QUANTITATIVE DETERMINATION OF SELENIUM

Abstract: Gaseous selenium is detected and determined quanti­ tavely by measuring absorption at the wavelength of 335 nm or at two or more wavelengths selected from 324 nm, 326 nm, 328 nm, 330 nm, 332.5 nm, 335 nm, 337.5 nm, 340 nm, 342 nm, 344.5 nm, 347 nm, 350 nm, 352.5 nm, 355 nm, 357.3 nm and 360 nm.

Description: This invention relates to a method of detecting and determining selenium quantitatively and a monitor therefor, and more particularly, it is concerned with a method of detecting and determining quantitatively gaseous selenium at a lower temperature than has been practiced hitherto by atomic absorption spectroscopic analysis. Sensitive detection and quantitative determination of selenium has lately been required by reason of the development of various compounds containing selenium for various purposes, for example, in the production of semiconductors, alloys, ceramics and glass. Atomic absorption spectroscopic analysis has hitherto been performed by atomizing selenium at high temperatures, e.g. 2000 o C or higher and then detecting the atomic absorption spectrum characteristic of selenium. see e.g. Analytical Chemistry, Vol. 56. no.4, April 1984 pages 829-831, Easton, Pennsylvania U.S.A., C.H. Chung et al "Graphite Furnace Atomic Absorption Spectrometry with Graphite Cloth Ribbon for Selenium Determination." The atomic absorption spectrum of selenium has a sharp peak at a wavelength of 196.03 nm, as shown in Figure 5 (quoted from Catalogue of Hamamatsu Photonics KK). The general structure of an apparatus for the atomic absorption spectroscopic analysis utilizing this peak is shown in Figure 6: a light from a source 1 is caused to pass through a chamber 2 in which a sample is atomized, the light then traversing a photoselective means 3 such as monochromator and then entering photometric means 4-6 comprising a detector 4, an amplifier 5 and a metering stage 6. In the chamber 2 a flame is used to provide an atomizing temperature of 2000 o C or higher. However such a method is not suitable for detecting selenium at a temperature below the atomizing temperature. That is, for a gaseous Se 2n at a temperature lower than the atomizing temperature, there is no convenient method of detection and quantitative analysis. It is an object of the present invention to provide a new method of detection and quantitative determination of selenium. The present invention is defined in claims 1,2 and 4 The temperature lower than the atomizing temperature of selenium may be in the range 220 to 1000 o C. By means of the invention, a determination of selenium down to 0.01 ppm can be made. Moreover, an in situ determination may be made. The accompanying drawings illustrate the invention in greater detail. Figure 1 is an absorption spectrum of gaseous selenium at 450 o C, in which 1 to 16 show peaks in the spectrum; Figure 2 is a schematic view to illustrate a method of detecting and determining selenium quantitatively according to the present invention; Figure 3 is a graph showing the relationship between the quantity of selenium and log 1 / T% ; Figure 4 is a schematic view of one embodiment of an apparatus for detecting and determining selenium quantitatively according to the present invention and a graph showing a temperature distribution across the apparatus of Figure 4; Figure 5 is an atomic absorption spectrum of selenium; Figure 6 is a schematic view of apparatus for the atomic absorption spectroscopic analysis. Selenium is in gaseous state and is considered to exist as Se₂, Se₄, Se₆ and the like at a temperature of lower than the atomizing temperature, particularly 220 to 1000 o C, more particularly 220 to 695 o C, but this is not fully established (Cf. 0. Kubaschewski "Metallurgical Thermochemistry" Pergamonpress (1967)). The inventor has found a total of sixteen absorption lines 1 to 16, as shown in Figure 1, relating to this gaseous selenium. In Figure 1, the ordinate shows the absorbance (voluntary units) and the abscissa shows the wavelength (nm). The wavelengths of the peaks numbered 1 to 16 are as follows: 1 ... 324 nm, 2 ... 326 nm, 3 ... 328 nm, 4 ... 330 nm, 5 ... 332.5 nm, 6 ... 335 nm, 7 ... 337.5 nm, 8 ... 340 nm, 9 ... 342 nm, 10 ... 344.5 nm. 11 ... 347 nm, 12 ... 350 nm 13 ... 352.5 nm, 14 ... 355 nm, 15 ... 357.5 nm 16 ... 360 nm In the absorption spectrum of Figure 1, the sixth peak at a wavelength of 335 nm is highest. Accordingly the present invention provides for the detection of selenium by selecting the peak at a wavelength of 335 nm or two or more peaks from the above-described peaks 1 to 16 and simultaneously measuring. In principle, the method of detecting and determining selenium quantitatively according to the present invention can be carried out by an apparatus exemplified in Figure 2. Referring to Figure 2, emitting stage 1 emits a light corresponding to the wavelength of one of the above-described peaks 1 to 16 of gaseous selenium. For example, the emitting stage 1 consists of a light source comprising a hollow-cathode lamp provided with filters each having a centre frequency corresponding to each of the spectral lines 1 to 16. Sample chamber 2 is a furnace or cell provided with a heating means, which has a structure capable of retaining selenium gas, a window 3 permitting the passage of incident light from emitting stage 1 and another window 4 permitting the passage of transmitted light, after absorption thereof by the selenium gas, to a subsequent photo-receiving stage 5 comprising an ordinary monochromator, detector, amplifier and meter. The principle of the method of detecting and determining selenium quantitatively according to the present invention lies in that the peak absorption of wavelengths corresponding to the lines 1 to 16 shown in Figure 1 can be obtained in proportion to the concentration of gaseous selenium. When the intensity of an incident light upon a sample chamber is represented by I o , the intensity of the transmitted light after absorption by gaseous selenium is represented by I, the absorption of the light by the gaseous selenium in the sample chamber is represented by T (%), the absorbance is D and the concentration of the gaseous selenium is C, there are the following relationships: T (%) = I/I o x 100 D = kC (where k is a constant of proportionality) On the other hand, it has been found that there is the relationship as shown in Figure 3 between the weight of selenium and absorbance D, i.e. Referring to Figure 3 , Point A represents the saturation point of selenium gas at a temperature t, which is defined by the vapour pressure of selenium as shown in the following formula: wherein t is an absolute temperature. The invention may be performed with the apparatus shown in Figure 4. A sample chamber 2 provided with heater 6 received a sample containing selenium. The sample is heated to and maintained at a temperature of 450 o C to obtain the absorption spectrum shown in Figure 1. When various samples are subjected to measurement or analysis selecting two or more peaks from the peaks 1 to 16, quantitative determination of selenium of the order of 0.01 ppm is possible. For the further purposes of controlling the quantity of selenium supplied in a process or controlling the pressure of selenium, the method and monitor apparatus of the present invention can be usefully applied in various processes and apparatus for the production of semiconductors or semiconductor devices using selenium or to waste disposal apparatus. Examples are apparatus for the epitaxial growth of compound semiconductors such as ZnSe, CdSe and the like (CVD furnaces, LPE furnaces, etc), high pressure HB furnaces, annealing furnaces, selenium pressure annealing furnaces, MBE apparatus, MOCVD apparatus and furnaces for melting alloys, ceramics and glasses containing selenium.

Claims: A method of quantitative determination of selenium, comprising illuminating a sample containing gaseous selenium with radiation at a wavelength of 335 nm, said sample being at a temperature lower than the atomizing temperature of selenium and measuring the absorption of the said component at said wavelength by the gaseous selenium in the sample. A method of quantitative determination of selenium comprising illuminating a sample containing gaseous selenium with radiation at at least two wavelengths selected from 324 nm, 326 nm, 328 nm, 330 nm, 332.5 nm, 335 nm, 337.5 nm, 340 nm. 342 nm, 344.5 nm, 347 nm, 350 nm, 352.5 nm, 355 nm, 357.5 nm, and 360 nm, said sample being at a temperature lower than the atomizing temperature of selenium, and measuring the absorption at the selected wavelengths by the gaseous selenium in the sample. A method according to claim 1 or claim 2 wherein the temperature of the selenium is between 220 and 1000 o C. An apparatus arranged to quantitatively determine gaseous selenium in a sample, comprising a chamber provided window portions and a heating means to heat the sample, only to temperatures lower than the atomising temperature of selenium, a source of light and means for receiving light from the source by way of the chamber, the means for receiving including means for measuring the absorbtion of light by gaseous selenium in the sample, wherein, the source provides a spectral line at a wavelength of 335 nm or spectral lines at two or more wavelengths selected from 324 nm, 326 nm, 328 nm, 330 nm, 332.5 nm, 335 nm, 337.5 nm, 340 nm, 342 nm, 344.5 nm, 347 nm, 350 nm, 352.5 nm, 355 nm, 357.5 nm and 360 nm.

Inventors: OOSAKA, HAJIME C/O OSAKA WORKS
Applicants: SUMITOMO ELECTRIC INDUSTRIES LIMITED
Application year: 1986
Main classification: G01N21
IPC codes: G01N21