Hollow cathode discharge tube

Abstract: A hollow cathode discharge tube of the type having a thermion emitting anode/cathode (1) together with a hollow cathode (11) and an anode in a bulb (3). The hollow cathode (2) is formed of an element to be analysed on a compound thereof and has therein a hollow space (9) consisting of mutually connected a small diameter one end open portion and a large diameter one end closed portion. The closed end of the hollow cathode (11) is pierced by the anode (6), the thermion emitting anode, or the anode commonly acting as the two anode interposing therebetween an electric insulator. The anode (6) the thermion emitting anode or the anode commonly acting as the two anode is disposed in the hollow space of the hollow cathode.

Description: The present invention relates to a hollow cathode discharge tube for use in atomic absorption analysis and, having improved atomic spectrum characteristics. In atomic spectrum analysis, the contour of atomic spectrum ray of the analytical element is important in improving the sensitivity of the analysis. For the end, a hollow cathode discharge tube having a low operation temperature is usually utilized in glow discharge region. The hollow cathode discharge tube comprises, as shown in Figs. 5 (a) and 5(b), a stem 13 having thereon a hollow cathode 11 and an anode 12 arranged in front of the cathode 11 and on the optical axis thereof, with the stem 13 being inserted into a bulb 3 and air-tightly welded together. The detailed construction of the cathode 11 and the anode 12 is shown in Fig.5(b). The cathode 11 is usually formed of a material same to the analytical element, but other material may be mixed in view of machinability or the strength of the atomic spectrum ray. The hollow cathode 11 has an opening 14 arranged on the optical axis and, is connected to a hollow cathode conductor 15 and is retained thereby. The anode 12 is electrically separated from the hollow cathode 11 and from the hollow cathode conductor 15 through an insulating porcelain 16 or an insulator 17 such as mica and the like and, is retained by anode lead-in wires 18 in front of and opposing the hollow cathode 11. Further, there is formed an opening 19 along the optical axis so as to pass through the atomic spectrum ray generated by the electric discharge. The hollow cathode discharge tube being constituted as described above is processed under a predetermined treatment and, thereafter, gas such as neon or argon is charged under the pressure of several hundred Pa. A hollow cathode discharge tube corresponding closely to that discussed above with reference to Figs. 5(a) and 5(b) has been disclosed in, for example, the Journal of the Illuminating Engineering Institute of Japan Vol. 58, No. 4 (1974) pages 47 to 51, and the supplement to the Journal of Japanese Chemistry, Serial No. 100, pages 11 to 38, and also sold by Koto Luminous Corp under reference KH-1002 to KH-1117. Hollow cathode discharge tubes generally similar to those discussed above are also disclosed in US-A-4833366, JP-A-57-107540 and JP-A-57-19941. The hollow cathode discharge tube for use in atomic absorption analysis requires the atomic spectrum ray of the analytical element itself and, thus, utilizes the phenomenon that when atomic condition of the analytical element exists in the discharge space according to the electric discharge the atomic spectrum ray is generated by giving and receiving the electric energy. For generating the atomic condition of the analytical element in the discharge space, electric ion is collided against the surface of the cathode by electric discharge phenomenon so as to scatter the atom of the cathode element, which phenomenon is called spattering. It is also possible to obtain the atomic element due to the evaporation from the inside of the cathode by applying Joule heat. Fig. 6(a) shows the electric relationship of the hollow cathode discharge tube and, as shown in Fig. 6(b), the electric field in the discharge space of the discharge tube is in equal electric field condition. While, according to the spattering condition on the surface of the cathode the atom scatters in the opposite direction to the injection of the ion due to the electric discharge, as shown in Fig.2(d) and the amount thereof varies according to the element, but depends on the angle of injection of the ion such that the maximum distribution appears in the range of 0 to 60 degrees of the injection angle. When the injection angle is 90 degrees, the atom does not scatter and charges into the cathode element, thereby the energy of the atom is converted into the heat. The evaporation caused of Joule heat generated by the charging of the ion is, as publicly known, distributed in the cosine direction on the surface of the cathode. The condition of scattering atom of the cathode element during the hollow cathode discharge takes the condition shown in Fig.6(c) and, the density is large at the bottom portion of the opening 14. Accordingly, the spectrum ray generates at the bottom portion of the opening 14 and moves toward the anode 12. A part of the spectrum ray affords the energy to the scattered atom element, thereby the intensity of the spectrum ray decreases gradually and, it is deemed that the atomic absorption analysis is carried out within the hollow cathode discharge tube. This phenomenon is called as self absorption. When the spectrum ray is in above described condition, the intensity decreases and the contour of the spectrum ray is damaged, thus, the sensitivity of the absorption analysis is decreased. The contour of the atomic spectrum ray affecting the sensitivity of the absorption analysis as described above is not a simple geometrical line and has an intensity distribution along a range of frequency. The above described intensity distribution is called as broadening of the atomic spectrum and, the cause of which are as follows. In particular, which are (1) natural or inherent broadening due to the fact that the life of the excited condition is limited; (2) Doppler broadening due to the motion of atoms and molecules constituting the gas; (3) Lorentz broadening due to the collision of atoms and molecules constituting the co-existing gas; (4) Holzmark broadening due to the collision of atoms and molecules constituting the gas with atoms and molecules of the same gas; and (5) Stark broadening due to the collision of electron or ion. The contour of the atomic spectrum is affected by these factors and, the contour determines the absorption factor as the characteristics of the spectrum ray in the atomic absorption analysis. Usually, the contour of the spectrum ray is determined by two or three factors among above mentioned five factors. Usually, the center of of the contour of the spectrum ray coincides with the center of the absorption frequency and, in this meaning, it is symmetrical. But when the contour is determined only by Doppler broadening, the center of of the contour of the spectrum ray does not coincide with the center of the absorption frequency and the contour of the spectrum ray is not symmetrical. The contour has a complex configuration and the value of the coefficient of absorption becomes the largest. In this case, it is possible to obtain the coefficient of absorption from the equation given by Voigt, thus, the contour is called as Voigt's contour. Therefore, for reducing the Doppler width, in the atomic absorption analysis, the hollow cathode discharge tube is utilized which operates with a cold cathode with the temperature of which being low. However, the strength of the spectrum ray generating from the hollow cathode discharge tube will also decreases and the contour is broadened. The spectrum ray generates from the transition between the energy levels due to the transfer of the energy between the electron and the element atom in the discharge space. While, the atomic spectrum ray used in the hollow cathode discharge tube is originated at a portion adjacent to the wall surface of cathode and, which is usually called as glow discharge. Since the density of the ion is thick in such portion, and secondary electrons are generated only by the ion impacting against the surface of the cathode, the number of scattering atom of the element is larger than the number of the ion having the energy, thereby the self absorption increases. The energy of the spectrum ray generating from the atom of the exciting element is decreased by the absorption when the ray passes through the element atom in the inexecuted state and, as the result, the intensity of the spectrum ray radiated from the discharge space is decreased, the contour of the spectrum ray is broadened, and the sensitivity of the absorption analysis is decreased. Such phenomenon will fully be understood from the following detailed description in conjunction with the comparison data relative to the embodiment of the present invention, which will be discussed later. As described above, when the atomic spectrum ray radiated from the hollow cathode discharge tube passes through the element atom in the base bottom condition, the intensity of the spectrum ray is decreased, the contour of the spectrum ray is broadened, and the characteristics such as the sensitivity of the absorption analysis will also be deteriorated. The present invention seeks to reduce or eliminate the self-absorption phenomenon in the hollow cathode discharge tube, and to obtain a high brightness hollow cathode discharge tube having the increased intensity of the atomic spectrum ray. According to the present invention, there is provided discharge tube including a cathode formed of an element to be analysed or any compound of the element to be analysed, a first anode, and a bulb containing the first anode and cathode, the cathode defining a blind hole terminated by an end wall; wherein: an inner portion of the hole is of larger cross-sectional area than an outer portion of the hole; the discharge tube further comprises a thermion emitting anode; and the first anode and the thermion emitting anode extend through the end wall into the hole. According to a preferred embodiment, another auxiliary cathode is provided in front of the open end of the hollow cathode for emitting thermion. The rod like anode and the thermion emitting auxiliary cathode are respectively arranged co-axially with the axis of the hollow cathode through insulating material, thus, it is possible to convert forcively the element atom of the base or bottom condition which causes the self absorption phenomenon into the element atom of the excited condition by the distinct auxiliary electrode effecting the thermion emission. The discharging current for the electric discharge of the auxiliary electrode is controlled such that the location of the anode is determined for effectively increasing and utilizing the discharge electric current of the auxiliary electrode. The location of the anode is determined such that the amount of scattering element atom of the hollow cathode is effectively increased and utilized and, further, the distribution the scattering element atom is determined such that the collision phenomenon of the atom in inequal electric field is performed suitably. The invention will now be explained in detail with reference to attached drawings, wherein: Fig.1(a) is a schematic partially broken side view of a hollow cathode discharge tube according to an embodiment of the present invention; Fig.1(b) is an enlarged sectional view of hollow cathode portion of the hollow cathode discharge tube of Fig.1(a); Fig.2(a) is a view showing the electric connection of the hollow cathode discharge tube of Fig.1(a); Fig.2(b) is a view showing inequal electric field in the hollow cathode discharge tube of Fig.1(a); Fig. 2(c) is an experimental equation relative to the electric field between a rod electrode and a hollow electrode; Fig. 2 (d) is a view showing scattering direction of element atom; Fig. 2 (e) is a view showing the distribution of the scattering element atom; Fig. 3(a) is a diagram of the intensity of the spectrum ray in the embodiment of Fig. 1(a); Fig.3(b) is a diagram showing the relationship between the electric current in the discharge tube and the thermion emitting electric current when the intensity of the spectrum ray is at the maximum; Fig.4 is a characteristic diagram showing the effect of absorption of atomic spectrum ray in the hollow cathode discharge tube; Fig. 5(a) is a side view of a prior art hollow cathode discharge tube. Fig. 5(b) is a view showing a section of electrode in the prior art hollow cathode discharge tube of Fig. 5(A); Fig. 6(a) shows the electric connection of the prior art hollow cathode discharge tube of Fig. 5(a); Fig. 6(b) is a view showing inequal electric field, and Fig.6(c) is a view showing the distribution of scattering element atom in the prior art hollow cathode discharge tube of Fig.5(a). A preferred embodiment of the present invention will now be explained with reference to the drawings, in which, as shown in Fig. 1(a), a bulb 3 formed of Silica glass enclosed therein Argon gas or Neon gas under the pressure of several hundred Pa and having an anode/cathode portion 1, a thermion emitting auxiliary cathode 2 opposing the anode/cathode portion 1, and a socket 5 retaining the bulb 3 and remedying the optical axis of the spectrum ray generated from the inside of the bulb 3. Shown at numeral 4 in the drawing are insulating tubes covering respective lead-in wires. The anode/cathode portion 1 is formed of a hollow cathode 11 defining therein a space consisting of two generally cylindrical and mutually connected spaces of different diameters, a rod like anode 6 and a thermion emitting auxiliary anode 8 encircling the rod like anode 6 interposing therebetween an insulator 7, with the anode 6 and the auxiliary anode 8 being arranged co-axial with the hollow cathode 11. The hollow cathode 11 is formed of a front hollow cathode 9 having a small diameter space and a rear hollow cathode 10 having a large diameter space and being tightly connected to the front hollow cathode 9. The front end of the front hollow cathode 9 is formed to have an opening which opposes the thermion emitting auxiliary cathode (booster) 2 being disposed in front of the hollow cathode 11 and on the optical axis thereof. The rear end of the rear hollow cathode 10 is closed and, through which the rod like anode 6 and the thermion emitting auxiliary anode 8 pass air-tightly interposing therebetween the insulating tube 7. There arises the thermion discharge phenomenon between the auxiliary anode 8 and the thermion emitting auxiliary cathode 2 which is disposed outside of the bundle of atomic spectrum ray discharging within the hollow space of the hollow cathode 11. The operational function of the hollow cathode discharge tube according to the present invention in generating the atomic spectrum ray will now be explained. As shown in the electrical connection diagram of Fig.2(a), one end of the hollow cathode 11, which is formed of the front hollow cathode 9 having a small diameter space and being connected to the rear hollow cathode 10 having a large diameter space, is connected through a resistance to a minus potential of an electric source. And the rod like anode 6 passing through the other end of the hollow cathode 11 is connected to the plus potential of the electric source. Thereby, the electric field in the electric discharge space in the hollow cathode 11 is an inequal electric field as shown in solid lines in Fig. 2(b) which mainly is observed in the front hollow cathode 9. When calculated by utilizing an experimental equation of the electric field between a rod like electrode and a hollow electrode shown in Fig.2(c), it will be understood that the electric field in the rear hollow electrode is substantially small. The surface of the front hollow cathode 9 being formed of element atom is attacked by ion due to the glow discharge, and the amount of scattering element atom is determined by the spattering rate of the elment atom and the angle of incidence of the ion. The directions of the scattering element atom are shown in Fig.2(d). Accordingly, as shown in Fig.2(e), the density of the scattering element atom in the discharge space of the hollow cathode 11 is thick in the tip end portion of the cathode 11, and thin in the hollow space of the front cathode 9 in which space the density of the electric field is thick. Accordingly, the density of the electric field is thin in the glow discharge portion of the hollow cathode 11, or in the tip end portion of the hollow cathode 11 and, the effect of the exciting phenomenon is small. In other words, the amount of unexcited scattering atom is large in the tip end portion of the hollow cathode. Further, in the glow discharge portion of the hollow cathode 11, the amount of the secondary atom emitted from the cathode surface of the hollow cathode 11 is smaller than the case of thermion discharge utilizing the thermion scattering cathode. Thus, according to the invention, the inexcited scattering atom of the electrode element are generated on the path of electric discharge which is co-axial with the optical axis of the hollow electrode 11, so that the thermion discharge is performed, as shown by broken lines in Fig. 2(b), in the inequal electric field being shown by solid lines in the drawing, therby converting the inexcited scattering atom of the electrode element into excited condition. Further, Fig.3(a) shows the intensity of the spectrum ray according to the present invention which utilizes Arsenic as the material of the electrode as compared with that of usual hollow cathode discharge tube. When the intensity of the electric current is 10 mA, the intensity of the spectrum ray according to the invention is increased by about 10.7 times of that of prior art. The electric current for discharging thermion is, as shown in Fig.3(b) showing the relationship between the electric current of the hollow cathode discharge tube and the thermion discharging electric current when the intensity of the spectrum ray, at the maximum 53 mA, and which electric current is required in converting inexcited element atom corresponding the amount of self-absorption into the excited element atom. Fig.4 shows the relationship between the effective intensity (Iv) of spectrum ray and the tube electric current and showing the rate of absorption of the atomic spectrum ray according to prior art. From the drawing, it will be understood that the intensity of the spectrum ray decreases steeply when the tube electric current is 5 mA, which shows that the absorption occurs when the atomic spectrum ray passes between the inexcited element atom in the discharge space of the hollow electrode. Two characteristics, namely, the intensity of the spectrum ray and the sensitiveness of the analysis effected by the absorption were examined with respect to various elements, and the result is that the intensity of the spectrum ray increases with respect to all of the elements and the sensitiveness of the analysis is remarkably improved with respect to elements having low melting point and high vapor pressure, but, in case of the elements having high melting point, the sensitiveness is low and is maintained at a nearly constant value even though the tube electric current is increased. In the above described embodiment, the space formed in the hollow cathode is a space formed of two generally cylindrical spaces having different inner diameters and being connected with each other, but these spaces should not necessarily be cylindrical, and it is required that the diametrical size of the front space should be smaller than that of the rear space. As described heretofore, the hollow cathode discharge tube according to the invention is of the type having a thermion emitting anode/cathode together with an anode and a hollow cathode in a bulb and, the hollow cathode is formed of an analytical element or the complex material thereof and has therein a hollow space consisting of mutually connected a small diameter one end open portion and a large diameter one end closed portion, with the anode, the thermion emitting anode or an anode commonly acting as the anode and the thermion emitting anode being disposed in the hollow space of the hollow cathode and piercing through the closed end of the hollow space of the hollow cathode interposing therebetween electric insulating material; thereby, it is possible to achieve a hollow cathode discharge tube excluding the self-absorption phenomenon in the hollow cathode discharge tube, narrowing the contour of the spectrum ray, increasing the intensity of the atomic spectrum ray and obtaining higher brightness as compared with prior art hollow cathode discharge tube. Further, according to a preferred embodiment, the hollow cathode discharge tube comprises a hollow cathode defining therein a hollow space consisting of mutually connected a small diameter one end open portion and a large diameter one end closed portion, a rod like anode piercing through the closed end of the hollow space and being encircled co-axially by such as a thermion emitting anode interposing therebetween electricaly insulating material, and a thermion emitting cathode provided in front of the open end of the hollow cathode, whereby it is possible to convert forcively the element atom of the base or bottom condition which causes the self absorption phenomenon into the element atom of the excited condition by the distinct auxiliary electrode effecting the thermion emission. Further, the discharging current for the electric discharge of the auxiliary electrode is controlled such that the location of the anode is determined for effectively increasing and utilizing the discharge electric current of the auxiliary electrode. And it is possible to effectively control the scattering element atom in the hollow cathode. In the above description, the term "analytical element" refers to the element to be analysed and "complex material thereof" refers to any compound of of such an element.

Claims: A discharge tube including a cathode (11) formed of an element to be analysed or any compound of the element to be analysed, a first anode (6), and a bulb (3) containing the first anode and cathode, the cathode (11) defining a blind hole terminated by an end wall; characterised in that: an inner portion of the hole is of larger cross-sectional area than an outer portion of the hole; the discharge tube further comprises a thermion emitting anode (8); and the first anode (6) and the thermion emitting anode (8) extend through the end wall into the hole. A discharge tube according to claim 1 in which the first anode and the thermion emitting anode are respective portions of an anode unit in which the first anode and the thermion emitting anode are spaced apart by an electrical insulator (7). A discharge tube according to claim 2 in which the anode unit is coaxial with an axis of the cathode. A discharge tube according to claim 1, claim 2 or claim 3 further comprising an auxiliary cathode (2) for emitting thermions, said auxiliary cathode being disposed in front of an open end of said hole. A discharge tube according to claim 1 in which the first anode and the thermion emitting anode are coaxial with an axis of the cathode, and either one of the first anode and the thermion emitting anode has an annular or ring-shaped form.

Inventors: ABE KAZUYA, ISHIZAKI HIROSHI, KAMEYA TAKAYUKI, OKAGAKI HIROSHI, ABE, KAZUYA, ISHIZAKI, HIROSHI, KAMEYA, TAKAYUKI, OKAGAKI, HIROSHI
Applicants: KOTO ELECTRIC CO LTD, KOTO ELECTRIC CO. LTD.
Application year: 1993
Main classification: G01J3
IPC codes: G01J3, G01N21, H01J17, H01J61