-raw-materials_en
kind: web
license: European Commission web page
license: CC-BY-4.0
updated: '2026-10-26'
review:
status: draft
method: assistant
checked_values: 30
unreachable: 4
caveats: 4
note: 'Written in this run from Sani et al. 2016 (Table 1), Sairam et al. 2014 (abstract), Kartal et al. 2011 (abstract), the Co2B 2016 abstract, NASA TPSX (ZrB2/SiC), PubChem GHS for five borides, USGS MCS 2026 chapters and the EU critical list. Unreachable or snippet-only: MDPI Coatings 2023 (403), Henschel 2019 Dalton (browser challenge), Gurcan HfB2 and Akcamli HfB2 papers, Sonber ZrB2 paper. Values are not yet checked by verify-values.'
story:
recipe:
line: These are hexagonal metal borides. ZrB2 and TaB2 take the AlB2-type structure (space group P6/mmm, Sani 2016 Table 1). Sani et al. made dense ZrB2 and TaB2 by reactive spark plasma sintering from metal and amorphous boron, or by spark plasma sintering of powders first made by self-propagating high-temperature synthesis. Sairam et al. made dense NbB2 (97.7 percent) from elemental niobium and boron, synthesised at 1200 degC and then densified at 1700 to 1900 degC by reaction spark plasma sintering. The iron borides form as layers on steel during electrochemical boriding in a borax electrolyte at 950 degC (Kartal 2011).
parts:
- name: Boron
symbol: B
share: two boron per metal in MB2 diborides (AlB2-type)
role: Forms the boron layers in the hexagonal structure. In Sani et al., amorphous boron of at least 95 percent purity was used as one reactant.
- name: Zirconium
symbol: Zr
share: one zirconium per two boron in ZrB2
role: Metal in ZrB2, the most-studied diboride in this family; Sani et al. used Zr powder below 44 micrometres.
- name: Tantalum
symbol: Ta
share: one tantalum per two boron in TaB2
role: Metal in TaB2, which is denser than ZrB2 (12.568 g/cm3 against 6.119 g/cm3).
risk_groups:
- title: For people
level: 0
verdict: Irritant or harmful; GHS data are partial
lead: PubChem aggregated notifications give harmful-category codes (H302, H312, H332) for ZrB2 and irritation codes (H315, H319, H335) for HfB2 and TaB2. Most reports agree, but a small share say the material is not classified. No supplier SDS was read for these borides.
points:
- label: Dust
line: Control dust when handling powders of any boride. PubChem lists irritation of skin, eyes and the respiratory tract for HfB2 and TaB2.
- label: Ingestion and skin
line: PubChem lists H302, H312 and H332 (harmful if swallowed, in contact with skin or inhaled) for ZrB2 in 85.2 percent of its 54 reports.
- title: If a part fails
lead: These are the numbers read for dense material at room temperature.
points:
- label: Brittleness
line: Dense NbB2 has an indentation fracture toughness of 4 MPa·m1/2, so a flaw can start a crack well below the hardness limit.
- label: Boride layer
line: The FeB layer is much harder than Fe2B but fractures or delaminates easily under high load (Kartal 2011).
why: Transition-metal borides are hard, high-melting ceramics or layers. Dense ZrB2 has a melting temperature of 3245 degC and a hardness of 23 GPa (Sani 2016), and dense NbB2 has a hardness of 20.25 GPa and an elastic modulus of 539 GPa (Sairam 2014). Steel boriding gives a surface boride layer of about 16 GPa microhardness. The sourced uses are heat shields for launch vehicles (NASA), solar absorbers (Sani) and wear layers on steel (Kartal).
uses:
- where: Heat-shield material for sharp leading edges
line: NASA Ames lists hot-pressed ZrB2 with 20 vol percent SiC for thermal protection, such as sharp leading edges on next-generation reusable launch vehicles.
- where: Solar thermal absorbers
line: Sani et al. studied dense ZrB2 and TaB2 for the first time as solar absorbers that work at very high temperature.
- where: Wear-resistant boride layers on steel
line: A single-phase Fe2B layer of 75 micrometres, grown by electrochemical boriding at 950 degC, has a microhardness of about 16 GPa (Kartal 2011).
can_do:
- label: Density
benchmark: density
value: 6.119 g/cm3
line: Dense ZrB2 has a density of 6.119 g/cm3, and TaB2 is much denser at 12.568 g/cm3 (Sani 2016).
- label: Heat resistance
benchmark: melting_point
value: 3245 degC
line: The melting temperature is 3245 degC for ZrB2 and 3037 degC for TaB2 (Sani 2016).
- label: Hardness
benchmark: hardness
value: 23 GPa
line: ZrB2 has a hardness of 23 GPa and TaB2 19.6 GPa (Sani 2016). NbB2 is 20.25 GPa at 97.7 percent density (Sairam 2014).
- label: Stiffness
benchmark: elastic_modulus
value: 539 GPa
line: NbB2 has an elastic modulus of 539 GPa (Sairam 2014). ZrB2 is 489 GPa and TaB2 248.2 GPa (Sani 2016).
compare: 'Within this family, ZrB2 is the lightest and hardest of the diborides with sourced bulk values: 6.119 g/cm3, 23 GPa and a melting temperature of 3245 degC. TaB2 is about twice as dense and has a lower melting point (3037 degC), hardness (19.6 GPa) and modulus (248.2 GPa). NbB2 has a hardness of 20.25 GPa and a modulus of 539 GPa at 97.7 percent density, so its stiffness is the highest of the sourced diborides. Hafnium diboride, tungsten boride and the cobalt and iron borides lack sourced bulk values here.'
compare_rows:
- label: Density
benchmark: density
- label: Hardness
benchmark: hardness
- label: Melting temperature
benchmark: melting_point
handling:
- PubChem lists H315, H319 and H335 for HfB2 and TaB2, so avoid skin and eye contact and do not breathe the dust.
- Zirconium and tantalum borides are hard to sinter. Sani et al. used spark plasma sintering to reach dense material.
- 'Oxidation in air at high temperature: NASA says SiC improves the oxidation resistance of ZrB2, so pure ZrB2 is less resistant. No rate data were read.'
good_for:
- Hard, stiff parts made from ZrB2 or NbB2. The sourced values are 23 GPa for ZrB2 and 20.25 GPa and 539 GPa for NbB2.
- Hard wear layers on steel from boriding, with a single-phase Fe2B layer of about 16 GPa microhardness.
watch_out:
- 'Brittleness: NbB2 has an indentation fracture toughness of 4 MPa·m1/2 (Sairam 2014). FeB fractures easily under high load (Kartal 2011).'
- 'Thin data: hafnium diboride and tungsten boride have no sourced density or hardness here, and Co and Fe boride bulk values are missing.'
- 'Mixed basis: the ZrB2 density 6.119 g/cm3 is for pure ZrB2, while the NASA ZrB2 density of 5.56 g/cm3 is for a SiC composite.'
verdict: The sourced family is a set of hard, high-melting ceramics and steel boride layers. ZrB2 and NbB2 have the best bulk values here, TaB2 is much denser, and the cobalt, iron, hafnium and tungsten borides still need measured data before they can be compared properly.
References
Every number above carries a reference number. Click one to see the source and where in it the value comes from.