Next Article in Journal
pXRF Measurements on Soil Samples for the Exploration of an Antimony Deposit: Example from the Vendean Antimony District (France)
Previous Article in Journal
Production, Reserves, and Processing of Feldspar and Feldspathoid Rocks in the Czech Republic from 2005 to 2019—An Overview
Previous Article in Special Issue
The Viscosity and Atomic Structure of Volatile-Bearing Melilititic Melts at High Pressure and Temperature and the Transport of Deep Carbon
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Editorial

Editorial for the Special Issue “Properties of Melt and Minerals at High Pressures and High Temperature”

Department of Sciences, University of Studies Roma Tre, L.go San Leonardo Murialdo 1, 00146 Rome, Italy
Minerals 2020, 10(8), 723; https://doi.org/10.3390/min10080723
Submission received: 27 July 2020 / Revised: 12 August 2020 / Accepted: 13 August 2020 / Published: 18 August 2020
This Special Volume sets out to summarize knowledge in the rapidly developing area of the high-pressure and high-temperature properties and structure of silicate melts and minerals.
A silicate melt phase is the essential component of nearly all igneous processes. Silicate melts have acted as transport agents in the chemical and physical differentiation of the earth into core, mantle and crust throughout the Earth since its early beginning. Although near-surface melts are observed directly during volcanic eruptions, the Earth’s interior is not easily accessible, and the quantitative understanding of the high P and T properties of magmas within the Earth must be achieved via the simultaneous development of theory, experiment and simulation. Our understanding of how silicate melts behave at depths of the Earth is vital because of our vulnerability to volcanic activity, as eruptions can vary widely in style, scale, duration and frequency depending on magma behavior.
High-pressure mineralogy studies have recently benefited from extraordinary developments in high-pressure high-temperature techniques. Minerals can now be investigated in the P-T conditions pertaining to the whole Earth, from the near-surface to the inner core, with a precision and accuracy that parallel ambient condition measurements. High-pressure and high-temperature physical and chemical properties of minerals must be properly characterized to understand, from the atomic to global scale, the structure and the dynamic evolution of our “living” planet.
In the last few years, rather fast progress has been made in these areas of science, mostly through an interdisciplinary effort, and it appeared timely to produce a review volume summarizing the current state of the art. Here, we present a collection of papers that significantly improves our understanding of the behavior of the liquid and solid state of silicates at high P and T and provides us with a glimpse of future directions and challenges.
The range of topics we have tried to cover is broad, spanning a wide range of experimental techniques, properties investigated and pressures within the Earth’s mantle, from the core–mantle boundary (CMB) to the upper mantle to more shallower depths pertaining to the volcanic realm.
In the study of Thorne et al. [1], new ultralow-velocity zones (ULVZs) at the core–mantle boundary (CMB) were identified based on the processing of a new collection of 58.155 broadband recordings of the seismic phase SPdKS in the epicentral distance range from 106° to 115°. The authors used a Bayesian approach to identify the regions of the CMB that have the highest probability of containing ULVZs, thereby identifying sixteen new regions of interest. These zones most likely contain partial melt, extremely high iron content ferropericlase, or combinations of both.
The ultralow-velocity zones are formed by the density contrast between the melt and the mantle material [2,3,4,5,6], which controls the migration of the magma during the differentiation process. Depending on the density contrast between silicate melts and the ambient mantle, melts can either migrate upwards or sink into the deep interior, resulting in melt pods, which have been suggested by geophysical observations, at the lithosphere–asthenosphere boundary, atop the 410 and 660 km discontinuities, and, as in [1], in the ultra-low velocity zone above the core–mantle boundary. Knowledge of the density of silicate melts at high pressures is therefore essential to evaluate their gravitational stability in the mantle as well as to model the solidification of the early magma ocean and the differentiation of the early Earth [7,8,9,10,11,12].
In the study of Xu et al. [13], the volumetric compression and the density of jadeite melts were obtained at high pressures and high temperatures up to 4.8 GPa and 1955 K by three-dimensional volume imaging using the synchrotron-based X-ray microtomography technique in a rotation-anvil device. Comparison with literature data shows that alkali-rich, polymerized melts are generally more compressible than those that are alkali-poor and depolymerized. The high compressibility of jadeite melt at high pressures implies that polymerized sodium aluminosilicate melts, if generated by low-degree partial melting of mantle peridotite at ~250–400 km depth in the deep upper mantle, are likely denser than surrounding mantle materials, and thus gravitationally stable.
Migration of the magmas upwards or downwards in the deep interior of our Earth strongly depends not only on density but also on the viscosity of magmas. Understanding the viscosity of mantle-derived magmas is therefore needed to model their migration mechanisms and ascent rate from the source rock to the surface [14,15,16,17,18,19,20,21,22]. The viscosity of volatile-bearing melilititic melts is investigated in the study by Stagno et al. [23], for their importance as plausible carriers of deep carbon in the present day as well as in the early Archaean. In their work, the authors experimentally determined the viscosity of synthetic liquids with ~31 and ~39 wt% SiO2, 1.60 and 1.42 wt% CO2 and 5.7 and 1 wt% H2O, respectively, at pressures from 1 to 4.7 GPa and temperatures between 1265 and 1755 °C, using the falling sphere technique combined with in situ X-ray radiography. The atomic structure of the melt was also determined at high pressure and temperature, using in situ multi-angle energy-dispersive X-ray diffraction supported by ex situ micro-FTIR and micro-Raman spectroscopic measurements. The experimental results, combined with thermal and rheological parameters of mantle rocks, suggest a much slower ascent rate of melilititic melts compared to carbonatitic melts, with important implications for the modeling of CO2 flux and differentiation processes in the present day and/or in the Archaean mantle.
Another undersaturated system of great interest in igneous petrology for its peculiar origin is represented by the ultrapotassic magma [24,25,26,27,28,29,30], object of two different studies in this volume.
The first of these studies by Föster et al. [31], focuses on the origin of such peculiar magmas in the deep interior of the Earth, where, for the first time, extremely K-enriched ultrapotassic melts have been generated experimentally. In this study, this two-stage formation of ultrapotassic magmas was simulated using an experimental approach that involves the re-melting of parts of an experimental product in a second experiment. The two experimental stages are (1) the heating of two-layer charges consisting of carbonate-bearing siliciclastic marine sediment and dunite, resulting in a phlogopite-rich pyroxenite metasomatic reaction layer, and (2) the partial melting of the phlogopite-rich pyroxenite synthesized in the first experiment to generate ultrapotassic (UP) melts with K2O > 6 wt%. The re-use of the sediment-melt metasomatized dunite confirms that two-stage formation can account for ultrapotassic magmatism with K2O > 6 wt% involving significant contributions from silicic crustal components, as seen in almost all post-collisional ultrapotassic magmas.
The second study regards the ascent and recharge rate of ultrapotassic melts derived from crystallization kinetics studies of clinopyroxenes at the particularly highly hazardous system of the Campi Flegrei Volcanic district [32]. Bonechi [32] performed time-series experiments using both natural and vitrified starting materials. Experiments were carried out at a pressure of 0.8 GPa, temperatures between 1220 and 1250 °C and dwell times ranging from 0.16 to 12 h. The influence of the starting material and the dwell time and undercooling on the nucleation and growth rates of clinopyroxenes was determined. The combination of the clinopyroxene growth rates with the thermobarometric estimates and crystal size analysis of natural clinopyroxenes from Procida island (CFVD) allowed them to estimate the magma ascent rate and the recharge rate of the deep reservoir, the top of which has been located in the CFVD at about 8 km depth. These data suggest that a deep reservoir of primitive parental magma, similar to that which fed the Campanian Ignimbrite eruption (39 ka), could have been formed in a time interval ranging from 104 to 105 years (absence of pre-existing nuclei) or from 103 to 104 years (presence of pre-existing nuclei).
The study of the corundum-bearing anatectic aluminous rocks exposed in the North Dabie orogen, Central China, with the micro-structural evidence of anatexis by dehydration melting of muscovite [33] serves as an ideal link between magmatic and metamorphic processes investigated in the study of shock metamorphic features of feldspar from the Xiuyan impact crater [34]. The partial melting of high-pressure (HP) and ultra-high-pressure (UHP) metamorphic rocks can profoundly influence the tectonothermal evolution of collisional orogens, the geochemical differentiation of the continental crust and the crust–mantle interaction dynamics within subduction zones [35,36,37,38]. Moreover, the partial melting of deeply buried continental crust also has critical effects on weakening rocks and promoting deformation, thus playing an important role in evolutional processes of continental collision orogens [35,36,37,38].
In his paper, Li et al. [33] report the occurrence of corundum-bearing aluminous rocks from the deeply subducted slice of the Dabie orogen, in Central China. Mineral textures and chemical data integrated with phase equilibria modeling indicate that corundum is a product of dehydration melting of muscovite in silica-undersaturated assemblages at T = 900–950 °C, and P = 9–14 kbar.
A wider range of P and T conditions is considered in the study of the shock-metamorphic features of feldspar from Xiuyan Impact Crater. The shock-metamorphic features can provide clues for the search for impact craters on Earth and can also enrich the understanding of the behavior of feldspar under high temperatures and high pressures. In the study of Yin et al. [34], shocked alkali feldspars in the lithic breccia and suevite from Xiuyan Impact Crater were investigated using polarizing optical microscopes, Raman spectroscopy and electron microprobes to better constrain the shock history of this crater. The alkali feldspar had developed a variety of shock-metamorphic features, including irregular fractures, undulatory extinction, PDFs, diaplectic glass, and vesicular glass indicating an impressive shock history of the crater with shock pressure and post-shock temperature varying from ~5 to >60 Gpa and T from ~100 to >1500 °C (shock stage), respectively.
Physical and chemical properties of the Earth’s mantle minerals, such as electrical conductivity and density, were investigated in various contributions. High-pressure conduction mechanisms in the Earth’s interior were analyzed in two contributions dealing with occupancy in hydrous forsterite by FTIR spectroscopy [39] and fluorine conduction in fluorine-bearing Earth material by means of complex impedance spectroscopy [40].
Water distribution in the deep Earth represents one of the most important topics in the field of geodynamics due to its large impact on the physical and chemical properties of the Earth’s mantle, such as electrical conductivity, seismic anisotropy, diffusion, and rheology [41,42,43,44,45,46,47,48,49].
To constrain the deep-water cycle, the knowledge of the storage capacity and mobility of H2O in nominally anhydrous minerals (NAMs) in the mantle is a key issue [50,51,52,53].
In the study of Del Vecchio et al. [39], in order to quantitatively investigate potential equilibria that might occur between H-bearing defect species present in hydrous forsterite synthesized at 4 GPa, high-temperature FTIR spectroscopy was used to evaluate the evolution of IR spectra as a function of water content and temperature. The seven vibrational bands identified at high frequencies (>3450 cm−1) were assigned to OH stretching vibrations where hydrogen is incorporated into silicon tetrahedral vacancies. The specific contribution of each type of defect was identified by considering their evolution in temperature, up to 500 °C. From these observations, the authors highlight the very low enthalpic contribution due to the topological changes of these defects that could play a role in the electrical behavior of hydrous minerals in addition to higher enthalpy processes such as protonic conduction.
In addition to protons, the electrical conduction of Earth materials, especially silicate minerals, is usually attributed to: the transfer of ions, such as Na+ occupying crystallographic sites [54,55]; small polarons, due to the hopping of electron holes between ferrous (Fe2+) and ferric (Fe3+) sites in the lattice framework [55,56,57] and oxygen vacancies, which are related to the transfer of point defects [58].
Recent experimental studies on fluorine-bearing silicate minerals have suggested that fluorine might also be an important charge carrier for electrical conduction of Earth materials at elevated conditions [59,60].
In the investigation by Liu et al. [40], the electrical conductivity of gem-quality natural single crystal fluorite, was determined at 1 GPa and 200–650 °C by complex impedance spectroscopy. The authors show that the electrical property is dominated by a single conduction mechanism from ~350 to 650 °C: the conductivity is very high, reaching ~0.01 S/m at 650 °C, and the activation enthalpy is ~130 kJ/mol. The authors suggest that the conduction is controlled by the transfer of fluoride, and that fluorine conduction may therefore be, in addition to more conventional charge carriers, a novel and important mechanism for the electrical conductivity of Earth materials in the deep crust and mantle.
In addition to electrical conductivity, elastic properties (e.g., bulk and shear modulus) of minerals present in the Earth’s interior at high pressures and high temperatures must be properly known to interpret seismological profiles needed to determine the structure and composition of the Earth’s interior and in order to understand the formation and evolution of the solid Earth [61]. To do so, accurate knowledge of the evolution of the elastic properties of olivine as a function of pressure and chemical composition is required [62,63].
The study by Pamato et al. [64] reports structural refinements from single-crystal X-ray diffraction data obtained on olivines with composition Fo100 (synthetic), Fo80, and Fo62 (natural) collected at room temperature and high pressure up to approximately 8 GPa. The new results, along with data from the literature on Fo0, are used to discuss and clarify the effect of Mg/Fe substitution on the structural deformation mechanisms occurring along the forsterite–fayalite join, relevant to upper-mantle compositions. In particular, this study discusses which structural mechanisms, on the atomic scale, can cause the very small variations of bulk modulus and its first pressure derivative that have been previously reported.
Finally, a glimpse towards the industrial application of minerals is offered by the study of new high-temperature phases produced during the spontaneous combustion of coal [65]. The occurrence of natural clinkers (calcined clays by coal combustion) associated with coal deposits has recently been described in some areas [66,67,68,69].
In the study of Laita et al. [65], natural clinkers from a lower Cretaceous coal outcrop in Ariño (Teruel, NE Spain) were investigated by X-ray diffraction and optical and electron microscopy, in order to describe mineral and textural transformations produced during the spontaneous combustion of coal. The studied natural clinkers are composed of vitreous phase mullite, hematite, hercynite, cristobalite, quartz, pyroxenes, cordierite, gypsum, pyrite, and calcium oxides. These new minerals are also particularly interesting on account of their similarity with those formed during ceramic processes often used in the manufacture of stoneware and ceramic tiles, as well as in refractory ceramics.

Funding

This research received no external funding.

Acknowledgments

I would like to acknowledge the many people who contributed to the realization of this Special Volume: the authors themselves, who managed to keep the deadlines; the reviewers, who provided detailed and valuable comments, often on extremely short notice, and the assistant editor Irwin Liang and all the editorial board, who made all of this possible.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Thorne, M.S.; Pachhai, S.; Leng, K.; Wicks, J.K.; Nissen-Meyer, T. New Candidate Ultralow-Velocity Zone Locations from Highly Anomalous SPdKS Waveforms. Minerals 2020, 10, 211. [Google Scholar] [CrossRef] [Green Version]
  2. Reasoner, C.; Revenaugh, J. ScP constraints on ultralow-velocity zone density and gradient thickness beneath the Pacific. J. Geophys. Res. 2000, 105, 28173–28182. [Google Scholar] [CrossRef]
  3. Havens, E.; Revenaugh, J. A broadband seismic study of the lowermost mantle beneath Mexico: Constraints on ultralow velocity zone elasticity and density. J. Geophys. Res. 2001, 106, 30809–30820. [Google Scholar] [CrossRef]
  4. Simmons, N.A.; Grand, S.P. Partial melting in the deepest mantle. Geophys. Res. Lett. 2002, 29, 1552–1555. [Google Scholar] [CrossRef]
  5. Rost, S.; Garnero, E.J.; Williams, Q.; Manga, M. Seismological constraints on a possible plume root at the core-mantle boundary. Nature 2005, 435, 666–669. [Google Scholar] [CrossRef] [PubMed]
  6. Zou, Z.; Leyton, F.; Koper, K.D. Partial melt in the lowermost mantle near the base of a plume. Geophys. J. Int. 2007, 168, 809–817. [Google Scholar] [CrossRef] [Green Version]
  7. Faul, U.H. Melt retention and segregation beneath mid-ocean ridges. Nature 2001, 410, 920–923. [Google Scholar] [CrossRef] [PubMed]
  8. Tauzin, B.; Debayle, E.; Wittlinger, G. Seismic evidence for a global low-velocity layer within the Earth’s upper mantle. Nat. Geosci. 2010, 3, 718–721. [Google Scholar] [CrossRef]
  9. Schmerr, N. The gutenberg discontinuity: Melt at the lithosphere-asthenosphere boundary. Science 2012, 335, 1480–1483. [Google Scholar] [CrossRef] [Green Version]
  10. Naif, S.; Key, K.; Constable, S.; Evans, R.L. Melt-rich channel observed at the lithosphere-asthenosphere boundary. Nature 2013, 495, 356–359. [Google Scholar] [CrossRef]
  11. Sanloup, C. Density of magmas at depth. Chem. Geol. 2016, 429, 51–59. [Google Scholar] [CrossRef] [Green Version]
  12. Schmandt, B.; Jacobsen, S.D.; Becker, T.W.; Liu, Z.; Dueker, K.G. Dehydration melting at the top of the lower mantle. Science 2014, 344, 1265–1268. [Google Scholar] [CrossRef] [PubMed]
  13. Xu, M.; Jing, Z.; Van Orman, J.A.; Yu, T.; Wang, Y. Density of NaAlSi2O6 Melt at High Pressure and Temperature Measured by In-Situ X-ray Microtomography. Minerals 2020, 10, 161. [Google Scholar] [CrossRef] [Green Version]
  14. Suzuki, A.; Ohtani, E.; Funakoshi, K.; Terasaki, H.; Kubo, T. Viscosity of albite melt at high pressure and high temperature. Phys. Chem. Miner. 2002, 29, 159–165. [Google Scholar] [CrossRef]
  15. Tinker, D.; Lesher, C.E.; Baxter, G.M.; Uchida, T.; Wang, Y. High-pressure viscometry of polymerized silicate melts and limitations of the Eyring equation. Am. Miner. 2004, 89, 1701–1708. [Google Scholar] [CrossRef]
  16. Liebske, C.; Schmickler, B.; Terasaki, H.; Poe, B.T.; Suzuki, A.; Funakoshi, K.-I.; Ando, R.; Rubie, D.C. Viscosity of peridotite liquid up to 13 GPa: Implications for magma ocean viscosities. Earth Planet. Sci. Lett. 2005, 240, 589–604. [Google Scholar] [CrossRef]
  17. Suzuki, A.; Ohtani, E.; Terasaki, H.; Funakoshi, K.-I. Viscosity of silicate melts in CaMgSi2O6eNaAlSi2O6 system at high pressure. Phys. Chem. Miner. 2005, 32, 140–145. [Google Scholar] [CrossRef]
  18. Abramson, E.H. Viscosity of water measured to pressures of 6 GPa and temperatures of 300 C. Phys. Rev. E 2007, 76, 051203. [Google Scholar] [CrossRef]
  19. Kono, Y.; Kenney-Benson, C.; Park, C.; Shen, G.; Wang, Y. Anomaly in the viscosity of liquid KCl at high pressures. Phys. Rev. B 2013, 87, 024302. [Google Scholar] [CrossRef] [Green Version]
  20. Kono, Y.; Kenney-Benson, C.; Hummer, D.; Ohfuji, H.; Park, C.; Shen, G.; Wang, Y.; Kavner, A.; Manning, C.E. Ultralow viscosity of carbonate melts at high pressures. Nat. Commun. 2014, 5, 5091. [Google Scholar] [CrossRef]
  21. Spice, H.; Sanloup, C.; Cochain, B.; De Grouchy, C.; Kono, Y. Viscosity of liquid fayalite up to 9 GPa. Geochim. Cosmochim. Acta 2015, 148, 219–227. [Google Scholar] [CrossRef] [Green Version]
  22. Cochain, B.; Sanloup, C.; Leroy, C.; Kono, Y. Viscosity of mafic magmas at high pressures. Geophys. Res. Lett. 2017, 44, 818–826. [Google Scholar] [CrossRef]
  23. Stagno, V.; Stopponi, V.; Kono, Y.; D’Arco, A.; Lupi, S.; Romano, C.; Poe, B.T.; Foustoukos, D.I.; Scarlato, P.; Manning, C.E. The Viscosity and Atomic Structure of Volatile-Bearing Melilititic Melts at High Pressure and Temperature and the Transport of Deep Carbon. Minerals 2020, 10, 267. [Google Scholar] [CrossRef] [Green Version]
  24. Campbell, I.H.; Stepanov, A.S.; Liang, H.-Y.; Allen, C.M.; Norman, M.D.; Zhang, Y.-Q.; Xie, Y.-W. The origin of shoshonites: New insights from the Tertiary high-potassium intrusions of eastern Tibet. Contrib. Miner. Petr. 2014, 167, 983. [Google Scholar] [CrossRef]
  25. Condamine, P.; Médard, E. Experimental melting of phlogopite-bearing mantle at 1 GPa: Implications for potassic magmatism. Earth Planet. Sci. Lett. 2014, 397, 80–92. [Google Scholar] [CrossRef]
  26. Conticelli, S.; Avanzinelli, R.; Ammannati, E.; Casalini, M. The role of carbon from recycled sediments in the origin of ultrapotassic igneous rocks in the Central Mediterranean. Lithos 2015, 232, 174–196. [Google Scholar] [CrossRef]
  27. Condamine, P.; Médard, E.; Devidal, J.-L. Experimental melting of phlogopite-peridotite in the garnet stability field. Contrib. Miner. Petr. 2016, 171, 95. [Google Scholar] [CrossRef]
  28. Xu, B.; Griffin, W.L.; Xiong, Q.; Hou, Z.-Q.; O’Reilly, S.Y.; Guo, Z.; Pearson, N.J.; Gréau, Y.; Yang, Z.; Zheng, Y.-C. Ultrapotassic rocks and xenoliths from South Tibet: Contrasting styles of interaction between lithospheric mantle and asthenosphere during continental collision. Geology 2017, 45, 51–54. [Google Scholar] [CrossRef]
  29. Wang, Y.; Prelević, D.; Buhre, S.; Foley, S.F. Constraints on the sources of post-collisional K-rich magmatism: The roles of continental clastic sediments and terrigenous blueschists. Chem. Geol. 2017, 455, 192–207. [Google Scholar] [CrossRef]
  30. Safonov, O.; Butvina, V.; Limanov, E. Phlogopite-Forming Reactions as Indicators of Metasomatism in the Lithospheric Mantle. Minerals 2019, 9, 685. [Google Scholar] [CrossRef] [Green Version]
  31. Förster, M.W.; Buhre, S.; Xu, B.; Prelević, D.; Mertz-Kraus, R.; Foley, S.F. Two-Stage Origin of K-Enrichment in Ultrapotassic Magmatism Simulated by Melting of Experimentally Metasomatized Mantle. Minerals 2020, 10, 41. [Google Scholar] [CrossRef] [Green Version]
  32. Bonechi, B. Influence of Pre-Existing Nuclei on the Crystallization Kinetics of Primitive Alkaline Magmas: Insights on the Deep Feeding System of the Campi Flegrei Volcanic District. Minerals 2020, 10, 234. [Google Scholar] [CrossRef] [Green Version]
  33. Li, Y.; Yang, Y.; Liu, Y.-C.; Groppo, C.; Rolfo, F. Muscovite Dehydration Melting in Silica-Undersaturated Systems: A Case Study from Corundum-Bearing Anatectic Rocks in the Dabie Orogen. Minerals 2020, 10, 213. [Google Scholar] [CrossRef] [Green Version]
  34. Yin, F.; Dai, D. A Study of Shock-Metamorphic Features of Feldspars from the Xiuyan Impact Crater. Minerals 2020, 10, 231. [Google Scholar] [CrossRef] [Green Version]
  35. Korsakov, A.V.; Hermann, J. Silicate and carbonate melt inclusions associated with diamonds in deeply subducted carbonate rocks. Earth Planet. Sci. Lett. 2006, 241, 104–118. [Google Scholar] [CrossRef]
  36. Stepanov, A.S.; Hermann, J.; Korsakov, A.V.; Rubatto, D. Geochemistry of ultrahigh-pressure anatexis: Fractionation of elements in the Kokchetav gneisses during melting at diamond-facies conditions. Contrib. Miner. Petr. 2014, 167, 1002–1263. [Google Scholar] [CrossRef]
  37. Labrousse, L.; Duretz, T.; Gerya, T. H2O-fluid-saturated melting of subducted continental crust facilitates exhumation of ultrahigh-pressure rocks in continental subduction zones. Earth Planet. Sci. Lett. 2015, 428, 151–161. [Google Scholar] [CrossRef]
  38. Liu, Y.C.; Deng, L.P.; Gu, X.F. Multistage exhumation and partial melting of high-Tultrahigh-pressure metamorphic rocks in continental subduction-collision zones. Sci. China Earth Sci. 2015, 58, 1084–1099. [Google Scholar] [CrossRef]
  39. Del Vecchio, A.; Poe, B.T.; Misiti, V.; Cestelli Guidi, M. High-Temperature Evolution of Point Defect Equilibria in Hydrous Forsterite Synthesized at 1100 °C and up to 4 GPa. Minerals 2019, 9, 574. [Google Scholar]
  40. Liu, H.; Zhu, Q.; Yang, X. Electrical Conductivity of Fluorite and Fluorine Conduction. Minerals 2019, 9, 72. [Google Scholar] [CrossRef] [Green Version]
  41. Mackwell, S.J.; Kohlstedt, D.L. Diffusion of hydrogen in olivine: Implications for water in the mantle. J. Geophys. Res. Space Phys. 1990, 95, 5079. [Google Scholar] [CrossRef]
  42. Hirth, G.; Kohlstedt, D.L. Water in the oceanic upper mantle: Implications for rheology, melt extraction and the evolution of the lithosphere. Earth Planet. Sci. Lett. 1996, 144, 93–108. [Google Scholar] [CrossRef]
  43. Karato, S.-I.; Jung, H. Water, partial melting and the origin of the seismic low velocity and high attenuation zone in the upper mantle. Earth Planet. Sci. Lett. 1998, 157, 193–207. [Google Scholar] [CrossRef]
  44. Xu, Y.; Poe, B.T.; Shankland, T.J.; Rubie, D.C. Electrical Conductivity of Olivine, Wadsleyite, and Ringwoodite Under Upper-Mantle Conditions. Science 1998, 280, 1415–1418. [Google Scholar] [CrossRef] [PubMed]
  45. Du Frane, W.L.; Roberts, J.J.; To_elmier, D.A.; Tyburczy, J.A. Anisotropy of electrical conductivity in dry olivine. Geophys. Res. Lett. 2005, 32, 32. [Google Scholar] [CrossRef] [Green Version]
  46. Wang, D.; Mookherjee, M.; Xu, Y.; Karato, S.-I. The effect of water on the electrical conductivity of olivine. Nature 2006, 443, 977–980. [Google Scholar] [CrossRef]
  47. Poe, B.T.; Romano, C.; Nestola, F.; Smyth, J.R. Electrical conductivity anisotropy of dry and hydrous olivine at 8 GPa. Phys. Earth Planet. Inter. 2010, 181, 103–111. [Google Scholar] [CrossRef] [Green Version]
  48. Du Frane, W.L.; Tyburczy, J.A. Deuterium-hydrogen exchange in olivine: Implications for point defects and electrical conductivity. Geochem. Geophys. Geosystems 2012, 13, 3. [Google Scholar] [CrossRef]
  49. Novella, D.; Dolejš, D.; Myhill, R.; Pamato, M.G.; Manthilake, G.; Frost, D.J. Melting phase relations in the systems Mg2SiO4–H2O and MgSiO3–H2O and the formation of hydrous melts in the upper mantle. Geochim. Cosmochim. Acta 2017, 204, 68–82. [Google Scholar] [CrossRef] [Green Version]
  50. Bolfan-Casanova, N. Water in the Earth’s mantle. Miner. Mag. 2005, 69, 229–257. [Google Scholar] [CrossRef]
  51. Beran, A.; Libowitzky, E. Water in natural mantle minerals II: Olivine, garnet and accessory minerals. Rev. Miner. Geochem. 2005, 62, 169–191. [Google Scholar] [CrossRef]
  52. Tenner, T.J.; Hirschmann, M.M.; Withers, A.C.; Hervig, R.L. Hydrogen partitioning between nominally anhydrous upper mantle minerals and melt between 3 and 5 GPa and applications to hydrous peridotite partial melting. Chem. Geol. 2009, 262, 42–56. [Google Scholar] [CrossRef]
  53. Ferot, A.; Bolfan-Casanova, N. Water storage capacity in olivine and pyroxene to 14 GPa: Implications for the water content of the Earth’s upper mantle and nature of seismic discontinuities. Earth Planet. Sci. Lett. 2012, 349, 218–230. [Google Scholar] [CrossRef]
  54. Hu, H.; Li, H.; Dai, L.; Shan, S.; Zhu, C. Electrical conductivity of albite at high temperatures and high pressures. Am. Miner. 2011, 96, 1821–1827. [Google Scholar] [CrossRef]
  55. Yang, X.; Keppler, H.; McCammon, C.; Ni, H.; Xia, Q.; Fan, Q. Effect of water on the electrical conductivity of lower crustal clinopyroxene. J. Geophys. Res. 2011, 116, B04208. [Google Scholar] [CrossRef]
  56. Xu, Y.; Shankland, T.J.; Duba, A.G. Pressure effect on electrical conductivity of mantle olivine. Phys. Earth Planet. Inter. 2000, 118, 149–161. [Google Scholar] [CrossRef]
  57. Yang, X.; McCammon, C. Fe3+-rich augite and high electrical conductivity in the deep lithosphere. Geology 2012, 40, 131–134. [Google Scholar] [CrossRef]
  58. Schock, R.N.; Duba, A.G.; Shankland, T.J. Electrical conduction in olivine. J. Geophys. Res. 1989, 94, 5829–5839. [Google Scholar] [CrossRef]
  59. Li, Y.; Yang, X.; Yu, J.-H.; Cai, Y.-F. Unusually high electrical conductivity of phlogopite: The possible role of fluorine and geophysical implications. Contrib. Miner. Petr. 2016, 171, 37. [Google Scholar] [CrossRef]
  60. Li, Y.; Jiang, H.; Yang, X. Fluorine follows water: Effect on electrical conductivity of silicate minerals by experimental constraints from phlogopite. Geochim. Cosmoch. Acta 2017, 217, 16–27. [Google Scholar] [CrossRef]
  61. Bass, J.D.; Parise, J.B. Deep-Earth and recent developments in mineral physics. Element 2008, 4, 157–163. [Google Scholar] [CrossRef]
  62. Agee, C.B. Phase transformations and seismic structure in the upper mantle and transition zone. In Ultrahigh-Pressure Mineralogy: Physics and Chemistry of the Earth’s Deep Interior; Hemley, R.J., Ed.; Mineralogical Society of America: Chantilly, VA, USA, 1998; Volume 37, pp. 165–203. [Google Scholar]
  63. Frost, D.J. Fe2+–Mg partitioning between garnet, magnesiowustite, and (Mg, Fe)2SiO4 phases of the transition zone. Am. Miner. 2003, 88, 387–397. [Google Scholar] [CrossRef]
  64. Pamato, M.G.; Nestola, F.; Novella, D.; Smyth, J.R.; Pasqual, D.; Gatta, G.D.; Alvaro, M.; Secco, L. The High-Pressure Structural Evolution of Olivine along the Forsterite–Fayalite Join. Minerals 2019, 9, 790. [Google Scholar] [CrossRef] [Green Version]
  65. Laita, E.; Bauluz, B.; Yuste, A. High-Temperature Mineral Phases Generated in Natural Clinkers by Spontaneous Combustion of Coal. Minerals 2019, 9, 213. [Google Scholar] [CrossRef] [Green Version]
  66. Henao, J.A.; Carreño, A.M.; Quintero, J.A.; Candela, S.A.; Ríos, C.A.; Ramos, M.A.; Pinilla, J.A. Petrography and application of the Rietveld method to the quantitative analysis of phases of natural Clinker generated by coal spontaneous combustion. Earth Sci. Res. J. 2010, 14, 17–30. [Google Scholar]
  67. Ciesielczuk, J.; Misz-Kennan, M.; Hower, J.C.; Fabiańska, M.J. Mineralogy and geochemistry of coal wastes from the Starzykowiec coal-waste dump (Upper Silesia, Poland). Int. J. Coal Geol. 2014, 127, 42–55. [Google Scholar] [CrossRef]
  68. Ribeiro, J.; Suárez-Ruiz, I.; Flores, D. Geochemistry of self-burning coal mining residues from El Bierzo Coalfield (NW Spain): Environmental implications. Int. J. Coal. Geol. 2016, 159, 155–168. [Google Scholar] [CrossRef]
  69. Baboolal, A.A.; Knight, J.; Wilson, B. Petrography and mineralogy of pyrometamorphic combustion metamorphic rocks associated with spontaneous oxidation of lignite seams of the Erin Formation, Trinidad. J. S. Am. Earth. Sci. 2018, 82, 181–192. [Google Scholar] [CrossRef]

Share and Cite

MDPI and ACS Style

Romano, C. Editorial for the Special Issue “Properties of Melt and Minerals at High Pressures and High Temperature”. Minerals 2020, 10, 723. https://doi.org/10.3390/min10080723

AMA Style

Romano C. Editorial for the Special Issue “Properties of Melt and Minerals at High Pressures and High Temperature”. Minerals. 2020; 10(8):723. https://doi.org/10.3390/min10080723

Chicago/Turabian Style

Romano, Claudia. 2020. "Editorial for the Special Issue “Properties of Melt and Minerals at High Pressures and High Temperature”" Minerals 10, no. 8: 723. https://doi.org/10.3390/min10080723

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop