Glass formation and crystallization in the GeSe2-GeTe-Sb2Te3 system

Glass formation and crystallization in the GeSe2-GeTe-Sb2Te3 system

Thermochimica Acta, 133 (1988) 287-292 Elsevier Science Publishers B.V., Amsterdam GLASS FORMATIOB AND CRYSTALLIZATIOB S. SURIffACHI, M.D. BARON, ...

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Thermochimica Acta, 133 (1988) 287-292 Elsevier Science Publishers B.V., Amsterdam

GLASS

FORMATIOB

AND CRYSTALLIZATIOB

S. SURIffACHI, M.D. BARON, 1 Departament

de Ffsica,

de Barcelona, 2 Departament

Facultat

de Clencies,

08193-Bellaterra,

Diagonal

III THE GeSe2-GeTe-Sb2Te3

W.T. CLAVAGUBRA-MORAl

d'Estructura

de Flsica,

287

and B. CLAVAGUBRA' Universitat

Autonoma

Spain

i Constituents

647,

SYSTEM

de la Materia,

08028-Barcelona,

Facultat

Spain

ABSTRACT

The

glass

GeSe2-GeTe-Sb2Te.8 differential

molten

scanning

forming

region

deduced.

The

process

and

formation

for

calorimetry

effective

compositions

parameters

that

of

the

type

of

the

of

glass

The

was

crystallization

that characterize former8

means

of 103 K/min

were analysed

best glass

the

by

diffraction.

of the order energy

activation

water-quenched

of

investigated

and X-ray

rate

All the results

empirical

It is concluded

was

alloys

a cooling

was obtained.

the current

crystallization

in the light glass

In

of

formation.

that system

are


IBTRODUCTIOK

As there

no absolute

is

parameters

are extensively

of the glass related reduced

to

forming the

glass

respectively takes

a value

Ill. Another

ability

equilibrium temperature,

the glass of about parameter,

for glass

criterium used

formation,

for quantitative

of molten phase

diagram.

Tgl=Tg/T1,

transition

alloys.

introduced

characterization

Some

T

and the liquidue

by

Hruby

parameters

One of

where

2/3 for a large number

of

empirical

them and

is Tl

8 temperature.

glassy

the are Tgl

substances

C21 is Kg1 defined

Thermal Analysis Proc. 9th ICTA Congress, Jerusalem, Israel, 21-25 Aug. 1988 004~6031/88/$03.50 Q 1988 Elsevier Science Publishers B.V.

are

as

Kgl=
have

kinetic,

for

crystallization subsequently parameter defined

peak.

instance the

of

give

Other

the

by

a measure

would,

parameters in

by

the glass

of

to

fundamentally energy

Turnbull

I41.Another

of the

according

are

free

introduced

Uhlmann

of the onset

formers

change

liquid

developed

to

Good glass

values.

high Kg1

as

T, is the temperature

where

kinetic forming

in

the

c31

and

empirical

ability

was

ES1 as A' = kOexp(-E/RTg>

where kg

activation

E is the effective

the

pre-exponential

an Arrhenius

factor

ability.

with

geometrical

atomic

(assumed

to have

of & or In(x) will be indicative

Other

glass-forming

and

of crystallizatlan

of the rate constant

Low values

form).

energy

parameters

and

deal

atomic

size

are structural bonding

arrangement,

and

of

effects.

In this paper and

we present

crystallization

molten

alloys.

characteristic

crystallization

scanning

calorimetry

EXPERIKRNTAL

procedure

given

obtained

by water

(estimated

quenching melting

lines of 48 mol

Z GeSe

eutectlcs

transformations

the effective

glasses

c51.

activation

from

differential

the

calorimetric

shown

and

The

state

OP

the

rate at

800 K

of

10"

The glass

forming

cooling

diffraction.

compound and

is the experimentally

the binary

and

been derived

of the

by X-ray

the congruently

figure

state

elsewhere

samples

was checked


of

have

formation

AND DISCUSSION

the preparation

water-quenched K/min>

to the glass

(DSC).

RESULTS

were

related

of the structural

the glassy

of

on

behaviour

The temperatures of

energies

Details

the results

glaasy

in Fig.1 C&Se2

is roughly

and

the

30 mol X Sb*Te3, determined

of the systems

eutectlc GeS--GeTe

limited

by

equicomposition

Also shown valley and

region

in

this

connecting

GeSeg-SkTea

289 There

is certntnfy

I relationship

and the microscopic it is likely The most

arrangamant

significant

of them,

studlees and spectroscopic and,

GeSe3,2,

SbpTe3

SbaSe+/2.

t&sing these

crass-linked forming

random

compositions

of atoms,

specific

that some

between

molecular

as deduced

analysis to

a

glassy

in the GeSe2-GeTe-Sb2Te3

fnsids

the dashed

lines and the limits

Figure

1

alloys

: C--->

quenching

forming

predicted

the melt

It is represented

region

for

. C--->>

exist.

distribution

may be GeSq,2r

GeSe,

and

G@T%/2 of a

fully

the resulting

glass

quasi-ternary in Pig.

section

1 by the region

of the composition

triangle,


by structural

in water

system

units

from radial

ws can guest

system.

.- G&ass

StructuraL

as the precursors

of the quaternary

region

In the Ce-Sb-Se-Te

extant,

unfts

network

forming

in the binaries,

lesser

molecular

the glass

units

eutectic

I

t-)

line

obtained

,

by

290 The

general

forming

conclusion

region

aforementioned

on

with

comparing

this

"theoretical"

la

the

experimental

one,

units

are probably

present

molecular

glass

that

In the

the

glasses

studied.

To get an estimate 1 the values

of the glass

of the temperatures

of crystallization, parameter.

the

most of the glasses crystallization

value

the effective

The values

and

and

B,

onset

the

HI

kinetics

of

of

the

161 has been used

and to estimate

formers

in

system,

the of

1 allows

103

glass are

K/min,

mol '5 GeTe and

shown

are also

to conclude

the

inside

about

of 155

x, was also estimated

for -In(X)

obtained of Table

composition

in Table

of the overlapping

energy,

of the parameter

analysis

rate

temperature

the peak method

activation

Careful

cooling

transltion

crystallization.

because

However

we present

the

~51.

the value

Therefore,

glass

of the

was hindered

exotherms.

of ln(kg)

glass.

study

ability

of the glass

reduced

The detailed

to obtain

forming

that

In Table

region alloys

1.

glass

the best

forming those

for each

for

a

with

a

12t5 mol X Sb2Te3.

CONCLUSIOBS

The glass

formation

water-quenched system

molten

the glasses

thermal

In

water

of these

the GeSe2

alloys

through glass

the use of

formers

parameter

some

by DSC

quantities the

thermal

of the system

coincide

of

activation

of

as

with those

on crystallization

the quasi-ternary

First

determined

From the values rich

behavlour

Then,

energy

and

kinetic

region

characteristic

for crystallization heating

the glass-forming

deduced deduced

the

on continuous

quasi-ternary

of

GeSe2-GeTe-Sb2Te3

all the glass-forming

was obtained.

and effective were

of

alloys

analysed.

have been

for quenching temperatures

and

was

parameters.

from the values

from the values

regime.

ability

system

of

of

studied The

of the

of the ';

best Kgi

291 Table

1 .- Temperatures

parameters Glass

for

effective


< * Hegting

composition x

Y

0

0 0

5

10 15 20 24 25 30 0 0 0 0 0 0 0 0 0 5 10 10 10 10 10 15 20 20 20 20 25 30

0 0 0 0 0 0

10 15 20 30 35 40 45 47 50 15 10 15 20 30 40 15 10 15 20 38 15 10

structural

energy

crystallization of

rate 20 K/min

667 613 563 536 526 501 497 480 650 642 637 617 608 595 585 581 579 572 552 547 542 536 527 518 507 510 515 497 485 485

crystallization

; Htuby parametet

temperatures (K) T T, g 777 725 685 652 630 593 587 545 746 764 734 725 722 710 686 674 652 701 683 682 680 645 605 652 610 603 578 552 548 531

transformations

(GeSe2)100-x-y
(T,g)w and

activation

temperatures

x.

glassy

transition

of

and kinetic samples CT,,)*;

temperatures (E);reduced


parameter

).

activatiotl energy B(kJ/g.at)

136 148 152 158 210 226 207 233 240

270 163 171 211 176 206 250 210 168 167 175 223 221 187

glass

glass forming parameters Kg1 XlogCAl Tgl A in (et-9 .656 .460 .477 .639 4.875 .578 * 628 ,648 .663 .658 .612 5.176 .651 .520 5.115 .471 .639 4.172 .608 .265 4.528 .659 .398 4.801 4.699 .692 .522 5.326 .690 .639 .694 .740 6.024 .865 .706 .721 .808 .782 .733 .704 .427 5.306 5.334 .634 .701 5.644 ,957 6.471 .665 5.068 .667 1.038 6.460 .693 .845 .633 .342 5.971 .653 7.066 .950 . 648 5.155 ,659 4.953 ,472 ,638 .278 4.339 .640 4.356 .605 .204 4.626 .600 .242 .594 .161 3.314

292 parameter. nearby

These

best

glass

of 15 mol X GeTe hgd

formers

have

a composition

in

the

12 mol %.S$Teg.

ACKBOWLBDGEMBBTS

This work was supported Cientifica

y TBcnica"

the "Comisi6n

by

(CAICYT)

project

Asesora

de

Investigaci6n

n0759/84.

REFERENCES

1 S. Sakka 2 A.

Hruby,

and J.D. Mackenzie, Czech.

3 D. Turnbull,

J. Phys.,

Contemp.

4 D.R. Uhlmann,

J. Bon-Cry&.

Sci.,

6 D.W. Henderson,

Bz

(1972)

Solids

5 (1971)

145.

1187.

&Q (1960) 473.

Phys.,

5 S. Surifiach, M.D. Barb, J. Mater.

J. Non-Cryst.

Solids,

7_ (1972) 337.

M.T. Clavaguera-Mora

and i. Clavaguera,

19 (1984) 3005. J. Non-Crlst.

Solids

30

(1979) 301.