At high pressure and temperatures, metallic hydrogen might exist as a liquid rather than a solid, and researchers think it is present in large quantities in the hot and gravitationally compressed interiors of Jupiter, Saturn, and in some extrasolar planets.
- 1 Theoretical predictions
- 2 Experimental pursuit
- 2.1 Shock-wave compression, 1996
- 2.2 Other experimental research, 1996–2004
- 2.3 Pulsed laser heating experiment, 2008
- 2.4 Observation of liquid metallic hydrogen, 2011
- 2.5 Z machine, 2015
- 2.6 Claimed observation of solid metallic hydrogen, 2016
- 2.7 Experiments on fluid deuterium at the National Ignition Facility, 2018
- 3 See also
- 4 References
Metallization of hydrogen under pressure
Though often placed at the top of the alkali metal column in the periodic table, hydrogen does not, under ordinary conditions, exhibit the properties of an alkali metal. Instead, it forms diatomic H
2 molecules, analogous to halogens and non-metals in the second row of the periodic table, such as nitrogen and oxygen. Diatomic hydrogen is a gas that, at atmospheric pressure, liquefies and solidifies only at very low temperature (20 degrees and 14 degrees above absolute zero, respectively). Eugene Wigner and Hillard Bell Huntington predicted that under an immense pressure of around 25 GPa (250,000 atm; 3,600,000 psi) hydrogen would display metallic properties: instead of discrete H
2 molecules (which consist of two electrons bound between two protons), a bulk phase would form with a solid lattice of protons and the electrons delocalized throughout. Since then, producing metallic hydrogen in the laboratory has been described as "...the holy grail of high-pressure physics."
The initial prediction about the amount of pressure needed was eventually shown to be too low. Since the first work by Wigner and Huntington, the more modern theoretical calculations point towards higher but nonetheless potentially accessible metallization pressures of around 400 GPa (3,900,000 atm; 58,000,000 psi).
Liquid metallic hydrogen
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 might be a range of densities, at pressures around 400 GPa, where hydrogen would be a liquid metal, even at low temperatures.
Geng predicted that the ZPE of protons indeed lowers the melting temperature of hydrogen to a minimum of 200–250 K (−73 – −23 °C) at pressures of 500–1,500 GPa (4,900,000–14,800,000 atm; 73,000,000–218,000,000 psi), within this flat region there might have an elemental mesophase intermediate between the liquid and solid state.
In 1968, Neil Ashcroft suggested that metallic hydrogen might be a superconductor, up to room temperature (290 K or 17 °C), far higher than any other known candidate material. This hypothesis is based on an expected strong coupling between conduction electrons and lattice vibrations.
Possibility of novel types of quantum fluid
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 might have quantum ordered states that cannot be classified as superconducting or superfluid in the usual sense. Instead, they might 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 a magnetic field, hydrogen might exhibit phase transitions from superconductivity to superfluidity and vice versa.
Lithium alloying reduces requisite pressure
In 2009, Zurek et al. predicted that the alloy LiH
6 would be a stable metal at only one quarter of the pressure required to metallize hydrogen, and that similar effects should hold for alloys of type LiHn and possibly "other alkali high-hydride systems", i.e. alloys of type XHn where X is an alkali metal.
Shock-wave compression, 1996
In March 1996, a group of scientists at Lawrence Livermore National Laboratory reported that they had serendipitously produced the first identifiably metallic hydrogen for about a microsecond at temperatures of thousands of kelvins, pressures of over 100 GPa (1,000,000 atm; 15,000,000 psi), and densities of approximately . 0.6 g/cm3 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 250 GPa (2,500,000 atm; 37,000,000 psi), did not confirm detectable metallization. The team had sought simply to measure the less extreme electrical conductivity changes they expected. 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 140 GPa (1,400,000 atm; 21,000,000 psi), 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 eV, making it an 15 insulator but, as the pressure increases significantly, the band-gap gradually fell to . Because the 0.3 eVthermal energy of the fluid (the temperature became about 3,000 K or 2,730 °C due to compression of the sample) was above , the hydrogen might be considered metallic. 0.3 eV
Other experimental research, 1996–2004
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, 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 (320–340 GPa or 3,200,000–3,400,000 atm) and temperatures of 100–300 K (−173–27 °C), 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. 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.
Pulsed laser heating experiment, 2008
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. Hydrogen-rich molecular silane (SiH
4) was claimed to be metallized and become superconducting by M.I. Eremets et al.. This claim is disputed, and their results have not been repeated.
Observation of liquid metallic hydrogen, 2011
In 2011 Eremets and Troyan reported observing the liquid metallic state of hydrogen and deuterium at static pressures of 260–300 GPa (2,600,000–3,000,000 atm). This claim was questioned by other researchers in 2012.
Z machine, 2015
In 2015, scientists at the Z Pulsed Power Facility announced the creation of metallic deuterium using dense liquid deuterium, an electrical insulator-to-conductor transition associated with an increase in optical reflectivity.
Claimed observation of solid metallic hydrogen, 2016
On 5 October 2016, Ranga Dias and Isaac F. Silvera of Harvard University released claims of experimental evidence that solid metallic hydrogen had been synthesised in the laboratory at a pressure of around 495 gigapascals (4,890,000 atm; 71,800,000 psi) using a diamond anvil cell. This manuscript was available in October 2016, and a revised version was subsequently published in the journal Science in January 2017.
In the preprint version of the paper, Dias and Silvera write:
With increasing pressure we observe changes in the sample, going from transparent, to black, to a reflective metal, the latter studied at a pressure of 495 GPa... the reflectance using a Drude free electron model to determine the plasma frequency of 30.1 eV at T = 5.5 K, with a corresponding electron carrier density of ×1023 particles/cm3, consistent with theoretical estimates. The properties are those of a metal. Solid metallic hydrogen has been produced in the laboratory. 6.7— Dias & Silvera (2016) 
Silvera stated that they did not repeat their experiment, since more tests could damage or destroy their existing sample, but assured the scientific community that more tests are coming. He also stated that the pressure would eventually be released, in order to find out whether the sample was metastable (i.e., whether it would persist in its metallic state even after the pressure was released).
Shortly after the claim was published in Science, Nature's news division published an article stating that some other physicists regarded the result with skepticism. Recently, prominent members of the high pressure research community have criticised the claimed results, questioning the claimed pressures or the presence of metallic hydrogen at the pressures claimed.
In February 2017, it was reported that the sample of claimed metallic hydrogen was lost, after the diamond anvils it was contained between broke.
In August 2017, Silvera and Dias issued an erratum to the Science article, regarding corrected reflectance values due to variations between the optical density of stressed natural diamonds and the synthetic diamonds used in their pre-compression diamond anvil cell.
Experiments on fluid deuterium at the National Ignition Facility, 2018
In August 2018, scientists announced new observations  regarding the rapid transformation of fluid deuterium from an insulating to a metallic form below 2000 K. Remarkable agreement is found between the experimental data and the predictions based on Quantum Monte Carlo simulations, which is expected to be the most accurate method to date. This may help researchers better understand giant gas planets, such as Jupiter, Saturn and related exoplanets, since such planets are thought to contain a lot of liquid metallic hydrogen, which may be responsible for their observed powerful magnetic fields.
- Stevenson, D. J. (2008). "Metallic helium in massive planets". Proceedings of the National Academy of Sciences. 105 (32): 11035–11036. Bibcode:2008PNAS..10511035S. doi:10.1073/pnas.0806430105. PMC 2516209.
- 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.
- Guillot, T.; Stevenson, D. J.; Hubbard, W. B.; Saumon, D. (2004). "Chapter 3: The Interior of Jupiter". In Bagenal, F.; Dowling, T. E.; McKinnon, W. B. Jupiter: The Planet, Satellites and Magnetosphere. Cambridge University Press. ISBN 0-521-81808-7.
- "High-pressure scientists 'journey' to the center of the Earth, but can't find elusive metallic hydrogen" (Press release). ScienceDaily. 6 May 1998. Retrieved 28 January 2017.
- Loubeyre, P.; et al. (1996). "X-ray diffraction and equation of state of hydrogen at megabar pressures". Nature. 383 (6602): 702–704. Bibcode:1996Natur.383..702L. doi:10.1038/383702a0.
- Azadi, S.; Monserrat, B.; Foulkes, W.M.C.; Needs, R.J. (2014). "Dissociation of High-Pressure Solid Molecular Hydrogen: A Quantum Monte Carlo and Anharmonic Vibrational Study". Phys. Rev. Lett. 112: 165501. arXiv:1403.3681. Bibcode:2014PhRvL.112p5501A. doi:10.1103/PhysRevLett.112.165501.
- McMinis, J.; Clay, R.C.; Lee, D.; Morales, M.A. (2015). "Molecular to Atomic Phase Transition in Hydrogen under High Pressure". Phys. Rev. Lett. 114: 105305. Bibcode:2015PhRvL.114j5305M. doi:10.1103/PhysRevLett.114.105305.
- Ashcroft, N. W. (2000). "The hydrogen liquids". Journal of Physics: Condensed Matter. 12 (8A): 129. Bibcode:2000JPCM...12..129A. doi:10.1088/0953-8984/12/8A/314.
- Bonev, S. A.; et al. (2004). "A quantum fluid of metallic hydrogen suggested by first-principles calculations". Nature. 431 (7009): 669–672. arXiv:cond-mat/0410425. Bibcode:2004Natur.431..669B. doi:10.1038/nature02968. PMID 15470423.
- Geng, H. Y.; et al. (2015). "Lattice stability and high-pressure melting mechanism of dense hydrogen up to 1.5 TPa". Physical Review B. 92: 104103. doi:10.1103/PhysRevB.92.104103.
- Geng, H. Y.; et al. (2016). "Predicted reentrant melting of dense hydrogen at ultra-high pressures". Scientific Reports. 6: 36745. doi:10.1038/srep36745.
- Geng, H. Y.; et al. (2017). "Prediction of a mobile solid state in dense hydrogen under high pressures". J. Phys. Chem. Lett. 8 (1): 223–228. doi:10.1021/acs.jpclett.6b02453.
- Ashcroft, N. W. (1968). "Metallic Hydrogen: A High-Temperature Superconductor?". Physical Review Letters. 21 (26): 1748–1749. Bibcode:1968PhRvL..21.1748A. doi:10.1103/PhysRevLett.21.1748.
- Babaev, E.; Ashcroft, N. W. (2007). "Violation of the London law and Onsager–Feynman quantization in multicomponent superconductors". Nature Physics. 3 (8): 530–533. arXiv:0706.2411. Bibcode:2007NatPh...3..530B. doi:10.1038/nphys646.
- Babaev, E.; Sudbø, A.; Ashcroft, N. W. (2004). "A superconductor to superfluid phase transition in liquid metallic hydrogen". Nature. 431 (7009): 666–668. arXiv:cond-mat/0410408. Bibcode:2004Natur.431..666B. doi:10.1038/nature02910. PMID 15470422.
- Babaev, 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.
- 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.
- Weir, S. T.; Mitchell, A. C.; Nellis, W. J. (1996). "Metallization of fluid molecular hydrogen at 140 GPa (1.4 Mbar)". Physical Review Letters. 76 (11): 1860–1863. Bibcode:1996PhRvL..76.1860W. doi:10.1103/PhysRevLett.76.1860.
0.28–0.36 mol/cm3 and 2200–4400 K
- 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
- Ruoff, A. L.; et al. (1998). "Solid hydrogen at 342 GPa: No evidence for an alkali metal". Nature. 393 (6680): 46–49. Bibcode:1998Natur.393...46N. doi:10.1038/29949.
- 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.
- 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): 7017–7023. Bibcode:2004JPCM...16.7017B. doi:10.1088/0953-8984/16/39/034.
- Deemyad, S.; Silvera, I. F (2008). "The melting line of hydrogen at high pressures". Physical Review Letters. 100 (15): 155701. arXiv:0803.2321. Bibcode:2008PhRvL.100o5701D. doi:10.1103/PhysRevLett.100.155701. PMID 18518124.
- Eremets, M. I.; et al. (2008). "Superconductivity in hydrogen dominant materials: Silane". Science. 319 (5869): 1506–9. Bibcode:2008Sci...319.1506E. doi:10.1126/science.1153282. PMID 18339933.
- Degtyareva, O.; et al. (2009). "Formation of transition metal hydrides at high pressures". Solid State Communications. 149 (39–40): 1583–1586. arXiv:0907.2128. Bibcode:2009SSCom.149.1583D. doi:10.1016/j.ssc.2009.07.022.
- Hanfland, M.; Proctor, J. E.; Guillaume, C. L.; Degtyareva, O.; Gregoryanz, E. (2011). "High-Pressure Synthesis, Amorphization, and Decomposition of Silane". Physical Review Letters. 106 (9): 095503. Bibcode:2011PhRvL.106i5503H. doi:10.1103/PhysRevLett.106.095503. PMID 21405634.
- Eremets, M. I.; Troyan, I. A. (2011). "Conductive dense hydrogen". Nature Materials. 10 (12): 927–931. Bibcode:2011NatMa..10..927E. doi:10.1038/nmat3175.
- Dalladay-Simpson, P.; Howie, R.; Gregoryanz, E. (2016). "Evidence for a new phase of dense hydrogen above 325 gigapascals". Nature. 529 (7584): 63–67. Bibcode:2016Natur.529...63D. doi:10.1038/nature16164. PMID 26738591.
- Nellis, W. J.; Ruoff, A. L.; Silvera, I. S. (2012). "Has Metallic Hydrogen Been Made in a Diamond Anvil Cell?". arXiv:1201.0407 [cond-mat.other].
no evidence for MH
- Amato, I. (2012). "Metallic hydrogen: Hard pressed". Nature. 486 (7402): 174–176. Bibcode:2012Natur.486..174A. doi:10.1038/486174a. PMID 22699591.
- Knudson, M.; Desjarlais, M.; Becker, A. (2015). "Direct observation of an abrupt insulator-to-metal transition in dense liquid deuterium". Science. 348 (6242): 1455–1460. Bibcode:2015Sci...348.1455K. doi:10.1126/science.aaa7471.
- "Z machine puts the squeeze on metallic deuterium". Chemistry World. Retrieved 27 January 2017.
- Crane, L. (26 January 2017). "Metallic hydrogen finally made in lab at mind-boggling pressure". New Scientist. Retrieved 26 January 2017.
- Dias, R. P.; Silvera, I. F. (2017). "Observation of the Wigner-Huntington transition to metallic hydrogen". Science. 355: 715–718. arXiv:1610.01634. Bibcode:2017Sci...355..715D. doi:10.1126/science.aal1579.
- Dias, R.; Silvera, I. F. (2016). "Observation of the Wigner-Huntington Transition to Solid Metallic Hydrogen". arXiv:1610.01634 [cond-mat.mtrl-sci].
- Lemmonick, S. (27 January 2017). "There's Reason To Be Skeptical About Metallic Hydrogen". Forbes. Retrieved 28 January 2017.
- Castelvecchi, D. (2017). "Physicists doubt bold report of metallic hydrogen". Nature. 542: 17. Bibcode:2017Natur.542...17C. doi:10.1038/nature.2017.21379.
- MacDonald, Fiona. "Metallic hydrogen has been created for the first time". Retrieved 24 December 2017.
- Goncharov, A.F.; Struzhkin, V. V. (2017). "Comment on Observation of the Wigner-Huntington Transition to Solid Metallic Hydrogen". arXiv:1702.04246 [cond-mat].
- Eremets, M.I.; Drozdov, A. P. (2017). "Comments on the claimed observation of the Wigner-Huntington Transition to Metallic Hydrogen". arXiv:1702.05125 [cond-mat].
- Loubeyre, P.; Occelli, F.; Dumas, P. (2017). "Comment on: Observation of the Wigner-Huntington Transition to Metallic Hydrogen". arXiv:1702.07192 [cond-mat].
- Geng, Hua Y. (2017). "Public debate on metallic hydrogen to boost high pressure research". Matter and Radiation at Extremes. 2 (6): 275–277. doi:10.1016/j.mre.2017.10.001.
- Johnston, Ian (13 February 2017). "World's only piece of a metal that could revolutionise technology has disappeared, scientists reveal". Independent.
- Dias, R.; Silvera, I. F. (18 August 2017). "Erratum for the Research Article "Observation of the Wigner-Huntington transition to metallic hydrogen"". Science. p. 6352.
- Celliers, Peter M.; Millot, Marius; Brygoo, Stephanie; McWilliams, R. Stewart; Fratanduono, Dayne E.; Rygg, J. Ryan; Goncharov, Alexander F.; Loubeyre, Paul; Eggert, Jon H.; Peterson, J. Luc; Meezan, Nathan B.; Pape, Sebastien Le; Collins, Gilbert W.; Jeanloz, Raymond; Hemley, Russell J. (17 August 2018). "Insulator-metal transition in dense fluid deuterium". Science. 361 (6403): 677–682. doi:10.1126/science.aat0970. ISSN 0036-8075.
- Chang, Kenneth (16 August 2018). "Settling Arguments About Hydrogen With 168 Giant Lasers". The New York Times. Retrieved 18 August 2018.
- "Under pressure, hydrogen offers a reflection of giant planet interiors". Carnegie Institution for Science. 15 August 2018. Retrieved 19 August 2018.