INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS: CONDENSED MATTER
J. Phys.: Condens. Matter 15 (2003) 8235–8252 PII: S0953-8984(03)69718-3
Structure of dysprosium and holmium phosphate
glasses by the method of isomorphic substitution in
neutron diffraction
Richard A Martin
1
, Philip S Salmon
1,4
, Henry E Fischer
2
and
Gabriel J Cuello
3
1
Department of Physics, University of Bath, Bath BA2 7AY, UK
2
LURE, Centre Universitaire Paris-Sud, BP 34, F-91898, Orsay C´ edex, France
3
Institut Laue–Langevin, BP 156, F-38042, Grenoble C´ edex 9, France
Received 28 September 2003
Published 25 November 2003
Online at stacks.iop.org/JPhysCM/15/8235
Abstract
The relative distribution of rare-earth ions R
3+
(Dy
3+
or Ho
3+
) in the phosphate
glass RAl
0.30
P
3.05
O
9.62
was measured by employing the method of isomorphic
substitution in neutron diffraction and, by taking the role of Al into explicit
account, a self-consistent model of the glass structure was developed. The
glass network is found to be made from corner sharing PO
4
tetrahedra in which
there are, on average, 2.32(9) terminal oxygen atoms, O
T
, at 1.50(1) Å and
1.68(9) bridging oxygen atoms, O
B
, at 1.60(1) Å. The network modifying R
3+
ions bind to an average of 6.7(1) O
T
and are distributed such that 7.9(7) R–
R nearest neighbours reside at 5.62(6) Å. The Al
3+
ion also has a network
modifying role in which it helps to strengthen the glass through the formation of
O
T
–Al–O
T
linkages. The connectivity of the R-centred coordination polyhedra
in (M
2
O
3
)
x
(P
2
O
5
)
1−x
glasses, where M
3+
denotes a network modifying cation
(R
3+
or Al
3+
), is quantified in terms of a parameter f
s
. Methods for reducing
the clustering of rare-earth ions in these materials are then discussed, based
on a reduction of f
s
via the replacement of R
3+
by Al
3+
at fixed total modifier
content or via a change of x to increase the number of O
T
available per network
modifying M
3+
cation.
1. Introduction
The incorporation of rare-earth ions, R
3+
, into phosphate glasses confers these materials with
many interesting opto-electronic and magneto-optical properties which give them application
as, for example, lasers and Faraday rotators [1–7]. It is therefore desirable to understand the
interactions between the rare-earth ions, and their mediation by the matrix material, in order
4
Author to whom any correspondence should be addressed.
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