Metallic hydrogen

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A diagram showing the inside of Jupiter
Gas giants such as Jupiter (pictured above) and Saturn may contain large amounts of metallic hydrogen (depicted in grey) and metallic helium[1]

Metallic hydrogen is a phase of hydrogen in which it behaves as an electrical conductor. This phase was predicted theoretically in 1935[2] but has yet to be unambiguously observed, but possibly some new phases of solid hydrogen have been observed under static conditions[3][4] and electrical insulator to conductor transitions have been reported associated with an increase in optical reflectivity in dense liquid deuterium which is consistent with metallic behaviour.[5] At high pressure, on the order of hundreds of gigapascals, hydrogen might exist as a liquid rather than a solid. Liquid and solid metallic hydrogen is thought to be present in large amounts in the gravitationally compressed interiors of Jupiter, Saturn, and in some extrasolar planets.

Theoretical predictions[edit]

Metallization of hydrogen under pressure[edit]

Though at the top of the alkali metal column in the periodic table, hydrogen is not, under ordinary conditions, an alkali metal. In 1935 physicists Eugene Wigner and Hillard Bell Huntington predicted that under an immense pressure of around 25 GPa (250000 atm or 3500000 psi), hydrogen atoms would display metallic properties, losing hold over their electrons.[2] Since then, metallic hydrogen has been described as "the holy grail of high-pressure physics".[6]

The initial prediction about the amount of pressure needed was eventually proven to be too low.[7] Since the first work by Wigner and Huntington, the more modern theoretical calculations were pointing toward higher but nonetheless potentially accessible metallization pressures. Techniques are being developed for creating pressures of up to 500 GPa, higher than the pressure at the center of the Earth, in hopes of creating metallic hydrogen.[8]

Liquid metallic hydrogen[edit]

Helium-4 is a liquid at normal pressure near absolute zero, a consequence of its high zero-point energy (ZPE). The ZPE of protons in a dense state is also high, and a decline in the ordering energy (relative to the ZPE) is expected at high pressures. Arguments have been advanced by Neil Ashcroft and others that there is a melting point maximum in compressed hydrogen, but also that there may be a range of densities (at pressures around 400 GPa) where hydrogen may be a liquid metal, even at low temperatures.[9][10]


In 1968, Neil Ashcroft put forward that metallic hydrogen may be a superconductor, up to room temperature (~290 K), far higher than any other known candidate material. This stems from its extremely high speed of sound and the expected strong coupling between the conduction electrons and the lattice vibrations.[11]

Possibility of novel types of quantum fluid[edit]

Presently known "super" states of matter are superconductors, superfluid liquids and gases, and supersolids. Egor Babaev predicted that if hydrogen and deuterium have liquid metallic states, they may have quantum ordered states which cannot be classified as superconducting or superfluid in the usual sense. Instead, they may represent two possible novel types of quantum fluids: "superconducting superfluids" and "metallic superfluids". Such fluids were predicted to have highly unusual reactions to external magnetic fields and rotations, which might provide a means for experimental verification of Babaev's predictions. It has also been suggested that, under the influence of magnetic field, hydrogen may exhibit phase transitions from superconductivity to superfluidity and vice versa.[12][13][14]

Lithium doping reduces requisite pressure[edit]

In 2009, Zurek et al. predicted that the alloy LiH6 would be a stable metal at only 14 of the pressure required to metallize hydrogen, and that similar effects should hold for alloys of type LiHn and possibly other alloys of type ?Lin.[15]

Experimental pursuit[edit]

Shock-wave compression, 1996[edit]

In March 1996, a group of scientists at Lawrence Livermore National Laboratory reported that they had serendipitously produced, for about a microsecond at temperatures of thousands of kelvins, pressures of over a million atmospheres (>100 GPa) and density of approximately 0.6 g/cm3,[16] the first identifiably metallic hydrogen.[17] The team did not expect to produce metallic hydrogen, as it was not using solid hydrogen, thought to be necessary, and was working at temperatures above those specified by metallization theory. Previous studies in which solid hydrogen was compressed inside diamond anvils to pressures of up to 2,500,000 atm (250 GPa), did not confirm detectable metallization. The team had sought simply to measure the less extreme electrical conductivity changes which were expected to occur. The researchers used a 1960s-era light-gas gun, originally employed in guided missile studies, to shoot an impactor plate into a sealed container containing a half-millimeter thick sample of liquid hydrogen. The liquid hydrogen was in contact with wires leading to a device measuring electrical resistance. The scientists found that, as pressure rose to 1,400,000 atm (140 GPa), the electronic energy band gap, a measure of electrical resistance, fell to almost zero. The band-gap of hydrogen in its uncompressed state is about 15 eV, making it an insulator but, as the pressure increases significantly, the band-gap gradually fell to 0.3 eV. Because the thermal energy of the fluid (the temperature became about 3000 K due to compression of the sample) was above 0.3 eV, the hydrogen might be considered metallic.

Other experimental research, 1996 – 2004[edit]

Many experiments are continuing in the production of metallic hydrogen in laboratory conditions at static compression and low temperature. Arthur Ruoff and Chandrabhas Narayana from Cornell University in 1998,[18] and later Paul Loubeyre and René LeToullec from Commissariat à l'Énergie Atomique, France in 2002, have shown that at pressures close to those at the center of the Earth (3.2 to 3.4 million atmospheres or 324 to 345 GPa) and temperatures of 100–300 K, hydrogen is still not a true alkali metal, because of the non-zero band gap. The quest to see metallic hydrogen in laboratory at low temperature and static compression continues. Studies are also ongoing on deuterium.[19] Shahriar Badiei and Leif Holmlid from the University of Gothenburg have shown in 2004 that condensed metallic states made of excited hydrogen atoms (Rydberg matter) are effective promoters to metallic hydrogen.[20]

Pulsed laser heating experiment, 2008[edit]

The theoretically predicted maximum of the melting curve (the prerequisite for the liquid metallic hydrogen) was discovered by Shanti Deemyad and Isaac F. Silvera by using pulsed laser heating.[21] Hydrogen-rich molecular SiH4 was claimed to be metallized and become superconducting by M.I. Eremets et al..[22] This claim is disputed, and their results have not been repeated.[23][24]

Observation of liquid metallic hydrogen, 2011[edit]

In 2011 Eremets and Troyan reported observing the liquid metallic state of hydrogen and deuterium at static pressures of 260–300 GPa.[25] This claim was questioned by other researchers in 2012.[26][27]

Z machine, 2015[edit]

Scientists at Z machine announced in 2015 creation of metallic deuterium.[28]

See also[edit]


  1. ^
  2. ^ a b Wigner, E.; Huntington, H.B. (1935). "On the possibility of a metallic modification of hydrogen". Journal of Chemical Physics 3 (12): 764. Bibcode:1935JChPh...3..764W. doi:10.1063/1.1749590. 
  3. ^ Eremets, M.I.; Troyan, I.A. (2011). "Conductive dense hydrogen". Nature Materials. Bibcode:2011NatMa..10..927E. doi:10.1038/nmat3175. 
  4. ^ Dalladay-Simpson, Philip; Howie, Ross; Gregoryanz, Eugene (2016). "Evidence for a new phase of dense hydrogen above 325 gigapascals". Nature 529: 63–67. doi:10.1038/nature16164. 
  5. ^ Knudson, M.; Desjarlais, M; Becker, A (2015). "Direct observation of an abrupt insulator-to-metal transition in dense liquid deuterium". Science 348 (6242). 
  6. ^ "High-pressure scientists 'journey' to the center of the Earth, but can't find elusive metallic hydrogen" (Press release). Cornell News. 6 May 1998. Retrieved 2010-01-02. 
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  8. ^ "Peanut butter diamonds on display". BBC News. 27 June 2007. Retrieved 2010-01-02. 
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  10. ^ Bonev, S.A.; et al. (2004). "A quantum fluid of metallic hydrogen suggested by first-principles calculations". Nature 431 (7009): 669. arXiv:cond-mat/0410425. Bibcode:2004Natur.431..669B. doi:10.1038/nature02968. 
  11. ^ Ashcroft, N.W. (1968). "Metallic Hydrogen: A High-Temperature Superconductor?". Physical Review Letters 21 (26): 1748. Bibcode:1968PhRvL..21.1748A. doi:10.1103/PhysRevLett.21.1748. 
  12. ^ Babaev, E.; Ashcroft, N.W. (2007). "Violation of the London law and Onsager–Feynman quantization in multicomponent superconductors". Nature Physics 3 (8): 530. arXiv:0706.2411. Bibcode:2007NatPh...3..530B. doi:10.1038/nphys646. 
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  14. ^ Babaev, Egor; E. (2002). "Vortices with fractional flux in two-gap superconductors and in extended Faddeev model". Physical Review Letters 89 (6): 067001. arXiv:cond-mat/0111192. Bibcode:2002PhRvL..89f7001B. doi:10.1103/PhysRevLett.89.067001. PMID 12190602. 
  15. ^ Zurek, E.; et al. (2009). "A little bit of lithium does a lot for hydrogen". Proceedings of the National Academy of Sciences 106 (42): 17640–3. Bibcode:2009PNAS..10617640Z. doi:10.1073/pnas.0908262106. PMC 2764941. PMID 19805046. 
  16. ^ Nellis, W.J. (2001). "Metastable Metallic Hydrogen Glass" (PDF). Lawrence Livermore Preprint UCRL-JC-142360. OSTI 15005772. minimum electrical conductivity of a metal at 140 GPa, 0.6 g/cm3, and 3000 K 
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  19. ^ Baer, B.J.; Evans, W.J.; Yoo, C.-S. (2007). "Coherent anti-Stokes Raman spectroscopy of highly compressed solid deuterium at 300 K: Evidence for a new phase and implications for the band gap". Physical Review Letters 98 (23): 235503. Bibcode:2007PhRvL..98w5503B. doi:10.1103/PhysRevLett.98.235503. 
  20. ^ Badiei, S.; Holmlid, L. (2004). "Experimental observation of an atomic hydrogen material with H–H bond distance of 150 pm suggesting metallic hydrogen". Journal of Physics: Condensed Matter 16 (39): 7017. Bibcode:2004JPCM...16.7017B. doi:10.1088/0953-8984/16/39/034. 
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  28. ^