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Standard X-ray Diffraction Powder Patterns

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Indium sulfide, ln z $ 3<br />

Sample<br />

The In 2 S 3 was made by W.S. Brower by heating the<br />

elements in a sealed silica tube at 460 °C for<br />

sixteen hours and at 880 °C for six hours.<br />

Color<br />

Unground: dark g<strong>ray</strong>ish red<br />

Ground: strong reddish brown<br />

Structure<br />

Tetragonal, I4i22 (98), Z=16. The structure was<br />

studied by Rooymans [1959] and by Goodyear and<br />

Steigmann [1961].<br />

NBS lattice constants: 0<br />

a = 7.619{1)A<br />

c = 32.329(4)<br />

Density n r^ .<br />

(calculated) 4 - 613 g/cm 3<br />

Reference intensity<br />

I/I corundum" 4.2<br />

d(A)<br />

8.09<br />

7.40<br />

6.21<br />

5.110<br />

4.927<br />

4.041<br />

3.947<br />

3.811<br />

3.445<br />

3.392<br />

3.249<br />

3.112<br />

3.015<br />

2.770<br />

2.741<br />

2.694<br />

2.557<br />

2.532<br />

2.472<br />

2.382<br />

0<br />

Internal standard W, a = 3.16516 A<br />

CuKaj A = 1.54056 A; temp. 25 C<br />

/<br />

4<br />

3<br />

30<br />

12<br />

2<br />

3<br />

2<br />

18<br />

2<br />

2<br />

100<br />

12<br />

1<br />

3<br />

3<br />

50<br />

1<br />

1<br />

4<br />

1<br />

hkl<br />

004<br />

101<br />

103<br />

112<br />

105<br />

008<br />

107<br />

200,116<br />

204<br />

211<br />

109,213<br />

206<br />

215<br />

208,1-1-10<br />

1-0-11,217<br />

0*0-12,220<br />

224<br />

301<br />

219,303<br />

312<br />

2>Y ><br />

10.93<br />

11.95<br />

14.24<br />

17.34<br />

17.99<br />

21.98<br />

22.51<br />

23.32<br />

25.84<br />

26.25<br />

27.43<br />

28.66<br />

29.60<br />

32.29<br />

32.64<br />

33.23<br />

35.07<br />

35.42<br />

36.31<br />

37.74<br />

Polymorphism<br />

Hahn and Klinger [1949] found that a low temper<br />

ature form transformed irreversibly at about<br />

330 C to a high form which they indexed as cu<br />

bic with a few extra non-cubic lines.<br />

2.364<br />

2.309<br />

2.225<br />

2.199<br />

2.123<br />

3<br />

1<br />

3<br />

9<br />

1<br />

1-0-13,305<br />

314<br />

2-1-11,307<br />

2-0-12,316<br />

1-M4<br />

38.04<br />

38.97<br />

40.51<br />

41.00<br />

42.54<br />

Additional patterns<br />

1. Goodyear and Steigmann [1961].<br />

2.107<br />

2.074<br />

2.009<br />

1.905<br />

1.845<br />

2<br />

45<br />

3<br />

65<br />

1<br />

321<br />

309,323<br />

2-1-13,325<br />

2-2-12,400<br />

1-0-17,411<br />

42.88<br />

43.61<br />

45.09<br />

47.71<br />

49.34<br />

References<br />

Goodyear, J. and Steigmann, G.A. (1961). Proc.<br />

Phys. Soc. 78 491.<br />

Hahn, H. and Klinger, W. (1949). Z. anorg. Chem.<br />

260, 97.<br />

Rooymans, C.J.M. (1959). J. Inorg. Nucl. Chem. 11,<br />

78.<br />

1.8213<br />

1.7766<br />

1.7224<br />

1.7161<br />

1.7037<br />

1.6673<br />

1.6615<br />

1.6429<br />

1.6242<br />

1.6161<br />

6<br />

1<br />

1<br />

1<br />

3<br />

3<br />

3<br />

13<br />

5<br />

3<br />

329,413,+<br />

3-0-13,415<br />

334,408,+<br />

3-2-11,417<br />

336,420,+<br />

3-1-14,424<br />

1-0-19, 2-1-17<br />

3-0-15,419<br />

426,2-0-18<br />

2-2-16.0-0-20<br />

50.04<br />

51.39<br />

53.13<br />

53.34<br />

53.76<br />

55.03<br />

55.24<br />

55.92<br />

56.62<br />

56.93<br />

1.5701<br />

1.5647<br />

1.5556<br />

1.5224<br />

1.5090<br />

2<br />

2<br />

10<br />

1<br />

4<br />

3-3-10,428<br />

4-1-11<br />

4-0-12<br />

2-1-19,431,+<br />

1-0-21,3-2-15<br />

58.76<br />

58.98<br />

59.36<br />

60.79<br />

61.39<br />

30<br />

1.4876<br />

1.4835<br />

1 .4475<br />

1 .4403<br />

1.4181<br />

3<br />

2<br />

1<br />

4<br />

2<br />

2-0-20,512<br />

4-1-13,435<br />

437<br />

3-1-18,516,+<br />

1-1-22,3-3-14<br />

62.37<br />

62.56<br />

64.30<br />

64.66<br />

65.80

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