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Influence of Fluorine and Nitrogen on the IR Transmission of Glasses<br />

C. M. Crowley a and S. Hampshire a ,<br />

a Department of Materials Science and Technology, University of Limerick, Ireland<br />

b Department of Chemical and Environmental Sciences, University of Limerick, Ireland<br />

Clare.Crowley@ul.ie<br />

Abstract<br />

The influence of glass chemistry and firing conditions<br />

on the thermomechanical properties and IR<br />

transmission of aluminosilicate, sialon, fluorinated<br />

aluminosilicate and fluorinated sialon glasses has been<br />

examined. Improvements in the thermomechanical<br />

properties were achieved with increasing nitrogen<br />

content while a concomitant improvement in IR<br />

transmission was achieved under specific firing<br />

conditions.<br />

Introduction<br />

Glass is commonly used as a medium to transmit<br />

infrared (IR) radiation in applications. Glasses,<br />

however, normally contain water impurities in their<br />

atomic structure which are efficient absorbers of IR<br />

radiation leading to energy loss and heat generation in<br />

the glass. Commercial producers of IR glasses<br />

overcome this by employing expensive processes and<br />

ultra pure materials. The incorporation of nitrogen into<br />

rare-earth aluminosilicate glasses has previously been<br />

shown to enhance infrared transmission due to the<br />

reduction in the formation of silanols in the glass<br />

network [1]. However, the production cost of rare-earth<br />

sialon glasses, fired under reducing conditions, is not<br />

commercially viable. In this study the feasibility of<br />

using nitrogen-based glasses to reduce the occurrence<br />

of ‘water’ impurities in alkali-earth sialon glasses has<br />

been examined.<br />

Materials and Methods<br />

Glass compositions<br />

Glass compositions (Figure 1) were prepared using high<br />

purity (99.9 %) reagents which were melted for 1 hr at<br />

1500 - 1600°C under nitrogen at a pressure of 0.1 MPa.<br />

The glass melts were annealed in a muffle furnace at Tg<br />

- 30°C for 1 hr.<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

6Ca<br />

0.0 1.0<br />

2+<br />

1.0 0.0<br />

0.0 0.2 0.4 0.6 0.8 1.0<br />

4Al 3+<br />

3Si 4+<br />

Figure 1: Vertical triangular plane of the Janecke<br />

triangular prism for Ca-sialon glasses examined<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

173<br />

Materials characterisation<br />

Powder X-ray diffraction (XRD) was performed<br />

between 10 to 70 degrees 2 with a CuKα radiation<br />

source at 35mA, 40kV ( = 1.540566) (Phillips X’Pert<br />

diffractometer) to confirm that the samples were<br />

amorphous. FTIR spectra (Perkin Elmer Spectrum 100)<br />

of the glass slices (thickness = 1.06 ± 0.1 mm; polished<br />

to 1m) were collected between 4000 <strong>–</strong> 450 cm -1<br />

(resolution = 1 cm -1 , number of scans = 50).<br />

Results<br />

Sialons and fluorinated sialons, with different modifier<br />

cations (Mg, Ca, Sr and Ba) have been produced that<br />

show improved thermomechanical properties, compared<br />

with their oxide/oxyfluoride counterparts, and<br />

improved infrared transmission in the 2.5 <strong>–</strong> 5 m range<br />

compared to a boro-aluminosilicate standard (Figure 2).<br />

Transmission (%)<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

3588cm -1<br />

2.8m<br />

10<br />

0<br />

2703 cm<br />

1.5 2 2.5 3 3.5 4 4.5 5 5.5 6<br />

-1<br />

3.7 m<br />

Wavelength (m)<br />

Aluminosilicate standard<br />

Series 6 N5 F1 Al20Ca24<br />

Series 2 N5 F1 Al24Ca20<br />

Figure 2: Comparison of the FTIR transmission of<br />

F1N5 glasses (High purity) and the boro-aluminosilicate<br />

standard (Glass slices 1.06 ± 0.1 mm thickness)<br />

Discussion<br />

For the Ca-oxyfluoronitrides examined there was an<br />

increased incidence of transparent glasses produced<br />

when the Al content = 20 eq.%. Transparency may<br />

therefore be related to the number of bridging oxygens<br />

per tetrahedra (BO/T) as no transparent glasses were<br />

obtained when the BO/T > 3.33 for the base oxide. This<br />

may be related to a shift in Si from Q 3 to Q 4 following<br />

the addition of nitrogen and is currently being examined<br />

by Raman spectroscopy.<br />

References<br />

[1] E. Dolekcekic, M.J. Pomeroy, S. Hampshire (2007)<br />

Structural characterisation of Er<strong>–</strong>Si<strong>–</strong>Al<strong>–</strong>O<strong>–</strong>N glasses by<br />

Raman spectroscopy. J. European Ceramic Society27(2-3):<br />

893-898.

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