Stability of Luminescent Trivalent Cerium in Silica Host
Glasses Modified by Boron and Phosphorus
Carmen Canevali,
²
Mariachiara Mattoni,
²
Franca Morazzoni,
²
Roberto Scotti,*
,²
Mariano Casu,
‡
Anna Musinu,
‡
Radenka Krsmanovic,
§
Stefano Polizzi,
§
Adolfo Speghini,
|
and Marco Bettinelli
|
Contribution from the Dipartimento di Scienza dei Materiali, UniVersita ` di Milano-Bicocca,
INSTM, Via Cozzi 53, 20125 Milano, Dipartimento di Scienze Chimiche,
UniVersita ` di Cagliari, INSTM, SS554 BiVio per Sestu, 09042 Monserrato (CA),
Dipartimento di Chimica Fisica, UniVersita ` Ca’ Foscari, INSTM, Via Torino 155/b,
30172 Venezia-Mestre, and Dipartimento di Scientifico e Tecnologico, UniVersita ` di Verona,
INSTM, strada le Grazie 15, 37134 Verona, Italy
Received April 18, 2005; E-mail: Roberto.Scotti@unimib.it
Abstract: Ce-doped borosilicate (BSG), phosphosilicate (PSG), and borophosphosilicate (BPSG) glasses
(B:P:Si molar ratios 8:0:92, 0:8:92, and 8:8:84; Ce:Si molar ratio 1 × 10
-4
to 1 × 10
-2
) were prepared by
the sol-gel method. High-resolution transmission electron microscopy (HRTEM),
31
P,
29
Si, and
11
B magic
angle spinning nuclear magnetic resonance (MAS NMR), electron paramagnetic resonance (EPR), and
UV-vis absorption investigations demonstrated that, in PSG and BPSG, Ce
3+
ions interact with phosphoryl,
[OdPO3/2], metaphosphate, [OdPO2/ 2O]
-
, and pyrophosphate, [OdPO1/2O2]
2-
, groups, linked to a silica
network. This inhibits both CeO2 segregation and oxidation of isolated Ce
3+
ions to Ce
4+
, up to Ce:Si ) 5
× 10
-3
. In BSG, neither trigonal [BO3/2] nor tetrahedral [BO4/2]
-
boron units coordinate cerium; thus, Ce
3+
oxidation occurs even at Ce:Si ) 1 × 10
-4
, as in pure silica glass (SG). The homogeneous rare-earth
dispersion in the host matrix and the stabilization of the Ce
3+
oxidation state enhanced the intensity of the
photoluminescence emission in PSG and BPSG with respect to BSG and SG. The energy of the Ce
3+
emission band in PSG and BPSG matrixes agrees with the phosphate environment of the rare earth.
Introduction
Ce-doped crystalline compounds have received great interest
owing to the rare-earth (RE) luminescence properties.
1,2
In fact,
trivalent cerium has a broad emission band in the UV-vis region
due to the allowed 5d-4f transition. As the energies of the 5d
levels are strongly affected by the crystal field around Ce
3+
,
significant shifts of the emission energy occur in different host
crystalline matrixes.
3
Notable properties of luminescent Ce
3+
ions are the fast 5d-4f decay time and the relatively high light
output, which make Ce
3+
-containing solids promising materials
in several applications such as phosphors for cathodolumines-
cence,
4
scintillators for applications in high-energy physics
5-7
and for the detection of X-rays, γ-rays, or neutrons,
8-12
and
tunable solid-state lasers operating in the near-UV, violet, and
blue regions.
13-18
The luminescence yield is unfavorably affected by Ce
3+
aggregation phenomena. When the RE concentration increases,
the ion distance becomes comparable to the critical distance, at
which the radiative decay probability equals the energy transfer
rate, leading to nonradiative processes
19,20
and, therefore, to
²
Universita ` di Milano-Bicocca.
‡
Universita ` di Cagliari.
§
Universita ` Ca’ Foscari.
|
Universita ` di Verona.
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Published on Web 10/01/2005
10.1021/ja052502o CCC: $30.25 © 2005 American Chemical Society J. AM. CHEM. SOC. 2005, 127, 14681-14691 9 14681