# Patent

## Title
Process for obtaining luminescent glass layers

## Abstract

A method of producing carbonyl fluoride by multiphoton decomposition of carbon dioxide-sulphur hexafluoride mixtures comprising irradiating gaseous carbon dioxide-sulphur hexafluoride mixtures in a reaction chamber at a pressure in the 10-50 Torr range with a laser beam at a frequency of about 944 wavenumbers and passing the material from the reaction chamber after irradiation through a chemical processing stage to obtain a carbonyl fluoride product.

## Background
This invention relates to the formation of carbonyl fluoride and more particularly to a method of production of this material by laser enhanced fluorination of carbon dioxide by sulfur hexafluoride.

The separation of isotopes using photochemical techniques especially laser irradiation is well known and fairly widely used. The following are representative patents in this field:

Formation of carbonyl fluoride (CF.sub.2 O) from carbon monoxide (CO) or carbon dioxide (CO.sub.2) requires extreme conditions and is achieved with relatively low yields. The high temperature reaction of sulfur hexafluoride (SF.sub.6) with CO.sub.2 gives only 10% CF.sub.2 O with CF.sub.4 being the main carbon bearing product. See W. R. Hasek, W. C. Smith and V. A. Engelhardt, J. Amer. Chem. Soc., 1960, 82, 543. Better yields (about 45%) of CF.sub.2 O are obtained during the electrolysis of carbon monoxide in liquid hydrofluoric acid (HF). See T. Nagase, H. Baba and T. Abe, Japanese Pat. No. 7026611, 1970. Other products in this method are CF.sub.4 (26%), CF.sub.3 OF (5%) and CO.sub.2 (23%). Direct fluorination of CO.sub.2 gives CF.sub.2 (OF).sub.2 as the dominant product. See R. L. Cauble and G. H. Cady, J.Amer. Chem. Soc. 1967, 89, 1962 and F. A. Hokoret and J. M. Shreeve, J. Amer. Chem. Soc., 1967, 89, 1809.

It is an object of the present invention to provide a process for converting carbon dioxide to carbonyl fluoride giving high yields but with no detectable carbon bearing side products.

This and other objects of the invention are achieved by a method of producing carbonyl fluoride by multiphoton decomposition of carbon dioxide-sulphur hexafluoride mixtures comprising irradiating gaseous carbon dioxide-sulphur hexafluoride mixtures in a reaction chamber at a pressure in the 10-50 Torr range with a laser beam at a frequency of about 944 wavenumbers causing the following reaction to take place: ##STR1## and passing the material from the reaction chamber after irradiation through a chemical processing stage to obtain a carbonyl fluoride product.

In drawings which illustrate an embodiment of the invention,

FIG. 1 is a schematic drawing of the irradiation apparatus,

FIG. 2 is a graph showing infrared spectral traces of a CO.sub.2, SF.sub.6 mixture before irradiation, and

FIG. 3 is a graph showing infrared spectral traces of the mixture after small fraction of the CO.sub.2 has been reacted.

Referring to FIG. 1, laser 10, preferably a CO.sub.2 -laser, irradiates a CO.sub.2 -SF.sub.6 mixture in reaction chamber 11 at a pressure in the 10-50 Torr range. The laser beam is preferably focussed at the centre of the reaction chamber by means of a short focal length lens 12. The P (20) line of the 10.6 .mu.m band (approx. 944 wavenumbers) of the laser is used and it is very strongly, absorbed by the SF.sub.6 component of the mixture. The process involves plasma breakdown or multiphoton decomposition in the mixture with the overall equation being: ##STR2##

After laser irradiation, the mixture is passed to separation stage 13 where CF.sub.2 O is separated from the SO.sub.2 F.sub.2. The only other product obtained is SiF.sub.4 which is presumed to be formed by interaction with the glass walls of the cell (reaction chamber) used.

In an experimental test, the mixture was contained in a 10 cm long. 2.4 cm diameter IR cell with a TEA CO.sub.2 -laser beam focussed at the centre of the cell by a 7.5 cm focal length germanium lens. Laser pulses of 4-6 joules per pulse were used. CO.sub.2 at a pressure of 3.8 Torr and SF.sub.6 at a pressure of 4 Torr were introduced into the IR cell and after four freeze-pump-thaw cycles, the gas mixture was irradiated. After 10 pulses (all giving rise to plasma breakdown) 93.5% of the SF.sub.6 was found to be decomposed and only traces of CO.sub.2 were still present. Similar behaviour was noted for higher pressure mixtures although as the pressure was increased more pulses were found to be necessary, for example at 10 Torr SF.sub.6, 10 Torr CO.sub.2, 200 pulses were found to be required to decompose all the SF.sub.6. Prolonged irradiation after the SF.sub.6 is decomposed leads to a steady, slow decline in the CF.sub.2 O content with an apparent regrowth in the CO.sub.2. The CO.sub.2 is quantitatively transformed to CF.sub.2 O but to achieve this, it is necessary to have excess (>2:1)SF.sub.6 to obviate the laser induced back reaction.

The effectiveness and integrity of the method is shown by FIGS. 2 and 3. FIG. 3 shows the spectrum before irradiation where CO.sub.2 (90% C-13) and SF.sub.6 are mixed.

FIG. 3 shows the composition of the mixture after a small fraction of the CO.sub.2 has been reacted. It can be seen that the isotopic composition of the CF.sub.2 O product exactly matches the initial composition of the CO.sub.2 substrate.

## Claims

1. A method of producing carbonyl fluoride by multiphoton decomposition of carbon dioxide-sulphur hexafluoride mixtures comprising: reaction chamber at a pressure in the 10-50 Torr range with a laser beam at a frequency of about 944 wavenumbers causing the following reaction to take place: ##STR3## and (b) passing the material from the reaction chamber after irradiation through a chemical processing stage to obtain a carbonyl fluoride product.

2. A method as in claim 1 wherein the irradiation is carried out by a CO.sub.2 laser focussed on the central region of the reaction chamber.