Theoretical structure and surface energy of the reconstructed {01.2} form of calcite (CaCO 3) crystal
Two different reconstructions of the (01.2) face (Ca or CO 3 terminated) of calcite (CaCO 3) were studied: (i) R1 reconstruction: the outermost layer is based on the [0 1 0] × 1/3[2 1 1] rectangular mesh, which is symmetrical with respect to the c glide plane of the crystal, thus fulfilling the 2D s...
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Veröffentlicht in: | Surface science 2008-08, Vol.602 (16), p.2774-2782 |
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Zusammenfassung: | Two different reconstructions of the (01.2) face (Ca or CO
3 terminated) of calcite (CaCO
3) were studied: (i) R1 reconstruction: the outermost layer is based on the [0
1
0]
×
1/3[2
1
1] rectangular mesh, which is symmetrical with respect to the
c glide plane of the crystal, thus fulfilling the 2D symmetry of the face and (ii) R2 reconstruction: the outermost layer is based on a
1
/
6
[
4
2
1
¯
]
×
1
/
6
[
2
2
¯
1
]
lozenge shaped mesh that does not respect the 2D symmetry of the face.
The
(
01.2
)
R
1
Ca
,
(
01.2
)
R
1
CO
3
,
(
01.2
)
R
2
Ca
and
(
01.2
)
R
2
CO
3
slabs geometry optimizations of calcite (CaCO
3) were performed either at DFT level or by using empirical potentials; the results obtained with these two different calculation methodologies are in good agreement. With respect to their arrangement in the bulk, the CO
3 groups of the outermost layer are significantly rotated about the crystallographic
a-axis and about the normal to the 01.2 plane; further, the thickness of the outermost layer is significantly lower than that of the underneath ones.
The surfaces energies (
γ) at 0
K, for relaxed and unrelaxed
(
01.2
)
R
1
Ca
,
(
01.2
)
R
1
CO
3
,
(
01.2
)
R
2
Ca
and
(
01.2
)
R
2
CO
3
faces, were determined either at DFT level or by using empirical potentials. Independently of the method of calculation employed, the stability order of the relaxed faces is
(
01.2
)
R
1
CO
3
<
(
01.2
)
R
2
Ca
<
(
01.2
)
R
2
CO
3
<
(
01.2
)
R
1
Ca
. Concerning the unrelaxed faces, whose energies were evaluated by using empirical potentials only, the stability order is instead
(
01.2
)
R
1
Ca
<
(
01.2
)
R
2
Ca
<
(
01.2
)
R
1
CO
3
<
(
01.2
)
R
2
CO
3
; such different ordering shows the importance of geometry relaxation in the calculation of the surface energy. The values of the relaxed surface energies are
γ
(
01.2
)
R
1
CO
3
≈
750
,
γ
(
01.2
)
R
2
Ca
≈
950
,
γ
(
01.2
)
R
2
CO
3
≈
980
and
γ
(
01.2
)
R
1
Ca
≈
1050
erg/cm
2. |
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ISSN: | 0039-6028 1879-2758 |
DOI: | 10.1016/j.susc.2008.07.002 |