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OPTICAL AND OTHER PHYSICAL PROPERTIES OF Al (PO3)3 - CONTAINING FLUOROPHOSPHATE GLASSES

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HAL Id: jpa-00222487

https://hal.archives-ouvertes.fr/jpa-00222487

Submitted on 1 Jan 1982

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OPTICAL AND OTHER PHYSICAL PROPERTIES OF Al (PO3)3 - CONTAINING FLUOROPHOSPHATE

GLASSES

J. Yasi, J. Fusong, G. Fuxi

To cite this version:

J. Yasi, J. Fusong, G. Fuxi. OPTICAL AND OTHER PHYSICAL PROPERTIES OF Al (PO3)3

- CONTAINING FLUOROPHOSPHATE GLASSES. Journal de Physique Colloques, 1982, 43 (C9),

pp.C9-315-C9-318. �10.1051/jphyscol:1982958�. �jpa-00222487�

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JOURNAL DE PHYSIQUE

Colloque C9, supplement au n°12, Tome 42, decembre 1982 page C9-315

OPTICAL AND OTHER PHYSICAL PROPERTIES OF A l ( P 0

3

)

3

- CONTAINING FLUORO- PHOSPHATE GLASSES

J . Y a s i , J . Fusang and G. Fuxi

Shanghai Institute of Optics and Fine Mechanics, Academia Sinica, Shanghai, China

Résumé.- Dans cet article, on étudie les propriétés optiques et d'autres pro- priétés physiques de verre fluorophosphate comprenant le système a deux com- posantes de A1(P0„)„ et l'influence de divers fluorures sur ces propriétés dans le verre de basse teneur de Al (PO.,), . On donne le site de verre de basse teneur de Al(P0,)

3

a la figure de n

d

„ v , et une partie des propriétés de

divers fluorures dans le verre.est calculée.

Abstract.- In this paper, the optical and some other physical properties of fluorophosphate glasses in binary systems containing A1(P0

3

)

3

and the influence of various fluorides on the properties of glass with low A1(P0

3

)

3

content have been studied. The positions of low A1(P0,), content glasses in n.~v diagram have been plotted and the partial properties of fluorides in glass have been calculated.

Fluorophosphate glass is a glass with special optical properties such as high Abbe value, transmittance in near UV and IR regions and low nonlinear refractive index (np), it is now under development. Comparing the properties of various glassy meta- phosphate, it shows that A1(P0.,), possesses a higher refractive index, a greater Abbe value

1

-

J

as well as better physical and chemical properties. Therefore A1(P0,)

3

has been introduced into many fluorophosphate glasses. The authors have already studied the formation and structure of Al(POo), - containing fluorophosphate glas- ses r2l

L

, and in the present work, the optical and some other physical properties of

those glasses are investigated with the emphasis placed on the low A1(P0,)

3

content glasses.

The following glass systems were selected for the investigation 1) (100-X),A1(P0

3

)

3

.X RF

p

( R = Li, Na, Ba, Sr, Al ) .

2) (10 A1(P0

3

)

3

.20 A1F

3

.5Q SrF

2

.20 LiF) + 5 RF

p

( R = Li, Na, K, Be, Mg, Ca, Sr, Ba, Zn, Cd, Pb, Al, Gd ) .

3) (5 A1(P0

3

)

3

.28 A1F

3

.30 SrF

2

-27 CaFg.lO LiF) + 3 RF

p

{ R = Li, Na, K, Mg, Ca, Sr, Ba, Zn, Al, Ga ) .

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1982958

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C9-316

JOURNAL DE PHYSIQUE

Aluminium metaphosphate and f l u o r i d e s were used as s t a r t i n g m a t e r i a l s . Glasses w i t h h i g h A1(P03)3 content were melted i n s i n t e r e d alumina c r u c i b l e s , and o t h e r s i n p l a t i n u m c r u c i b l e s . D i f f e r e n t m e l t i n g c o n d i t i o n s were selected according t o d i f - f e r e n t glass systems.

The r e f r a c t i v e i n d i c e s (nd, nF, nC, n ) , t h e thermal expansion c o e f f i c i e n t s a, t h e moduli of e l a s t i c i t y E, and t h e d e n s i t i e s of t h e glasses were determined, t h e 9 molecular volumes o f glasses, t h e average atomic volumes o f f l u o r i n e and oxygen V

OF' and t h e p a r t i a1 r e f r a c t i v e i n d i c e s and Abbe values o f v a r i o u s f l u o r i d e s i n glasses were c a l c u l a t e d .

1 ) I n t h e previous workLz1, on t h e b a s i s of experimental r e s u l t s o f glass formation, d e v i t r i f i c a t i o n and s t r u c t u r e study, we p o i n t e d o u t t h a t t h e network o f t h e glasses w i t h 1 ow A1 (P03)3 c o n t e n t i s g r e a t l y destroyed. Therefore t h e p r o p e r t y v a r i a t i o n of these glasses should be s i m i l a r t o t h a t of t h e oxide glasses i n t h e destroyed region. I n general, t h e r e f r a c t i v e index and d i s p e r s i o n increase w i t h i n c r e a s i n g i o n i c r a d i u s r, w h i l e

a

and E v a r y w i t h the e l e c t r o s t a t i c f o r c e z/a2 between ca- t i o n s and f l u o r i n e i o n s ( Fig.1 and 2 ) .

F i g . 1 nd vs r ( A ) i n t h e Fig.2 a30-Tg vs z/aL i n t h e system w i t h 10 mol% A1 (P03)3 system w i t h 10 mol% A1 (P03)3

2) I n t h e r e g i o n w i t h low A1(P03)3 content, some f l u o r i d e s such as L i F , MgF2 and AlF3 c o u l d reconnect t h e d i s r u p t e d glass network[21. T h i s i s a l s o r e f l e c t e d i n t h e v a r i a t i o n o f t h e p h y s i c a l p r o p e r t i e s o f glass. I n A1(P03)3 - RFn systems, those c o n t a i n i n g L i F o r AlF3 possess s m a l l e r VOF (Fig.3), and w i t h t h e increase i n the RFn content, t h e increase i n VOF i s r e l a t i v e l y slow. The LiF, MgFz, A1F3- c o n t a i n i n g glasses a l l have h i g h e r E and lower VOF (Fig.4,5), i t can be considered as t h e increase i n compactness o f glass s t r u c t u r e .

3) I n t h e glasses w i t h v e r y low A1(P03)3 content, besides t h e p a t i c u l a r r o l e o f

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A1 (PO*) rMol%

F i g . 3 Dependence o f VOF on t h e A1(P03)3 c o n t e n t i n A1(P03)3 - RFn systems

10

\ BaF2 S r h

F i g . 4 Dependence o f E on t h e A1 (P03)3 c o n t e n t i n A1 (P03)3- RFn systems

L i F , MgF2, AlF3 mentioned above, o t h e r c a t i o n s f i l l i n g i n t h e i n t e r s p a c e between s t r u c t u r a l c h a i n s can a l s o enhance t h e g l a s s s t r u c t u r e t o some e x t e n t due t o t h e e l e c t r o s t a t i c a t t r a c t i o n . G e n e r a l l y speaking, VOF depends on t h e r e l a t e d i o n i c r a d i i . However, f o r t h e g l a s s e s w i t h l o w A1(P03)3 c o n t e n t , f r o m t h e diagram o f V

2 O5

vs Z/a ( F i g . 5 ) , i t can be o b v i o u s l y seen t h a t VOF decreases w i t h i n c r e a s i n g Z/a .

Combining t h i s and t h e v a r i a t i o n s i n

a

as w e l l as E, i t can be c o n s i d e r e d t h a t e l e c t r o s t a t i c f o r c e has r e l a t i v e l y g r e a t i n f l u e n c e on t h e p r o p e r t i e s o f g l a s s when t h e g l a s s network i s h e a v i l y destroyed.

0 0.5 1.0

Zid

Fig.5 V a r i a t i o n o f VOF i n systems w i t h 10% A1 (P03)3 as a f u n c t i o n o f Z/a 2

4) F i g . 6 shows t h e p o s i t i o n o f t h e s t u d i @ d

g l a s s e s c o n t a i n i n g 5%, 10% A1 (P03)3 i n nd-v

diagram w i t h t h e a d d i t i o n o f v a r i o u s f l u o r i d e s .

U s i n g t h e o p t i c a l c o n s t a n t s o f a l l t h e g l a s s e s

s t u d i e d i n t h i s work, t h e p a r t i a l r e f r a c t i v e

i n d i c e s and Abbe v a l u e s o f some f l u o r i d e s

i n t r o d u c e d have been c a l c u l a t e d , and t h e r e -

s u l t s o b t a i n e d a r e l i s t e d i n T a b l e 1 t o g e t h e r

w i t h some d a t a f r o m l i t e r a t u r e . From T a b l e 1,

we can see t h a t t h e r e i s g r e a t d e v i a t i o n s

among t h e d a t a f r o m d i f f e r e n t sources. Never-

t h e l e s s , we can a l s o see t h a t w i t h t h e i n c r e a s e

i n t h e metaphosphate c o n t e n t , t h e p a r t i a l r e -

f r a c t i v e i n d e x i n c r e a s e s , w h i l e t h e v de-

creases and t h e i n f l u e n c e o f f l u o r i d e s on t h e

p r o p e r t i e s o f g l a s s l e s s e n s . Hence, t h e p a r -

t i a l p r o p e r t i e s o f f l u o r i d e s can o n l y be

s u i t a b l e f o r c a l c u l a t i n g p h y s i c a l p r o p e r t i e s

o f g l a s s e s i n a c e r t a i n r e g i o n .

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JOURNAL DE PHYSIQUE

I.

Fig.6 P o s i t i o n s o f glasses

w i t h a d d i t i o n o f f l u o r i d e s on nd-v diagram

1.60

a. A1 (P03)3 = 5 mol%

b. A1(P03)3 = 10 mol%

90 S 80 ?O

a b

Table 1. The Partial Properties of Some Fluorides

1 source Our work Ref. [I] Ref. [3] Ref. [31

A1 (P03)3<10 A1 (P03)3>30 A1 (P03)3<15 A1 (PO3I3-30 -

F l u o r i d e

-.-n,, v nd "d nd

L i F 1.43 110 1.549 - 1.45 109 1.479 78

NaF 1.314 121 - - 1.37 118 - -

MgF2 1.321 121 1.47 - 1.41 133 1.461 86

CaF2 1.413 104 1.516 - 1.47 81 1.465 80

SrFp 1.455 84 1.53 62 1.531 70.8 1.471 79

BaF2 1.567 74 1.607 - 1.59 63.4 - -

A1F3 1.333 120 1.486 78.6 1.40 128 1.424 98

References

[I] GAN FUXI, " C a l c u l a t i o n o f P r o p e r t i e s and Design o f Composition o f I n o r g a n i c Glasses", Shanghai Science Press, 1981, Shanghai.

[2] GAN FUXI e t a l . , " O p t i c a l Glass", Science Press, 1964, China.

[3] PETROVSKII G.T. e t a l . , The S o v i e t Journal o f Glass Physics and Chemistry, 5(1979) 85.

-

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