Commonly recognised as a metalloid
Recognition status, as metalloids, of some elements in the p-block of the standard periodic table. Elements with green shading (B, Si, Ge, As, Sb, Te) are commonly recognised as metalloids. Elements with blue shading (Po, At) are inconsistently recognised, due to their status as metalloids being disputed. Selenium (Se), the element with pink shading, is still less commonly recognised as metalloid. Elements with yellow shading (C, Al) are rarely recognised as metalloids.
The grey staircase-shaped line, which passes between B-Al, Al-Si, Si-Ge, Ge-As, As-Sb, Sb-Te, Te-Po and Po-At, is a typical example of the arbitrary metal–nonmetal dividing line that can be found on some periodic tables. Germanium, if classified as a nonmetal, then appears to fall on the wrong side of the line. This is a result of the publicity this form of the line received in the late 1920s and early '30s. Germanium was thought to be a poorly conducting metal, up to at least the late 1930s.
A metalloid is a chemical element that has properties in between those of metals and nonmetals. There is no standard definition of a metalloid, nor is there complete agreement as to which elements are appropriately classified as such. Despite this lack of specificity the term remains in use in chemistry literature.
The six commonly recognised metalloids are boron, silicon, germanium, arsenic, antimony and tellurium. Elements less commonly recognised as metalloids include carbon, aluminium, selenium, polonium and astatine. On a standard periodic table all of these elements can be found in a diagonal region of the p-block, extending from boron at one end to astatine at the other. Some periodic tables include a dividing line between metals and nonmetals and it is generally the elements adjacent to this line or, less often, one or more of the elements adjacent to those elements, which are identified as metalloids.
Typical metalloids have a metallic appearance but they are brittle and only fair conductors of electricity. Chemically, they mostly behave as (weak) nonmetals. They can form alloys with metals. Most of their other physical and chemical properties are intermediate in nature. Metalloids are usually too brittle to have any structural uses. They and their compounds are used in alloys, biological agents, flame retardants, glasses, optical storage, pyrotechnics, semiconductors and electronics. The electrical properties of silicon and germanium enabled the establishment of the semiconductor industry in the 1950s and the development of solid-state electronics from the early 1960s.
The term metalloid originally referred to nonmetals. Its more recent meaning, as a category of elements with intermediate or hybrid properties, became widespread in 1940–1960. Metalloids are sometimes called semimetals, a practice that has been discouraged as the term semimetal has a different meaning in physics than in chemistry. In physics it more specifically refers to the electronic band structure of a substance.
Broadly, the recognised metalloids occupy middle ground in terms of their abundance, extraction methods, and costs. Silicon is the second most abundant element in the Earth's crust after oxygen; tellurium is rarer than gold, but more abundant than rhenium, the rarest of the stable metals. Extraction can be achieved by ordinary chemical reduction of the oxides or sulfides.
- 1 Definitions
- 2 Periodic table territory
- 3 Properties
- 4 Common applications
- 5 Nomenclature and history
- 6 Elements commonly recognised as metalloids
- 7 Elements less commonly recognised as metalloids
- 8 Related concepts
- 9 Abundance, extraction and cost
- 10 Notes
- 11 Citations
- 12 References
- 13 Further reading
A metalloid is an element with properties that are in between, or a mixture of, the properties of metals and nonmetals and thus is hard to classify as either a metal or a nonmetal. This is a generic definition that draws on metalloid attributes that are consistently cited in the literature.[n 2] Difficulty of categorisation is a key attribute. Most elements have a mixture of metallic and nonmetallic properties, and can be classified according to which set of properties is more pronounced.[n 3] Only the elements at or near the margins, lacking a sufficiently clear preponderance of either metallic or nonmetallic properties, are classified as metalloids.
Boron, silicon, germanium, arsenic, antimony and tellurium are commonly recognised as metalloids.[n 4] Depending on the author, one or more from selenium, polonium or astatine are sometimes added to the list. Boron is sometimes excluded, by itself or with silicon. Tellurium is sometimes not regarded as a metalloid. The inclusion of antimony, polonium and astatine as metalloids has also been questioned.
Other elements are occasionally classified as metalloids. These elements include hydrogen, beryllium, nitrogen, phosphorus, sulfur, zinc, gallium, tin, iodine, lead, bismuth and radon. The term metalloid has also been used for elements that exhibit metallic lustre and electrical conductivity, and that are amphoteric, such as arsenic, antimony, vanadium, chromium, molybdenum, tungsten, tin, lead and aluminium. The other metals, and nonmetals (such as carbon or nitrogen) that can form alloys with metals or modify their properties have also occasionally been considered as metalloids.
|The elements commonly recognised as metalloids, and their ionization energies; electronegativities (revised Pauling scale); and electronic band structures (most thermodynamically stable forms under ambient conditions).|
There is no widely agreed upon definition of a metalloid. Hawkes questioned the feasibility of establishing a specific definition and added that anomalies can be found in several attempted constructs. Classifying an element as a metalloid has been described by Sharp as "arbitrary".
How many and which elements are metalloids depends on the classification criteria being used. There is no standardized division of the periodic table into metals, metalloids and nonmetals. Emsley recognised four metalloids: germanium, arsenic, antimony and tellurium; James et al. listed twelve: boron, carbon, silicon, germanium, arsenic, selenium, antimony, tellurium, bismuth, polonium, ununpentium and livermorium. On average, seven elements are included in such lists. Individual classification arrangements tend to share common ground; most variations occur around the indistinct margins.[n 5][n 6]
A single quantitative criterion, such as electronegativity, is commonly used. Metalloids have electronegativity values of from 1.8 or 1.9 to 2.2. Further examples are packing efficiency, and the Goldhammer-Herzfeld criterion ratio. Packing efficiency is the fraction of volume in a crystal structure occupied by atoms. The commonly recognised metalloids have packing efficiencies of between 34% and 41%.[n 7] The Goldhammer-Herzfeld ratio is a simple measure of how metallic a chemical element is; it is about equal to the cube of the atomic radius divided by the molar volume.[n 8] The recognised metalloids have Goldhammer-Herzfeld criterion ratios of between ~0.85 and 1.1, averaging 1.0.[n 9] Other authors have relied on, for example, atomic conductance[n 10] or bulk coordination number.
Jones, writing on the role of classification in science, observed that, "Classes are usually defined by more than two attributes". Masterton and Slowinski used three criteria to describe the six elements commonly recognised as metalloids. They wrote that metalloids have ionization energies around 200 kcal/mol (837 kJ/mol), and electronegativity values close to 2.0. They also said that metalloids are typically semiconductors, though antimony and arsenic (semimetals in the physics sense) have electrical conductivities that approach those of metals. Selenium and polonium are probably excluded from this scheme; astatine may or may not be included.[n 11]
Periodic table territory
|Distribution of elements
sometimes classified as metalloids[n 12]
|Periodic table groups 1, 2, and 12 through 18:
Periodic table extract showing groups 1–2 and 12–18, and a dividing line between metals and nonmetals passing between H-Li, Be-B, B-Al, Al-Si, Si-Ge, Ge-As, As-Sb, Sb-Te, Te-Po, Po-At, At-Uus and Uus-Uuo. Elements with grey shading (B, C, Al, Si, Ge, As, Se, Sb, Te, Po, At) appear commonly to rarely in the list of metalloid lists. Elements with light tan shading (H, Be, P, S, Ga, Sn, I, Pb, Bi, Fl, Uup, Lv, Uus) appear still less frequently. Elements with pale blue shading (N, Zn, Rn) are outliers that show that the metalloid net is sometimes cast very widely. Although they do not appear in the list of metalloid lists, isolated references to their designation as metalloids can be found in the literature (as cited in this article).
Metalloids lie on either side of the dividing line between metals and nonmetals. This can be found, in varying configurations, on some periodic tables. Elements to the lower left of the line generally display increasing metallic behaviour; elements to the upper right display increasing nonmetallic behaviour. When presented as a regular stairstep, elements with the highest critical temperature for their groups (Li, Be, Al, Ge, Sb, Po) lie just below the line.
The diagonal positioning of the metalloids represents an exception to the observation that elements with similar properties tend to occur in vertical groups. A related effect can be seen in other diagonal similarities between some elements and their lower right neighbours, specifically lithium-magnesium, beryllium-aluminium, and boron-silicon. Rayner-Canham has argued that these similarities extend to carbon-phosphorus, nitrogen-sulfur, and into three d-block series.
This exception arises due to competing horizontal and vertical trends in the nuclear charge. Going along a period, the nuclear charge increases with atomic number as there is as an increase in electrons. The additional pull on outer electrons as nuclear charge increases generally outweighs the screening effect of having more electrons. With some irregularities, atoms therefore become smaller, ionization energy increases, and there is a gradual change in character, across a period, from strongly metallic, to weakly metallic, to weakly nonmetallic, to strongly nonmetallic elements. Going down a main group, the effect of increasing nuclear charge is generally outweighed by the effect of additional electrons being further away from the nucleus. Atoms generally become larger, ionization energy falls, and metallic character increases. The net effect is that the location of the metal-nonmetal transition zone shifts to the right in going down a group, and analogous diagonal similarities are seen elsewhere in the periodic table, as noted.
Depictions of metalloids vary according to the author. Some do not classify elements bordering the metal-nonmetal dividing line as metalloids, noting that a binary classification can facilitate the establishment of rules for determining bond types between metals and nonmetals. Metalloids are variously grouped with metals, regarded as nonmetals or treated as a sub-category of nonmetals.[n 13] Other authors have suggested that classifying some elements as metalloids "emphasizes that properties change gradually rather than abruptly as one moves across or down the periodic table". Some periodic tables distinguish elements that are metalloids and display no formal dividing line between metals and nonmetals. Metalloids are shown as occurring in a diagonal band or diffuse region.
Metalloids usually look like metals but behave largely like nonmetals. Physically, they are shiny, brittle solids with intermediate to relatively good electrical conductivity and the electronic band structure of a semimetal or semiconductor. Chemically, they mostly behave as (weak) nonmetals, have intermediate ionization energies and electronegativity values, and amphoteric or weakly acidic oxides. They can form alloys with metals. Most of their other physical and chemical properties are intermediate in nature.
Compared to metals and nonmetals
Characteristic properties of metals, metalloids and nonmetals are summarized in the table. Physical properties are listed in order of ease of determination; chemical properties run from general to specific, and then to descriptive.
|Form||solid; a few liquid at or near room temperature (Ga, Hg, Rb, Cs, Fr)[n 14]||solid||mostly gases|
|Appearance||lustrous (at least when freshly fractured)||lustrous||several colourless; others coloured, or metallic grey to black|
|Elasticity||typically elastic, ductile, malleable (when solid)||brittle||brittle, if solid|
|Electrical conductivity||good to high[n 15]||intermediate to good[n 16]||poor to good[n 17]|
|Band structure||metallic (Bi = semimetallic)||are semiconductors or, if not (As, Sb = semimetallic), exist in semiconducting forms||semiconductor or insulator|
|General chemical behaviour||metallic||nonmetallic||nonmetallic|
|Ionization energy||relatively low||intermediate ionization energies, usually falling between those of metals and nonmetals||relatively high|
|Electronegativity||usually low||have electronegativity values close to 2 (revised Pauling scale) or within the range of 1.9–2.2 (Allen scale)[n 18]||high|
|give alloys||can form alloys||ionic or interstitial compounds formed|
|Oxides||lower oxides basic; higher oxides increasingly acidic||amphoteric or weakly acidic||acidic|
The above table reflects the hybrid nature of metalloids. The properties of form, appearance, and behaviour when mixed with metals are more like metals. Elasticity and general chemical behaviour are more like nonmetals. Electrical conductivity, band structure, ionization energy, electronegativity, and oxides are intermediate between the two.
- The focus of this section is on the recognised metalloids. Elements less often recognised as metalloids are ordinarily classified as either metals or nonmetals; some of these are included here for comparative purposes.
Metalloids are too brittle to have any structural uses in their pure forms. They and their compounds are used as (or in) alloying components, biological agents (toxicological, nutritional and medicinal), flame retardants, glasses (oxide and metallic), optical storage media, pyrotechnics, semiconductors and electronics.[n 19]
Writing early in the history of intermetallic compounds, the British metallurgist Cecil Desch observed that "certain non-metallic elements are capable of forming compounds of distinctly metallic character with metals, and these elements may therefore enter into the composition of alloys". He associated silicon, arsenic and tellurium, in particular, with the alloy-forming elements. Phillips and Williams suggested that compounds of silicon, germanium, arsenic and antimony with B metals, "are probably best classed as alloys".
Among the lighter metalloids, alloys with transition metals are well-represented. Boron can form intermetallic compounds and alloys with such metals of the composition MnB, if n > 2. Ferroboron (15% boron) is used to introduce boron into steel; nickel-boron alloys are ingredients in welding alloys and case hardening compositions for the engineering industry. Alloys of silicon with iron and with aluminium are widely used by the steel and automotive industries, respectively. Germanium forms many alloys, most importantly with the coinage metals.
The heavier metalloids continue the theme. Arsenic can form alloys with metals, including platinum and copper; it is also added to copper and its alloys to improve corrosion resistance and appears to confer the same benefit when added to magnesium. Antimony is well known as an alloy-former, including with the coinage metals. Its alloys include pewter (a tin alloy with up to 20% antimony) and type metal (a lead alloy with up to 25% antimony). Tellurium readily alloys with iron, as ferrotellurium (50–58% tellurium), and with copper, in the form of copper tellurium (40–50% tellurium). Ferrotellurium is used as a stabilizer for carbon in steel casting. Of the non-metallic elements less often recognised as metalloids, selenium—in the form of ferroselenium (50–58% selenium)—is used to improve the machinability of stainless steels.
All six of the elements commonly recognised as metalloids have toxic, dietary or medicinal properties. Arsenic and antimony compounds are especially toxic; boron, silicon, and possibly arsenic, are essential trace elements. Boron, silicon, arsenic and antimony have medical applications, and germanium and tellurium are thought to have potential.
Silicon is present in silatrane, a highly toxic rodenticide. Long-term inhalation of silica dust causes silicosis, a fatal disease of the lungs. Silicon is an essential trace element. Silicone gel can be applied to badly burned patients to reduce scarring.
Salts of germanium are potentially harmful to humans and animals if ingested on a prolonged basis. There is interest in the pharmacological actions of germanium compounds but no licensed medicine as yet.
Arsenic is notoriously poisonous and may also be an essential element in ultratrace amounts. It has been used as a pharmaceutical agent since antiquity, including for the treatment of syphilis before the development of antibiotics. Arsenic is also a component of melarsoprol, a medicinal drug used in the treatment of human African trypanosomiasis or sleeping sickness. In 2003, arsenic trioxide (under the trade name Trisenox) was re-introduced for the treatment of acute promyelocytic leukaemia, a cancer of the blood and bone marrow.
Elemental tellurium is not considered particularly toxic; two grams of sodium tellurate, if administered, can be lethal. People exposed to small amounts of airborne tellurium exude a foul and persistent garlic-like odour. Tellurium dioxide has been used to treat seborrhoeic dermatitis; other tellurium compounds were used as antimicrobial agents before the development of antibiotics. In future, such compounds may need to be substituted for antibiotics that have become ineffective due to bacterial resistance.
Of the elements less often recognised as metalloids, beryllium and lead are noted for their toxicity; lead arsenate has been extensively used as an insecticide. Sulfur is one of the oldest of the fungicides and pesticides. Phosphorus, sulfur, zinc, selenium and iodine are essential nutrients, and aluminium, tin and lead may be. Sulfur, gallium, selenium, iodine and bismuth have medicinal applications. Sulfur is a constituent of sulfonamide drugs, still widely used for conditions such as acne and urinary tract infections. Gallium nitrate is used to treat the side effects of cancer; gallium citrate, a radiopharmaceutical, facilitates imaging of inflamed body areas. Selenium sulfide is used in medicinal shampoos and to treat skin infections such as tinea versicolor. Iodine is used as a disinfectant in various forms. Bismuth is an ingredient in some antibacterials.
Compounds of boron, silicon, arsenic and antimony have been used as flame retardants. Boron, in the form of borax, has been used as a textile flame retardant since at least the 18th century. Silicon compounds such as silicones, silanes, silsesquioxane, silica and silicates, some of which were developed as alternatives to more toxic halogenated products, can considerably improve the flame retardancy of plastic materials. Arsenic compounds such as sodium arsenite or sodium arsenate are effective flame retardants for wood but have been less frequently used due to their toxicity. Antimony trioxide is a flame retardant. Aluminium hydroxide has been used as a wood-fibre, rubber, plastic and textile flame retardant since the 1890s. Apart from aluminium hydroxide, use of phosphorus based flame-retardants—in the form of, for example, organophosphates—now exceeds that of any of the other main retardant types. These employ boron, antimony or halogenated hydrocarbon compounds.
The oxides B2O3, SiO2, GeO2, As2O3 and Sb2O3 readily form glasses. TeO2 forms a glass but this requires a "heroic quench rate" or the addition of an impurity, otherwise the crystalline form results. These compounds are used in chemical, domestic and industrial glassware and optics. Boron trioxide is used as a glass fibre additive, and is also a component of borosilicate glass, widely used for laboratory glassware and domestic ovenware for its low thermal expansion. Most ordinary glassware is made from silicon dioxide. Germanium dioxide is used as a glass fibre additive, as well as in infrared optical systems. Arsenic trioxide is used in the glass industry as a decolourizing and fining agent (for the removal of bubbles), as is antimony trioxide. Tellurium dioxide finds application in laser and nonlinear optics.
Amorphous metallic glasses are generally most easily prepared if one of the components is a metalloid or 'near metalloid' such as boron, carbon, silicon, phosphorus or germanium.[n 20] Aside from thin films deposited at very low temperatures, the first known metallic glass was an alloy of composition Au75Si25 reported in 1960. A metallic glass having a strength and toughness not previously seen, of composition Pd82.5P6Si9.5Ge2, was reported in 2011.
Phosphorus, selenium and lead, which are less often recognised as metalloids, are also used in glasses. Phosphate glass has a substrate of phosphorus pentoxide (P2O5), rather than the silica (SiO2) of conventional silicate glasses. It is used, for example, to make sodium lamps. Selenium compounds can be used both as decolourising agents and to add a red colour to glass. Decorative glassware made of traditional lead glass contains at least 30% lead(II) oxide (PbO); lead glass used for radiation shielding may have up to 65% PbO. Lead-based glasses have also been extensively used in electronics components; enamelling; sealing and glazing materials; and solar cells. Bismuth based oxide glasses have emerged as a less toxic replacement for lead in many of these applications.
Varying compositions of GeSbTe ("GST alloys") and Ag- and In- doped Sb2Te ("AIST alloys"), being examples of phase-change materials, are widely used in rewritable optical discs and phase-change memory devices. By applying heat, they can be switched between amorphous (glassy) and crystalline states. The change in optical and electrical properties can be used for information storage purposes.
The recognised metalloids have either pyrotechnic applications or associated properties. Boron and silicon are commonly encountered; they act somewhat like metal fuels. Boron is used in pyrotechnic initiator compositions (for igniting other hard-to-start compositions), and in delay compositions that burn at a constant rate. Boron carbide has been identified as a possible replacement for more toxic barium or hexachloroethane mixtures in smoke munitions, signal flares and fireworks. Silicon, like boron, is a component of initiator and delay mixtures. Doped germanium can act as a variable speed thermite fuel.[n 21] Arsenic trisulfide As2S3 was used in old naval signal lights; in fireworks to make white stars; in yellow smoke screen mixtures; and in initiator compositions. Antimony trisulfide Sb2S3 is found in white-light fireworks and in flash and sound mixtures. Tellurium has been used in delay mixtures and in blasting cap initiator compositions.
Carbon, aluminium, phosphorus and selenium continue the theme. Carbon, in black powder, is a constituent of fireworks rocket propellants, bursting charges, and effects mixtures, and military delay fuses and igniters.[n 22] Aluminium is a common pyrotechnic ingredient, and is widely employed for its capacity to generate light and heat, including in thermite mixtures. Phosphorus can be found in smoke and incendiary munitions, paper caps used in toy guns, and party poppers. Selenium has been used in the same way as tellurium.
Semiconductors and electronics
All the elements commonly recognised as metalloids (or their compounds) have been used in the semiconductor or solid-state electronic industries.
Some properties of boron have limited its use as a semiconductor. It has a high melting point, single crystals are relatively hard to obtain, and introducing and retaining controlled impurities is difficult.
Silicon is the leading commercial semiconductor; it forms the basis of modern electronics (including standard solar cells) and information and communication technologies. This was despite the study of semiconductors, early in the 20th century, having been regarded as the "physics of dirt" and not deserving of close attention.
Germanium has largely been replaced by silicon in semiconducting devices, being cheaper, more resilient at higher operating temperatures, and easier to work during the microelectronic fabrication process. Germanium is still a constituent of semiconducting silicon-germanium 'alloys' and these have been growing in use, particularly for wireless communication devices; such alloys exploit the higher carrier mobility of germanium. The synthesis of gram-scale quantities of semiconducting germanane was reported in 2013. This comprises one-atom thick sheets of hydrogen-terminated germanium atoms, analogous to graphane. It conducts electrons more than ten times faster than silicon and five times faster than germanium, and is thought to have potential for optoelectronic and sensing applications. The development of a germanium-wire based anode that more than doubles the capacity of lithium-ion batteries was reported in 2014. In the same year, Lee at al. reported that defect-free crystals of graphene large enough to have electronic uses could be grown on, and removed from, a germanium substrate.
Arsenic and antimony are not semiconductors in their standard states. Both form type III-V semiconductors (such as GaAs, AlSb or GaInAsSb) in which the average number of valence electrons per atom is the same as that of Group 14 elements. These compounds are preferred for some special applications. Antimony nanocrystals may enable lithium-ion batteries to be replaced by more powerful sodium ion batteries.
Tellurium, which is a semiconductor in its standard state, is used mainly as a component in type II/VI semiconducting-chalcogenides; these have applications in electro-optics and electronics. Cadmium telluride (CdTe) is used in solar modules for its high conversion efficiency, low manufacturing costs, and large band gap of 1.44 eV, letting it absorb a wide range of wavelengths. Bismuth telluride (Bi2Te3), alloyed with selenium and antimony, is a component of thermoelectric devices used for refrigeration or portable power generation.
Five metalloids—boron, silicon, germanium, arsenic and antimony—can be found in cell phones (along with at least 39 other metals and nonmetals). Tellurium is expected to find such use. Of the less often recognised metalloids, phosphorus, gallium (in particular) and selenium have semiconductor applications. Phosphorus is used in trace amounts as a dopant for n-type semiconductors. The commercial use of gallium compounds is dominated by semiconductor applications—in integrated circuits; cell phones; laser diodes; light-emitting diodes; photodetectors; and solar cells. Selenium is used in the production of solar cells and in high-energy surge protectors.
Nomenclature and history
Derivation and other names
The word metalloid comes from the Latin metallum ("metal") and the Greek oeides ("resembling in form or appearance"). Several names are sometimes used synonymously although some of these have other meanings that are not necessarily interchangeable: amphoteric element, boundary element, half-metal, half-way element, near metal, meta-metal, semiconductor, semimetal and submetal. 'Amphoteric element' is sometimes used more broadly to include transition metals capable of forming oxyanions, such as chromium and manganese. 'Half-metal' is used in physics to refer to a compound (such as chromium dioxide) or alloy that can act as a conductor and an insulator. 'Meta-metal' is sometimes used instead to refer to certain metals (Be, Zn, Cd, Hg, In, Tl, β-Sn, Pb) located just to the left of the metalloids on standard periodic tables. These metals are mostly diamagnetic and tend to have distorted crystalline structures, electrical conductivity values at the lower end of those of metals, and amphoteric (weakly basic) oxides. 'Semimetal' sometimes refers, loosely or explicitly, to metals with incomplete metallic character in crystalline structure, electrical conductivity or electronic structure. Examples include gallium, ytterbium, bismuth and neptunium. The names amphoteric element and semiconductor are problematic as some elements referred to as metalloids do not show marked amphoteric behaviour (bismuth, for example) or semiconductivity (polonium) in their most stable forms.
Origin and usage
The origin and usage of the term 'metalloid' is convoluted. Its origin lies in attempts, dating from antiquity, to describe metals and to distinguish between typical and less typical forms. It was first applied in the early 19th century to metals that floated on water (sodium and potassium), and then more popularly to nonmetals. Earlier usage in mineralogy, to describe a mineral having a metallic appearance, can be sourced to as early as 1800. Since the mid-20th century it has been used to refer to intermediate or borderline chemical elements.[n 23] The International Union of Pure and Applied Chemistry (IUPAC) previously recommended abandoning the term metalloid, and suggested using the term 'semimetal' instead. Use of this latter term has more recently been discouraged by Atkins et al. as it has a different meaning in physics—one that more specifically refers to the electronic band structure of a substance rather than the overall classification of an element. The most recent IUPAC publications on nomenclature and terminology do not include any recommendations on the usage of the terms 'metalloid' or 'semimetal'.
Elements commonly recognised as metalloids
- Properties noted in this section refer to the elements in their most thermodynamically stable forms under ambient conditions.
Pure boron is a shiny, silver-grey crystalline solid. It is less dense than aluminium (2.34 v 2.70 g/cm3), and is hard and brittle. It is barely reactive under normal conditions, except for attack by fluorine, and has a melting point of 2076 °C (cf. steel ~1370 °C). Boron is a semiconductor; its room temperature electrical conductivity is 1.5 × 10−6 S•cm−1 (about 200 times less than that of tap water) and a band gap of about 1.56 eV.[n 24]
The chemistry of boron is dominated by its small atomic size, and relatively high ionization energy. With only three valence electrons, simple covalent bonding cannot fulfil the octet rule. Metallic bonding is the usual result among the heavier congenors of boron but this generally requires a low ionization energy. Being small and having a high ionization energy boron instead forms delocalized covalent bonds, in which three atoms share two electrons. The associated structural unit, the icosahedral B12 cluster, pervades the allotropic forms of boron. The same motif can be seen, as are deltahedral variants or fragments, in metal borides and hydride derivatives, and in some halides.
The bonding in boron has been described as being characteristic of behaviour intermediate between metals and nonmetallic covalent network solids (such as diamond). The energy required to transform B, C, N, Si and P from nonmetallic to metallic states has been estimated as 30, 100, 240, 33 and 50 kJ/mol, respectively. This indicates how close boron is to the metal-nonmetal borderline.
Most of the chemistry of boron is nonmetallic in nature. The small size of the boron atom enables the preparation of many interstitial alloy-type borides. Analogies between boron and transition metals have been noted in the formation of complexes, and adducts (for example, BH3 + CO →BH3CO and, similarly, Fe(CO)4 + CO →Fe(CO)5), as well as in the geometric and electronic structures of cluster species such as [B6H6]2– and [Ru6(CO)18]2–.[n 25] The aqueous chemistry of boron is characterised by the formation of many different polyborate anions. Given its high charge-to-size ratio, nearly all compounds of boron are covalent, with a few complexed anionic and cationic species. Boron has a strong affinity for oxygen and a duly extensive borate chemistry. The oxide B2O3 is polymeric in structure, weakly acidic, and a glass former. Organometallic compounds of boron[n 26] have been known since the 19th century (see organoboron chemistry).
Silicon is a crystalline solid with a blue-grey metallic lustre. Like boron, it is less dense (at 2.33 g/cm3) than aluminium, and is hard and brittle. It is a relatively unreactive element. According to Rochow, the massive crystalline form (especially if pure) is "remarkably inert to all acids, including hydrofluoric".[n 27] Less pure silicon, and the powdered form, are variously susceptible to attack by strong or heated acids, as well as by steam and fluorine. Silicon dissolves in hot aqueous alkalis with the evolution of hydrogen, as do metals such as beryllium, aluminium, zinc, gallium or indium. It melts at 1414 °C. Silicon is a semiconductor with an electrical conductivity of 10−4 S•cm−1 and a band gap of about 1.11 eV. When it melts, silicon becomes a reasonable metal with an electrical conductivity of 1.0–1.3 × 104 S•cm−1, similar to that of liquid mercury.
The chemistry of silicon is generally nonmetallic (covalent) in nature. It can form alloys with metals such as iron and copper. Silicon shows fewer tendencies to anionic behaviour than ordinary nonmetals. Its solution chemistry is characterised by the formation of oxyanions. The high strength of the silicon-oxygen bond dominates the chemical behaviour of silicon. Polymeric silicates, built up by tetrahedral SiO4 units sharing their oxygen atoms, are the most abundant and important compounds of silicon. The polymeric borates, comprising linked trigonal and tetrahedral BO3 or BO4 units, are built on similar structural principles. The oxide SiO2 is polymeric in structure, weakly acidic,[n 28] and a glass former. Traditional organometallic chemistry includes the carbon compounds of silicon (see organosilicon).
Germanium is a shiny grey-white solid. It has a density of 5.323 g/cm3 and is hard and brittle. It is mostly unreactive at room temperature[n 29] but is slowly attacked by hot concentrated sulfuric or nitric acid. Germanium also reacts with molten caustic soda to yield sodium germanate Na2GeO3 and hydrogen gas. It melts at 938 °C. Germanium is a semiconductor with an electrical conductivity of around 2 × 10−2 S•cm−1 and a band gap of 0.67 eV. Liquid germanium is a metallic conductor, with an electrical conductivity similar to that of liquid mercury.
Most of the chemistry of germanium is characteristic of a nonmetal. It can form alloys with metals such as aluminium and gold. Germanium shows fewer tendencies to anionic behaviour than ordinary nonmetals. Its solution chemistry is characterised by the formation of oxyanions. Germanium generally forms tetravalent (IV) compounds, and it can also form less stable divalent (II) compounds, in which it behaves more like a metal. Germanium analogues of all of the major types of silicates have been prepared. The metallic character of germanium is also suggested by the formation of various oxoacid salts. A phosphate [(HPO4)2Ge·H2O] and highly stable trifluoroacetate Ge(OCOCF3)4 have been described, as have Ge2(SO4)2, Ge(ClO4)4 and GeH2(C2O4)3. The oxide GeO2 is polymeric, amphoteric, and a glass former. The dioxide is soluble in acidic solutions (the monoxide GeO, is even more so), and this is sometimes used to classify germanium as a metal. Up to the 1930s germanium was considered to be a poorly conducting metal rather than a nonmetal. As with all the elements commonly recognised as metalloids, germanium has an established organometallic chemistry (see organogermanium chemistry).
Arsenic is a grey, metallic looking solid. It has a density of 5.727 g/cm3 and is brittle, and moderately hard (more than aluminium; less than iron). It is stable in dry air but develops a golden bronze patina in moist air, which blackens on further exposure. Arsenic is attacked by nitric acid and concentrated sulfuric acid. It reacts with fused caustic soda to give the arsenate Na3AsO3 and hydrogen gas. Arsenic sublimes at 615 °C. The vapour is lemon-yellow and smells like garlic. Arsenic only melts under a pressure of 38.6 atm, at 817 °C. It is a semimetal with an electrical conductivity of around 3.9 × 104 S•cm−1 and a band overlap of 0.5 eV.[n 30] Liquid arsenic is a semiconductor with a band gap of 0.15 eV.
The chemistry of arsenic is predominately nonmetallic. Its many metal alloys are mostly brittle. Arsenic shows fewer tendencies to anionic behaviour than ordinary nonmetals. Its solution chemistry is characterised by the formation of oxyanions. Arsenic generally forms compounds in which it has an oxidation state of +3 or +5. The halides, and the oxides and their derivatives are illustrative examples. In the trivalent state, arsenic shows some incipient metallic properties. The halides are hydrolysed by water but these reactions, particularly those of the chloride, are reversible with the addition of a hydrohalic acid. The oxide is acidic but, as noted below, (weakly) amphoteric. The higher, less stable, pentavalent state has strongly acidic (nonmetallic) properties. Compared to phosphorus, the stronger metallic character of arsenic is indicated by the formation of oxoacid salts such as AsPO4, As2(SO4)3[n 31] and arsenic acetate As(CH3COO)3. The oxide As2O3 is polymeric, amphoteric,[n 32] and a glass former. Arsenic has an extensive organometallic chemistry (see organoarsenic chemistry).
Antimony is a silver-white solid with a blue tint and a brilliant lustre. It has a density of 6.697 g/cm3 and is brittle, and moderately hard (more so than arsenic; less so than iron; about the same as copper). It is stable in air and moisture at room temperature. It is attacked by concentrated nitric acid, yielding the hydrated pentoxide Sb2O5. Aqua regia gives the pentachloride SbCl5 and hot concentrated sulfuric acid results in the sulfate Sb2(SO4)3. It is not affected by molten alkali. Antimony is capable of displacing hydrogen from water, when heated: 2 Sb + 3 H2O → Sb2O3 + 3 H2. It melts at 631 °C. Antimony is a semimetal whose electrical conductivity is around 3.1 × 104 S•cm−1 and a band overlap of 0.16 eV.[n 33] Liquid antimony is a metallic conductor with an electrical conductivity of around 5.3 × 104 S•cm−1.
Most of the chemistry of antimony is characteristic of a nonmetal. It can form alloys with one or more metals such as aluminium, iron, nickel, copper, zinc, tin, lead and bismuth. Antimony has fewer tendencies to anionic behaviour than ordinary nonmetals. Its solution chemistry is characterised by the formation of oxyanions. Like arsenic, antimony generally forms compounds in which it has an oxidation state of +3 or +5. The halides, and the oxides and their derivatives are illustrative examples. The +5 state is less stable than the +3, but relatively easier to attain than with arsenic. This is explained by the poor shielding afforded the arsenic nucleus by its 3d10 electrons. In comparison, the tendency of antimony to oxidize more easily partially offsets the effect of its 4d10 shell. Tripositive antimony is amphoteric; pentapositive antimony is (predominately) acidic. Consistent with an increase in metallic character down group 15, antimony forms salts or salt-like compounds including a nitrate Sb(NO3)3, phosphate SbPO4, sulfate Sb2(SO4)3 and perchlorate Sb(ClO4)3. The otherwise acidic pentoxide Sb2O5 shows some basic (metallic) behaviour in that it can be dissolved in very acidic solutions, with the formation of the oxycation SbO+
2. The oxide Sb2O3 is polymeric, amphoteric, and a glass former. Antimony has an extensive organometallic chemistry (see organoantimony chemistry).
Tellurium is a silvery-white shiny solid. It has a density of 6.24 g/cm3, is brittle, and is the softest of the commonly recognised metalloids, being marginally harder than sulfur. Large pieces of tellurium are stable in air. The finely powdered form is oxidized by air in the presence of moisture. Tellurium reacts with boiling water, or when freshly precipitated even at 50 °C, to give the dioxide and hydrogen: Te + 2 H2O → TeO2 + 2 H2. It reacts (to varying degrees) with nitric, sulfuric and hydrochloric acids to give compounds such as the sulfoxide TeSO3 or tellurous acid H2TeO3, the basic nitrate (Te2O4H)+(NO3)–, or the oxide sulfate Te2O3(SO4). It dissolves in boiling alkalis, to give the tellurite and telluride (chemistry): 3 Te + 6 KOH = K2TeO3 + 2 K2Te + 3 H2O, a reaction that proceeds or is reversible with increasing or decreasing temperature.
At higher temperatures tellurium is sufficiently plastic to extrude. It melts at 449.51 °C. Crystalline tellurium has a structure consisting of parallel infinite spiral chains. The bonding between adjacent atoms in a chain is covalent, but there is evidence of a weak metallic interaction between the neighbouring atoms of different chains. Tellurium is a semiconductor with an (intrinsic) electrical conductivity of around 1.0 S•cm−1 and a band gap of 0.32 to 0.38 eV. Liquid tellurium is a semiconductor, with an electrical conductivity, on melting, of around 1.9 × 103 S•cm−1 Superheated liquid tellurium is a metallic conductor.
Most of the chemistry of tellurium is characteristic of a nonmetal. It can form alloys with aluminium, silver and tin. Tellurium shows fewer tendencies to anionic behaviour than ordinary nonmetals. Its solution chemistry is characterised by the formation of oxyanions. Tellurium generally forms compounds in which it has an oxidation state of −2, +4 or +6. The +4 state is the most stable. Tellurides of composition XxTey are easily formed with most other elements and represent the most common tellurium minerals. Nonstoichiometry is pervasive, especially with transition metals. Many tellurides can be regarded as metallic alloys. The increase in metallic character evident in tellurium, as compared to the lighter chalcogens, is further reflected in the reported formation of various other oxyacid salts, such as a basic selenate 2TeO2·SeO3 and an analogous perchlorate and periodate 2TeO2·HXO4. Tellurium forms a polymeric, amphoteric, glass-forming oxide TeO2. The latter is a 'conditional' glass-forming oxide—it forms a glass with a very small amount of additive. Tellurium has an extensive organometallic chemistry (see organotellurium chemistry).
Elements less commonly recognised as metalloids
Carbon is ordinarily classified as a nonmetal but has some metallic properties and is occasionally classified as a metalloid. Hexagonal graphitic carbon (graphite) is the most thermodynamically stable allotrope of carbon under ambient conditions. It has a lustrous appearance and is a fairly good electrical conductor. Graphite has a layered structure. Each layer comprises carbon atoms bonded to three other carbon atoms in a honeycomb lattice arrangement. The layers are stacked together and held loosely by van der Waals forces and delocalized valence electrons.
Like a metal, the conductivity of graphite in the direction of its planes decreases as the temperature is raised;[n 34] it has the electronic band structure of a semimetal. The allotropes of carbon, including graphite, can accept foreign atoms or compounds into their structures via substitution, intercalation or doping. The resulting materials are referred to as 'carbon alloys'. Carbon can form ionic salts, including a hydrogen sulfate, perchlorate, and nitrate (C+
24X–.2HX, where X = HSO4, ClO4; and C+
3.3HNO3).[n 35] In organic chemistry, carbon can form complex cations—termed carbocations—in which the positive charge is on the carbon atom; examples are CH+
3 and CH+
5, and their derivatives.
Carbon is brittle, and behaves as a semiconductor in a direction perpendicular to its planes. Most of its chemistry is nonmetallic; it has a relatively high ionization energy and, compared to most metals, a relatively high electronegativity. Carbon can form anions such as C4– (methanide), C2–
2 (acetylide) and C3–
4 (sesquicarbide or allylenide), in compounds with metals of main groups 1–3, and with the lanthanides and actinides. Its oxide CO2 forms carbonic acid H2CO3.[n 36]
Aluminium is ordinarily classified as a metal. It is lustrous, malleable and ductile, and has high electrical and thermal conductivity. Like most metals it has a close-packed crystalline structure, and forms a cation in aqueous solution.
It has some properties that are unusual for a metal; taken together, these are sometimes used as a basis to classify aluminium as a metalloid. Its crystalline structure shows some evidence of directional bonding. Aluminium bonds covalently in most compounds. The oxide Al2O3 is amphoteric, and a conditional glass-former. Aluminium can form anionic aluminates, such behaviour being considered nonmetallic in character.
Classifying aluminium as a metalloid has been disputed given its many metallic properties. It is therefore, arguably, an exception to the mnemonic that elements adjacent to the metal-nonmetal dividing line are metalloids.[n 37]
Stott labels aluminium as a weak metal. It has the physical properties of a metal but some of the chemical properties of a nonmetal. Steele notes the paradoxical chemical behaviour of aluminium: "It resembles a weak metal in its amphoteric oxide and in the covalent character of many of its compounds ... Yet it is a highly electropositive metal ... [with] a high negative electrode potential".
Its most stable form, the grey trigonal allotrope, is sometimes called 'metallic' selenium because its electrical conductivity is several orders of magnitude greater than that of the red monoclinic form. The metallic character of selenium is further shown by its lustre and its crystalline structure, the latter of which is thought to include weakly 'metallic' interchain bonding. Selenium can be drawn into thin threads when molten. It shows reluctance to acquire "the high positive oxidation numbers characteristic of nonmetals". It can form cyclic polycations (such as Se2+
8) when dissolved in oleums (an attribute it shares with sulfur and tellurium), and a hydrolysed cationic salt in the form of trihydroxoselenium (IV) perchlorate [Se(OH)3]+·ClO–
The nonmetallic character of selenium is shown by its brittleness and the low electrical conductivity (~10−9 to 10−12 S•cm−1) of its highly purified form. This is comparable to or less than that of bromine (7.95×10–12 S•cm−1), a nonmetal. Selenium has the electronic band structure of a semiconductor and retains its semiconducting properties in liquid form. It has a relatively high electronegativity (2.55 revised Pauling scale). Its reaction chemistry is mainly that of its nonmetallic anionic forms Se2–, SeO2−
3 and SeO2−
Selenium is commonly described as a metalloid in the environmental chemistry literature. It moves through the aquatic environment similarly to arsenic and antimony; its water-soluble salts, in higher concentrations, have a similar toxicological profile to that of arsenic.
Polonium is "distinctly metallic" in some ways. Both of its allotropic forms are metallic conductors. It is soluble in acids, forming the rose-coloured Po2+ cation and displacing hydrogen: Po + 2 H+ → Po2+ + H2. Many polonium salts are known. The oxide PoO2 is predominantly basic in nature. Polonium is a reluctant oxidizing agent, unlike its lighter congener oxygen: highly reducing conditions are required for the formation of the Po2– anion in aqueous solution.
Whether polonium is ductile or brittle is unclear. It is predicted to be ductile based on its calculated elastic constants. It has a simple cubic crystalline structure. Such a structure has few slip systems and "leads to very low ductility and hence low fracture resistance".
Polonium shows nonmetallic character in its halides, and by the existence of polonides. The halides have properties generally characteristic of nonmetal halides (being volatile, easily hydrolyzed, and soluble in organic solvents). Many metal polonides, obtained by heating the elements together at 500–1,000 °C, and containing the Po2– anion, are also known.
As a halogen, astatine tends to be classified as a nonmetal. It has some marked metallic properties and is sometimes instead classified as either a metalloid or (less often) as a metal.[n 39] Immediately following its production in 1940, early investigators considered it a metal. In 1949 it was called the most noble (difficult to reduce) nonmetal as well as being a relatively noble (difficult to oxidize) metal. In 1950 astatine was described as a halogen and (therefore) a reactive nonmetal. In 2013, on the basis of relativistic modelling, astatine was predicted to be a monatomic metal, with a face-centred cubic crystalline structure.
Several authors have commented on the metallic nature of some of the properties of astatine. Since iodine is a semiconductor in the direction of its planes, and since the halogens become more metallic with increasing atomic number, it has been presumed that astatine would be a metal if it could form a condensed phase.[n 40] Astatine may be metallic in the liquid state on the basis that elements with an enthalpy of vaporization (EoV) greater than ~42 kJ/mol are metallic when liquid. Such elements include boron,[n 41] silicon, germanium, antimony, selenium and tellurium. Estimated values for the EoV of diatomic astatine are 50 kJ/mol or higher; diatomic iodine, with an EoV of 41.71, falls just short of the threshold figure.
"Like typical metals, it [astatine] is precipitated by hydrogen sulfide even from strongly acid solutions and is displaced in a free form from sulfate solutions; it is deposited on the cathode on electrolysis."[n 42] Further indications of a tendency for astatine to behave like a (heavy) metal are: "... the formation of pseudohalide compounds ... complexes of astatine cations ... complex anions of trivalent astatine ... as well as complexes with a variety of organic solvents". It has also been argued that astatine demonstrates cationic behaviour, by way of stable At+ and AtO+ forms, in strongly acidic aqueous solutions.
Some of astatine's reported properties are nonmetallic. It has the narrow liquid range ordinarily associated with nonmetals (mp 302 °C; bp 337 °C). Batsanov gives a calculated band gap energy for astatine of 0.7 eV; this is consistent with nonmetals (in physics) having separated valence and conduction bands and thereby being either semiconductors or insulators. The chemistry of astatine in aqueous solution is mainly characterised by the formation of various anionic species. Most of its known compounds resemble those of iodine, which is a halogen and a nonmetal. Such compounds include astatides (XAt), astatates (XAtO3), and monovalent interhalogen compounds.
Restrepo et al. reported that astatine appeared to be more polonium-like than halogen-like. They did so on the basis of detailed comparative studies of the known and interpolated properties of 72 elements.
In the periodic table, some of the elements adjacent to the commonly recognised metalloids, although usually classified as either metals or nonmetals, are occasionally referred to as near-metalloids or noted for their metalloidal character. To the left of the metal-nonmetal dividing line, such elements include gallium, tin and bismuth. They show unusual packing structures, marked covalent chemistry (molecular or polymeric), and amphoterism. To the right of the dividing line are carbon, phosphorus, selenium and iodine. They exhibit metallic lustre, semiconducting properties[n 44] and bonding or valence bands with delocalized character. This applies to their most thermodynamically stable forms under ambient conditions: carbon as graphite; phosphorus as black phosphorus;[n 45] and selenium as grey selenium.
Different crystalline forms of an element are called allotropes. Some allotropes, particularly those of elements located (in periodic table terms) alongside or near the notional dividing line between metals and nonmetals, exhibit more pronounced metallic, metalloidal or nonmetallic behaviour than others. The existence of such allotropes can complicate the classification of the elements involved.
Tin, for example, has two allotropes: tetragonal 'white' β-tin and cubic 'grey' α-tin. White tin is a very shiny, ductile and malleable metal. It is the stable form at or above room temperature and has an electrical conductivity of 9.17×104 S·cm−1 (~1/6th that of copper). Grey tin usually has the appearance of a grey micro-crystalline powder, and can also be prepared in brittle semi-lustrous crystalline or polycrystalline forms. It is the stable form below 13.2 °C and has an electrical conductivity of between (2–5)×102 S·cm−1 (~1/250th that of white tin). Grey tin has the same crystalline structure as that of diamond. It behaves as a semiconductor (with a band gap of 0.08 eV), but has the electronic band structure of a semimetal. It has been referred to as either a very poor metal, a metalloid, a nonmetal or a near metalloid.
The diamond allotrope of carbon is clearly nonmetallic, being translucent and having a low electrical conductivity of 10−14 to 10−16 S·cm−1. Graphite has an electrical conductivity of 3×104 S·cm−1, a figure more characteristic of a metal. Phosphorus, sulfur, arsenic, selenium, antimony and bismuth also have less stable allotropes that display different behaviours.
Abundance, extraction and cost
The table gives crustal abundances of the elements commonly to rarely recognised as metalloids. Some other elements are included for comparison: oxygen and xenon (the most and least abundant elements with stable isotopes); iron and the coinage metals copper, silver and gold; and rhenium, the least abundant stable metal (aluminium is normally the most abundant metal). Various abundance estimates have been published; these often disagree to some extent.
The recognised metalloids can be obtained by chemical reduction of either their oxides or their sulfides. Simpler or more complex extraction methods may be employed depending on the starting form and economic factors. Boron is routinely obtained by reducing the trioxide with magnesium: B2O3 + 3 Mg → 2 B + 3MgO; after secondary processing the resulting brown powder has a purity of up to 97%. Boron of higher purity (> 99%) is prepared by heating volatile boron compounds, such as BCl3 or BBr3, either in a hydrogen atmosphere (2 BX3 + 3 H2 → 2 B + 6 HX) or to the point of thermal decomposition. Silicon and germanium are obtained from their oxides by heating the oxide with carbon or hydrogen: SiO2 + C → Si + CO2; GeO2 + 2 H2 → Ge + 2 H2O. Arsenic is isolated from its pyrite (FeAsS) or arsenical pyrite (FeAs2) by heating; alternatively, it can be obtained from its oxide by reduction with carbon: 2 As2O3 + 3 C → 2 As + 3 CO2. Antimony is derived from its sulfide by reduction with iron: Sb2S3 → 2 Sb + 3 FeS. Tellurium is prepared from its oxide by dissolving it in aqueous NaOH, yielding tellurite, then by electrolytic reduction: TeO2 + 2 NaOH → Na2TeO3 + H2O; Na2TeO3 + H2O → Te + 2 NaOH + O2. Another option is reduction of the oxide by roasting with carbon: TeO2 + C → Te + CO2.
Production methods for the elements less frequently recognised as metalloids involve natural processing, electrolytic or chemical reduction, or irradiation. Carbon (as graphite) occurs naturally and is extracted by crushing the parent rock and floating the lighter graphite to the surface. Aluminium is extracted by dissolving its oxide Al2O3 in molten cryolite Na3AlF6 and then by high temperature electrolytic reduction. Selenium is produced by roasting its coinage metal selenides X2Se (X = Cu, Ag, Au) with soda ash to give the selenite: X2Se + O2 + Na2CO3 → Na2SeO3 + 2 X + CO2; the selenide is neutralized by sulfuric acid H2SO4 to give selenous acid H2SeO3; this is reduced by bubbling with SO2 to yield elemental selenium. Polonium and astatine are produced in minute quantities by irradiating bismuth.
The recognised metalloids and their closer neighbours mostly cost less than silver; only polonium and astatine are more expensive than gold. As of 5 April 2014, prices for small samples (up to 100 g) of silicon, antimony and tellurium, and graphite, aluminium and selenium, average around one third the cost of silver (US$1.5 per gram or about $45 an ounce). Boron, germanium and arsenic samples average about three-and-a-half times the cost of silver.[n 46] Polonium is available for about $100 per microgram, which is $100,000,000 a gram. Zalutsky and Pruszynski estimate a similar cost for producing astatine. Prices for the applicable elements traded as commodities tend to range from two to three times cheaper than the sample price (Ge), to nearly three thousand times cheaper (As).[n 47]
- See also Vernon, for a related commentary.
- Definitions and extracts by different authors, illustrating aspects of the generic definition, follow:
- "In chemistry a metalloid is an element with properties intermediate between those of metals and nonmetals."
- "Between the metals and nonmetals in the periodic table we find elements ... [that] share some of the characteristic properties of both the metals and nonmetals, making it difficult to place them in either of these two main categories."
- "Chemists sometimes use the name metalloid ... for these elements which are difficult to classify one way or the other."
- "Because the traits distinguishing metals and nonmetals are qualitative in nature, some elements do not fall unambiguously in either category. These elements ... are called metalloids ..."
- Gold, for example, has mixed properties but is still recognised as "king of metals". Besides metallic behaviour (such as high electrical conductivity, and cation formation), gold shows nonmetallic behaviour:
- It has the highest electrode potential.
- It has the third-highest ionization energy among the metals (after zinc and mercury).
- It has the lowest electron affinity.
- Its electronegativity of 2.54 is highest among the metals and exceeds that of some nonmetals (hydrogen 2.2; phosphorus 2.19; and radon 2.2).
- It forms the Au– auride anion, acting in this way like a halogen.
- It sometimes has a tendency, known as 'aurophilicity', to bond to itself.
- Mann et al. refer to these elements as "the recognized metalloids".
- Jones writes: "Though classification is an essential feature in all branches of science, there are always hard cases at the boundaries. Indeed the boundary of a class is rarely sharp."
- The lack of a standard division of the elements into metals, metalloids and nonmetals is not necessarily an issue. There is more or less a continuous progression from the metallic to the nonmetallic. A specified subset of this continuum can potentially serve its particular purpose as well as any other.
- The packing efficiency of boron is 38%; silicon and germanium 34; arsenic 38.5; antimony 41; and tellurium 36.4. These values are lower than in most metals (80% of which have a packing efficiency of at least 68%) but higher than those of elements usually classified as nonmetals. (Gallium is unusual, for a metal, in having a packing efficiency of just 39%. Other notable values for metals are 42.9 for bismuth and 58.5 for liquid mercury.) Packing efficiencies for nonmetals are: graphite 17%, sulfur 19.2, iodine 23.9, selenium 24.2, and black phosphorus 28.5.
- More specifically, the Goldhammer-Herzfeld criterion is the ratio of the force holding an individual atom's valence electrons in place with the forces on the same electrons from interactions between the atoms in the solid or liquid element. When the interatomic forces are greater than or equal to the atomic force, valence electron itinerancy is indicated and metallic behaviour is predicted. Otherwise nonmetallic behaviour is anticipated.
- As the ratio is based on classical arguments it does not accommodate the finding that polonium, which has a value of ~0.95, adopts a metallic (rather than covalent) crystalline structure, on relativistic grounds. Even so it offers a first order rationalization for the occurrence of metallic character amongst the elements.
- Atomic conductance is the electrical conductivity of one mole of a substance. It is equal to electrical conductivity divided by molar volume.
- Selenium has an ionization energy (IE) of 225 kcal/mol (941 kJ/mol) and is sometimes described as a semiconductor. It has a relatively high 2.55 electronegativity (EN). Polonium has an IE of 194 kcal/mol (812 kJ/mol) and a 2.0 EN, but has a metallic band structure. Astatine has an IE of 215 kJ/mol (899 kJ/mol) and an EN of 2.2. Its electronic band structure is not known with any certainty.
- Some authors only recognize elements as either metals or nonmetals.
- Oderberg argues on ontological grounds that anything not a metal is therefore a nonmetal, and that this includes semi-metals (i.e. metalloids).
- Copernicium is reportedly the only metal known to be a gas at room temperature.
- Metals have electrical conductivity values of from 6.9 × 103 S•cm−1 for manganese to 6.3 × 105 for silver.
- Metalloids have electrical conductivity values of from 1.5 × 10−6 S•cm−1 for boron to 3.9 × 104 for arsenic. If selenium is included as a metalloid the applicable conductivity range would start from ~10−9 to 10−12 S•cm−1.
- Nonmetals have electrical conductivity values of from ~10−18 S•cm−1 for the elemental gases to 3 × 104 in graphite.
- Chedd defines metalloids as having electronegativity values of 1.8 to 2.2 (Allred-Rochow scale). He included boron, silicon, germanium, arsenic, antimony, tellurium, polonium and astatine in this category. In reviewing Chedd's work, Adler described this choice as arbitrary, as other elements whose electronegativities lie in this range include copper, silver, phosphorus, mercury and bismuth. He went on to suggest defining a metalloid as "a semiconductor or semimetal" and to include bismuth and selenium in this category.
- Olmsted and Williams commented that, "Until quite recently, chemical interest in the metalloids consisted mainly of isolated curiosities, such as the poisonous nature of arsenic and the mildly therapeutic value of borax. With the development of metalloid semiconductors, however, these elements have become among the most intensely studied".
- Research published in 2012 suggests that metal-metalloid glasses can be characterised by an interconnected atomic packing scheme in which metallic and covalent bonding structures coexist.
- The reaction involved is Ge + 2 MoO3 → GeO2 + 2 MoO2. Adding arsenic or antimony (n-type electron donors) increases the rate of reaction; adding gallium or indium (p-type electron acceptors) decreases it.
- Ellern, writing in Military and Civilian Pyrotechnics (1968), comments that carbon black 'has been specified for and used in a nuclear air-burst simulator.'
- For a post-1960 example of the former use of the term metalloid to refer to nonmetals see Zhdanov, who divides the elements into metals; intermediate elements (H, B, C, Si, Ge, Se, Te); and metalloids (of which the most typical are given as O, F and Cl).
- Boron, at 1.56 eV, has the largest band gap amongst the commonly recognised (semiconducting) metalloids. Of nearby elements in periodic table terms, selenium has the next highest band gap (close to 1.8 eV) followed by white phosphorus (around 2.1 eV).
- On the analogy between boron and metals, Greenwood commented that: "The extent to which metallic elements mimic boron (in having fewer electrons than orbitals available for bonding) has been a fruitful cohering concept in the development of metalloborane chemistry ... Indeed, metals have been referred to as 'honorary boron atoms' or even as 'flexiboron atoms'. The converse of this relationship is clearly also valid ..."
- Organic derivatives of metalloids are traditionally counted as organometallic compounds.
- In air, silicon forms a thin coating of amorphous silicon dioxide, 2 to 3 nm thick. This coating is dissolved by hydrogen fluoride at a very low pace—on the order of two to three hours per nanometre. Silicon dioxide, and silicate glasses (of which silicon dioxide is a major component), are otherwise readily attacked by hydrofluoric acid.
- Although SiO2 is classified as an acidic oxide, and hence reacts with alkalis to give silicates, it reacts with phosphoric acid to yield a silicon oxide orthophosphate Si5O(PO4)6, and with hydrofluoric acid to give hexafluorosilicic acid H2SiF6. The latter reaction "is sometimes quoted as evidence of basic [that is, metallic] properties".
- Temperatures above 400 °C are required to form a noticeable surface oxide layer.
- Arsenic also exists as a naturally occurring (but rare) allotrope (arsenolamprite), a crystalline semiconductor with a band gap of around 0.3 eV or 0.4 eV. It can also be prepared in a semiconducting amorphous form, with a band gap of around 1.2–1.4 eV.
- The formulae of AsPO4 and As2(SO4)3 suggest straightforward ionic formulations, with As3+, but compounds in which arsenic is present as a cation are extremely rare. AsPO4, "which is virtually a covalent oxide", has been referred to as a double oxide, of the form As2O3·P2O5. It comprises AsO3 pyramids and PO4 tetrahedra, joined together by all their corner atoms to form a continuous polymeric network. As2(SO4)3 has a structure in which each SO4 tetrahedron is bridged by two AsO3 trigonal pyramida.
- As2O3 is usually regarded as being amphoteric but a few sources say it is (weakly) acidic. They describe its "basic" properties (its reaction with concentrated hydrochloric acid to form arsenic trichloride) as being alcoholic, in analogy with the formation of covalent alkyl chlorides by covalent alcohols (e.g., R-OH + HCl → RCl + H2O)
- Antimony can also be prepared in an amorphous semiconducting black form, with an estimated (temperature-dependent) band gap of 0.06–0.18 eV.
- Liquid carbon may or may not be a metallic conductor, depending on pressure and temperature; see also.
- For the sulfate, the method of preparation is (careful) direct oxidation of graphite in concentrated sulfuric acid by an oxidising agent, such as nitric acid, chromium trioxide or ammonium persulfate; in this instance the concentrated sulfuric acid is acting as an inorganic nonaqueous solvent.
- Only a small fraction of dissolved CO2 is present in water as carbonic acid so, even though H2CO3 is a medium-strong acid, solutions of carbonic acid are only weakly acidic.
- A mnemonic that captures the elements commonly recognised as metalloids goes: Up, up-down, up-down, up ... are the metalloids!
- Rochow, who later wrote his 1966 monograph The metalloids, commented that, "In some respects selenium acts like a metalloid and tellurium certainly does".
- A further option is to include astatine both as a nonmetal and as a metalloid.
- A visible piece of astatine would be immediately and completely vaporized because of the heat generated by its intense radioactivity.
- The literature is contradictory as to whether boron exhibits metallic conductivity in liquid form. Krishnan et al. found that liquid boron behaved like a metal. Glorieux et al. characterised liquid boron as a semiconductor, on the basis of its low electrical conductivity. Millot et al. reported that the emissivity of liquid boron was not consistent with that of a liquid metal.
- Korenman similarly noted that "the ability to precipitate with hydrogen sulfide distinguishes astatine from other halogens and brings it closer to bismuth and other heavy metals".
- The separation between molecules in the layers of iodine (350 pm) is much less than the separation between iodine layers (427 pm; cf. twice the van der Waals radius of 430 pm). This is thought to be caused by electronic interactions between the molecules in each layer of iodine, which in turn give rise to its semiconducting properties and shiny appearance.
- For example: intermediate electrical conductivity; a relatively narrow band gap; light sensitivity.
- White phosphorus is the least stable and most reactive form. It is also the most common, industrially important, and easily reproducible allotrope, and for these three reasons is regarded as the standard state of the element.
- Sample prices of gold, in comparison, start at roughly thirty-five times that of silver. Based on sample prices for B, C, Al, Si, Ge, As, Se, Ag, Sb, Te and Au available on-line from Alfa Aesa; Goodfellow; Metallium; and United Nuclear Scientific.
- Based on spot prices for Al, Si, Ge, As, Sb, Se, and Te available on-line from FastMarkets: Minor Metals; Fast Markets: Base Metals; EnergyTrend: PV Market Status, Polysilicon; and Metal-Pages: Arsenic metal prices, news and information.
- Vernon 2013
- Haller 2006, p. 3
- Chedd 1969, pp. 58, 78; National Research Council 1984, p. 43
- Atkins et al. 2010, p. 20
- Cusack 1987, p. 360
- Kelter, Mosher & Scott 2009, p. 268
- Hill & Holman 2000, p. 41
- King 1979, p. 13
- Moore 2011, p. 81
- Gray 2010
- Hopkins & Bailar 1956, p. 458
- Glinka 1965, p. 77
- Wiberg 2001, p. 1279
- Belpassi et al. 2006, pp. 4543–4
- Schmidbaur & Schier 2008, pp. 1931–51
- Tyler Miller 1987, p. 59
- Goldsmith 1982, p. 526; Kotz, Treichel & Weaver 2009, p. 62; Bettelheim et al. 2010, p. 46
- Mann et al. 2000, p. 2783
- Hawkes 2001, p. 1686; Segal 1989, p. 965; McMurray & Fay 2009, p. 767
- Bucat 1983, p. 26; Brown c. 2007
- Swift & Schaefer 1962, p. 100
- Hawkes 2001, p. 1686; Hawkes 2010; Holt, Rinehart & Wilson c. 2007
- Dunstan 1968, pp. 310, 409. Dunstan lists Be, Al, Ge (maybe), As, Se (maybe), Sn, Sb, Te, Pb, Bi and Po as metalloids (pp. 310, 323, 409, 419).
- Tilden 1876, pp. 172, 198–201; Smith 1994, p. 252; Bodner & Pardue 1993, p. 354
- Bassett et al. 1966, p. 127
- Rausch 1960
- Thayer 1977, p. 604; Warren & Geballe 1981; Masters & Ela 2008, p. 190
- Warren & Geballe 1981; Chalmers 1959, p. 72; US Bureau of Naval Personnel 1965, p. 26
- Siebring 1967, p. 513
- Wiberg 2001, p. 282
- Rausch 1960; Friend 1953, p. 68
- Murray 1928, p. 1295
- Hampel & Hawley 1966, p. 950; Stein 1985; Stein 1987, pp. 240, 247–8
- Hatcher 1949, p. 223; Secrist & Powers 1966, p. 459
- Taylor 1960, p. 614
- Considine & Considine 1984, p. 568; Cegielski 1998, p. 147; The American heritage science dictionary 2005 p. 397
- Woodward 1948, p. 1
- NIST 2010. Values shown in the above table have been converted from the NIST values, which are given in eV.
- Berger 1997; Lovett 1977, p. 3
- Goldsmith 1982, p. 526; Hawkes 2001, p. 1686
- Hawkes 2001, p. 1687
- Sharp 1981, p. 299
- Emsley 1971, p. 1
- James et al. 2000, p. 480
- Chatt 1951, p. 417: "The boundary between metals and metalloids is indefinite ..."; Burrows et al. 2009, p. 1192: "Although the elements are conveniently described as metals, metalloids, and nonmetals, the transitions are not exact ..."
- Jones 2010, p. 170
- Kneen, Rogers & Simpson 1972, pp. 218–220
- Rochow 1966, pp. 1, 4–7
- Rochow 1977, p. 76; Mann et al. 2000, p. 2783
- Askeland, Phulé & Wright 2011, p. 69
- Van Setten et al. 2007, pp. 2460–1; Russell & Lee 2005, p. 7 (Si, Ge); Pearson 1972, p. 264 (As, Sb, Te; also black P)
- Russell & Lee 2005, p. 1
- Russell & Lee 2005, pp. 6–7, 387
- Pearson 1972, p. 264
- Okakjima & Shomoji 1972, p. 258
- Kitaĭgorodskiĭ 1961, p. 108
- Neuburger 1936
- Edwards & Sienko 1983, p. 693
- Herzfeld 1927; Edwards 2000, pp. 100–3
- Edwards & Sienko 1983, p. 695; Edwards et al. 2010
- Edwards 1999, p. 416
- Steurer 2007, p. 142; Pyykkö 2012, p. 56
- Edwards & Sienko 1983, p. 695
- Hill & Holman 2000, p. 41. They characterise metalloids (in part) on the basis that they are "poor conductors of electricity with atomic conductance usually less than 10−3 but greater than 10−5 ohm−1 cm−4".
- Bond 2005, p. 3: "One criterion for distinguishing semi-metals from true metals under normal conditions is that the bulk coordination number of the former is never greater than eight, while for metals it is usually twelve (or more, if for the body-centred cubic structure one counts next-nearest neighbours as well)."
- Jones 2010, p. 169
- Masterton & Slowinski 1977, p. 160 list B, Si, Ge, As, Sb and Te as metalloids, and comment that Po and At are ordinarily classified as metalloids but add that this is arbitrary as so little is known about them.
- Kraig, Roundy & Cohen 2004, p. 412; Alloul 2010, p. 83
- Vernon 2013, pp. 1704
- Hamm 1969, p. 653
- Horvath 1973, p. 336
- Gray 2009, p. 9
- Rayner-Canham 2011
- Booth & Bloom 1972, p. 426; Cox 2004, pp. 17, 18, 27–8; Silberberg 2006, p. 305–13
- Cox 2004, pp. 17–18, 27–8; Silberberg 2006, p. 305–13
- Rodgers 2011, pp. 232–3; 240–1
- Roher 2001, pp. 4–6
- Tyler 1948, p. 105; Reilly 2002, pp. 5–6
- Hampel & Hawley 1976, p. 174
- Goodrich 1844, p. 264; The Chemical News 1897, p. 189; Hampel & Hawley 1976, p. 191; Lewis 1993, p. 835; Hérold 2006, pp. 149–50
- Oderberg 2007, p. 97
- Brown & Holme 2006, p. 57
- Wiberg 2001, p. 282; Simple Memory Art c. 2005
- Chedd 1969, pp. 12–13
- Kneen, Rogers & Simpson, 1972, p. 263. Columns 2 and 4 are sourced from this reference unless otherwise indicated.
- Stoker 2010, p. 62; Chang 2002, p. 304. Chang speculates that the melting point of francium would be about 23 °C.
- New Scientist 1975; Soverna 2004; Eichler et al. 2007; Austen 2012
- Rochow 1966, p. 4
- Hunt 2000, p. 256
- McQuarrie & Rock 1987, p. 85
- Desai, James & Ho 1984, p. 1160; Matula 1979, p. 1260
- Choppin & Johnsen 1972, p. 351
- Schaefer 1968, p. 76; Carapella 1968, p. 30
- Kozyrev 1959, p. 104; Chizhikov & Shchastlivyi 1968, p. 25; Glazov, Chizhevskaya & Glagoleva 1969, p. 86
- Bogoroditskii & Pasynkov 1967, p. 77; Jenkins & Kawamura 1976, p. 88
- Hampel & Hawley 1976, p. 191; Wulfsberg 2000, p. 620
- Swalin 1962, p. 216
- Bailar et al. 1989, p. 742
- Metcalfe, Williams & Castka 1974, p. 86
- Chang 2002, p. 306
- Pauling 1988, p. 183
- Chedd 1969, pp. 24–5
- Adler 1969, pp. 18–19
- Hultgren 1966, p. 648; Young & Sessine 2000, p. 849; Bassett et al. 1966, p. 602
- Rochow 1966, p. 4; Atkins et al. 2006, pp. 8, 122–3
- Russell & Lee 2005, pp. 421, 423; Gray 2009, p. 23
- Olmsted & Williams 1997, p. 975
- Russell & Lee 2005, p. 401; Büchel, Moretto & Woditsch 2003, p. 278
- Desch 1914, p. 86
- Phillips & Williams 1965, p. 620
- Van der Put 1998, p. 123
- Klug & Brasted 1958, p. 199
- Good et al. 1813
- Sequeira 2011, p. 776
- Gary 2013
- Russell & Lee 2005, pp. 423–4; 405–6
- Davidson & Lakin 1973, p. 627
- Wiberg 2001, p. 589
- Greenwood & Earnshaw 2002, p. 749; Schwartz 2002, p. 679
- Antman 2001
- Řezanka & Sigler 2008; Sekhon 2012
- Emsley 2001, p. 67
- Zhang et al. 2008, p. 360
- Science Learning Hub 2009
- Skinner et al. 1979; Tom, Elden & Marsh 2004, p. 135
- Büchel 1983, p. 226
- Emsley 2001, p. 391
- Schauss 1991; Tao & Bolger 1997
- Eagleson 1994, p. 450; EVM 2003, pp. 197‒202
- Nielsen 1998
- Jaouen & Gibaud 2010
- Stevens & Klarner, p. 205
- Sneader 2005, pp. 57–59
- Keall, Martin and Tunbridge 1946
- Emsley 2001, p. 426
- Oldfield et al. 1974, p. 65; Turner 2011
- Ba et al. 2010; Daniel-Hoffmann, Sredni & Nitzan 2012; Molina-Quiroz et al. 2012
- Peryea 1998
- Hager 2006, p. 299
- Apseloff 1999
- Trivedi, Yung & Katz 2013, p. 209
- Emsley 2001, p. 382; Burkhart, Burkhart & Morrell 2011
- Thomas, Bialek & Hensel 2013, p. 1
- Le Bras, Wilkie & Bourbigot 2005, p. v
- Wilkie & Morgan 2009, p. 187
- Locke et al. 1956, p. 88
- Carlin 2011, p. 6.2
- Evans 1993, pp. 257–8
- Corbridge 2013, p. 1149
- Kaminow & Li 2002, p. 118
- Deming 1925, pp. 330 (As2O3), 418 (B2O3; SiO2; Sb2O3); Witt & Gatos 1968, p. 242 (GeO2)
- Eagleson 1994, p. 421 (GeO2); Rothenberg 1976, 56, 118–19 (TeO2)
- Geckeler 1987, p. 20
- Kreith & Goswami 2005, p. 12–109
- Russell & Lee 2005, p. 397
- Butterman & Jorgenson 2005, pp. 9–10
- Shelby 2005, p. 43
- Butterman & Carlin 2004, p. 22; Russell & Lee 2005, p. 422
- Träger 2007, pp. 438, 958; Eranna 2011, p. 98
- Rao 2002, p. 552; Löffler, Kündig & Dalla Torre 2007, p. 17–11
- Guan et al. 2012; WPI-AIM 2012
- Klement, Willens & Duwez 1960; Wanga, Dongb & Shek 2004, p. 45
- Demetriou et al 2011; Oliwenstein 2011
- Karabulut et al. 2001, p. 15; Haynes 2012, p. 4–26
- Schwartz 2002, pp. 679–680
- Carter & Norton 2013, p. 403
- Maeder 2013, pp. 3, 9–11
- Tominaga 2006, p. 327–8; Chung 2010, p. 285–6; Kolobov & Tominaga 2012, p. 149
- Ordnance Office 1863, p. 293
- Kosanke 2002, p. 110
- Ellern 1968, pp. 246, 326–7
- Conkling & Mocella 2010, p. 82
- Crow 2011; DailyRecord 2014
- Schwab & Gerlach 1967; Yetter 2012, pp. 81; Lipscomb 1972, pp. 2–3, 5–6, 15
- Ellern 1968, p. 135; Weingart 1947, p. 9
- Conkling & Mocella 2010, p. 83
- Conkling & Mocella 2010, pp. 181, 213
- Ellern 1968, pp. 209–10; 322
- Russell 2009, pp. 15, 17, 41, 79–80
- Ellern 1968, p. 324
- Ellern 1968, p. 328
- Conkling & Mocella 2010, p. 171
- Conkling & Mocella 2011, pp. 83–4
- Berger 1997, p. 91; Hampel 1968, passim
- Rochow 1966, p. 41; Berger 1997, pp. 42–3
- Bomgardner 2013, p. 20
- Russell & Lee 2005, p. 395; Brown et al. 2009, p. 489
- Haller 2006, p. 4: "The study and understanding of the physics of semiconductors progressed slowly in the 19th and early 20th centuries ... Impurities and defects ... could not be controlled to the degree necessary to obtain reproducible results. This led influential physicists, including W. Pauli and I. Rabi, to comment derogatorily on the 'Physics of Dirt'."; Hoddeson 2007, pp. 25–34 (29)
- Bianco et. al. 2013
- University of Limerick 2014; Kennedy et al. 2014
- Lee et al. 2014
- Russell & Lee 2005, pp. 421–2, 424
- He et al. 2014
- Berger 1997, p. 91
- ScienceDaily 2012
- Reardon 2005; Meskers, Hagelüken & Van Damme 2009, p. 1131
- The Economist 2012
- Whitten 2007, p. 488
- Jaskula 2013
- German Energy Society 2008, p. 43–44
- Patel 2012, p. 248
- Oxford English Dictionary 1989, 'metalloid'; Gordh, Gordh & Headrick 2003, p. 753
- Foster 1936, pp. 212–13; Brownlee et al. 1943, p. 293
- Calderazzo, Ercoli & Natta 1968, p. 257
- Klemm 1950, pp. 133–42; Reilly 2004, p. 4
- Walters 1982, pp. 32–3
- Tyler 1948, p. 105
- Foster & Wrigley 1958, p. 218: 'The elements may be grouped into two classes: those that are metals and those that are nonmetals. There is also an intermediate group known variously as metalloids, meta-metals, semiconductors, or semimetals.'
- Slade 2006, p. 16
- Corwin 2005, p. 80
- Barsanov & Ginzburg 1974, p. 330
- Bradbury et al. 1957, pp. 157, 659
- Miller, Lee & Choe 2002, p. 21
- King 2004, pp. 196–8; Ferro & Saccone 2008, p. 233
- Pashaey & Seleznev 1973, p. 565; Gladyshev & Kovaleva 1998, p. 1445; Eason 2007, p. 294
- Johansen & Mackintosh 1970, pp. 121–4; Divakar, Mohan & Singh 1984, p. 2337; Dávila et al. 2002, p. 035411-3
- Jezequel & Thomas 1997, pp. 6620–6
- Hindman 1968, p. 434: "The high values obtained for the [electrical] resistivity indicate that the metallic properties of neptunium are closer to the semimetals than the true metals. This is also true for other metals in the actinide series."; Dunlap et al. 1970, pp. 44, 46: "... α-Np is a semimetal, in which covalency effects are believed to also be of importance ... For a semimetal having strong covalent bonding, like α-Np ..."
- Lister 1965, p. 54
- Cotton et al. 1999, p. 502
- Pinkerton 1800, p. 81
- Goldsmith 1982, p. 526
- Zhdanov 1965, pp. 74–5
- Friend 1953, p. 68; IUPAC 1959, p. 10; IUPAC 1971, p. 11
- IUPAC 2005; IUPAC 2006–
- Van Setten et al. 2007, pp. 2460–1; Oganov et al. 2009, pp. 863–4
- Housecroft & Sharpe 2008, p. 331; Oganov 2010, p. 212
- Housecroft & Sharpe 2008, p. 333
- Kross 2011
- Berger 1997, p. 37
- Greenwood & Earnshaw 2002, p. 144
- Kopp, Lipták & Eren 2003, p. 221
- Prudenziati 1977, p. 242
- Berger 1997, pp. 87, 84
- Rayner-Canham & Overton 2006, p. 291
- Siekierski & Burgess 2002, p. 63
- Bowser 1993, p. 393; Grimes 2011, pp. 17–18
- Greenwood & Earnshaw 2002, p. 141; Henderson 2000, p. 58; Housecroft & Sharpe 2008, pp. 360–72
- Parry et al. 1970, pp. 438, 448–51
- Fehlner 1990, p. 202
- Greenwood & Earnshaw 2002, p. 145
- Houghton 1979, p. 59
- Fehlner 1990, pp. 204, 207
- Greenwood 2001, p. 2057
- Salentine 1987, pp. 128–32; MacKay, MacKay & Henderson 2002, pp. 439–40; Kneen, Rogers & Simpson 1972, p. 394; Hiller & Herber 1960, inside front cover; p. 225
- Watt 1958, p. 387; Sharp 1983
- Puddephatt & Monaghan 1989, p. 59
- Mahan 1965, p. 485
- Rao 2002, p. 22
- Fehlner 1992, p. 1
- Haiduc & Zuckerman 1985, p. 82
- Greenwood & Earnshaw 2002, p. 331
- Wiberg 2001, p. 824
- Rochow 1973, p. 1337‒38
- Russell & Lee 2005, p. 393
- Zhang 2002, p. 70
- Sacks 1998, p. 287
- Rochow 1973, p. 1337, 1340
- Allen & Ordway 1968, p. 152
- Eagleson 1994, pp. 48, 127, 438, 1194; Massey 2000, p. 191
- Orton 2004, p. 7. This is a typical value for high-purity silicon.
- Coles & Caplin 1976, p. 106
- Glazov, Chizhevskaya & Glagoleva 1969, pp. 59–63; Allen & Broughton 1987, p. 4967
- Cotton, Wilkinson & Gaus 1995, p. 393
- Partington 1944, p. 723
- Cox 2004, p. 27
- Hiller & Herber 1960, inside front cover; p. 225
- Kneen, Rogers and Simpson 1972, p. 384
- Bailar, Moeller & Kleinberg 1965, p. 513
- Cotton, Wilkinson & Gaus 1995, pp. 319, 321
- Smith 1990, p. 175
- Poojary, Borade & Clearfield 1993
- Wiberg 2001, pp. 851, 858
- Barmett & Wilson 1959, p. 332
- Powell 1988, p. 1
- Greenwood & Earnshaw 2002, p. 371
- Cusack 1967, p. 193
- Russell & Lee 2005, pp. 399–400
- Greenwood & Earnshaw 2002, p. 373
- Moody 1991, p. 273
- Russell & Lee 2005, p. 399
- Berger 1997, pp. 71–2
- Jolly 1966, pp. 125–6
- Schwartz 2002, p. 269
- Eggins 1972, p. 66; Wiberg 2001, p. 895
- Greenwood & Earnshaw 2002, p. 383
- Glockling 1969, p. 38; Wells 1984, p. 1175
- Cooper 1968, pp. 28–9
- Steele 1966, pp. 178, 188–9
- Wiberg 2001, p. 742
- Gray, Whitby & Mann 2011
- Greenwood & Earnshaw 2002, p. 552
- Parkes & Mellor 1943, p. 740
- Russell & Lee 2005, p. 420
- Carapella 1968, p. 30
- Barfuß et al. 1981, p. 967
- Greaves, Knights & Davis 1974, p. 369; Madelung 2004, pp. 405, 410
- Bailar & Trotman-Dickenson 1973, p. 558; Li 1990
- Bailar, Moeller & Kleinberg 1965, p. 477
- Eagleson 1994, p. 91
- Massey 2000, p. 267
- Timm 1944, p. 454
- Partington 1944, p. 641; Kleinberg, Argersinger & Griswold 1960, p. 419
- Morgan 1906, p. 163; Moeller 1954, p. 559
- Burford & Royan 1989, p. 3746
- Corbridge 2013, pp. 122, 215
- Douglade 1982
- Zingaro 1994, p. 197; Emeleús & Sharpe 1959, p. 418; Addison & Sowerby 1972, p. 209; Mellor 1964, p. 337
- Pourbaix 1974, p. 521; Eagleson 1994, p. 92; Greenwood & Earnshaw 2002, p. 572
- Wiberg 2001, pp. 750, 975; Silberberg 2006, p. 314
- Sidgwick 1950, p. 784; Moody 1991, pp. 248–9, 319
- Krannich & Watkins 2006
- Greenwood & Earnshaw 2002, p. 553
- Dunstan 1968, p. 433
- Parise 1996, p. 112
- Carapella 1968a, p. 23
- Moss 1952, pp. 174, 179
- Dupree, Kirby & Freyland 1982, p. 604; Mhiaoui, Sar, & Gasser 2003
- Kotz, Treichel & Weaver 2009, p. 62
- Friend 1953, p. 87
- Fesquet 1872, pp. 109–14
- Greenwood & Earnshaw 2002, p. 553; Massey 2000, p. 269
- King 1994, p.171
- Turova 2011, p. 46
- Pourbaix 1974, p. 530
- Wiberg 2001, p. 764
- House 2008, p. 497
- Mendeléeff 1897, p. 274
- Emsley 2001, p. 428
- Kudryavtsev 1974, p. 78
- Bagnall 1966, pp. 32–3, 59, 137
- Swink et al. 1966; Anderson et al. 1980
- Ahmed, Fjellvåg & Kjekshus 2000
- Chizhikov & Shchastlivyi 1970, p. 28
- Kudryavtsev 1974, p. 77
- Stuke 1974, p. 178; Donohue 1982, pp. 386–7; Cotton et al. 1999, p. 501
- Becker, Johnson & Nussbaum 1971, p. 56
- Berger 1997, p. 90
- Chizhikov & Shchastlivyi 1970, p. 16
- Jolly 1966, pp. 66–7
- Mellor 1964a, p. 30; Wiberg 2001, p. 589
- Greenwood & Earnshaw 2002, p. 765–6
- Bagnall 1966, p. 134–51; Greenwood & Earnshaw 2002, p. 786
- Detty & O'Regan 1994, pp. 1–2
- Hill & Holman 2000, p. 124
- Chang 2002, p. 314
- Kent 1950, pp. 1–2; Clark 1960, p. 588; Warren & Geballe 1981
- Housecroft & Sharpe 2008, p. 384; IUPAC 2006–, rhombohedral graphite entry
- Mingos 1998, p. 171
- Wiberg 2001, p. 781
- Charlier, Gonze & Michenaud 1994
- Atkins et al. 2006, pp. 320–1
- Savvatimskiy 2005, p. 1138
- Togaya 2000
- Savvatimskiy 2009
- Inagaki 2000, p. 216; Yasuda et al. 2003, pp. 3–11
- O'Hare 1997, p. 230
- Traynham 1989, pp. 930–1; Prakash & Schleyer 1997
- Olmsted & Williams 1997, p. 436
- Bailar et al. 1989, p. 743
- Moore et al. 1985
- House & House 2010, p. 526
- Wiberg 2001, p. 798
- Eagleson 1994, p. 175
- Atkins et al. 2006, p. 121
- Russell & Lee 2005, pp. 358–9
- Keevil 1989, p. 103
- Russell & Lee 2005, pp. 358–60 et seq
- Harding, Janes & Johnson 2002, pp. 118
- Metcalfe, Williams & Castka 1974, p. 539
- Cobb & Fetterolf 2005, p. 64; Metcalfe, Williams & Castka 1974, p. 539
- Ogata, Li & Yip 2002; Boyer et al. 2004, p. 1023; Russell & Lee 2005, p. 359
- Cooper 1968, p. 25; Henderson 2000, p. 5; Silberberg 2006, p. 314
- Wiberg 2001, p. 1014
- Daub & Seese 1996, pp. 70, 109: "Aluminum is not a metalloid but a metal because it has mostly metallic properties."; Denniston, Topping & Caret 2004, p. 57: "Note that aluminum (Al) is classified as a metal, not a metalloid."; Hasan 2009, p. 16: "Aluminum does not have the characteristics of a metalloid but rather those of a metal."
- Holt, Rinehart & Wilson c. 2007
- Tuthill 2011
- Stott 1956, p. 100
- Steele 1966, p. 60
- Emsley 2001, p. 382
- Young et al. 2010, p. 9; Craig 2003, p. 391. Selenium is "near metalloidal".
- Rochow 1957
- Rochow 1966, p. 224
- Moss 1952, p. 192
- Evans 1966, pp. 124–5
- Regnault 1853, p. 208
- Scott & Kanda 1962, p. 311
- Cotton et al. 1999, pp. 496, 503–4
- Arlman 1939; Bagnall 1966, pp. 135, 142–3
- Chao & Stenger 1964
- Berger 1997, pp. 86–7
- Snyder 1966, p. 242
- Fritz & Gjerde 2008, p. 235
- Meyer et al. 2005, p. 284; Manahan 2001, p. 911; Szpunar et al. 2004, p. 17
- US Environmental Protection Agency 1988, p. 1; Uden 2005, pp. 347‒8
- De Zuane 1997, p. 93; Dev 2008, pp. 2‒3
- Wiberg 2001, p. 594
- Greenwood & Earnshaw 2002, p. 786; Schwietzer & Pesterfield 2010, pp. 242–3
- Bagnall 1966, p. 41; Nickless 1968, p. 79
- Bagnall 1990, pp. 313–14; Lehto & Hou 2011, p. 220; Siekierski & Burgess 2002, p. 117: "The tendency to form X2– anions decreases down the Group [16 elements] ..."
- Legit, Friák & Šob 2010, p. 214118-18
- Manson & Halford 2006, pp. 378, 410
- Bagnall 1957, p. 62; Fernelius 1982, p. 741
- Bagnall 1966, p. 41; Barrett 2003, p. 119
- Hawkes 2010; Holt, Rinehart & Wilson c. 2007; Hawkes 1999, p. 14; Roza 2009, p. 12
- Keller 1985
- Harding, Johnson & Janes 2002, p. 61
- Long & Hentz 1986, p. 58
- Vasáros & Berei 1985, p. 109
- Haissinsky & Coche 1949, p. 400
- Brownlee et al. 1950, p. 173
- Hermann, Hoffmann & Ashcroft 2013
- Siekierski & Burgess 2002, pp. 65, 122
- Emsley 2001, p. 48
- Rao & Ganguly 1986
- Krishnan et al. 1998
- Glorieux, Saboungi & Enderby 2001
- Millot et al. 2002
- Vasáros & Berei 1985, p. 117
- Kaye & Laby 1973, p. 228
- Samsonov 1968, p. 590
- Korenman 1959, p. 1368
- Rossler 1985, pp. 143–4
- Champion et al. 2010
- Borst 1982, pp. 465, 473
- Batsanov 1971, p. 811
- Swalin 1962, p. 216; Feng & Lin 2005, p. 157
- Schwietzer & Pesterfield 2010, pp. 258–60
- Hawkes 1999, p. 14
- Olmsted & Williams 1997, p. 328; Daintith 2004, p. 277
- Eberle1985, pp. 213–16, 222–7
- Restrepo et al. 2004, p. 69; Restrepo et al. 2006, p. 411
- Greenwood & Earnshaw 2002, p. 804
- Greenwood & Earnshaw 2002, p. 803
- Wiberg 2001, p. 416
- Craig 2003, p. 391; Schroers 2013, p. 32; Vernon 2013, pp. 1704–1705
- Cotton et al. 1999, p. 42
- Marezio & Licci 2000, p. 11
- Russell & Lee 2005, p. 5
- Parish 1977, pp. 178, 192–3
- Eggins 1972, p. 66; Rayner-Canham & Overton 2006, pp. 29–30
- Atkins et al. 2006, pp. 320–1; Bailar et al. 1989, p. 742–3
- Rochow 1966, p. 7; Taniguchi et al. 1984, p. 867: "... black phosphorus ... [is] characterized by the wide valence bands with rather delocalized nature."; Morita 1986, p. 230; Carmalt & Norman 1998, p. 7: "Phosphorus ... should therefore be expected to have some metalloid properties."; Du et al. 2010. Interlayer interactions in black phosphorus, which are attributed to van der Waals-Keesom forces, are thought to contribute to the smaller band gap of the bulk material (calculated 0.19 eV; observed 0.3 eV) as opposed to the larger band gap of a single layer (calculated ~0.75 eV).
- Stuke 1974, p. 178; Cotton et al. 1999, p. 501; Craig 2003, p. 391
- Steudel 1977, p. 240: "... considerable orbital overlap must exist, to form intermolecular, many-center ... [sigma] bonds, spread through the layer and populated with delocalized electrons, reflected in the properties of iodine (lustre, color, moderate electrical conductivity)."; Segal 1989, p. 481: "Iodine exhibits some metallic properties ..."
- Lutz et al. 2011, p. 16
- Yacobi & Holt 1990, p. 10; Wiberg 2001, p. 160
- Greenwood & Earnshaw 2002, pp. 479, 482
- Eagleson 1994, p. 820
- Oxtoby, Gillis & Campion 2008, p. 508
- Brescia et al. 1980, pp. 166–71
- Fine & Beall 1990, p. 578
- Wiberg 2001, p. 901
- Berger 1997, p. 80
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|Periodic table (Large version)|