Ames Laboratory ISC Technical Reports Ames Laboratory
9-1-1956
Tabulation, bibliography, and structure of binary
intermetallic compounds. I. Compounds of
lithium, sodium, potassiu, and rubidium.
S. G. EpsteinIowa State College D. M. Bailey Iowa State College R. L. Smythe Iowa State College G. R. Kilp Iowa State College J. F. Smith Iowa State College
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Recommended Citation
Tabulation, bibliography, and structure of binary intermetallic compounds.
I. Compounds of lithium, sodium, potassiu, and rubidium.
Abstract
The compilation of the material in this report was undertaken to provide a convenient reference source for intermetallic compounds. An adequate bibliography is required for most efficient use. It is in this sense and because of the addition of more compounds that the compilation is considered an extension of the
compilation in Smithell's "Metals Reference Book."
Disciplines
Ceramic Materials | Engineering | Materials Science and Engineering | Metallurgy
ISC-795
U N I T E D S T A T E S A T 0 M I C E N E R G Y C 0 M M I S S I 0 N
TABULATION, BIBLIOGRAPHY, AIID STRUCTURE OF BINARY INTERMETALLIC COMPOUNDS.
I. COMPOUNDS OF LITHIUM, SODIUM, POTASSIUM, AND RUBIDIUM.
by
S. G. Epstein, D. M. Bailey, R. L. Smythe,
G. R. Kilp and J. F. Smith
September 1, 1956
Physical Scicnc ~s {eudi 1 ":' F.ooro
Ames Laboratory at
Iowa State College F. H. Spedding, Director
This report is distributed according to the catagory Metallurgy and Ceramics, as listed in TID-4500, July 15, 19.56.,
This report was prepared as an account of Government sponsored work.
Neither the United States, nor the Commission, nor any person acting on behalf of the Commission:
A.. Makes any warranty or representation, express or implied, with
respect to the accuracy, completeness, or usefulness of the infor-mation contained in this report, or that the use of any inforinfor-mation apparatus, method, or process discl~sed in this report may not infringe privately owned rights; or
B. Assumes any liabilities with respect to the use of, or for damages resulting from the use of any information, apparatus,
method, or process disclosed in this report.
As used in the above, 11person,acting on behalf of the Commission" includes any employee or contractor of the Commissio~ to the extent that such employee or contractor prepares, handles or distributes, or provides access to, any information pursuant to his employment or contract with the Commission.
Printed in the USA. Price
25
cents. Available from theTABLE OF CONTENTS
Introduction. • • •
. . .
. . . .
. .
. . .
.
Part I~ Tabulation of Compounds.
. . .
.
. . . .
.
. .
Part II~ References • • • • •
Part III: Structure Details.
. .
. .
. . .
.
. . .
. .
. .
. . .
.
. . .
. . . .
. .
6
22
5
TABULATION, BIBLIOGRAPHY, AND STRUCTURE OF BINARY INTERMETALLIC COMPOONDS. I. COMPOUNDS OF LITHIUM, SODIUM, POTASSIUM, AND RUBIDIUM.
By S. ,G. Epstein, D. M. Bailey, R. L. S~the, G. R. Kilp, and J. F. Smith
INTRODUCTION
The compilation of the material in this report was undertaken to provide a convenient reference source for intermetallic compounds. An adequate
bibliograpny is required for most efficient use. It is in this sense and because of the addition of more compounds that the compilation is considered an exten~ion of the compilation in Smi thell 1 s "Metals Reference Book."
Undoubtedly there are some compounds listed in the compilation which either do not exist or have been assigned the wrong formulae. It seems
o~vious, for instance, that not. all of the reported sodium-mercury compounds should exist. For purposes of evaluation, the experimental basis for the report of a compound is included under "Remarks" after the comp911nd.
The material is, separated into three·sections. The first 1part consists
of a tabulation and includes the crystal class, lattice parameters, and
COMPOUNDS LiAg CRYSTAL CLASS, cubic cubic hexag-onal hexag-onal hexag-onal
PART I: TABUlATION OF COMPOUNOO
LATTICE 0 PARAMETERS (A)
a=J.l7
a:6.261 c=l0.25
a•2. 788 c=4.J94
a=4.37l
c=2 .515
REJ.<"ER-STRUCTURE REMARKS ENCES
B2 X-ray powder data, numeri-cal intensitief?, thermal
analysis, metallography. 1, 2,3,4
X-r~ powder data, quali-tative intensities, numer-ical intensities; formulae Li9Ag1,, Li10Ag1 , and Li12Ag also ~eported ~nd are
probably indicative of a region of solid solubility.
1, 2.,
5
Some evidence for super-lattice, possibly Fe3Al type below ~420°C; superiattice formulae reported also as Li1Mg~, cubic with a=9.7,
ana
as Li2Mg~, cubic with 91,92, a•J.513; still in debate. 6,7cl4
Thermal analysis and hardness data.
X-ray powder data, numer-8
ical intensities. 9
A3 Numerical intensities,
x-ray powder data. 9,10
X-ray powder data. 6
LD~h--
X-ray powder data, numerical intensities, thermal analysis, P63/mm~ electrical resistance;formulae Li3zn7, Lin Rzn2, and LiZn2 also report~d with same lattice
CRYSTAL LATTICE 0
REFER-COMPOUND CLASS PARAMETERS(A) STRUCTURE REMARKS ENCES
Li2Zn3 cubic a:4.27 Thermal analysis, electric resistance, and x-ray
powder data. 3,6,11
LiZn cubic a=6.222 B32 X-ray powder data,
numer-ical intensities. 3,.4
LiCd3 hexag- a:3.089 A3 X-ray powder data, numer-onal c=4.899 ical intensities, thermal
analysis, conductivity and
dilatometric data. 12,13
LiCd3 cubic a=8.62 compli- X-ray powder data, thermal
cated analysis. 3,14
cubic
LiCd2 Phase diagram. 15
LiCd cubic a::6. 701 B32 X-ray powder data,
numer-ical intensities. 4,12
LiCd cubic a:3.33 B2 X-ray powder data, numer-ical intensities, thermal
data. 3,16,14
Li3Cd cubic a::4.259 Al X-ray powder data, numer-ical intensities, thermal
analysis. 3,12,16
LiHg5 Phase diagram--doubtful. 17
LiHg3 hexag- a:6.253 D019 X-ray powder data, numer-onal c=4.804 ical intensities, thermal
analysis. 3,18,19
LiHg2 II 18,19
LiHg cubic a:3.24 B2 X-ray powder data, numer-ical intensities; parameter
values reported as high 3,4,18,
as 3.294. 19
Li 2Hg X-ray powder data, thermal
CRYSTAL LATTICE 0
REFER-COMPOUND CLASS PARA.METERS(A) STRUCTURE REMARKS ENCES
Li3Hg cubic a:::6.561
no
3 X-ray powder data, numer-ical intensities, thermalanalysis. 18,19
Li6Hg Thermal analysis. 19
LiAl cubic a::6.372 B32 X-ray powder data, quali-tative intensities, thermal
analysis, temperature- 20,21 resistance and micrographic 22,23,
data. 24
Li2Al Thermal analysis,
tempera-ture-resistance and
micro-graphic data. 23,24
LiGa cubic a::6.208 B32 X-ray powder data,
numer-ical intensities. 3,4
Liin cubic a:6.8oo B32 X-ray powder data, numer-ical intensities, thermal
analysis. 3,4,19
Li2T13 Thermal analysis and
tern-perature-resistance data. 25
LiTl cubic a::3.431 B2 Thermal analysis, x-ray pow-der, numerical intensity and
temperature-resistance data.3,4,25
Li2Tl Thermal analysis and
tem-perature-resistance data. 25
Li5T12 II 25
Li3Tl II 25
Li4Tl II 25
Li2Si X-ray powder data; no
intensities given. 26
CRYSTAL LATTICE 0
REFER-COMPOUND CLASS PARAMETERS (A) STRUCTURE REMARKS ENCES .
----
----Lisn4 Thermal analysiso 27
Li 2sn5 Thermal analysis and
tem-perature-res istcn ce data. 15,28
LiSn2
"
27,28LiSn Thermal analysis, temper- 27,2.:3,4
ature-resistance data, x-ray powder data; no intensities given.
Li3Sn2 Thermal analysis. 15,27
Li2Sn Thermal analysis and
tern-perature-resistance data. 27,28
Li5Sn2 II 27,28
Li7Sn2 II 27,28
Li4Sn
"
27,28LiPb cubic a=3.529 B2 Thermal analysis, tem
pera-ture-resistance and x-ray
powder data. 4,29,30
Li5Pb2 Thermal analysis and
tem-perature-resistance data. 30
Li10Pb3 cubic a=lO.OlO D83 X-ray powder data,
numer-ical intensities. 31
Li3Pb hexag- a:4.27 D018 Thermal analysis and
tem-onal c=7
.59
perature-resistance data. 30Li7Pb2 II 30
Li4Pb II 30
Li3N hexag- a=3 .. 665 X-ray powder data,
numer-onal c=3.890 ical intensities. 32
Li3N cubic a=5 .51 X-ray povrder data, q1
COMPOUND
Li3P
Li3As
o<-Li3Sb
fJ
-Li3SbLiBi
Li3Bi
Li2S
Li2Se Li2Te NaAu CRYSTA.L CLASS hexag-onal hexag-onal hexag-onal cubic tetrag-onal cubic cubic cubic cubic
· hexag-onal
LATTICE o PARAMETERS (A)
a•4.273 c:7 .594
a=4.396 c:7 .. 826
a::4.no c:8.J26 a:6.572 a:3.368 c::4.256 a=6. 722 a:5. 720
a:6 •. 0l7
a::6.517
a=7 .5ot2 c=l2. 29
REFER-STRUC'IURE REMARKS
- -
ENCESn~s X-ray powder data, numer-ical intensities. 34
Do-18 It 34
DO:J.s It 34
no
3 It 34110 X-ray powder data, numer-ical intensities, thermal analysis and electrical
resistances. 3,4,3.5
D03 Thermal analysis and
electrical resistances.
3,35,36
Cl X-ray powder data,
numer-ical intensities. 3,37
Cl
"
37Cl
"
37Cl4
X-ray powder data,Debye-Scherrer. 38.
Thermal analysis.
CRYSTAL LATTICE 0 REFER-COMPOOND ClASS PARAMETERS (A) STRUCTURE REMARKS ENC&S
NaAu2 cubic a=7. 7872
±
.0023 Cl5 X-ray powder data. 40,41,59
Na2Au tetrag- a:7 .402 Cl6 Rotation, Weissenberg,
onal c:5.511 and x-ray powder data. 41
Nazn13 cubic a=l2.2836 D23 X-ray powder data, compar-! 0.0003 ison of F0 and F~; F
obtained by multlple0film
technique. 61,40
NaCd2 cubic X-ray powder data, thermal,
micrographic, and
electri-cal investigations. 42,53
NaCd5 Thermal, microbTaphic, and
electrical investigations.
53
Nacd6 II
53
NaHg or tho- a=7 .19 - 2h--/i517 Weissenberg and precession rhombic b:l0 •. 79 x-ray data, visual
estima-c=5.21 Cmc_!!!7 tion of intensities, least squares refinement of data;
R
=~I
F0 - Fe J~ iFol
=
20.3't.62NaHg2 hexag- a=5 .0290 C32 X-ray powder data. 62 onal :!: .0005
c=3.2304 ! .0016
NaHg4 hexag- a:61.5 ~230 NaHg4 per cell;
onal c=9. 7 Weissenberg data. 62
NaHg5 Thermal preparation (grown
from melt); existence
doubtful. 64
NaH~ It 64
COMPOUND NaHg8 NaHg9 NaHg10 NaHg12 NaH;gl4
Na3Hg
Na3Hg2
Nain NaTl NaSi CRYSTAL CLASS tetrag-anal rhombo-hedral cubic cubic
LATTICE 0
PARAMETERS(A)
a:S.52 c:7 .80
a=7 .312
REFER-STRUCTURE REMARKS ENCES
Thermal preparation{grown from melt); existence 64 doubtful.
It 64
"
64II 64
II 64
Thermal analysis. 46
LOG~--
Weissenberg and precessionx-ray data, visual
estima-P42/mn~tion of intensities refined
B32
B32
by electron density maps, least squares refinement
of data. 62
Precession x-ray data. 62
Thermal analysis. 46
X-ray powder data. 43,59
II 44,59
Thermal analysis and tem -perature-resistance data. 54
II 54
Thermal analysis; existence
cp. estionable. 47
Thermal analysis and
tem-perature-resistance data. 54,47
COMPOUND NaSi2 NaGe NaSn NaSn2 NaSn3 NaSn4 Nasn6 Na2Sn Na3sn Na4sn Na4sn3 Na4sn9
Na1~n4
NaPb
Na Pb 2.
CRYSTAL LATTICE 0
CLASS PARAMETERS (A) STRUCTURE REMARKS
REl<"'ER-ENCES
tetrag- a=4.98 X-ray powder data; possi-onal c:l6~ 7 bility of different cell. 60
Reported as formed by method used above for NaSi. 55
fhase diagram. 66
It 66
It 66
II 66
II 66
It 66
It 66
It 66
II 66
Reported on basis of for-mation of precipitate~ and discontinuity in potentia-metric titration curve \men Na was titrated with Sni 2 in aqueous NH3 • 67 or tho- a=9.82 """D86 Powder, rotation, and
rhombic b=22.82 Weissenberg x~ray data. 45 c:5.59
tetrag- a:lo.58o fj520 Crude single crystal data anal ±o.oo5 4h- plus x-ray powder data;
c::l7 .. 746 ~/acE_? least s~ares refinement of
:0.015 Pb positions; (FQ-FC) refine-ment of Na posit~ons; powder intensities gotten by compar-ison with calibrated film. 63,59 H298: -11.& kcal/mol.
CRYSTAL LATTICE REFER-COMPOUND CLASS PARAMETERS(A) STRUCTURE REMARKS ENCES
Na2Pb5 a=4.88 Ll2. Conflicting x-ray evidence l about compound's existence. 17,65
Na!J'b Phase diagram. 17
Na4Pb7 cubic a.=4.873 Reported on basis of precip-itation during potentiometric titraticn, and discontinuity
in potentiometric titration
curve. 67,3
Na4Pb9 lti 67
Na5Pb2: Phase diagram. Ji.7
Na15Pb
4
cubic a=l3 .31 D86 Powder, rotation, and Weissenberg x-ray data; visual estimation ofinten-sities. 45,33
Na3;1Pba ~.=13.2.7 78 atoms per cell. 69,94
NaJJ hexag- a:4 .• 99 DOJ.B
J4
onal c=8.81
Na3~s hexag- ~=5.089 DO~e X-ray powder data. 34,59
anal c=8.99 67
Na3!ts3~ Reported on basis of precip-itation during potentiometric titration, and discontinuity in potentiometric titration
curve 67
Na~s5
"
'
67Na_t.s 7 Ill 67
NaSb Analog of NaBi 44,67
Na3Sb hexag- a.=5 .367 D018 34
CRYSTAL LATTICE
REFER-COMPOUND CLASS PARAMETERS(£) STRUCTURE REMARKS ENCES
NaBi tetrag- a=3 .47 LlO Superlattice; x-ray powder
onal c=4.81 data. 44,59,3
Na3Bi hexag- a=5.459 D018 X-ray powder data. 34,59 onal c=9.674
Na3Bi5 Reported on basis of
precip-itation during potentiometric titrAtion, and discontinuity ip potentiometric titration
curve. 67
Na2
o
f.c.cubic a=5.56 Cl X-ray powder data, visualestimation of intensities. 37,49
Na2S f.c.cubic a::6.526 (Cl X-ray powder data. 37,59,)
Na~2 Reported on basis of
precip-itation during potentiometric titration, and discontinuity in potentiometric titration
curve. 67
Na2S3
"
67Na2s4
"
67Na2s5 II 67
Na2s6
"
67Na2S7 It 67
Na2se f.c.cubic a:6.81 Cl II 37,67,3~
Na2se2 It 67
Na2se3 II 67
Na2se4 It 67
Na2Se5 II 67
16
COMPOUND
CRYSTAL LATTICE CLASS P ARA:Mh'TERS (
j)
NaTe
f.c.cubic a=7 .32
N01 K-Li compounds
No K-Rb compounds
KCs
STRUCTURE REMARKS
REFER-ENCES
Cl
Reported on basis of pre-cipitation during titration, and discontinuity in poten-tiometric titration curve;
thermal analysis.
57,6
7Phase diagram; thermal
analysis.
Thermal analysis.
57
Reported on basis of pre-cipitation during titration,
m d discontinuity .in poten-tiometric titration curve.
67
II
Phase diagram; thermal
analysis.
67
Complete solid insolubility .)9·
Complete solid solubility. 39
Very doubtful thermal analy-sis; later work (39) dis-putes evidence of CsK
compound. 50,39
Both Au2K and AuhK were pos-tulated on grounas of their x-r~- powder spectra, which were distinctly different from both pure K and Au. No struc-tures or parameters were deter-mined from the x-ray patterns.
COMPOOND
KAu
CRYSTAL CLASS
No K-Mg compounds
KCd 13 KCd7 KHg cubic cubic tri-clinic
LATTICE 0 PARAMETERS (A) a=l2 .38 a•l3.81 a::6.62 b::6.91 c::6.94 cx:lo6°, fi= 102°191 ' ~=92°481
KHg2
KHg3
KHg4
KHg8 or 9
KHgll cubic
No K-Al compounds
a::9.65
STRUCTURE REMARKS
REFER-ENCES D23 D23
/C~---
~Pfl
Determined by vacuum fusion~-doubtful.
Complete solid immisci-bility.
X-ray powder data.
tt
Thermal analysis.
Viscosity measurements in liquid amalgam indicated
51
82
71,72
71,72
82.
solid stable compound K2Hg. 73
Determined AHform., llF,
and AHsoln. from emf. cells. 81
Precession x-ray data, single crystal; Patterson and elec-tron density refinemen~s.
Thermal analysis.
n n II 80,93
52
52
52.5-2
(Same structure as BaHg11 .) 80,68
Complete solid
immisci-bility. 82
18
COMPOUND
KTl
KSi
KGe
KSn
KSn 2
KSn4
CRYSTAL LATTICE 0
CLASS PARAMETERS (A) STRUCTURE REMARKS
RE.F'ER-ENCES
Thermal analYsis; structure of KTl not isomorphous w.i. th NaTl, as determined by
Debye-scherrer method.
4,58
X-ray powder data and thermal analyses indicated
exis-tence of these compounds.
55
II
55
"
55
II
55
Thermal analysis and phase diagram; (work done in
1907). 69
" 69
" 69
II 69
" 76
11 76
Thermal analysis, phase diagram; compound checked with hardness tests and electrical resistivity by
(83). 76,83
II 76 J 83
CRYSTAL LATTICE 0
REBER-COMPOUND ClASS PARAMETERS(A) STRUCTURE REMARKS ENCES
K3As hexag- a=5. 793 0018 X-ray powder, De bye -Scherrer
onal c:l0.242 data. 34
K3Sb hexag- a=6.037
onal c=lO. 717 0018 II 34,74
KSb Thermal analysis. 48
K3Bi hexa.g- a=6.180 oo·l8 Debye-Scherrer x-ray powder
on&l c:l0.955 data.. 34,84
K9Bi? Thermal analysis.
lh
K3Bi2
"
84
KBi 2 cubic a=9.52 Cl5 Debye-Scherrer x-ray powder
data. 75,84
K2Se cubic a:7 .691 Cl De bye-S c herrer x-ray powder
data. 37,77
K2se2 Phase diagram constructed
from thermal analysis; com-pounds determined by Debye-Scherrer x-ray powder method, but structures not
deter-mined. 17
K2se3 II 71
K2Se4
"
77K~se5
"
77K2Te cubic a=8.168 Cl Debye-Scherrer x-ray powder
data. 37,77
K2Te2 Phase diagram by thermal
analysis and Debye-Scherrer x-ray powder data for com-pound determination, but
COMPOUND
CRYSTAL LATTICE
CLASS ~ETERS(~) STRUCTURE REMARKS
REFER-ENCES
KRe
No K-Fe compounds
RbAu2
RbAu
RbHg5
Rb2Hg9
Rb5Hgl8
Rb2Hg7
RbHg2
cubic a.=l3 .88
Phase diagram by thermal
analysis and Debye-3cherrer x-ray poVIder data for com-pound determination, but structures not determined.
77
n
77
Paramagnetic properties of alloy of composition ReK indi-cates probable compound
for-mation by Re with K. 78
Solid and liquid
immisci-bility. 79
Both gold compounds made by vapor diffusion; no struc-ture details.
X-ray powder data. 71
Compounds postulated by
magnetic susceptability
meas-urer:1ents and thermal
analysis. 86,90
II
II
II
II
II
86,90
86,90
86,90
86,90
CRYSTAL LATTICE 0 REFER-COMPOUND CLASS PARAMETERS(!) STRUCTURE REMARKS ENCES
RbJH% Compounds postulated by
magnetic susceptability meas-urements and therm~
analysis. 86,90
Rb7HgB II 86,90
RbHg11 cubic Similar to KHg~~; no
param-eters determin • 87
RbHgl2 cubic a=lO. 71 87
RbC,1 hexag- a=4.95 Method of preparation not
onal c=22. 70 given. 88
RbC16 hexa.;;- a=4.95
onal c=l7 .99 II 88
RbSi X-ray patterns of RbSi,
RbSi , RbGe, and RbGe4 were
RbSis
take~,
but only shown, notworked out; samples prepared by direct union and
subse-H.bGe quent volatilization of one
component~
RbGe4 55
a=6. 29 4 X-ray powder data; sample
Rb3Sb hexag- ffis
h--onal c=ll. 23 prepared by addition of C6/mmE_7 alkaline metal vapor to
PART II: REFERENCES
1. Pastorello, S., Gazz. chim. ital. 60, 493 (1930).
2. }reeth and Raynor, J. Inst. Metals 82, 569 (1954).
3. Taylor, A., "X-Ray Metallography," pp. 373-375 (John Wiley & Sons Inc., New York, 1952).
4. Zintl and Brauer,
z.
physik. Chern. B20, 245-252 (1933).5. Perlitz, H.,
z.
Krist. 86, 155 (1933).6. Baroni, A., Congr. intern. quim pura y apl.--Frao,o IX~' 75 (1934).
7. Grube, V. Zeppelin, and Bumm,
z.
E1ektrochem. 40, 160 (19.34).8. Zamatorin, M., Metallurgist
1'
96 (1938).9. Hellner and Laves,
z.
Krist. 105, 134 (1943).10. Zint1 and Schneider,
z.
Elektrochern. h1, 764 (1935).11. :}rube and VosskU.hler, Z. anorg. Chern. 215, 211 (1933).
12. Zint1 and Schneider,
z.
E1ektrochem. 41, 294 (1935).13. Grube, VosskUhler, and Vogt,
z.
E1ektrochem. 38, 869 (1932).14. Baroni, A., Atti accad. naz. Lincei, Rend. 6 18, 41 (1933).
15. Masing and Tamrnann,
z.
anorg. Chern. 67, 183 (1910).16. Baroni, A.,
z.
Elektrochem. 40, 565 (1934).17. Hansen, M., 11Aufbau der Zweistofflegierungen, 11 p. 919 (Edwards Brothers,
Inc., Ann Arbor, Michigan, 1943).
18. Zintl and Schneider,
z.
E1ektrochem~ 41, 771 (1935).19. Grube and Wolf,
z.
Elektrochern. 41, 675 (1935).20. Pastorello, S., Gazz.chirn. ital. 61, 47 (1931).
21. Komovsky and Maxirnow,
z.
Krist. A92, 275 (1935).22. Zintl and Woltersdorf,
z.
Elektrochern~ 41, 876 (1935).24. Shamray and Saldau, Izvest. Akad. Na1~ S.S.S.R. (khirn.)
l,
631 (1937). 2.5. Grube and Schaufler,z.
Elektrochem. 40, .593 (1934).26. Klemm and Struck,
z.
anorg. Chern. 278, 117 (19.5.5).27. Baroni, A., Rend. reale accad. nazl. Lincei 16, 153 (1932).
28. Grube and Meyer, Z. Elektrochem •. 40 771 (1934).
29. Nowotny, H., Z. Metallkunde 33, 388 (1941).
30. Grube and Klaiber,
z.
Elektrochem. 40, 745 (1934).31. Rollicr and Arreghini,
z.
Krist. 101, 470 (1939).32. Zintl and Brauer,
z.
Elektrochem. 41, 102 (193.5).33.
Brill, R.,z.
Krist. 6.5, 94 (1927).34. Brauer and Zintl,
z.
physik. Chern. B37, 323 (1937).3.5. Grube, Vossklihler, and Schlecht,
z.
Elektroche~. 40, 270 (1934).36. Zintl and Brauer,
z.
Elektrochem. 41, 297 (193.5).37. Zintl, Harder, and Dauth,
z.
Elektrochern. 40,588
(1934).38. Laves and Wallbaum, Z. anorg. Chern. 250, 110-120 (1942).
39. B5hm and Klemm,
z.
anorg. Chern. 243, 69-85 (1939).40. Perlitz and An1ja,
z.
Krist. AlOO, 1.57-166 (1938).hl. Haucke, W.,
z.
Elektrochem. 43, 712-719 (1937).42. Pauling, L., J. Am. Chern. Soc. 4.5, 2777-2780 (192-3).
-.
43. Zintl and Neumayr, Z. physik. Chern. 20, 272-27.5 (1933).
44.
Zintl and Dullenkopf, Z. physik. Chern. Bl6, 193 (193c).4.5. Zintl and Harder,
z.
physik. Chern. B34, 238-254 (1936).46. Hansen,
M.,
op. cit., p. 792.47. Hansen, M., op. cit., p. 933.
49. Zintl and v. Baumbach,
z.
anorg. Chern. 198, 88-101 (1931).50. Goria, C., Gazz. chim. ital. 65 (2), 1226-1230 (1935).
51. Sommer, A., Nature 152, 215 (1943).
52. Hansen, M., op, cit., p. 778.
53. Allaria, S., Atti reale accad. sci. Torino,_ Classe sci. fis. mat. e
nat. 78, 145 (1942-3).
54. Grube and Schmidt,
z.
Elektrochem. 42, 201-209 (1936).55. Hohmann, E.,
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637 (1952).62. Nielsen and Baenziger, Acta Cryst.
1,
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A l: oh--Fm3m
s
PART III: STRUCTURE DETAILS
A=4: atoms at 000;~!; ~;0~}
Reported compounds: Li3Cd
Remarks: Implied in this structure is a random distribution
of the atomic species on the lattice sites. This probably is not true at low temperatures.
A 3:
D~h--P6
3
/mmc
B 2:
B 32:
A=2: atoms at l/3,2/3,1/4; 2/3,1/3,3/4
Reported compounds: LiCd3 and LiZn9
Remarks: See Remarks under A 1 structure.
1
Oh--Pm3m
A :2: ordered ,1.9 -brass or CsCl structure
with Cs (Oh): 000
Cl (Oh): ~~g
Reported compounds: LiAg, LiCd, LiHg, LiTl, and LiPb
Remarks: LiAl was originally reported in this structure, but
more recent work indicates the B 32 structure. LiCd has
also been reported in both B 2 and B 32 structures, but
which is the correct structure for LiCd is less clear.
7
Oh--Fd3m
A:16: NaTl structure
with 8 Na (Td): 000;
tH;
+F. C.8 Tl (Tq): ~~~; fH; +F. C.
IF.
C. - add 000 • .wL l.~ • 0--4..· and o~11 to all coordina te_s7LJ: - ' 2 2'22 , 22' 22
Reported compounds: LiZn, LiCd, LiAl, LiGa, Liin, NaTl, and Nain
C 1:
0~
--Fm.3mA:l2: fluorite structure, Ca}2
with 4 Ca (0 ): 000 +F. C.
8
F
(Td~: ±(
!
!
~
)+F.
C.
Reported compounds: Li2S, LizSe, LizTe, Na2
o,
Na2s, Na2se, Na2Te,K2Se, and K2_Te.
C 14:
D~h--
r
6
3
/mmc
A=l2: Laves Phase--MgZn2 structure
with 4 Mg (C3v): ~(l/3,2/3,z; l/3,2/3,1/2-z); z-:::d./16
2 Zn (n3d): OOO;OO!
6 Zn ( C2v): !(x, 2x,. ~; 2x,i, :};
x,x,
;j); x~-1/6Reported compounds: Li2Ca, Na2K.
C 15:
O~--Fd3m
c
16:A:24: Laves Phase--MgCu2 structure with 8 Mg ( T d) : 000; -~ 11
+
F'. C.16 Cu (D3d):
5/B,SJB,5/8; 7/8,7/8,5/8; 7/8,5/8,7/8;
5/8,7/8,7/B
,
+F.
c.
Reported compounds: KBi2, NaAu2·
nt~--I4/mcm
A=l2: CuAl2 structure
with 4 cu (D4): :!:(oat) B. c.
8 Al (C2v):1 ~(x,tTx,O;
t
+x,x,O)
+B. C.LB·
C.=
add 000 and 2~J to all coordinate~?Reported compounds: Na2Au with x=O.l60.
C 32: Dgh--P6/mmm
A:3: AlB2 structure
with l A1 (D6h): 000
2 B (D3h): 1/3,2/3,1/2; 2/3,1/3,1/2
28
D ~9:
<{-Fm3m
A=l.6: Biti3 structure with 4 Bi (Oh):
4
Li (Oh): 8 Li (Td):000 t-F. C •
.1.il ' 221_ +F,.
c •
.±( 4U) +F.c.
Reported compounds: Li3Hg, Li3Sb, Li3Bi
Remarks,:· Li3Sb exists also in tm hexagonal D o18 structure.
D~h
--P63/llll00A=8: Na3As structure with 2 As (n3h):
· 2 Na (DJh):
4
Na (C3v):!(1/3,2/3,1/4) :t( 00t)
±(l/3,2,.13,z; 2/3,1/3,1/2+z);,z-o.583
Reported compounds: Li3Pb, Li3Sb, Li3P, Li3As, Na3As, Na3P, Na3Sb, Na3Bi, K3!s, K3Sb, K3Bi, Rb3Sb
Remarks: See also D 03.
D~h--P6
3
/mmc
A::8: Mg3Cd structure with 2 Cd (Djh) :
6 Mg (C2v):
±(1/3,2/3,1/4)
:t( 2x,x,
i;
x,x,
i;
x,
Zx, i); x -::::::1/6Reported compounds: LiHg3•
6
oh--Fm3c
A:llZ: NaZn13 structure
with B Na (0): ±(~H) +F.
c.
8 Zn (Th): 000;~~~ +F. C.
96 zn (C8 ): ±(o,y,z;~; f,z,y; ~; o,y,z;
?;
f,z,y;~)+F. C.
~~ = permutation!?
Reported compounds: NaZn13 with y=O.l8o6 and z:O.ll9Z, RbCd13 with y:O.l78 and z:O.l22,
L 10:
L 12:
Oh--Im3m;
T~--I43m;
andT~--P43m
A=$2: a-brass structures. The basic structure consists of a cubic unit cell whose edge is three times the edge of a simple body-centered cubic cell. From this large cell of 54 atomic sites is abstracted 2 atomic sites with small attendant shifts in parameters of some of the 52 occupied sites. The space group depends upon the formula of the compound and the atomic species occupying the various atomic sites.
Reported compounds: L~~Ag (reported formula varies from Li1zAg to Li3Ag), Li10Pb3 •. (Li5P!>2)
Remarks: l-brass structures usua],.ly exhibit extensive compo-sition variation.
T~--I43d
A=7~: c~
5
~a typew~th
1~
Cu (S4): O,l/4,3/8;~l
0,3/4,1/8i~
+
~·
C. 48 Cu (C1 ): x,y,z; ? ; x,y,~z; 'i); ;a-x,y,z; j) ;i,!-y,z; Yi); -!+y,i+x,~; ~; ~y,-l-tx,3/4-z; ~;
i-t-y,3/4-x,~z; Q; 3/4-y,-}-x,~z; ';);+B. Ca x:O.l2, y=O.l6, z-o.o4
16 Si (c3):
xxx;x,x,!-x;
~;:l+x, i-tx,
i.,.x;
~x, :t+x,3/4-x; ~ : x:0.208Reported compounds: Na15Sn4, Na15Pb4 (Na31Pb8).
1
n
4h--P4/mmmA=2: CuAu type superlattice with 1 Cu (D4h): 000 1 Au (D
4
h): ~~~Reported compounds: LiBi, NaBi, NaSb
(?).
1
Oh--Pm3m
A=4: Cu3Au type superlattice with 1 Au (Oh): 000
3 Cu (D 4h • ) • 1;{).l. 2 2J 22J22 o.:u • ~
Reported compounds: Na2Pb5
2.0 .
n
4h-I4/acdA::64: NaPb structure
with 3 2 Pb (
c
1 ) :Remarks:
14
4 ;
·
n
4
h--P 2 mnmA:20: Na3Hg2 structure
with
a
Hg(Cs):
(x,x,z; ~x,~-x,~z; x,x,z; !-x,~~x,~+Z): x=0.12.5
:t
0.0005, z:0.190 ± 0.0014
Na (c2v): !:(x,x,O;t+-x,rx,t):
x-0.210 ±0.010 4Na (C2v): ±(x,x,O; 2+x,2-x,2): x:0.368±0.0104
Na (C2h): 0~;~0;0~~;~~Remarks: R(hko)=
~JFo-
Fcl=
8.4~
~IFol
A:16: NaHg structure
with
8
Hg(Cs):
4
Na (c2v):.
4
Na (c2v):Remarks : R
··
=
ill
o- F cI
~I
Fo/
Oh--Pm3m
A=36: KHg11 structure with 3 K (Dhh):
1 Hg (Oh):
8 Hg (c3v):
12 Hg (
c
2v) :12
Hg(C2
v):A~3: Li
7
zn1R
structurewith 2 Zn (~3tJ:
±(l/3,2/3il/2)
~.8 L~ tD
3
d):000;002
Reported compounds: Li
7
zn18 (and formula variations)Remarks: Evidently a high percentage of the Li sites are unoccupied, and the symmetry would indicate that the vacancies are random.
1
-C. --Pl
~
A=8: KHg structure
with 2 Hg (
c
1 ) :2 Hg (C1 ): 2 K (C1J:
2_ K (C1):