|Lanthanides in the periodic table|
The lanthanide // or lanthanoid // series of chemical elements comprises the fifteen metallic chemical elements with atomic numbers 57 through 71, from lanthanum through lutetium. These fifteen lanthanide elements, along with the chemically similar elements scandium and yttrium, are often collectively known as the rare earth elements.
The informal chemical symbol Ln is used in general discussions of lanthanide chemistry to refer to any lanthanide. All but one of the lanthanides are f-block elements, corresponding to the filling of the 4f electron shell; lutetium, a d-block element, is also generally considered to be a lanthanide due to its chemical similarities with the other fourteen. All lanthanide elements form trivalent cations, Ln3+, whose chemistry is largely determined by the ionic radius, which decreases steadily from lanthanum to lutetium.
They are termed as lanthanides because the lighter elements in the series are chemically similar to lanthanum. Strictly speaking, both lanthanum and lutetium have been labeled as group 3 elements, because they both have a single valence electron in the d shell. However, both elements are often included in any general discussion of the chemistry of the lanthanide elements.
In presentations of the periodic table, the lanthanides and the actinides are customarily shown as two additional rows below the main body of the table, with placeholders or else a selected single element of each series (either lanthanum and actinium, or lutetium and lawrencium) shown in a single cell of the main table, between barium and hafnium, and radium and rutherfordium, respectively. This convention is entirely a matter of aesthetics and formatting practicality; a rarely used wide-formatted periodic table inserts the lanthanide and actinide series in their proper places, as parts of the table's sixth and seventh rows (periods).
- 1 Etymology
- 2 Physical properties of the elements
- 3 Chemistry and compounds
- 3.1 Effect of 4f orbitals
- 3.2 Lanthanide oxidation states
- 3.3 Separation of lanthanides
- 3.4 Coordination chemistry and catalysis
- 4 Physical properties
- 5 Occurrence
- 6 Applications
- 7 Biological effects
- 8 See also
- 9 References
- 10 Cited sources
- 11 External links
Together with scandium and yttrium, the trivial name "rare earths" is sometimes used to describe all the lanthanides. This name arises from the minerals from which they were isolated, which were uncommon oxide-type minerals. However, the use of the name is deprecated by IUPAC, as the elements are neither rare in abundance nor "earths" (an obsolete term for water-insoluble strongly basic oxides of electropositive metals incapable of being smelted into metal using late 18th century technology). Cerium is the 26th most abundant element in the Earth's crust, neodymium is more abundant than gold and even thulium (the least common naturally occurring lanthanide) is more abundant than iodine, which is itself common enough for biology to have evolved critical usages thereof. Despite their abundance, even the technical term "lanthanides" could be interpreted to reflect a sense of elusiveness on the part of these elements, as it comes from the Greek λανθανειν (lanthanein), "to lie hidden". However, if not referring to their natural abundance, but rather to their property of "hiding" behind each other in minerals, this interpretation is in fact appropriate. The etymology of the term must be sought in the first discovery of lanthanum, at that time a so-called new rare earth element "lying hidden" in a cerium mineral, and it is an irony that lanthanum was later identified as the first in an entire series of chemically similar elements and could give name to the whole series. The term "lanthanide" was introduced by Victor Goldschmidt in 1925.
Physical properties of the elements
|Melting point (°C)||920||795||935||1024||1042||1072||826||1312||1356||1407||1461||1529||1545||824||1652|
|Boiling point (°C)||3464||3443||3520||3074||3000||1794||1529||3273||3230||2567||2720||2868||1950||1196||3402|
|Atomic electron configuration*||5d1||4f15d1||4f3||4f4||4f5||4f6||4f7||4f75d1||4f9||4f10||4f11||4f12||4f13||4f14||4f145d1|
|Metal lattice (RT)||dhcp||fcc||dhcp||dhcp||dhcp||**||bcc||hcp||hcp||hcp||hcp||hcp||hcp||hcp||hcp|
|Metallic radius pm||162||181.8||182.4||181.4||183.4||180.4||208.4||180.4||177.3||178.1||176.2||176.1||175.9||193.3||173.8|
|Resistivity (25 °C) /μ Ohm cm||57–80
|+95.9||+2500 (β)||+5530(α)||+5930 (α)||+1278(α)||+30900||+185000
|+170000 (α)||+98000||+72900||+48000||+24700||+67 (β)||+183|
* Between initial [Xe] and final 6s2 electronic shells ** Sm has a close packed structure like the other lanthanides but has an unusual 9 layer repeat
Gschneider and Daane (1988) attribute the trend in melting point which increases across the series, (lanthanum (920 °C) – lutetium (1622 °C)) to the extent of hybridisation of the 6s, 5d and 4f orbitals. The hybridisation is believed to be at its greatest for cerium which has the lowest melting point of all, 795 °C. The lanthanide metals are soft, their hardness increases across the series. Europium stands out as it has the lowest density in the series at 5.24 g/cm3 and the largest metallic radius in the series at 208.4 pm. It can be compared to barium which has a metallic radius of 222 pm. It is believed that the metal contains the larger Eu2+ ion and that there are only two electrons in the conduction band. Ytterbium also has large metallic radius and a similar explanation is suggested. The resistivities of the lanthanide metals are relatively high, ranging from 29 to 134 μ Ohm·cm. These values can be compared to a good conductor such as aluminium which has a resistivity of 2.655 μ Ohm·cm. With the exceptions of La, Yb and Lu (which have no unpaired f electrons) the lanthanides are strongly paramagnetic and this is reflected in their magnetic susceptibilities. Gadolinium becomes ferromagnetic at below 16 °C (Curie point). The other heavier lanthanides, terbium, dysprosium, holmium, erbium, thulium and ytterbium become ferromagnetic at much lower temperatures.
Chemistry and compounds
|Ln3+ electron configuration*||4f0||4f1||4f2||4f3||4f4||4f5||4f6||4f7||4f8||4f9||4f10||4f11||4f12||4f13||
|Ln3+ radius (pm)||103||102||99||98.3||97||95.8||94.7||93.8||92.3||91.2||90.1||89||88||86.8||86.1|
|Ln4+ ion colour in aqueous solution||—||Orange-yellow||Yellow||Blue-violet||—||—||—||—||Red-brown||Orange-yellow||—||—||—||—||—|
|Ln3+ ion colour in aqueous solution||Colorless||Colorless||Green||Violet||Pink||Pale yellow||Colorless||Colorless||V. pale pink||Pale yellow||Yellow||Rose||Pale green||Colorless||Colorless|
|Ln2+ ion colour in aqueous solution||—||—||—||—||—||Blood red||Colorless||—||—||—||—||—||Violet-red||Yellow-green||—|
* Between initial [Xe] and final 6s2 electronic shells
It should be noted that the colours of lanthanide complexes originate almost entirely from charge transfer interactions between the metal and the ligand. f → f transitions are symmetry forbidden (or Laporte-forbidden), which is also true of transition metals, however t-metals are able to use vibronic coupling to break this rule. The valence orbitals in lanthanides are almost entirely non-bonding and as such little effective vibronic coupling takes, hence the spectra from f → f transitions are much weaker and narrower than those from d → d transitions. In general this makes the colours of lanthanide complexes far fainter than those of transition metal complexes.
Effect of 4f orbitals
Going across the lanthanides, in the periodic table, the 4f orbitals are usually being filled. The effect of the 4f orbitals on the chemistry of the lanthanides is profound and is the factor that distinguishes them from the transition metals. There are seven 4f orbitals and there are two different ways in which they are depicted, firstly as a "cubic set" or as a general set. The cubic set is fz3, fxz2, fyz2, fxyz, fz(x2−y2), fx(x2−3y2) and fy(3x2−y2). The 4f orbitals penetrate the [Xe] core and are isolated and do not participate in bonding. This explains why crystal field effects are small and why they do not form π bonds. As there are seven 4f orbitals the number of unpaired electrons can be as high as 7 which gives rise to the large magnetic moments observed for lanthanide compounds. Measuring the magnetic moment can be used to investigate the 4f electron configuration and this is a useful tool in providing an insight into the chemical bonding. The lanthanide contraction, the reduction in size of the Ln3+ ion from La3+(103 pm)- Lu3+(86.1 pm) is often explained by the poor shielding of the 5s and 5p electrons by the 4f electrons.
The electronic structure of the lanthanide elements, with minor exceptions, is [Xe]6s24fn. The chemistry of the lanthanides is dominated by the +3 oxidation state and in LnIII compounds the 6s electrons and (usually) one 4f electron are lost and the ions have the configuration [Xe]4fm. All the lanthanide elements exhibit the oxidation state +3. In addition Ce3+ can lose its single f electron to form Ce4+ with the stable electronic configuration of xenon. Also, Eu3+ can gain an electron to form Eu2+ with the f7 configuration which has the extra stability of a half-filled shell. Other than Ce(IV) and Eu(II), none of the lanthanides are stable in oxidation states other than +3 in aqueous solution. Promethium is effectively a man-made element as all its isotopes are radioactive with half-lives shorter than 20 years.
In terms of reduction potentials, the Ln0/3+ couples are nearly the same for all lanthanides, ranging from −1.99 (for Eu) to −2.35 V (for Pr). Thus, these metals are highly reducing, with reducing power similar to alkaline earth metals such as Mg (−2.36 V).
Lanthanide oxidation states
All of the lanthanide elements are commonly known to have the +3 oxidation state and it was thought that only samarium, europium, and ytterbium had the +2 oxidation readily accessible in solution. Now, it is known that all of the lanthanides can form +2 complexes in solution.
above [Xe] core
|1st Ionisation energy
|2nd Ionisation energy
|1st + 2nd Ionisation energy
|3rd Ionisation energy
|1st+2d+3rd Ionisation energy
|4th Ionisation energy
The ionisation energies for the lanthanides can be compared with aluminium. In aluminium the sum of the first three ionisation energies is 5139 kJ·mol−1, whereas the lanthanides fall in the range 3455 – 4186 kJ·mol−1. This correlates with the highly reactive nature of the lanthanides.
The sum of the first two ionisation energies for europium, 1632 kJ·mol−1 can be compared with that of barium 1468.1 kJ·mol−1 and europium's third ionisation energy is the highest of the lanthanides. The sum of the first two ionisation energies for ytterbium are the second lowest in the series and its third ionisation energy is the second highest. The high third ionisation energy for Eu and Yb correlate with the half filling 4f7 and complete filling 4f14 of the 4f sub shell, and the stability afforded by such configurations due to exchange energy. Europium and ytterbium form salt like compounds with Eu2+ and Yb2+, for example the salt like dihydrides,. Both europium and ytterbium dissolve in liquid ammonia forming solutions of Ln2+(NH3)x again demonstrating their similarities to the alkaline earth metals.
The relative ease with which the 4th electron can be removed in cerium and (to a lesser extent praseodymium) indicates why Ce(IV) and Pr(IV) compounds can be formed, for example CeO2 is formed rather than Ce2O3 when cerium reacts with oxygen.
Separation of lanthanides
The similarity in ionic radius between adjacent lanthanide elements makes it difficult to separate them from each other in naturally occurring ores and other mixtures. Historically, the very laborious processes of cascading and fractional crystallization were used. Because the lanthanide ions have slightly different radii, the lattice energy of their salts and hydration energies of the ions will be slightly different, leading to a small difference in solubility. Salts of the formula Ln(NO3)3·2NH4NO3·4H2O can be used. Industrially, the elements are separated from each other by solvent extraction. Typically an aqueous solution of nitrates is extracted into kerosene containing tri-n-butylphosphate. The strength of the complexes formed increases as the ionic radius decreases, so solubility in the organic phase increases. Complete separation can be achieved continuously by use of countercurrent exchange methods. The elements can also be separated by ion-exchange chromatography, making use of the fact that the stability constant for formation of EDTA complexes increases for log K ≈ 15.5 for [La(EDTA)]− to log K ≈ 19.8 for [Lu(EDTA)]−.
Coordination chemistry and catalysis
When in the form of coordination complexes, lanthanides exist overwhelmingly in their +3 oxidation state, although particularly stable 4f configurations can also give +4 (Ce, Tb) or +2 (Eu, Yb) ions. All of these forms are strongly electropositive and thus lanthanide ions are hard Lewis acids. The oxidation states are also very stable and with the exception of SmI2 and cerium(IV) salts lanthanides are not used for redox chemistry. 4f electrons have a high probability of being found close to the nucleus and are thus strongly affected as the nuclear charge increases across the series; this results in a corresponding decrease in ionic radii referred to as the lanthanide contraction.
The low probability of the 4f electrons existing at the outer region of the atom or ion permits little effective overlap between the orbitals of a lanthanide ion and any binding ligand. Thus lanthanide complexes typically have little or no covalent character and are not influenced by orbital geometries. The lack of orbital interaction also means that varying the metal typically has little effect on the complex (other than size), especially when compared to transition metals. Complexes are held together by weaker electrostatic forces which are omni-directional and thus the ligands alone dictate the symmetry and coordination of complexes. Steric factors therefore dominate, with coordinative saturation of the metal being balanced against inter-ligand repulsion. This results in a diverse range of coordination geometries, many of which are irregular, and also manifests itself in the highly fluxional nature of the complexes. As there is no energetic reason to be locked into a single geometry, rapid intramolecular and intermolecular ligand exchange will take place. This typically results in complexes that rapidly fluctuate between all possible configurations.
Many of these features make lanthanide complexes effective catalysts. Hard Lewis acids are able to polarise bonds upon coordination and thus alter the electrophilicity of compounds, with a classic example being the Luche reduction. The large size of the ions coupled with their labile ionic bonding allows even bulky coordinating species to bind and dissociate rapidly, resulting in very high turnover rates; thus excellent yields can often be achieved with loadings of only a few mol%. The lack of orbital interactions combined with the lanthanide contraction means that the lanthanides change in size across the series but that their chemistry remains much the same. This allows for easy tuning of the steric environments and examples exist where this has been used to improve the catalytic activity of the complex and change the nuclearity of metal clusters.
Despite this, the use of lanthanide coordination complexes as homogeneous catalysts is largely restricted to the laboratory and there are currently few examples them being used on an industrial scale. It should be noted however, that lanthanides exist in many forms other that coordination complexes and many of these are industrially useful. In particular lanthanide metal oxides are used as heterogeneous catalysts in various industrial processes.
The trivalent lanthanides mostly form ionic salts. The trivalent ions are hard acceptors and form more stable complexes with oxygen-donor ligands than with nitrogen-donor ligands. The larger ions are 9-coordinate in aqueous solution, [Ln(H2O)9]3+ but the smaller ions are 8-coordinate, [Ln(H2O)8]3+. There is some evidence that the later lanthanides have more water molecules in the second coordination sphere. Complexation with monodentate ligands is generally weak because it is difficult to displace water molecules from the first coordination sphere. Stronger complexes are formed with chelating ligands because of the chelate effect, such as the tetra-anion derived from 1,4,7,10-tetraazacyclododecane-1,4,7,10-tetraacetic acid (DOTA).
Ln(II) and Ln(IV) compounds
The most common divalent derivatives of the lanthanides are for Eu(II), which achieves a favorable f7 configuration. Divalent halide derivatives are known for all of the lanthanides. They are either conventional salts or are Ln(III) "electride"-like salts. The simple salts include YbI2, EuI2, and SmI2. The electride-like salts, described as Ln3+, 2I−, e−, include LaI2, CeI2 and GdI2. Many of the iodides form soluble complexes with ethers, e.g. TmI2(dimethoxyethane)3. Samarium(II) iodide is a useful reducing agent. Ln(II) complexes can be synthesized by transmetalation reactions.
Ce(IV) in ceric ammonium nitrate is a useful oxidizing agent. Otherwise tetravalent lanthanides are rare. The Ce(IV) is the exception owing to the tendency to form an unfilled f shell.
|Metal lattice (RT)||dhcp||fcc||dhcp||dhcp||dhcp||r||bcc||hcp||hcp||hcp||hcp||hcp||hcp||hcp||hcp|
|GdH2+x||TbH2+x||DyH2+x||HoH2+x||ErH2+x||TmH2+x||YbH2+x o, fcc
|metal sub lattice||fcc||fcc||fcc||fcc||fcc||fcc||o||fcc||fcc||fcc||fcc||fcc||fcc||o fcc||fcc|
|metal sub lattice||fcc||fcc||fcc||hcp||hcp||hcp||fcc||hcp||hcp||hcp||hcp||hcp||hcp||hcp||hcp|
(color where recorded)
|red||bronze to grey||PrH3-x fcc||NdH3-x hcp||golden greenish||EuH3-x fcc||GdH3-x hcp||TbH3-x hcp||DyH3-x hcp||HoH3-x hcp||ErH3-x hcp||TmH3-x hcp||LuH3-x hcp|
Lanthanide metals react exothermically with hydrogen to form LnH2, dihydrides. With the exception of Eu and Yb which resemble the Ba and Ca hydrides (non conducting,transparent salt like compounds) they form black pyrophoric, conducting compounds where the metal sub-lattice is face centred cubic and the H atoms occupy tetrahedral sites. Further hydrogenation produces a trihydride which is non-stoichiometric, non-conducting, more salt like. The formation of trihydride is associated with and increase in 8–10% volume and this is linked to greater localisation of charge on the hydrogen atoms which become more anionic (H− hydride anion) in character.
|Color m.p. °C||white dec||white dec||white dec|
|Structure C.N.||UF4 8||UF4 8||UF4 8|
|Color m.p. °C||white 1493||white 1430||green 1395||violet 1374||green 1399||white 1306||white 1276||white 1231||white 1172||green 1154||pink 1143||pink 1140||white 1158||white 1157||white 1182|
|Structure C.N.||LaF3 9||LaF3 9||LaF3 9||LaF3 9||YF3 8||YF3 8||YF3 8||YF3 8||YF3 8||YF3 8||YF3 8||YF3 8||YF3 8||YF3 8|
|Color m.p. °C||La||white 817||green 786||mauve 758||green 786||yellow 682||yellow dec||white 602||white 582||white 647||yellow 720||violet 776||yellow 824||white 865||white 925|
|Structure C.N.||UCl3 9||UCl3 9||UCl3 9||UCl3 9||UCl3 9||UCl3 9||UCl3 9||PuBr3 8||PuBr3 8||YCl3 6||YCl3 6||YCl3 6||YCl3 6||YCl3 6|
|Color m.p. °C||white 733||green 691||violet 682||green 693||yellow 640||grey dec||white 770||white 828||white 879||yellow 919||violet 923||white 954||white dec||white 1025|
|Structure C.N.||UCl3 9||UCl3 9||UCl3 9||PuBr3 8||PuBr3 8||PuBr3 8||6||6||6||6||6||6||6||6|
|Color m.p. °C||yellow 766||PrF4||green 784||green 737||orange 850||dec.||yellow 925||957||green 978||yellow 994||violet 1015||yellow 1021||white dec||brown 1050|
|Structure C.N.||PuBr3 8||PuBr3 8||PuBr3 8||PuBr3 8||BiI3 6||BiI3 6||BiI3 6||BiI3 6||BiI3 6||BiI3 6||BiI3 6||BiI3 6||BiI3 6||BiI3 6|
|Color m.p. °C||purple 1417||yellow 1416||grey|
|Structure C.N.||CaF2 8||CaF2 8||CaF2 8|
|Color m.p. °C||green 841||brown 859||white 731||black dec.||green 718||green 720|
|Structure C.N.||PbCl2 9||PbCl2 9||PbCl2 9||SrBr2||SrI2 7||SrI2 7|
|Color m.p. °C||green 725||brown 669||white 731||black||green||yellow 673|
|Structure C.N.||PbCl2 9||SrBr2 8||SrBr2 8||SrI2 7||SrI2 7||SrI2 7|
high pressure metallic
|Color m.p. °C||bronze 808||bronze 758||violet 562||green 520||green 580||bronze 831||purple 721||black 756||yellow 780||Lu|
|Structure C.N.||CuTi2 8||CuTi2 8||CuTi2 8||SrBr2 8
|EuI2 7||EuI2 7||2H-MoS2 6||CdI2 6||CdI2 6|
The only tetrahalides known are those of cerium, praseodymium and terbium mirroring the formation of the dioxides. All of the lanthanides form trihalides with fluorine, chlorine, bromine and iodine. They are all high melting and predominantly ionic in nature. The fluorides are only slightly soluble in water and are not sensitive to air, and this contrasts with the other halides which are air sensitive, readily soluble in water and react at high temperature to form oxohalides. The trihalides were important as pure metal can be prepared from them. In the gas phase the trihalides are planar or approximately planar, the lighter lanthanides have a lower % of dimers, the heavier lanthanides a higher proportion. The dimers have a similar structure to Al2Cl6
Some of the dihalides are conducting while the rest are insulators. The conducting forms can be considered as LnIII electride compounds where the electron is delocalised into a conduction band, Ln3+ (X−)2(e−). All of the diodides have relatively short metal-metal separations. The CuTi2 structure of the lanthanum, cerium and praseodymium diodides along with HP-NdI2 contain 44 nets of metal and iodine atoms with short metal-metal bonds (393-386 La-Pr). these compounds should be considered to be two-dimensional metals (two-dimensional in the same way that graphite is). The salt like dihalides include those of Eu Dy Tm and Yb. The formation of a relatively stable +2 oxidation state for Eu and Yb is usually explained by the stability (exchange energy) of half filled (f7) and fully filled f14. GdI2 possesses the layered MoS2 structure, is ferromagnetic and exhibits colossal magnetoresistance The sesquihalides Ln2X3 and the Ln7I12 compounds listed in the table contain metal clusters, discrete Ln6I12 clusters in Ln7I12 and condensed clusters forming chains in the sesquihalides. Scandium forms a similar cluster compound with chlorine, Sc7Cl12 Unlike many transition metal clusters these lanthanide clusters do not have strong metal-metal interactions and this is due to the low number of valence electrons involved, but instead are stabilised by the surrounding halogen atoms.
LaI is the only known monohalide. Prepared from the reaction of LaI3 and La metal, it has a NiAs type structure and can be formulated La3+ (I−)(e−)2.
Oxides and hydroxides
All of the lanthanides form sesquioxides, Ln2O3. The lighter/larger lanthanides adopt a hexagonal 7-coordinate structure while the heavier/smaller ones adopt a cubic 6-coordinate "C-M2O3" structure. All of the sesquioxides are basic, and absorb water and carbon dioxide from air to form carbonates, hydroxides and hydroxycarbonates. They dissolve in acids to form salts.
Cerium forms a stoichiometric dioxide, CeO2, where cerium has an oxidation state of +4. CeO2 is basic and dissolves with difficulty in acid to form Ce4+ solutions, from which CeIV salts can be isolated, for example the hydrated nitrate Ce(NO3)4.5H2O. CeO2 is used as an oxidation catalyst in catalytic converters. Praseodymium and terbium form non-stoichiometric oxides containing LnIV, although more extreme reaction conditions can produce stoichiometric (or near stoichiometric) PrO2 and TbO2.
Europium and ytterbium form salt-like monoxides, EuO and YbO, which have a rock salt structure. EuO is ferromagnetic at low temperatures, and is a semiconductor with possible applications in spintronics. A mixed EuII/EuIII oxide Eu3O4 can be produced by reducing Eu2O3 in a stream of hydrogen. Neodymium and samarium also form monoxides, but these are shiny conducting solids, although the existence of samarium monoxide is considered dubious.
All of the lanthanides form hydroxides, Ln(OH)3. With the exception of lutetium hydroxide, which has a cubic structure, they have the hexagonal UCl3 structure. The hydroxides can be precipitated from solutions of LnIII. They can also be formed by the reaction of the sesquioxide, Ln2O3, with water, but although this reaction is thermodynamically favourable it is kinetically slow for the heavier members of the series. Fajan's rules indicate that the smaller Ln3+ ions will be more polarizing and their salts correspondingly less ionic. The hydroxides of the heavier lanthanides become less basic, for example Yb(OH)3 and Lu(OH)3 are still basic hydroxides but will dissolve in hot concentrated NaOH.
Chalcogenides (S, Se, Te)
All of the lanthanides form Ln2Q3 (Q= S, Se, Te). The sesquisulfides can be produced by reaction of the elements or (with the exception of Eu2S3) sulfidizing the oxide (Ln2O3) with H2S. The sesquisulfides, Ln2S3 generally lose sulfur when heated and can form a range of compositions between Ln2S3 and Ln3S4. The sesquisulfides are insulators but some of the Ln3S4 are metallic conductors (e.g. Ce3S4) formulated (Ln3+)3 (S2−)4 (e−), while others (e.g. Eu3S4 and Sm3S4) are semiconductors. Structurally the sesquisulfides adopt structures that vary according to the size of the Ln metal. The lighter and larger lanthanides favouring 7 coordinate metal atoms, the heaviest and smallest lanthanides (Yb and Lu) favouring 6 coordination and the rest structures with a mixture of 6 and 7 coordination. Polymorphism is common amongst the sesquisulfides. The colors of the sesquisulfides vary metal to metal and depend on the polymorphic form. The colors of the γ-sesquisulfides are La2S3, white/yellow; Ce2S3, dark red; Pr2S3, green; Nd2S3, light green; Gd2S3, sand; Tb2S3, light yellow and Dy2S3, orange. The shade of γ-Ce2S3 can be varied by doping with Na or Ca with hues ranging from dark red to yellow, and Ce2S3 based pigments are used commercially and are seen as low toxicity substitutes for cadmium based pigments.
All of the lanthanides form monochalcogenides, LnQ, (Q= S, Se, Te). The majority of the monochalcogenides are conducting, indicating a formulation LnIIIQ2−(e-) where the electron is in conduction bands. The exceptions are SmQ, EuQ and YbQ which are semiconductors or insulators but exhibit a pressure induced transition to a conducting state. Compounds LnQ2 are known but these do not contain LnIV but are LnIII compounds containing polychalcogenide anions.
Oxysulfides Ln2O2S are well known, they all have the same structure with 7 coordinate Ln atoms with 3 sulfur atoms and 4 oxygen as near neighbours. Doping these with other lanthanide elements produces phosphors. As an example, gadolinium oxysulfide, Gd2O2S doped with Tb3+ produces visible photons when irradiated with high energy X-rays and is used as a scintillator in flat panel detectors. When mischmetal, an alloy of lanthanide metals, is added to molten steel to remove oxygen and sulfur, stable oxysulfides are produced that form an immiscible solid.
Pnictides (group 15)
All of the lanthanides form a mononitride, LnN, with the rock salt structure. The mononitrides have attracted interest because of their unusual physical properties. SmN and EuN are reported as being "half metals". NdN, GdN, TbN and DyN are ferromagnetic, SmN is antiferromagnetic. Applications in the field of spintronics are being investigated. CeN is unusual as it is a metallic conductor, contrasting with the other nitrides also with the other cerium pnictides. A simple description is Ce4+ N3− (e–) but the interatomic distances are a better match for the trivalent state rather than for the tetravalent state. A number of different explanations have been offered. The nitrides can be prepared by the reaction of lanthanum metals with nitrogen. Some nitride is produced along with the oxide, when lanthanum metals are ignited in air. Alternative methods of synthesis are a high temperature reaction of lanthanide metals with ammonia or the decomposition of lanthanide amides, Ln(NH2)3. Achieving pure stoichiometric compounds, and crystals with low defect density has proved difficult. The lanthanide nitrides are sensitive to air and hydrolyse producing ammonia.
The other pnictides phosphorus, arsenic, antimony and bismuth also react with the lanthanide metals to form monopnictides, LnQ. Additionally a range of other compounds can be produced with varying stoichiometries, such as LnP2, LnP5, LnP7 Ln3As, Ln5As3 and LnAs2.
Carbides of varying stoichiometries are known for the lanthanides. Non-stoichiometry is common. All of the lanthanides form LnC2 and Ln2C3 which both contain C2 units. The dicarbides with exception of EuC2, are metallic conductors with the calcium carbide structure and can be formulated as Ln3+C22−(e–). The C-C bond length is longer than that in CaC2, which contains the C22− anion, indicating that the antibonding orbitals of the C22− anion are involved in the conduction band. These dicarbides hydrolyse to form hydrogen and a mixture of hydrocarbons. EuC2 and to a lesser extent YbC2 hydrolyse differently producing a higher percentage of acetylene (ethyne). The sesquicarbides, Ln2C3 can be formulated as Ln4(C2)3. These compounds adopt the Pu2C3 structure which has been described as having C22− anions in bisphenoid holes formed by eight near Ln neighbours. The lengthening of the C-C bond is less marked in the sesquicarbides than in the dicarbides, with the exception of Ce2C3. Other carbon rich stoichiometries are known for some lanthanides. Ln3C4 (Ho-Lu) containing C, C2 and C3 units; Ln4C7 (Ho- Lu) contain C atoms and C3 units and Ln4C5 (Gd-Ho) containing C and C2 units. Metal rich carbides contain interstitial C atoms and no C2 or C3 units. These are Ln4C3 (Tb and Lu); Ln2C (Dy, Ho, Tm) and Ln3C (Sm-Lu).
All of the lanthanides form a number of borides. The "higher" borides (LnBx where x > 12) are insulators/semiconductors whereas the lower borides are typically conducting. The lower borides have stoichiometries of LnB2, LnB4, LnB6 and LnB12. Applications in the field of spintronics are being investigated. The range of borides formed by the lanthanides can be compared to those formed by the transition metals. The boron rich borides are typical of the lanthanides (and groups 1–3) whereas for the transition metals tend to form metal rich, "lower" borides. The lanthanide borides are typically grouped together with the group 3 metals with which they share many similarities of reactivity, stoichiometry and structure. Collectively these are then termed the rare earth borides.
Many methods of producing lanthanide borides have been used, amongst them are direct reaction of the elements; the reduction of Ln2O3 with boron; reduction of boron oxide, B2O3, and Ln2O3 together with carbon; reduction of metal oxide with boron carbide, B4C. Producing high purity samples has proved to be difficult. Single crystals of the higher borides have been grown in a low melting metal (e.g. Sn, Cu, Al).
Diborides, LnB2, have been reported for Sm, Gd, Tb, Dy, Ho, Er, Tm, Yb and Lu. All have the same, AlB2, structure containing a graphitic layer of boron atoms. Low temperature ferromagnetic transitions for Tb, Dy, Ho and Er. TmB2 is ferromagnetic at 7.2 K.
Tetraborides, LnB4 have been reported for all of the lanthanides except EuB4, all have the same UB4 structure. The structure has a boron sub-lattice consists of chains of octahedral B6 clusters linked by boron atoms. The unit cell decreases in size successively from LaB4 to LuB4. The tetraborides of the lighter lanthanides melt with decomposition to LnB6. Attempts to make EuB4 have failed. The LnB4 are good conductors and typically antiferromagnetic.
Hexaborides, LnB6 have been reported for all of the lanthanides. They all have the CaB6 structure, containing B6 clusters. They are non-stoichiometric due to cation defects. The hexaborides of the lighter lanthanides (La – Sm) melt without decomposition, EuB6 decomposes to boron and metal and the heavier lanthanides decompose to LnB4 with exception of YbB6 which decomposes forming YbB12. The stability has in part been correlated to differences in volatility between the lanthanide metals. In EuB6 and YbB6 the metals have an oxidation state of +2 whereas in the rest of the lanthanide hexaborides it is +3. This rationalises the differences in conductivity, the extra electrons in the LnIII hexaborides entering conduction bands. EuB6 is a semiconductor and the rest are good conductors. LaB6 and CeB6 are thermionic emitters, used, for example, in scanning electron microscopes.
Dodecaborides, LnB12, are formed by the heavier smaller lanthanides, but not by the lighter larger metals, La – Eu. With the exception YbB12 (where Yb takes an intermediate valence and is a Kondo insulator), the dodecaborides are all metallic compounds. They all have the UB12 structure containing a 3 dimensional framework of cubooctahedral B12 clusters.
The higher boride LnB66 is known for all lanthanide metals. The composition is approximate as the compounds are non-stoichiometric. They all have similar complex structure with over 1600 atoms in the unit cell. The boron cubic sub lattice contains super icosahedra made up of a central B12 icosahedra surrounded by 12 others, B12(B12)12. Other complex higher borides LnB50 (Tb, Dy, Ho Er Tm Lu) and LnB25 are known (Gd, Tb, Dy, Ho, Er) and these contain boron icosahedra in the boron framework.
Lanthanide-carbon σ bonds are well known; however as the 4f electrons have a low probability of existing at the outer region of the atom there is little effective orbital overlap, resulting in bonds with significant ionic character. As such organo-lanthanide compounds exhibit carbanion-like behaviour, unlike the behaviour in transition metal organometallic compounds. Because of their large size, lanthanides tend to form more stable organometallic derivatives with bulky ligands to give compounds such as Ln[CH(SiMe3)3]. Analogues of uranocene are derived from dilithiocyclooctatetraene, Li2C8H8. Organic lanthanide(II) compounds are also known, such as Cp*2Eu.
Magnetic and spectroscopic
All the trivalent lanthanide ions, except lanthanum and lutetium, have unpaired f electrons. However, the magnetic moments deviate considerably from the spin-only values because of strong spin-orbit coupling. The maximum number of unpaired electrons is 7, in Gd3+, with a magnetic moment of 7.94 B.M., but the largest magnetic moments, at 10.4–10.7 B.M., are exhibited by Dy3+ and Ho3+. However, in Gd3+ all the electrons have parallel spin and this property is important for the use of gadolinium complexes as contrast reagent in MRI scans.
Crystal field splitting is rather small for the lanthanide ions and is less important than spin-orbit coupling in regard to energy levels. Transitions of electrons between f orbitals are forbidden by the Laporte rule. Furthermore, because of the "buried" nature of the f orbitals, coupling with molecular vibrations is weak. Consequently, the spectra of lanthanide ions are rather weak and the absorption bands are similarly narrow. Glass containing holmium oxide and holmium oxide solutions (usually in perchloric acid) have sharp optical absorption peaks in the spectral range 200–900 nm and can be used as a wavelength calibration standard for optical spectrophotometers, and are available commercially.
As f-f transitions are Laporte-forbidden, once an electron has been excited, decay to the ground state will be slow. This makes them suitable for use in lasers as it makes the population inversion easy to achieve. The Nd:YAG laser is one that is widely used. Europium-doped yttrium vanadate was the first red phosphor to enable the development of color television screens. Lanthanide ions have notable luminescent properties due to their unique 4f orbitals. Laporte forbidden f-f transitions can be activated by excitation of a bound "antenna" ligand. This leads to sharp emission bands throughout the visible, NIR, and IR and relatively long luminescence lifetimes.
The lanthanide contraction is responsible for the great geochemical divide that splits the lanthanides into light and heavy-lanthanide enriched minerals, the latter being almost inevitably associated with and dominated by yttrium. This divide is reflected in the first two "rare earths" that were discovered: yttria (1794) and ceria (1803). The geochemical divide has put more of the light lanthanides in the Earth's crust, but more of the heavy members in the Earth's mantle. The result is that although large rich ore-bodies are found that are enriched in the light lanthanides, correspondingly large ore-bodies for the heavy members are few. The principal ores are monazite and bastnäsite. Monazite sands usually contain all the lanthanide elements, but the heavier elements are lacking in bastnäsite. The lanthanides obey the Oddo-Harkins rule – odd-numbered elements are less abundant than their even-numbered neighbors.
Three of the lanthanide elements have radioactive isotopes with long half-lives (138La, 147Sm and 176Lu) that can be used to date minerals and rocks from Earth, the Moon and meteorites.
Lanthanide elements and their compounds have many uses but the quantities consumed are relatively small in comparison to other elements. About 15000 ton/year of the lanthanides are consumed as catalysts and in the production of glasses. This 15000 tons corresponds to about 85% of the lanthanide production. From the perspective of value, however, applications in phosphors and magnets are more important.
The devices lanthanide elements are used in include superconductors, samarium-cobalt and neodymium-iron-boron high-flux rare-earth magnets, magnesium alloys, electronic polishers, refining catalysts and hybrid car components (primarily batteries and magnets). Lanthanide ions are used as the active ions in luminescent materials used in optoelectronics applications, most notably the Nd:YAG laser. Erbium-doped fiber amplifiers are significant devices in optical-fiber communication systems. Phosphors with lanthanide dopants are also widely used in cathode ray tube technology such as television sets. The earliest color television CRTs had a poor-quality red; europium as a phosphor dopant made good red phosphors possible. Yttrium iron garnet (YIG) spheres can act as tunable microwave resonators. Lanthanide oxides are mixed with tungsten to improve their high temperature properties for welding, replacing thorium, which was mildly hazardous to work with. Many defense-related products also use lanthanide elements such as night vision goggles and rangefinders. The SPY-1 radar used in some Aegis equipped warships, and the hybrid propulsion system of Arleigh Burke-class destroyers all use rare earth magnets in critical capacities. The price for lanthanum oxide used in fluid catalytic cracking has risen from $5 per kilogram in early 2010 to $140 per kilogram in June 2011.
Most lanthanides are widely used in lasers, and as (co-)dopants in doped-fiber optical amplifiers; for example, in Er-doped fiber amplifiers, which are used as repeaters in the terrestrial and submarine fiber-optic transmission links that carry internet traffic. These elements deflect ultraviolet and infrared radiation and are commonly used in the production of sunglass lenses. Other applications are summarized in the following table:
|Petroleum refining catalysts||25|
|Glass polishing and ceramics||7|
As mentioned in the industrial applications section above, lanthanide metals are particularly useful in technologies that take advantage of their reactivity to specific wavelengths of light. Certain life science applications take advantage of the unique fluorescence properties of lanthanide ion complexes (Ln(III) chelates or cryptates). These are well-suited for this application due to their large Stokes shifts and extremely long emission lifetimes (from microseconds to milliseconds) compared to more traditional fluorophores (e.g., fluorescein, allophycocyanin, phycoerythrin, and rhodamine). The biological fluids or serum commonly used in these research applications contain many compounds and proteins which are naturally fluorescent. Therefore, the use of conventional, steady-state fluorescence measurement presents serious limitations in assay sensitivity. Long-lived fluorophores, such as lanthanides, combined with time-resolved detection (a delay between excitation and emission detection) minimizes prompt fluorescence interference.
Time-resolved fluorometry (TRF) combined with fluorescence resonance energy transfer (FRET) offers a powerful tool for drug discovery researchers: Time-Resolved Fluorescence Resonance Energy Transfer or TR-FRET. TR-FRET combines the low background aspect of TRF with the homogeneous assay format of FRET. The resulting assay provides an increase in flexibility, reliability and sensitivity in addition to higher throughput and fewer false positive/false negative results.
This method involves two fluorophores: a donor and an acceptor. Excitation of the donor fluorophore (in this case, the lanthanide ion complex) by an energy source (e.g. flash lamp or laser) produces an energy transfer to the acceptor fluorophore if they are within a given proximity to each other (known as the Förster’s radius). The acceptor fluorophore in turn emits light at its characteristic wavelength.
The two most commonly used lanthanides in life science assays are shown below along with their corresponding acceptor dye as well as their excitation and emission wavelengths and resultant Stokes shift (separation of excitation and emission wavelengths).
|Donor||Excitation⇒Emission λ (nm)||Acceptor||Excitation⇒Emission λ (nm)||Stoke's Shift (nm)|
Upcoming Medical Uses
Currently there is research showing that lanthanides elements can be used as anticancer agents. The main role of the lanthanides in these studies is to inhibit proliferation of the cancer cells. Specifically cerium and lanthanum have been studied for their role as anti-cancer agents.
One of the specific elements from the lanthanide group that has been tested and used is cerium (Ce). There have been studies that use a protein-cerium complex to observe the effect of cerium on the cancer cells. The hope was to inhibit cell proliferation and promote cytotoxicity. Transferrin receptors in cancer cells, such as those in breast cancer cells and epithelial cervical cells, promote the cell proliferation and malignancy of the cancer. Transferrin is a protein used to transport iron into the cells and is needed to aid the cancer cells in DNA replication. Transferrin acts as a growth factor for the cancerous cells and is dependent on iron. Cancer cells have much higher levels of transferrin receptors than normal cells and are very dependent on iron for their proliferation. Cerium has shown results as an anti-cancer agent due to its similarities in structure and biochemistry to iron. Cerium may bind in the place of iron on to the transferrin and then be brought into the cancer cells by transferrin-receptor mediated endocytosis. The cerium binding to the transferrin in place of the iron inhibits the transferrin activity in the cell. This creates a toxic environment for the cancer cells and causes a decrease in cell growth. This is the proposed mechanism for cerium’s effect on cancer cells, though the real mechanism may be more complex in how cerium inhibits cancer cell proliferation. Specifically in HeLa cancer cells studied in vitro, cell viability was decreased after 48 to 72 hours of cerium treatments. Cells treated with just cerium had decreases in cell viability, but cells treated with both cerium and transferrin had more significant inhibition for cellular activity.
Another specific element that has be tested and used as an anti-cancer agent is lanthanum, more specifically lanthanum chloride (LaCl3 ). The lanthanum ion is used to affect the levels of let-7a and microRNAs miR-34a in a cell throughout the cell cycle. When the lanthanum ion was introduced to the cell in vivo or in vitro, it inhibited the rapid growth and induced apoptosis of the cancer cells (specifically cervical cancer cells). This effect was caused by the regulation of the let-7a and microRNAs by the lanthanum ions. The mechanism for this effect is still unclear but it is possible that the lanthanum is acting in a similar way as the cerium and binding to a ligand necessary for cancer cell proliferation.
Due to their sparse distribution in the earth's crust and low aqueous solubility, the lanthanides have a low availability in the biosphere, and are not known to naturally form part of any biological molecules. Compared to most other nondietary elements, non-radioactive lanthanides are classified as having low toxicity.
- The current IUPAC recommendation is that the name lanthanoid be used rather than lanthanide, as the suffix "-ide" is preferred for negative ions, whereas the suffix "-oid" indicates similarity to one of the members of the containing family of elements. However, lanthanide is still favored in most (~90%) scientific articles and is currently adopted on Wikipedia. In the older literature, the name "lanthanon" was often used.
- Gray, Theodore (2009). The Elements: A Visual Exploration of Every Known Atom in the Universe. New York: Black Dog & Leventhal Publishers. p. 240. ISBN 978-1-57912-814-2.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Lanthanide, Encyclopædia Britannica on-line
- Lua error in Module:Citation/CS1/Identifiers at line 47: attempt to index field 'wikibase' (a nil value).
- Helen C. Aspinall (2001). Chemistry of the f-block elements. CRC Press. p. 8. ISBN 90-5699-333-X.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Lua error in Module:Citation/CS1/Identifiers at line 47: attempt to index field 'wikibase' (a nil value).
- Krishnamurthy, Nagaiyar and Gupta, Chiranjib Kumar (2004) Extractive Metallurgy of Rare Earths, CRC Press, ISBN 0-415-33340-7
- Greenwood, Norman N.; Earnshaw, Alan (1997). Chemistry of the Elements (2nd ed.). Butterworth-Heinemann. pp. 1230–1242. ISBN 0-08-037941-9.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Cullity, B. D. and Graham, C. D. (2011) Introduction to Magnetic Materials, John Wiley & Sons, ISBN 9781118211496
- Cotton, Simon (2006). Lanthanide and Actinide Chemistry. John Wiley & Sons Ltd.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Lua error in Module:Citation/CS1/Identifiers at line 47: attempt to index field 'wikibase' (a nil value).
- Holleman, p. 1937.
- dtv-Atlas zur Chemie 1981, Vol. 1, p. 220.
- Winter, Mark. Lanthanum ionisation energies. WebElements Ltd, UK. Retrieved 2010-09-02.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Fukai, Y (2005). The Metal-Hydrogen System, Basic Bulk Properties, 2d edition. Springer. ISBN 978-3-540-00494-3.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Pettit, L. and Powell, K. SC-database. Acadsoft.co.uk. Retrieved on 2012-01-15.
- Aspinall, Helen C. (2001). Chemistry of the f-block elements. Amsterdam [u.a.]: Gordon & Breach. ISBN 905699333X.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Burgess,, J. (1978). 'Metal ions in solution'. , New York: Ellis Horwood. ISBN 0-85312-027-7.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- David A. Atwood, ed. (19 February 2013). The Rare Earth Elements: Fundamentals and Applications (eBook). John Wiley & Sons. ISBN 9781118632635.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Wells, A.F. (1984). Structural Inorganic Chemistry. Oxford Science Publication:ISBN=0-19-855370-6. Unknown parameter
|in=ignored (help)<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Holleman, p. 1942
- Perry, Dale L. (2011). Handbook of Inorganic Compounds, Second Edition. Boca Raton, Florida: CRC Press. p. 125. ISBN 978-1-43981462-8. Retrieved 2014-02-17.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Haschke, John. M. (1979). "Chapter 32:Halides". In Gschneider Jr., K.A. Handbook on the Physics and Chemistry of Rare Earths vol 4. North Holland Publishing Company. pp. 100–110. ISBN 0-444-85216-6.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Binary Rare Earth Oxides, eds. G. Adachi, Nobuhito Imanaka, Zhen Chuan Kang; Springer, 2006, ISBN 1-4020-2568-8
- Nanomagnetism and Spintronics: Fabrication, Materials, Characterization and Applications, ed. Farzad Nasirpouri, Alain Nogaret, World Scientific, 2011, ISBN 9789814273053
- Flahaut, Jean (1979). "Chapter 31:Sulfides, Selenides and Tellurides". In Gschneider Jr., K.A. Handbook on the Physics and Chemistry of Rare Earths vol 4. North Holland Publishing Company. pp. 100–110. ISBN 0-444-85216-6.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Berte, Jean-Noel (2009). "Cerium pigments". In Smith, Hugh M. High Performance Pigments. Wiley-VCH. ISBN 3-527-30204-2.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Holleman, p. 1944.
- Liu, Guokui and Jacquier, Bernard (eds) (2006) Spectroscopic Properties of Rare Earths in Optical Materials, Springer
- Sisniga, Alejandro (2012). "Chapter 15". In Iniewski, Krzysztof. Integrated Microsystems: Electronics, Photonics, and Biotechnology. CRC Press. ISBN 978-3-527-31405-8.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Temmerman, W.M. (2009). "Chapter 241:The Dual, Localized or Band‐Like, Character of the 4f‐States". In Gschneider Jr., K.A. Handbook on the Physics and Chemistry of Rare Earths vol 39. Elsevier. pp. 100–110. ISBN 978-0-444-53221-3.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Dronskowski, R. (2005) Computational Chemistry of Solid State Materials: A Guide for Materials Scientists, Chemists, Physicists and Others, Wiley, ISBN 9783527314102
- Hulliger, F (1979). "Chapter 33:Rare Earth Pnictides". In Gschneider Jr., K.A. Handbook on the Physics and Chemistry of Rare Earths vol 4. North Holland Publishing Company. pp. 100–110. ISBN 0-444-85216-6.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Greenwood, Norman N.; Earnshaw, Alan (1997). Chemistry of the Elements (2nd ed.). Butterworth-Heinemann. pp. 297–299. ISBN 0-08-037941-9.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Mori, Takao (2008). "Chapter 238:Higher Borides". In Gschneider Jr., K.A. Handbook on the Physics and Chemistry of Rare Earths vol 38. North Holland. pp. 105–174. ISBN 978-0-444-521439.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Greenwood, Norman N.; Earnshaw, Alan (1997). Chemistry of the Elements (2nd ed.). Butterworth-Heinemann. p. 147. ISBN 0-08-037941-9.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Refractory Materials, Volume 6-IV: 1976, ed. Allen Alper, Elsevier, ISBN 0-12-053204-2
- Zuckerman, J. J. (2009) Inorganic Reactions and Methods, The Formation of Bonds to Group-I, -II, and -IIIb Elements, Vol. 13, John Wiley & Sons, ISBN 089573-263-7
- Ludwig Reimer (1993). Image Formation in Low-voltage Scanning Electron Microscopy. SPIE Press. ISBN 978-0-8194-1206-5.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- R. P. MacDonald (1964). "Uses for a Holmium Oxide Filter in Spectrophotometry" (PDF). Clinical Chemistry. 10 (12): 1117–20. PMID 14240747.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- "Holmium Glass Filter for Spectrophotometer Calibration". Retrieved 2009-06-06.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- There exist other naturally occurred radioactive isotopes of lanthanides with long half-lives (144Nd, 150Nd, 148Sm, 151Eu, 152Gd) but they are not used as chronometers.
- McGill, Ian (2005) "Rare Earth Elements" in Ullmann's Encyclopedia of Industrial Chemistry, Wiley-VCH, Weinheim. doi:10.1002/14356007.a22 607.
- "Haxel G, Hedrick J, Orris J. 2006. Rare earth elements critical resources for high technology. Reston (VA): United States Geological Survey. USGS Fact Sheet: 087‐02" (PDF). Retrieved 2008-04-19.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Livergood R. (2010). "Rare Earth Elements: A Wrench in the Supply Chain" (PDF). Center for Strategic and International Studies. Retrieved 2010-10-22.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- Chu, Steven. Critical Materials Strategy p. 17 United States Department of Energy, December 2011. Accessed: 23 December 2011.
- Holleman, Arnold F.; Wiberg, Egon; Wiberg, Nils (2007). Lehrbuch der Anorganischen Chemie (in German) (102 ed.). Walter de Gruyter. p. 1942. ISBN 978-3-11-017770-1. <templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
- lanthanide Sparkle Model, used in the computational chemistry of lanthanide complexes
- USGS Rare Earths Statistics and Information
- Ana de Bettencourt-Dias: Chemistry of the lanthanides and lanthanide-containing materials
|Periodic table (Large cells)|