C O M M U N I C A T I O N S
with traces of a ferromagnetic impurity. After taking the impurities
into account, the molar susceptibilities were calculated to be ø(300
K) ) -5 × 10-4 emu mol-1 for Na8-xSi46 and ø(300 K) ) -3 ×
10-4 emu mol-1 for K8-xSi46. The electrical resistivity F(T) of a
cold pressed sample of K8-xSi46 powder is almost temperature-
independent with F ≈ 0.025 Ω m.19 No phase transition or
superconductivity is observed above 1.8 K. For the composition
M8-xSi46, a bad-metallic behavior and a Pauli-paramagnetic con-
tribution to ø(T) is expected. The observed diamagnetic behavior
of the filled clathrates can be attributed to large additional
diamagnetic contributions from ring currents.20
We have demonstrated a viable controlled oxidation of Zintl
phases that results in metastable compounds with open-framework
structures. The synthesis route to silicon clathrates is a general route
and can therefore be applied to Zintl-phases of other elements, as
well as, other saltlike intermetallics.
Figure 2. SEM image of Na8-xSi46 agglomerates obtained from oxidation
of Na4Si4 by HCl after 1 h, setup 1. (Au sputtered sample, SE contrast.)
spectroscopy (EDXS; EDAX Si(Li) detector) confirms the presence
of solely Na (K) and Si in the products.13
Acknowledgment. The authors thank P. Scheppan, Dr. S.
Hoffmann, R. Koban and the Kompetenzgruppe Struktur. A.M.G.
and Z.T. acknowledge support from the NSF and the Welch
Foundation.
After 1 h reaction of Na4Si4, through the use of setup 1, the
XRPD data revealed a mixture of two crystalline products,
clathrate-I Na8-xSi46 (≈70 mass %) and clathrate-II Na24-xSi136
(≈30 mass %). No R-Si was detected in the products (page S3).
Full-profile Rietveld refinement of the clathrate-I crystal structure
showed full occupancies at the three Si sites.14 Both Na positions
were found to be partially occupied giving a final composition of
Na6.2(1)Si46 (page S4). The observed lattice parameter of a )
10.199(1) Å is close to that reported in the literature for Na8Si46
(page S6).7,15 The crystal structure of the minor byproduct, clathrate-
II NaxSi136, was refined only as a first approximation. Its silicon
framework seems to be fully occupied, and of the two possible
Supporting Information Available: SEM images, XRPD patterns
and crystallographic data of Na6.2(1)Si46 and K7.0(1)Si46, comparison and
evaluation of lattice parameters with literature data. The material is
References
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cation positions only one is occupied (partially) leading to a
(3) Moriguchi, K.; Munetoh, S.; Shintani, A. Phys. ReV. B 2000, 62, 7138-
16
composition of Na0.6Si136
,
thus revealing a viable route to the
7143.
formation of the empty silicon clathrate-II. Through the use of setup
2, Na4Si4 was reacted for 20 h to form a mixture of clathrate-I
Na8-xSi46, a ) 10.198(1) Å, and clathrate-II NaxSi136, a )
14.645(1) Å. XRPD indicated that crystalline silicon is not formed.
The 1 h treatment of K4Si4, using setup 1, results in only one
crystalline product (page S3), clathrate-I K8-xSi46 with a )
10.278(1) Å and an amorphous phase. The occupancy of the cation
positions in this case is higher compared with the Na compound,
and yields a composition of K7.0(1)Si46 (page S5).17 Through the
use of setup 2, K4Si4 was reacted to form clathrate-I K8-xSi46 with
a ) 10.280(1) Å (page S6).
To distinguish the effects of thermal decomposition from the
oxidation with HCl, the stability of the precursors was investigated
for all reaction temperatures without an oxidizing agent. After 1 h
treatment (Na4Si4 at 400 °C; K4Si4 at 450 °C), XRPD indicated
that both precursors remain unchanged. Only thermal treatments
for 20 h result in significant amounts of clathrate-I with residues
of M4Si4. Moreover, the lattice parameter of K8-xSi46 obtained from
thermal decomposition of K4Si4, a ) 10.267(1) Å, is smaller than
that of the product obtained from the reaction with HCl (a )
10.280(1) Å). These results prove that the M8-xSi46 phases obtained
with both experimental setups result from the reaction of M4Si4
with HCl.
(4) Adams, G. B.; O’Keeffe, M.; Demkov, A. A.; Sankey, O. F.; Huang,
Y.-M. Phys. ReV. B 1994, 49, 8048-8053.
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M.; Nesper, R. Z. Kristallogr. New Cryst. Struct. 2005, 220, 525-527.
(10) For safety reasons all heat treatments under HCl pressure were performed
in a laboratory hood.
(11) Smits, A.; de Lange, W. J. Chem. Soc. 1928, 2944-2952.
(12) Oppermann, H.; Huong, D. Q. Z. Anorg. Allg. Chem. 1995, 621, 665-
670.
(13) A low intensity Cl K line, the only significant minority line beside small
contribution of O or N K line, indicates small residues of NH4Cl or MCl.
(14) Crystallographic data of Na6.2(1)Si46: space group Pm-3n, a ) 10.199(1)
Å; 1.70(4) Na in 2a 000; 4.50(5) Na in 6c 1/4 1/2 0; 6 Si in 6d 1/4 0 1/2,
16 Si in 16i xxx, x ) 0.1840(3), 24 Si in 24k 0yz, y ) 0.3053(3), z )
0.1184(4).
(15) Ramachandran, G. K.; Dong, J.; Diefenbacher, J.; Gryko, J.; Marzke, R.
F.; Sankey, O. F.; McMillan, P. F. J. Solid State Chem. 1999, 145, 716-
730.
(16) Crystallographic data of Na0.6Si136: space group Fd3hm, a ) 14.645(1)
Å; 0.6(3) Na in 8b 3/8 3/8 3/8; 8 Si in 8a 7/8 7/8 7/8; 32 Si in 32e xxx,
x ) 0.7832(6), 96 Si in 96h xxz, x ) 0.8200(4), z ) 0.6324(5).
(17) Crystallographic data of K7.0(1)Si46: space group Pm3hn, a ) 10.278(1)
Å; 1.60(2) K in 2a 000; 5.40(4) K in 6c 1/4 1/2 0; 6 Si in 6d 1/4 0 1/2,
16 Si in 16i xxx, x ) 0.1842(3), 24 Si in 24k 0yz, y ) 0.3061(4), z )
0.1180(4).
(18) Magnetization was measured at various external fields between 100 Oe
and 70 kOe (1.8-400 K) in a SQUID magnetometer (MPMS XL-7,
Quantum Design) on polycrystalline samples (m ≈ 4.5 mg). The
contribution of the glass sample holder was subtracted.
(19) The electrical resistivity measurements were performed on a cuboid-shaped
cold-pressed sample, annealed at 300 °C. Conventional dc four-point
method, 4-320 K; inaccuracy of absolute values are (20 %.
(20) Paschen, S.; Baenitz, M.; Tran, V. H.; Rabis, A.; Steglich, F.; Carrillo-
Cabrera, W.; Grin, Yu.; Strydom, A. M.; Du Plessis, P. de V. J. Phys.
Chem. Solids 2002, 63, 1183-1188.
Differential scanning calorimetry measurements in welded Nb
ampoules exhibit an exothermic effect at 594 °C for Na8-xSi46 and
at 716 °C for K8-xSi46 (obtained from setup 1), indicating the
metastable character of both clathrates. Annealing Na8-xSi46 at 600
°C for 18 h results in a partial decomposition of the clathrate-I
compound to R-Si (XRPD data). K8-xSi46 is completely decomposed
to R-Si within 18 h at 720 °C.
Magnetic susceptibility measurements18 ø(T) ) M/H on Na8-xSi46
and K8-xSi46 samples consistently showed a diamagnetic substance
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