The use of hydrothermal procedures to synthesize NASICON and some comments on the stoichiometry of NASICON phases

The use of hydrothermal procedures to synthesize NASICON and some comments on the stoichiometry of NASICON phases

895 Solid State Ionics 9 & 10 (1983) 895-902 North-Hoard ~bli~jng Company THE USE OF HYDROTHERMAL PROCEDURES TO SYNTHESIZE NASICON AND SOME COMMEN...

557KB Sizes 16 Downloads 385 Views

895

Solid State Ionics 9 & 10 (1983) 895-902 North-Hoard ~bli~jng Company

THE USE OF HYDROTHERMAL

PROCEDURES TO SYNTHESIZE NASICON

AND SOME COMMENTS ON THE STOICHIOMETRY

OF NASICON PHASES

Abraham Clearfield, M. A, Subramanian, W. Wang, * P. Jerus

Department of Chemistry, Texas A&M University, College Station, Texas 77843, U.S.A. *Visiting Scholar, Fuzhou University, People's Republic of China NASICON was prepared by a two step process. and Na4Si04 are treated hydrothermally approximate composition an orthorhombic

at 300°C.

In the first step zirconium phosphate This produced a hydrated phase with

Na4Zr2Si2 25P1 80 15 'H2 0 which could be indexed on the basis of

cell with a = 8.743(l); b = 10.317(4), c = 7.317(l)&

this orthorhombic

phase to llOO"C, P205 splits out to yield monoclinic

Upon heating NASICON of com-

This formula reflects both a deficiency of ZrO2

;;;i;;;; Na3.3Zr1.65Si1.9P~.1011.5compensated by Na for charge balance,over that required by Nal+xZr2SixP3_xO12. It is proposed that both a NASICON series of the latter type and the defect type described in this paper exist,with the stoichiometric

one being unstable and degrading to

the defect structure upon heating. 1.

INTRODUCTION

NaZr2(P04)3 and Na4ZrSi30,D and not Na4Zr2Si3-

Interest in ceramic solid-state electrolytes for use in battery applications

has led to

a widespread search for new ionically conducting materials

[l].

@,2 as Hong proposed for NAS~CON.

Thus, an

extended study to reconcile these differences was initiated.

Until recently B-alumina and

Our work with zirconium phosphate [9] led

~~-alumina were the premier materials with the

us to new preparations of NaZr~(PO4)3

requisite high conductivity and favorable cera-

high temperature reactions [lO,ll] and by hy-

mic properties.

drothermal methods

More recent discoveries of NA-

SICON [2] and Na5M(III)Si40,2

type compounds [3]

indicate that fast ion conduction materials may be more widespread thought.

in ceramic than originally

Intensive investigation of these ma-

terials is warranted

both fromthepoint

of practical applications

of view

formed NAS~CON, could also thermally.

this synthesis and a comparison of the products

EXPERIMENTAL

2.1 Materials

that a complete solid solution of the type

A highly crystalline a-zirconium

existed over a range of x =

l+xZrZSixP3-x012 o-3. Maximum conductivity was reported for x = Subseouently,

be prepared hydro-

In this paper we present details of

with high temperature solid state preparations.

2.

In the case of NASICON, it was reported [4]

2-2.3.

It was also shown

[ll] thata precursor phase, which on heating

and the structure-con-

duction mechanism relationships.

Na

[13].

both by

other workers [5-71 re-

phosphate

(hereafter referred to as a-ZrP) was prepared by refluxing the gel in 12M H3PO4 for 36 hours [12].

It was characterized

by X-ray diffraction

ported that excess Zr02 was always present in

and TGA which showed it to be a-Zr(HP04)2'H20,

their preparations.

while electron microprobe analysis showed less

In fact, Von Alpen et al.

CS] stated that pure NASICON cannot be prepared

than 50 ppm total impurities.

by Hong's method [4].

phosphate (ZrP207) was prepared from d-ZrP by

They proposed instead

a new series of the type Na,+xZr2_x,3SixP3 '12-2/3x'

x-

The end members of this series are

0 167-2738/83/0000-0000/$03.00 0 1983 North-Holland

Zirconium pyro-

heating in a platinum crucible at 1OOO'C for several hours.

Zr02 (99.9975%) and Si02

~99.999~~) were Puratronic grade (Johnson Matthey).

Na4SiO4 and Na2Si03 were Fisher cer-

was determined as Mg2P207.

The details of the

analytical procedures were given elsewhere

tified and Na2C03 (99.999%) was from Aldrich.

[12].

The starting materials were dried at 200°C and

by electron microprobe and X-ray fluorescence

stored in a desiccator before weighing.

techniques

2.2 Hydrothermal Hydrothermal

In addition, the samples were analysed (Micron, Inc., Wilmington,

Delaware).

Synthesis

The standards for the above analyses were pre-

reactions were carried out in

pared from highly pure starting materials

by

teflon lined Parr bombs of 300ml capacity. The

solid state reactions in sealed Pt tubes (4mm

procedure is given in the form of a flowchart

dia.) to avoid evaporation of P and Na.

in Figure

and Si were also determined by an ICPA method.

1 and outlined in our earlier paper

[131. 2.3 Compositional Analysis Quantitative

Thermogravimetric

The Na

analysis was carried out with

a Columbia Scientific Industries model TGA=3A

elemental analyses were per-

formed by wet chemical and instrumental methods.

unit at heating rate of lO"/min. 2.4 X-ray Methods

In wet chemical analysis, the sample was

X-ray powder diffraction patterns were ta-

brought into solution in HF and zirconium was

ken with a PAD11 (Scintag) computer automated

determined by precipitating

diffractometer

as Zr-Cupferron

complex and igniting to Zr02.

The phosphorous

i ).

using CuK(l radiation

(I = 1.5418

The patterns were run by step scanning the

samples at O.O3"/5sec and the position of each peak was determined by PEAK SEARCH programs (locally modified)

supplied with the PADII.

Guinier patterns were obtained with a camera (Enraf-Nonius) with quartz monochromator, In all the cases, silicon 1 powder NBS-SR 640 with a = 5.43088A, was used r(CuK;b = 1.54056i).

as an internal standard.

lattice parameters

were obtained by least-squares fitting of accuTRANSFER TEFLON LINED BOMBSAND STIR 60% FILLING I 3OOOC HYDROTHERMAL. -120ATM.

20HRS.

rately determined d-spacings using program LSUCRE (141. 2.5 Ionic Conductivity Measurements Ionic conductivities

were measured by an

impedance technique on sintered discs (13 lnm dia. and 3-4 mm thick) from room temperature to 300°C using Hewlett Packard impedance meters (models 4800A and 4815A) in the frequency range

HEATED

1200°C

5Hz to 108MHz.

The discs were prepared by

pressing the powders in an evacuable die at 20 tons/sq. in. for 15-20 hr.

They were sintered at 1150-12OC"C The hydrothermally

prepared

NASICONS gave pellets of density 92 - 95:, of Figure

1

:

The discs were polished

Block diagram of the hydrothermal

theoretical values.

synthesis of NASICON.

with 400 grit emery paper and the faces were coated with conductive silver paint (E-Kote 3027, Acme Industries Co.) and dried at 200°C for 6 hours.

The sample was sandwiched between

A. Clearfield et al. / The use of hydrothermal procedures

891

two platinum plates which were spring loaded to

Na4Si04 in varying proportions at 300°C and 120

ensure good electrode/electrolyte

Atm. pressures are given in Table 1.

contact.

The

Among the

entire cell assembly was placed in a tubular

various new phases formed, the most interesting

furnace whose temperature could be controlled

compound for the present purpose is one desig-

to +2"C using a Barber-Coleman

nated as the 6.06 phase [the number designates

524D).

controller

(model

The furnace and the cell assembly were

grounded to avoid stray A. C. fields.

the first interplanar spacing (i) in the X-ray

For a

diffraction pattern].

particular solid sample, at a constant tempe-

This phase could be iso-

lated in pure form when the ratio of a-ZrP to

rature, the values of Z'(/Zlsine) and -Z"(iZl-

Na4Si04 were 1:1.4 to 1:1.7. The X-ray diffrac-

cos8) were calculated and plotted.

tion patterns looked similar (but with a slight

The elec-

trolyte resistance was obtained by extrapola-

shift in d-spacings) and were hydrates with one

ting the electrode characteristics

mole of H20.

3.

to -Z" = 0.

Wet chemical and microprobe ana-

RESULTS

lysis showed the phase to be a sodium zirconium

The results of a number of hydrothermal

silicophosphate monohydrate.

reactions obtained by heating u-ZrP with

TABLE 1:

RESULTS OF HYDROTHERMAL

Expt. No.

Reactant Ratio a-ZrP:Na4Si04

NPJ 17A

1.O:l.O

The chemical for-

mula as derived from the analytical data for

SYNTHESIS - Zr(HP04)2 H20 (c+ZrP) + Na4Si04 AT 3OO'C

Time

20

Hydrothermally Phases

Formed

High Temperature (1200°C) Phases Formed

6.06(10) + 6.3(5) + 6.5(5) + F(80)

NPJ 17B

1.O:l.O

98

6.06(40) + 6.5(5) + F(5)

*R-N(75)

+

I(25)

**

+ 9.2(50) MSW 15

l.O:l.O(2NaCl)

20

6.06(80) + F(20)

R-N(90)

+

U(10)

MSW 24

l.O:l.l(:2NaOH)

20

6.06(40) + 6.47(20)

M-N(88)

+

Zr02(12)

R-N(83)

+

I(17)

+

I(4)

+

Zr02(20)

+ 7.90(20) f 11.1(20) MSW 16

1.0:1.2

20

6.06(70) + 11.5A(20) + F(10)

MSW

9

1.0:1.3

20

6.06(95) + 12.9(5)

M-N(96)

MSW 10

1.0:1.4

20

6.06(100)

M-N(lOO)

MSW

7

1.0:1.5

20

6.06(100)

M-N(lOO)

MSW 11

1.0:1.6

20

6.06(100)

M-N(lOO)

MSW 12

1.0:1.7

20

6.06(100)

M-N(lOO)

MSW 13

1.0:1.8

20

6.06(60) + 6.5(40)

M-N(80)

MSW 14

1.0:2.0

20

6.06(50) + 6.5(50)

MSW 20

1.0:3.0

20

6.5(100)

*R-N = Rhombohedral NASICON, M-N = Monoclinic NASICON; for other phases see Text ** Numbers in parenthesis are approximate

percentages

A. Clewfield et al. / The use of‘ hydrothermal procedures

898

the 6.06 pears

phase

obtained

from a 1:1.5

sample

to be Na4Zr2Si2.25P1.8015*H20.

analytical

data

are

ap-

The

6.06

(wt%)

Found:

Na, 13.93;

Zr, 27.6;

Si, 9.85;

P, 8.56

Calc:

Na, 14.1;

Zr, 28.0;

Si, 9.7;

P, 8.5

X-ray

diffraction

samples

showed

on heating, phase

dexed

broadened

these

change

patterns

patterns

and gave

(Figure

crease sized

The

in Table

phases

around

sion was much more fraction phases solid

patterns

were

Thermogravimetric phase

from

the unit cell unit cell increase

data

the Na4Si04

TABLE

2:

parameters

heated

loss

. 9'1 . 1'11 . 5

Found:

Na, 14.8;

Zr, 29.8;

Si, 10.8;

P, 7.1

Calc.:

Na, 15.1;

Zr, 30.1;

Si,

P, 6.9

The TGA pattern There

is a weight is attributed

from

the 6.06 phase

there

is observed continuous

6.06

phase.

in

temperatures

weight

amounting

loss

in a

to about

experiment,

from a sample

It was only

by the bands

4;:.

to the loss of P205 from

decomposition

contained

absorption

a further

In a separate

component

perature

is confirmed

At higher

manner

is attributed

latile

which

spectrum.

This

3.

to the split out of water

of the water

infrared

10.7;

in Figure

loss of ?,2.85 up to 150°C.

This

disappearance

is shown

of the high

of the 6.06

soluble

phosphorus

phase

in water,

tem-

was

acidic

as analysed

the

the vo-

and

by plasma

arc technique.

(A)

HYDROTHERMAL

(6)

NASICON

(6.06)

PHASE

with

3.

The

but small, due

of the sample

in the reactant

as

PHASE

I

ratio.

fluorescence

CELL PARAMETERS OF HYDROTHERMALLY PREPARED PHASES (6.06)

aZrP: Na4Si04

a(A)

I

I

35

30

0

b(%

c(A)

25

I

I

20

15

28

MSWW7

1:1.5

8.743

10.317

7.317

MSWW12

1:1.7

a.777

10.611

7.354

Variation

Na3.3Zrl.65Sil data are (wtX)

(1:1.4

possibly

0

Sample

The analytical

to,

from

in Table

parameters

X-ray

is close

the NASICONS

a systematic,

and

which

the

28).

a weight

were monoclinic

in Si content

microprobe

from

from

gave a formula

collected.

(Figure

All

given

indicate

increased

UNIT

dif-

but were

preparations

Na4Si04)

in the lattice

to an increase

Electron

of 6.7% when

hydrothermal

:

[4,6]

showed

to 1100°C.

n-ZrP

X-ray

obtained

impurities

analysis

temperature

to 1:1.7;

at 1200°C.

obtained

(tr-ZrP:NaSiO4 = 1:1.5)

slow,

but the conver-

by others

free of Zr02 and other

obtained

was

the 6.06

a slow conver-

to NASICONS

reactions

for the 6.06

in-

sample

phase

the

of the high temperature

similar

state

the in-

to a-ZrP

compounds,

rapid

cell and

phases

Heating

indicated

type

in-

it is hypothe-

of Na4Si04

1OOO'C

sion to NASICON

diffraction

From

in these

1.4 to 1.7.

but

of the NASICON

precursor

without

data were

2.

parameters,

as the ratio from

X-ray

X-ray

that the Si content

increased

peaks,

dehydrated

of an orthorhombic

are given

in lattice

creased

room

diffraction

sharper

2).

on the basis

the results

of the air dried

compounds

analyses

due to Si content

& heating

treatment

Figure

2

:

Comparison

of X-ray

powder

terns

of the hydrothermally

pared

6.06 phase

heated

- (A) and to 1200°C

patpre-

to 600°C

- (B)

899

A. Clearfield et pl. 1 The use of hydrothermal procedures

In another experiment,

the 6.06 phase was

a small amount of impurities so the conductivity

treated with 6M HCl at 300°C in a sealed teflon lined Parr bomb.

data was not obtained.

The product was a rhombdhedral

proton form of NASICON.

Some interesting facts emerge from consider-

The filtrate contained

Nat and PO:- (phosphomolybdate

test).

ation

of the mixed products which arise from

the hydrothermal study.

Thus, it

The starting material,

appears that the 6.06 phase has a framework

aZrP, is an ion exchanger with a layered struc-

structure which is robust and stable to water

ture [16] which forms a half-exchanged

loss but converts to NASICON phases when enough

ion phase and a fully exchanged one, Zr(NaP04)2-

P205 is removed, either by acid extraction, or

3H20, referred to as phase II [lo].

by evolution at high temperatures.

On heating

phase D to lOO'C, it forms a monohydrate

In order to confirm the stoichiometry of the hydrothermally

sodium

E) and at 200°C an anhydrous phase F.

prepared NASICON a solid

(phase

The ma-

jor product obtained in the hydrothermal exper-

state reaction, using a mixture of Na3P04, Zr02,

iment NPJ#17A (Table 1) was this phase F.

SiO2 and ZrP207 in the correct ratio was carried

er heating times (NPJ#17B) produces more of the

out at 1200°C for 20 hr in sealed platinum

6.06 phase together with a new compound labelled

tubes.

This reaction yielded a pure phase

9.2.

Long-

Heating this mixture to 1100°C produces

whose X-ray pattern matched that shown in

rhombohedral NASICON and phase I.

Figure 28.

phase was reported earlier [ll] as resulting

Ionic conductivity data on all the hydro-

from the decomposition

This latter

of Zr(NaP04)2 at 1100°C.

thermally prepared NASICONS, in the form of sin-

In a subsequent paper it will be shown that

tered disks, are given in Table 3 and Figure 3.

phase I belongs to a solid solution series of

The data show that all the NASICONS behave like

the type Nal+4xZr2_x (P04)3 where x = 0.85-1.0

superionic conductors with the highest conduc-1 -1 tivity of 0.17 ohm cm at 300°C for the sample

[13,15].

the NASICON phase and observation of a rhombo-

prepared from the reactant ratio of 1:1.7.

hedral NASICON indicates that insufficient Si

The

Thus, most of the silicon resides in

conductivity at room temperature and 300°C

is incoporated into the hydrothermal phases

showed a slight increase as the Na4Si04 content

when the ratio of reactants is 1:l.

increased in the hydrothermal reaction.

of this hydrothermal experiment

The

sample obtained from the ratio 1:1.3 contained

TABLE 3:

aZrP: Na4Si04

a(i)

MSWW9A

1:1.3

MSWWlOB

in the presence

of excess NaCl (MSW#15) increased the yield of

UNIT CELL PARAMETERS AND ELECTRICAL DATA OF HYDROTHERMALLY

SAMPLE

Repetition

'RT

PREPARED NASICONS

a300"c -1

Ea(<200) ev

Ea(>200) ev

b(i)

c(i)

B(O)

15.591

8.992

9.215

123.75

1:1.4

15.603

9.013

9.214

123.62

6.6x10-4

0.11

0.38

0.21

MSWW7A

1:1.5

15.609

9.023

9.214

123.60

2.5~10-~

0.15

0.39

0.20

MSWWllA

1:1.6

15.623

9.020

9.215

123.2d

3.1x10-4

0.17

0.41

0.20

MSWW12A

1:1.7

15.627

9.018

91223

123.23

3.3x1o-4

0.17

0.40

0.21

a, b, c values are ?O.OOli; B values are ?O.Ol"

ohm-'cm-'

ohm-'cm

900

A. Clewfield

e[ al. / The use of’hydrothermal

TEMP

Figure

3

Weight

:

loss as a function

Heating

6.06 phase

which

hedral

NASICON

latter

phase

on heating

together

ceeded

state

of Na4Si04

1.7 a new phase, This

(MSW#20) similar

phase

and gave

4.

and

study

has shown

NASICON-like

route.

This

result

in which

hydrothermally materials

requires licate

its

pattern

CON,

of NASICON

In this formulation NASICON

solid

it is possible

were

prepared

relative et al.

both end members

solution,

to

out of our earlier

by Hong,

NaZr2(P04)3

twelve

solutions

the anions

are present.

and

that Zr02

anionic

0.50 moles

groups

of oxygen

also

Thus,

contain

are either

ortho-

Loss of oxygen

condensed

by assuming

oxygens.

phosphate

This

then

or si-

loss can be

-that the ortho-system orecipitates behind. and

leaving

In our NASI-

therefore

0.25

of Zr are thus eliminated ilydrothermally. c+ is missing and In addition, 0.1 mole of 7r

via a hydrothermal

some comment

phase.

moles

The stoichiometry

[ll].

groups

condensed

[13] and

and

that either

is unstable

some-

solid

or orthosilicate.

rationalized

in a pure

We original-

Nai'r2(P04)3 phases

requires

formulation

arose

oxygens

ex-

NASICON

that

phases

twelve

to w-ZrP

6.5, made

contain

the intermediate

phosphate

DISCUSSION This

(TGA) for the 6.06

and Na4Zr2Si30,2,

This

it at a later date.

prepare

work

U.

[15].

an X-ray

it as a hydrated

rhombo-

Na5Zr(P04)3

to that of NASICON.

upon

of temperature

I series

labelled

ly labelled report

gave

was obtained

will

("Cl

5"/minute.

some phase

of the phase

the ratio

appearance.

what

again

has the composition

is the end member When

with

rate

procedures

of our to the [2,4].

of the and

the charge Thus

deficiency

the formula

can

is corpcnsated be represented

by Na+. as

Nal+z+4vZr2_x_vSizP3_z012_0.,. Tr ?'?e formula iA for our hydrothermal p;‘er;arat'on, x =

given

0.25, y = 0.1, and z = 1.9. Von Alpen stoichiometric cate groups their

series

et al. phases

[8,17].

have also based The

is Na4ZrSi30

obtained

on condensed

silicate

nonsili-

end member

of

,. and they succeeded

A. Clearfield et al. / The use

in preparing this compound and showing that it is a fair conductor

[18].

However, their com-

positions do not fit the proposed solid solu-

of hydrothermal procedures

901

or employment of special gel methods of synthesis [4,19,20].

A similar ciaim is made for

Na3Hf2Si2P012 and As and Ge substituted composiIn fact, Weunsch et al. [20] have

tion formula of Nal+xZr2_,,3xSixP3_x0,2_2,3x,

tions [Zl].

nor do they fit our general formula.

carried out a neutron diffraction

Since no

study on

details of their analytical methods were given,

Nal+xZr2SixP3_x072

it is not possible to assess the limits of er-

They confirmed the structure proposed by Hong

ror in these formulas.

and were able to explain the volume changes

They did not observe a

change in slope in the curve of conductivity,as

with x = 7, 1.6, 2.0 and 2.5.

with increasing values of x.

Thus, we believe

a function of temperature, for Na3 lZr, 55 -

that Hong's series does exist, but the phases

Si2.3Po 7011 as is observed for our prepara-

are quite unstable when x = 1.5-2.5.

tions. 'Thus the von Alpen phases may in fact

Gordon et al. [7] found that Zr02 precipitates

be quite different in structure from NASICON.

from such compositions

*

.

In fact,

if they are heated above

On the other hand, our unit cell dimensions

1200°C.

and conductivity

to obtain singie phase NASICON until they re-

data are very close to those

reported earlier for Nal+xZr2SixP3_xO12

[4,61.

The question arises as to what the correct formulation for NASICON really is.

Several

moved 0.5 moles of Zr02.

Thus, their composi-

tion is close to Na3Zr, SSi2PO,, and must then contain condensed silicate groups. In an earlier study [13] we showed that

groups have reported a single phase NASICON, achieved either by thorough mixing of reagents

Boilot et al. [6] likewise were unable

stoichiometric

NaZr2(PO4)3 does not exist, or

is very difficult to prepare.

Rather, a solid

solution of the type Nal+4xZr2_x (PO4)3 with x = 0.02-0.06 was synthesized.

Although it is

difficult to see why the defect structure would be preferred (except perhaps to fill some of the empty type II cavities for added stability) the 4xNa+ could account for the conductivity of the triphosphate.

We are checking this point.

However, we make the point that our hydrother4+ ma1 preparation shows both the ZrO2 and Zr deficiency for maximum stability and the more stoichiometric

phases may degrade to the defect

type on heating by precjpitation of fro;. 5.

ACKNOWLEDGMENT This work was supported by NSF grant number

DMR 80-25184 for which grateful acknowledgment is made, 6. 2

I

3

4

1000/T,(K)

Figure

4

:

Conductivity as a function of l/T for the hydrothermal samples. ZrP:Na4SiO4

=

1.5,

ZrP:NaSiO4

=

1.7,

0

0.

,

REFERENCES

[ 11 P. Hagenmuller and W. von Gool, eds., Solid Electrolytes (Academic Press, New York, 1978). ['2] J. B. Goodenough, H.Y.-P. Hong and J.. A. Kafalas, Mat. Res. Bull. 11 (1976) 203. [ 33 R. D. Shannon, H. Y. Chen and T. Berzins, Mat. Res. Bull. 12 (1977) 969. [ 41 yi3Y.-P. Hong, Mat. Res. Bull. 11 (1976) [ S] M. i. Bayard and G. G. Barna, 3. Electroanal. Chem. 91 (1978) 201.

902

A. Clearfield et al. / The use of hydrothermal procedures

[ 61 J. P. Boilot, J. P. Salanie, G. Desplanches and D. LePotier, Mat. Res. Bull. 14 (1979) 1469. [ 71 R. S. Gordon, G. R. Miller, B. J. McEntire, E. 0. Beck and J. R. Rasmussen, Solid State Ionics 3/4 (1981) 243. [ 81 U. Von Alpen, M. .F. Bell and H. H. Hofer, Solid State Ionics 3/4 (1981) 215. [ 91 A. Clearfield, in: Inorganic Ion Exchange Materials, ed.A. Clearfield (CRC Press, Boca Raton, Florida, 1982) ch. 1. [lo] A. Clearfield, W, L. Duax, A. S. Medina, G. D. Smith and J. R. Thomas, J. Phys. Chem. 73 (1969) 3424. [ll] A. Clearfield, P. Jirustithipong, R. N. Cotman and S. P. Pack, Mat. Res. Bull. 15 (1980) 1603. [12] A. Clearfield and J. A. Stynes, J. Inorg. Nucl. Chem. 26 (1964) 117. [13] A. Clearfield, P. Jerus and R. N. Cotman, Solid State Ionics 5 (1981) 301.

[14] LSUCRE, Least Squares Unit Cell Refinement, Univ. Freiburg i. Br., West Germany (1972). [15] A. Clearfield, R. Guerra, A. Oskarsson, M. A. Subramanian and W. Wang, Mat. Res. Bull., submitted for publication. [16] A. Clearfield and G. D. Smith, Inorg. Chem. 8 (1969) 431. [17] U. Von Alpen and M. F. Bell, Extended Abstracts, Spring Meeting, The Electrochem. sot., Montreal, No. 732 (1982) 1170. [18] U. Von Alpen, M. F. Bell and H. H. Hofer, Solid State Ionics 7 (1982) 345. [19] D. H. H. &on, T. A. Wheat and W. Nesbitt, Mat. Res. Bull. 15 (1980) 1533. [20] B. J. Wuensch, L. J. Shioler and E. Prince, Abst. Amer. Cryst. Assoc. Winter Meeting, Univ. of Missouri, Columbia, MO., March 1983. [21] R. J. Cava, E. M. Vogel and D. Johnson, Jr., Amer. Ceram. Sot. Comm. C-157 (1982).