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Notizen 929

Ternary Molybdenum Sulfides of the Heavy Alkali Metals

Monika Kümpers and Robert Schöllhorn*

Anorganisch-Chemisches Institut der Universität Münster,

Gievenbecker Weg 9, D-4400 Münster Z. Naturforsch. 35b, 929-930 (1980);

received April, 1980

Ternary, Molybdenum Sulfides, Molybdenum Disulfide

Two series of ternary molybdenum sulfides, ASMO4S6 ( A = K , R b , Cs) a n d A2M015S20 (A = K, Rb), were prepared by reduction of molybdenum disulfide with alkali metals in alkali halide melts at 1100-1300 K. All com- pounds are hexagonal and show electronic conductivity; structural characteristics suggest isolated [Mo/S]^ chains as lattice elements for AzMo4S6.

Ternary molybdenum sulfides A^Mo^Sz with the oxidation state of molybdenum < + 6 are of actual interest with respect to their structural features and their unusual physical properties [1-3]. Whereas compounds with transition and post transition elements have been studied rather thoroughly, the information on ternary molybdenum sulfides with strongly electropositive elements is much less satis- factory. Metastable alkali phases AJMoSa with layered structures [2, 4, 5] and AZMOÖSS with frame- work structure [6] can be obtained at ~300 K via chemical or electrochemical intercalation. Com- pounds prepared at high temperatures have been described by several authors [7-9]; their detailed structures are, however, unknown so far. W e report here on the formation and characterization of two new series of ternary molybdenum chalcogenides w hich were obtained from alkali halide melts.

The reduction of M0S2 with the corresponding alkali metal in molybdenum autoclaves at 1100 to 1300 K under argon atmosphere in KCl, RbCl and CsCl melts results in the formation of whisker-like grey needles with metallic appearance up to 5 mm in length. They are stable towards air and H2O and were isolated from the salt matrix by washing with water; the analytical composition corresponds to AZM02S3 with x ~ 1/3. X-ray powder diagrams and single crystal Weissenberg photographs revealed that the three compounds are isomorphous with hexagonal symmetry and the space group P63/m;

lattice parameters are given in Table I. The ex- perimental density observed for the Cs+ compound (x = 0.33) corresponds to £ = 3.49 g/cm3; the calcu- lated density with Z — 2 amounts to q = 3.35 g/cm3.

* Reprint requests to Prof. Dr. R. Schöllhorn.

0340-5087/80/0700-0929/$ 01.00/0

( p m )

442 440

438 270 290 310 330

d ( p m )

Fig. 1. Ternary alkali molybdenum sulfides Aa;Mo4S6:

dependance of hexagonal lattice parameters on cation diameter d.

From Fig. 1 it can be seen that the a axis varies linearly with the cation diameter, while the c axis remains almost constant. This fact along with the observation of strongly anisometric crystal mor- phology, high elasticity and perfect cleavage of the crystals parallel to the hexagonal c axis suggests a structure consisting of isolated rigid (Mo4Se)Sö o n e"

dimensional matrix units held together by the alkali cations. All single crystals investigated so far exhibited specific structure defects, however, and a complete structure determination will have to wait for crystals of better quality by improved growth techniques. Preliminary studies on the physical properties of these phase indicate a rather high electronic conductivity which is likely to be due to metal-metal bonding.

Extended reaction times at 1300 K led to the formation of additional molybdenum rich phases in KCl and RbCl melts which crystallize as compact brittle grey needles with hexagonal cross section and metallic lustre. The stoichiometry of the potassium compound (electron microprobe data using K2Pd3S4

as reference sample) was found to correspond to K0.4MO3S4. X-ray powder diagrams can be indexed hexagonally; lattice parameters are given in Table I.

The density observed for Ko.3Mo3S4 is equivalent to q = 3.89 g/cm3; the calculated value amounts to q = 4.11 g/cm3 with Z = 5, i.e. a stoichiometry of K2M015S20 per unit cell. The rubidium phase was found to be isomorphous with the potassium com- pound (Table I). Although symmetry and lattice Table I. Hexagonal lattice parameters of alkali molyb- d e n u m sulfides A*MO4S6 a n d A2MOISS2O-

Ternary phase a [pm] c [pm]

KsMo4S6 873.8 441.3

RbaMo4S6 895.9 441.2

CszMO4S6 928.8 441.0

K 2 M 0 1 5 S 2 0 922.7 1181.0

Rb2Moi5S2o 923.6 1174.1

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930 Notizen.

parameters suggest a structural similarity to the well-known ternary molybdenum sulfides TxMoeSs [1], intensity values and systematic extinctions do not agree with this assumption. It is more likely that these sulfides are structurally related to In3Moi5Sei9 which shows both MoöSeg and MogSen building blocks [10]. The minor quality of single crystals isolated so far prevented a complete X-ray structure analysis.

With decreasing reaction temperature the ap- pearance of layered alkali molybdenum sulfides AxMoS2 is observed which exhibit a distorted M0S2 sublattice with considerable stacking disorder. As described by us earlier these compounds easily undergo topotactic solvation [9]. Electron diffrac- tion studies on hydrated samples of improved crystal quality now indicate that their symmetry is not hexagonal as reported originally but ortho- rhombic (Table II) with the following correlation:

ao = 2 ay, bo = 2 an • YS; Co = cy

The orthorhombic distortion of the [MoS2]x_ sub- lattice is supposedly due to the formation of metal- metal chains similar to those found for a series of

Table II. Orthorhombic lattice parameters of hydrated layered alkali molybdenum sulfides

Aa:+(H20)2/[MoS2?-.

A a [pm] b [pm] c [pm]

Na 655.1 1137.2 2492.9

K 648.4 1122.9 1842.3

Rb 648.7 1124.1 1875.7

Cs 649.4 1125.3 1915.3

related layered binary and ternary dichalcogenides [3, 11].

According to electron diffraction and X-ray powder data the hydrogen bronze H0.3M0S2 [9] was found to exist in two modifications: (i) ortho- rhombic, a = 647 pm, b — 1120 pm, c = n • 599 pm

(n = 1, 2, 3); (ii) hexagonal, a = 560 pm, c — n • 599 pm. Both phases show considerable stacking disorder.

The authors are grateful to Dr. G. A. Wiegers, Groningen, for discussions on defect structure prob- lems.

[1] K. Yvon, in E. Kaldis (ed.): Current Topics in Materials Science 8, 53 (1978), North Holland Publ. Co.; 0 . Fischer, Appl. Phys. 16, 1 (1978).

[2] R. B. Samoano and J. A. Woollam, in F. Levy ed.): Intercalated Layered Materials, D. Reidel Publ. Co, Dordrecht 1979.

[3] J. Guillevic, J. Y. le Marouille, and D. Grandjean, Acta Crystallogr. B 30, 111 (1974); J. Guillevic and D. Grandjean, Ann. Chim. 11 (1977).

[4] W. Rüdorff, Chimia 19, 489 (1965).

[5] J. O. Besenhard, H. Meyer, and R. Schöllhorn, Z. Naturforsch. 31b, 907 (1976); R. Schöllhorn and A. Weiss, J. Less-Common Metals 36, 229 (1974).

[6] R. Schöllhorn, M. Kümpers, and J. O. Besenhard, Mat. Res. Bull. 12, 781 (1977); R. Schöllhorn, M. Kümpers, A. Lerf, E. Umlauf, and W.

Schmidt, Mat. Res. Bull. 14, 1039 (1979).

[7] R. Chevrel, M. Sergent, and J. Prigent, J. Solid State Chem. 3, 515 (1971).

[8] W. Bronger and J. Huster, Naturwissenschaften 56, 88 (1969).

[9] R. Schöllhorn, M. Kümpers, and D. Plorin, J. Less-Common Metals 58, 55 (1978).

[10] R. Chevrel, M. Sergent, B. Seeber, 0 . Fischer, A. Grüttner, and K. Yvon, Mat. Res. Bull. 14, 567 (1979).

[11] J. A. Wilson and A. D. Yoffe, Adv. Phys. 18, 193 (1969).

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