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Tetrahedrally Coordinated Carbonates in Earth’s Lower Mantle Eglantine Boulard 1,2 , Ding Pan 3 , Giulia Galli 3 , Zenxhian Liu 4 and Wendy L. Mao 1,5 1 Geological and Environmental Sciences, Stanford University, Stanford, California 94305, USA. 2 PSICHE Beamline, Synchrotron SOLEIL, L'Orme des Merisiers, 91190 Saint-Aubin, France 3 Institute for Molecular Engineering, University of Chicago, Chicago, Illinois 60637, USA. 4 Geophysical Laboratory, Carnegie Institution of Washington, Washington, District Of Columbia 20015, USA. 5 Photon Science, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA. Carbonates such as ferromagnesite ((Fe,Mg)CO 3 ) are likely to be the carbon-bearing phases in the deep mantle [e.g. 1]. Determination of their stability, thermodynamic properties and phase diagrams are therefore of great interest for understanding the global carbon cycle. Although these results may indicate a possible new local environment for C in HP-HT structures, this drastic change is still controversial and further in situ characterizations are needed. We address this problem with in situ IR spectroscopy on (Mg,Fe)CO 3 at high pressure. Sid CO 3 2- C 3 O 9 6 - CO C K d) HP carb Energy loss (eV) 285 295 305 290 300 2-Theta, deg 2-Theta, deg Counts Counts 4 4 6 6 8 8 10 10 12 12 14 14 16 16 18 18 Previous in situ X-Ray Diffraction (XRD) study shows transformation of (Mg, Fe)CO 3 into a new structure above 80 GPa - 2300 K that is quenchable at room temperature (RT) [Ref. 2]. However, no Rietveld refinements could be performed and therefore no atom positions were proposed. When quenched to ambient pressure and temperature conditions, the transformed (Mg, Fe)-rich carbonate presents a C-K edge different from a carbonate suggesting a change of carbon environment [Ref.2]. Possible new local environment for C ? Introduction in situ XRD pattern of (Mg, Fe)CO 3 at 80 GPa-2300 K [Ref. 2] ex situ EELS spectra at the C-K edge of recovered samples. Sid : Siderite; HP carb : high pressure phase [Ref. 2] IR spectra collected at RT upon compression and decompression IR spectra collected at RT upon decompression after transformation at 103 GPa - 2100 K by laser heating Synchrotron based infrared (IR) spectroscopy was performed on natural (Mg 0.25 ,Fe 0.75 )CO 3 sample. Spectra were collected at high pressure (HP) and room temperature (RT) through diamond anvil cells. In situ Infrared spectroscopy IR ruby sample KBr IR spectra collected upon decompression after transformation at HT. Several new infrared bands are observed and can be follow down to 43 GPa, i.e.: * Method: 3000 2500 2000 1500 1000 500 Wavenumber (cm -1 ) 0 GPa 43 GPa 58 GPa 81 GPa 85 GPa 103 GPa 1 * * * * * * ν 2 ν 3 ν 4 Absorbance 3000 2500 2000 1500 1000 500 Wavenumber (cm -1 ) 0.5 58 GPa 54 GPa 0 GPa ν 4 ν 3 ν 2 ν 4 ν 3 ν 2 (Mg,Fe)CO 3 IR active modes : * * Absorbance Ø X Z Y X Z Y C O Mg, Fe Density functional theory (DFT) Absorbance 2000 1500 1000 500 0 Wavenumber (cm -1 ) 0.5 IR spectra calculated for a pure MgCO 3 without allowing for any phase transition: IR spectrum calculated for the postmagnesite structure: R-3c structure of magnesite postmagnesite structure measured at 82 GPa - 2,300 K [Ref. 2] 1.37 Å 1.39 Å Conclusions Implications on C reservoirs and fluxes in the lower mantle : Chemical and physical properties of carbonates Increase in carbonate melt viscosity due to the ability of CO 4 to form polymerizable networks. This would inhibit mobility of carbonate melts in the lower mantle and might lead to the presence of deep carbon reservoirs. 4 1 2 3 1 2 3 3 (A) (B) 5 4 5 4 5 The IR spectra of the high-pressure phase can be assigned to sp 3 hybridized configurations. trigonal magnesite structure : sp 2 Carbon bonds New mode at ~1300 cm -1 : IR Fingerprint of tetrahedrally bonded carbon: New carbon - oxygen bonds: References : Present work: Boulard E., Pan D. et al. 2015, Nature Communications, 6, 6311 for comparison, the C-O length in the CO 3 ion is 1.30 Å at ambient conditions [1] Wood, B.J. et al., 1996, Phil. T. R. Soc. Lond. A, v. 354, p. 1495-1511 [2] Boulard, E et al., 2011, PNAS, v. 108, no. 13, p. 5184-5187 [email protected]
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Page 1: Tetrahedrally Coordinated Carbonates in Earth’s Lower Mantle · Tetrahedrally Coordinated Carbonates in Earth’s Lower Mantle Eglantine Boulard1,2, Ding Pan3, Giulia Galli3, Zenxhian

Tetrahedrally Coordinated Carbonates in Earth’s Lower MantleEglantine Boulard1,2, Ding Pan3, Giulia Galli3, Zenxhian Liu 4 and Wendy L. Mao1,5

1 Geological and Environmental Sciences, Stanford University, Stanford, California 94305, USA.2 PSICHE Beamline, Synchrotron SOLEIL, L'Orme des Merisiers, 91190 Saint-Aubin, France3 Institute for Molecular Engineering, University of Chicago, Chicago, Illinois 60637, USA.

4 Geophysical Laboratory, Carnegie Institution of Washington, Washington, District Of Columbia 20015, USA.5 Photon Science, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.

Carbonates such as ferromagnesite ((Fe,Mg)CO3) are likely to be the carbon-bearing phases in the deep mantle [e.g. 1]. Determination of their stability, thermodynamic properties and phase diagrams are therefore of great interest for understanding the global carbon cycle.

Although these results may indicate a possible new local environment for C in HP-HT structures, this drastic change is still controversial and further in situ characterizations are needed. We address this problem with in situ IR spectroscopy on (Mg,Fe)CO3 at high pressure.

Sid

CO32-

C3O 96-

CO

C Kd)

HP carb

Energy loss (eV)285 295 305290 300

2-Theta, deg 2-Theta, deg

Coun

ts

Coun

ts

4 4 6 6 8 8 10 10 12 12 14 14 16 16 18 18

Previous in situ X-Ray Diffraction (XRD) study shows transformation of (Mg, Fe)CO3 into a new structure above 80 GPa - 2300 K that is quenchable at room temperature (RT) [Ref. 2]. However, no Rietveld refinements could be performed and therefore no atom positions were proposed.

When quenched to ambient pressure and temperature conditions, the transformed (Mg, Fe)-rich carbonate presents a C-K edge different from a carbonate suggesting a change of carbon environment [Ref.2].

Possible new local environment for C ?Introduction

in situ XRD pattern of (Mg, Fe)CO3 at 80 GPa-2300 K [Ref. 2]

ex situ EELS spectra at the C-K edge of recovered samples. Sid : Siderite; HP carb : high pressure phase [Ref. 2]

IR spectra collected at RT upon compression and decompression

IR spectra collected at RT upon decompression after transformation at 103 GPa - 2100 K by laser heatingSynchrotron based infrared

(IR) spectroscopy was performed on natural (Mg0.25,Fe0.75)CO3 sample. Spectra were collected at high pressure (HP) and room temperature (RT) through diamond anvil cells.

In situ Infrared spectroscopy

IR

rubysampleKBr

IR spectra collected upon decompression after transformation at HT. Several new infrared bands are observed and can be follow down to 43 GPa, i.e.: *

Method:

30002500200015001000500

Wavenumber (cm-1)

0 GPa43 GPa

58 GPa

81 GPa

85 GPa

103 GPa

1*

*

*

*

*

*

ν2ν3ν4A

bsor

banc

e

30002500200015001000500

Wavenumber (cm-1 )

0.5

58 GPa54 GPa

0 GPaν4

ν3ν2

ν4

ν3

ν2

(Mg,Fe)CO3 IR active modes :

*

*

Abs

orba

nce

Ø

X

Z

YXZ

Y

C O Mg, Fe

Density functional theory (DFT)

Abso

rban

ce

2000150010005000Wavenumber (cm-1)

0.5

IR spectra calculated for a pure MgCO3 without allowing for any phase transition:

IR spectrum calculated for the postmagnesite structure:

R-3c structure of magnesite postmagnesite structure measured at 82 GPa - 2,300 K [Ref. 2]

1.37 Å

1.39 Å

ConclusionsImplications on C reservoirs and fluxes in the lower mantle :● Chemical and physical properties of carbonates ● Increase in carbonate melt viscosity due to the ability of CO4 to form polymerizable networks. This would inhibit mobility of carbonate melts in the lower mantle and might lead to the presence of deep carbon reservoirs.

4

1

2

31 2

33(A)

(B)

545

4

5

The IR spectra of the high-pressure phase can be assigned to sp3 hybridized configurations.

trigonal magnesite structure : sp2 Carbon bonds New mode at ~1300 cm-1 :

IR Fingerprint of tetrahedrally bonded carbon:

New carbon - oxygen bonds:

References :

Present work: Boulard E., Pan D. et al. 2015, Nature Communications, 6, 6311

for comparison, the C-O length in the CO3 ion is 1.30 Å at ambient conditions

[1] Wood, B.J. et al., 1996, Phil. T. R. Soc. Lond. A, v. 354, p. 1495-1511[2] Boulard, E et al., 2011, PNAS, v. 108, no. 13, p. 5184-5187

[email protected]

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