The crystal chemistry of the solid solution series between chalcostibite (CuSbS2) and emplectite (CuBiS2)

被引:35
作者
Razmara, MF [1 ]
Henderson, CMB [1 ]
Pattrick, RAD [1 ]
Bell, AMT [1 ]
Charnock, JM [1 ]
机构
[1] SERC,DARESBURY LAB,WARRINGTON WA4 4AD,CHESHIRE,ENGLAND
关键词
chalcostibite; emplectite; crystal chemistry; sulphosalts;
D O I
10.1180/minmag.1997.061.404.08
中图分类号
P57 [矿物学];
学科分类号
070901 ;
摘要
Sulphosalts in the system CuSbS2-CuBiS2 (chalcostibite-emplectite) form a complete solid solution series. Seven compositions with the general formula Cu(SbxBi1-x)S-2 have been synthesized using dry methods at 310 degrees C. All members of the series are orthorhombic (space group Pnma) and show smoothly increasing a and b cell parameters with substitution of Bi for Sb; the c cell parameter increases up to 50% CuBiS2 substitution and then becomes constant. DSC experiments on CuBiS2 show an endothermic heat effect (2.35 kJ/mol.) at 472 degrees C due to the breakdown reaction to Cu3BiS3 (wittichenite) plus Bi2S3 (bismuthinite). With the addition of 10% CuSbS2 to CuBiS2, the decomposition temperature increases and the endothermic peak is broadened but the energy remains essentially the same (2.53 kJ/mol.). No evidence of this decomposition was observed when the amount of the CuSbS2 component was >30%. The local structure and co-ordination of Cu in the samples were studied by EXAFS analysis of the Cu-K edge but no significant variation occurs in the local Cu environment. The Debye-Waller factor for the first shell of S atoms surrounding Cu in end member CuSbS2 tends to be slightly smaller than for the intermediate solid solutions, suggesting that the tetrahedral Cu environments in the intermediate composition samples is somewhat more disordered than in the end-member. The low expansion characteristics along c appear to be controlled by the linkages between the (CuS3 + BiS2) sheets perpendicular to c being relatively inflexible.
引用
收藏
页码:79 / 88
页数:10
相关论文
共 15 条
[1]  
BINSTED N, 1991, CCLRC DARESBURY LAB
[2]  
BROWN GE, 1988, REV MINERAL, V18, P431
[3]   A 2-CIRCLE POWDER DIFFRACTOMETER FOR SYNCHROTRON RADIATION WITH A CLOSED-LOOP ENCODER FEEDBACK-SYSTEM [J].
CERNIK, RJ ;
MURRAY, PK ;
PATTISON, P ;
FITCH, AN .
JOURNAL OF APPLIED CRYSTALLOGRAPHY, 1990, 23 :292-296
[4]  
CHEN TT, 1971, GEOL SOC AM ABSTR, V3, P524
[5]   A 2-CIRCLE POWDER DIFFRACTOMETER FOR SYNCHROTRON RADIATION ON STATION 2.3 AT THE SRS [J].
COLLINS, SP ;
CERNIK, RJ ;
PATTISON, P ;
BELL, AMT ;
FITCH, AN .
REVIEW OF SCIENTIFIC INSTRUMENTS, 1992, 63 (01) :1013-1014
[6]  
GRIGAS, 1975, SOV PHYS-CRYSTALLOGR, V20, P741
[7]   A RAPID, EXACT CURVED-WAVE THEORY FOR EXAFS CALCULATIONS [J].
GURMAN, SJ ;
BINSTED, N ;
ROSS, I .
JOURNAL OF PHYSICS C-SOLID STATE PHYSICS, 1984, 17 (01) :143-151
[8]  
Hedin L., 1969, Solid State Physics, Advanced in Research and Applications, V23, DOI DOI 10.1016/S0081-1947(08)60615-3
[9]  
Hofmann W, 1933, Z KRISTALLOGR, V84, P177
[10]   THEORY OF EXTENDED X-RAY ABSORPTION FINE-STRUCTURE [J].
LEE, PA ;
PENDRY, JB .
PHYSICAL REVIEW B, 1975, 11 (08) :2795-2811