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hafnon

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Journal Article
Published: 01 November 2016
European Journal of Mineralogy (2016) 28 (4): 721–733.
...Anja Maria Grüneberger; Christian Schmidt; Sandro Jahn; Dieter Rhede; Anselm Loges; Max Wilke Abstract Zircon (ZrSiO 4 ), hafnon (HfSiO 4 ) and five intermediate compositions were synthesized from a Pb silicate melt. The resulting crystals were 20–300 µm in size and displayed sector and growth...
FIGURES | View All (11)
Journal Article
Published: 01 November 2015
The Canadian Mineralogist (2015) 53 (6): 1073–1081.
...Alysha G. McNeil; Robert L. Linnen; Roberta L. Flemming Fully ordered columbite-(Mn), tantalite-(Mn), hafnon, and zircon were successfully synthesized using an acid solution of 6N:1N (N = normal) HF:H 2 SO 4 and stoichiometric oxide mixtures. The mixtures and solutions were sealed and placed...
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Journal Article
Published: 01 October 2013
American Mineralogist (2013) 98 (10): 1714–1724.
... the presence of hafnian zircon to zirconian hafnon. Large HfO 2 content variations of up to 34.8 wt% were also observed within single zoned crystals. We suggest that the increase of HfO 2 in the magmatic zircon from 9.4 wt% in the contact zone to 19.5 wt% in the cleavelandite–quartz–spodumene zone mainly...
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Journal Article
Published: 01 November 2006
American Mineralogist (2006) 91 (11-12): 1888–1892.
...Bouchaib Manoun; Robert T. Downs; Surendra K. Saxena Abstract Raman spectra of synthetic HfSiO 4 were determined to pressures of 38.2 GPa. Changes in the spectra indicate that HfSiO 4 undergoes a room-temperature phase transition from the hafnon structure ( I 4 1 / amd space group) to the scheelite...
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Journal Article
Published: 01 July 2006
American Mineralogist (2006) 91 (7): 1134–1141.
... of 1430 K for the martensitic phase transition between the tetragonal and monoclinic forms of ZrO 2 (baddeleyite), with an enthalpy of transition of 8.67 kJ/mol. The same experimental approach was used also to determine the free energy of formation of hafnon (HfSiO 4 ). The entropy of hafnon ( S 0 298K...
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Journal Article
Published: 01 August 1982
American Mineralogist (1982) 67 (7-8): 804–808.
...J. Alexander Speer; Brian J. Cooper Abstract A crystal structure refinement of a synthetic hafnon, HfSiO 4 , space group I 4 1 / amd with a = 6.5725(7)Å, c = 5.9632(4)Å, Z = 4, D = 6.97 gm cm −3 , produced positional parameters for oxygen of y = 0.0655(13) and z = 0.1948(14) at R = 0.054. Hafnon...
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Raman frequencies of HfSiO4 as a function of pressure. Up to 18.7 GPa, HfSiO4, has the hafnon structure. The appearance of a new vibrational mode at 618 cm−1 at the pressure of 20.6 GPa indicates that the transition to scheelite-structured hafnon has occurred.
Published: 01 November 2006
F igure 3. Raman frequencies of HfSiO 4 as a function of pressure. Up to 18.7 GPa, HfSiO 4 , has the hafnon structure. The appearance of a new vibrational mode at 618 cm −1 at the pressure of 20.6 GPa indicates that the transition to scheelite-structured hafnon has occurred.
Journal Article
Journal: Economic Geology
Published: 01 November 1998
Economic Geology (1998) 93 (7): 1013–1025.
... on the solubilities of columbite (MnNb 2 O 6 ), zircon (ZrSiO 4 ), hafnon (HfSiO 4 ), and hbnerite (MnWO 4 ) in granitic melts was also investigated. The haplogranitic melt compositions used in these experiments have constant mole percent Si and Al, and the Al/(Li + Na + K) ratio was 1.0 for all experiments, i.e...
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Ambient-pressure Raman spectra for HfSiO4 (hafnon structure = *) starting material and for the sample quenched from 38.2 GPa and 300 K, which has converted to the scheelite-structured HfSiO4 phase (arrows). Peak assignments for the two spectra are given in Tables 1 and 2. The high-pressure resulting spectrum is clearly distinct from the spectrum obtained from the hafnon (starting material) and similar to the reidite spectrum decompressed from the zircon phase transformation.
Published: 01 November 2006
F igure 1. Ambient-pressure Raman spectra for HfSiO 4 (hafnon structure = *) starting material and for the sample quenched from 38.2 GPa and 300 K, which has converted to the scheelite-structured HfSiO 4 phase (arrows). Peak assignments for the two spectra are given in Tables 1 and 2
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Experimental procedure for the synthesis of zircon, hafnon, and five intermediate compositions. (a) Schematic sketch of the capsules used for the synthesis. (b) Temperature–time path of the syntheses.
Published: 01 November 2016
Fig. 1 Experimental procedure for the synthesis of zircon, hafnon, and five intermediate compositions. (a) Schematic sketch of the capsules used for the synthesis. (b) Temperature–time path of the syntheses.
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(a) Comparison between experimental spectra of zircon and hafnon end-member compositions and theoretical spectra from DFT calculations as indicated. For both compositions, different spectra were computed for a structure optimized at 0 GPa and for another structure optimized using the experimental density at ambient conditions as a constraint. (b) Variation of theoretical Raman spectra as a function of composition. Data shown were simulated at 0 GPa. The intermediate spectrum for Hfn0.5 was derived for a hypothetical ordered structure, where one of the two Zr atoms in the tetragonal unit cell was replaced by Hf. The lower graphs show a zoom of the upper ones, magnifying the low-intensity bands. (online version in colour)
Published: 01 November 2016
Fig. 10 (a) Comparison between experimental spectra of zircon and hafnon end-member compositions and theoretical spectra from DFT calculations as indicated. For both compositions, different spectra were computed for a structure optimized at 0 GPa and for another structure optimized using
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Published: 01 November 2015
TABLE 6. μXRD DATA FROM HAFNON AND ZIRCON EXPERIMENTS
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Raman spectra through the phase transition from hafnon to scheelite-structured HfSiO4. The spectrum at 20.6 GPa shows the first appearance of a vibration of the scheelite-structured phase at 618 cm−1, and the spectrum at 25.5 GPa shows the appearance of a second peak in the scheelite-structured phase at 525 cm−1. The peak observed at 214 cm−1 (1 atm) became undetectable and the 351.3 cm−1 peak disappeared after 25.5 GPa.
Published: 01 November 2006
F igure 2. Raman spectra through the phase transition from hafnon to scheelite-structured HfSiO 4 . The spectrum at 20.6 GPa shows the first appearance of a vibration of the scheelite-structured phase at 618 cm −1 , and the spectrum at 25.5 GPa shows the appearance of a second peak
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Schematic phase diagram showing crystallization of zircon-hafnon solid solution. Note that as zircon crystallizes, Zr/Hf in the remaining melt decreases.
Published: 01 October 2006
F ig . 1. Schematic phase diagram showing crystallization of zircon-hafnon solid solution. Note that as zircon crystallizes, Zr/Hf in the remaining melt decreases.
Journal Article
Published: 01 April 2007
The Canadian Mineralogist (2007) 45 (2): 185–202.
... by Zr/Hf. The Zr/Hf value in the (Nb,Ta)-oxide minerals generally corresponds to its range in associated zircon–hafnon. Considerable depolymerization of highly fractionated, (F, B, P)- and H 2 O-rich pegmatite-forming melts, in part alkaline in boundary layers (particularly significant in final stages...
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Journal Article
Published: 17 January 2025
American Mineralogist (2025)
... the largest unit cell volume among tetravalent metal orthosilicates. The pressure derivatives of the vibrational modes of thorite were found to be consistent with those previously reported for other orthosilicates ( e.g. , zircon, hafnon, stetindite, and coffinite), while having the smallest Grüneisen...
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Dependence of ZrO2 and HfO2 contents (wt.%) on the composition of melts saturated with zircon and hafnon, respectively. a, 800 °C (Linnen and Keppler, 2002); b, 1400 °C (Ellison and Hess, 1986). Linear-dependence equations and correlation coefficients are also given.
Published: 01 May 2020
Fig. 7. Dependence of ZrO 2 and HfO 2 contents (wt.%) on the composition of melts saturated with zircon and hafnon, respectively. a , 800 °C ( Linnen and Keppler, 2002 ); b , 1400 °C ( Ellison and Hess, 1986 ). Linear-dependence equations and correlation coefficients are also given.
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High-mass resolution spectra (m/Δm = 4500) of high-U zircon BP-1 (Buff Peak; ~3 wt% UO2), low-U zircon G42792 (~24 ppm U), synthetic cubic zirconia, hafnon, and epoxy mounting medium.
Published: 01 April 2007
F igure 2. High-mass resolution spectra (m/Δm = 4500) of high-U zircon BP-1 (Buff Peak; ~3 wt% UO 2 ), low-U zircon G42792 (~24 ppm U), synthetic cubic zirconia, hafnon, and epoxy mounting medium.
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Raman spectra of scheelite-structured HfSiO4 upon release of pressure to room conditions. The transformation of hafnon to a scheelite-structured HfSiO4 type is quenchable. The inset shows that the high-frequency SiO4 internal modes of the scheelite-structured HfSiO4 are not resolved until pressures below 5.5 GPa are reached.
Published: 01 November 2006
F igure 4. Raman spectra of scheelite-structured HfSiO 4 upon release of pressure to room conditions. The transformation of hafnon to a scheelite-structured HfSiO 4 type is quenchable. The inset shows that the high-frequency SiO 4 internal modes of the scheelite-structured HfSiO 4
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XZ projections of the displacement vectors of the three external modes Eg(II), B1g(II) and Eg(III) obtained from the ab initio simulations. The B1g(II) mode is purely translational, whereas the Eg modes of zircon have both translational and rotational components. For hafnon, Eg(II) is predominantly translational and Eg(III) rotational. (online version in colour)
Published: 01 November 2016
Fig. 11 XZ projections of the displacement vectors of the three external modes Eg(II), B1g(II) and Eg(III) obtained from the ab initio simulations. The B1g(II) mode is purely translational, whereas the Eg modes of zircon have both translational and rotational components. For hafnon, Eg(II