Copper(I) oxide

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Template:Chembox E numberTemplate:Chembox SolubilityInWater
Copper(I) oxide
IUPAC name Copper(I) oxide
Other names Cuprous oxide
Cuprite (mineral)
Red copper oxide
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RTECS number GL8050000
Molar mass 143.09 g/mol
Appearance Brownish-red solid
Density 6.0 g/cm3, solid
Melting point
Crystal structure cubic
R/S statement R: 22
S: 22
Related compounds
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Except where noted otherwise, data are given for
materials in their standard state
(at 25 °C, 100 kPa)

Infobox disclaimer and references

Copper(I) oxide or cuprous oxide (Cu2O) is an oxide of copper. It is insoluble in water and organic solvents. Copper(I) oxide dissolves in concentrated ammonia solution to form the colourless complex[Cu(NH3)2]+, which easily oxidizes in air to the blue[Cu(NH3)4(H2O)2]2+. It dissolves in hydrochloric acid to form HCuCl2 (a complex of CuCl), while dilute sulfuric acid and nitric acid produce copper(II) sulfate and copper(II) nitrate, respectively.

Copper(I) oxide is found as the mineral cuprite in some red-colored rocks. When it is exposed to oxygen, copper will naturally oxidize to copper(I) oxide, but this takes extensive periods of time. Artificial formation is usually accomplished at high temperature or at high oxygen pressure. With further heating, copper(I) oxide will form copper(II) oxide.

Formation of copper(I) oxide is the basis of the Fehling's test and Benedict's test for reducing sugars which reduce an alkaline solution of a copper(II) salt and give a precipitate of Cu2O.

Cuprous oxide forms on silver-plated copper parts exposed to moisture when the silver layer is porous or damaged; this kind of corrosion is known as red plague.

General applications

Cuprous oxide is commonly used as a pigment, a fungicide and an antifouling agent for marine paints.

Applications as semiconductor

Copper(I) oxide was the first substance known to behave as a semiconductor. Rectifier diodes based on this material were used industrially as early as 1924, long before silicon became the standard.

Copper(I) oxide shows four well understood series of excitons with resonance widths in the range of neV. The associated polaritons are also well understood; their group velocity turns out to be very low, almost down to the speed of sound. That means light moves almost as slow as sound in this medium. This results in high polariton densities, and effects like Bose-Einstein condensation, the dynamical Stark effect and phonoritons have been demonstrated.

Another extraordinary feature of the ground state excitons is that all primary scattering mechanisms are known quantitatively. Cu2O was the first substance where an entirely parameter-free model of absorption linewidth broadening by temperature could be established, allowing the corresponding absorption coefficient to be deduced. It can be shown using Cu2O that the Kramers-Krönig relations do not apply to polaritons.

See also


  1. N. N. Greenwood, A. Earnshaw, Chemistry of the Elements, 2nd ed., Butterworth-Heinemann, Oxford, UK, 1997.
  2. Handbook of Chemistry and Physics, 71st edition, CRC Press, Ann Arbor, Michigan, 1990.
  3. The Merck Index, 7th edition, Merck & Co, Rahway, New Jersey, USA, 1960.
  4. D. Nicholls, Complexes and First-Row Transition Elements, Macmillan Press, London, 1973.
  5. P.W. Baumeister: Optical Absorption of Cuprous Oxide, Phys. Rev. 121 (1961), 359.
  6. L. Brillouin: Wave Propagation and Group Velocity, Academic Press, New York, 1960.
  7. D. Fröhlich, A. Kulik, B. Uebbing, and A. Mysyrovicz: Coherent Propagation and Quantum Beats of Quadrupole Polaritons in Cu2O, Phys. Rev. Lett. 67 (1991), 2343.
  8. L. Hanke: Transformation von Licht in Wärme in Kristallen - Lineare Absorption in Cu2O, ISBN 3-8265-7269-6, Shaker, Aachen, 2000; (Transformation of light into heat in crystals - Linear absorption in Cu2O).
  9. L. Hanke, D. Fröhlich, A.L. Ivanov, P.B. Littlewood, and H. Stolz: LA-Phonoritons in Cu2O, Phys. Rev. Lett. 83 (1999), 4365.
  10. L. Hanke, D. Fröhlich, and H. Stolz: Direct observation of longitudinal acoustic phonon absorption to the 1S-exciton in Cu2O, Sol. Stat. Comm. 112 (1999), 455.
  11. J.J. Hopfield, Theory of the Contribution of Excitons to the Complex Dielectric Constant of Crystals, Phys. Rev. 112 (1958), 1555.
  12. J.P. Wolfe and A. Mysyrowicz: Excitonic Matter, Scientific American 250 (1984), No. 3, 98.
  13. Knovel Critical Tables., Knovel, 2003.

External links

ar:أكسيد نحاس أحادي cs:Oxid měďný da:Kobber(I)oxid de:Kupfer(I)-oxid hu:Réz(I)-oxid