1. Field of the Invention
The present invention relates to a micro-focus X-ray generation apparatus and an X-ray imaging apparatus including the micro-focus X-ray generation apparatus, which are used for nondestructive radiation imaging in medical and industrial fields.
2. Description of the Related Art
There are transmission type X-ray tubes that generate X-rays from a surface of a target opposite to an electron irradiation surface of the target by irradiating the electron irradiation surface with electrons emitted from an electron source.
Japanese Patent Application Laid-Open No. 09-171788 describes a transmission type micro-focus X-ray tube including an anode member which faces an electron source. The anode member includes a conical channel in which an inlet opening is larger than an outlet opening. Japanese Patent Application Laid-Open No. 07-057668 describes an X-ray target in which an X-ray generator is integrally formed with a housing made of a material which is the same as that of the X-ray generator.
To date, the combination of the material of a target and the material of a cone-shaped channel of micro-focus X-ray generation apparatuses has not been appropriately selected. As a result, efficiency in the use of electrons reflected by a cone-shaped channel has not been sufficiently high.
The present invention provides a transmission type micro-focus X-ray generation apparatus in which the efficiency in use of reflected electrons is increased by appropriately selecting the combination of the material of a target and the material of an electron reflector.
According to an aspect of the present invention, a transmission type micro-focus X-ray generation apparatus includes an electron reflector, an electron passage surrounded by the electron reflector, an electron source, and a target. X-rays are generated by irradiating the target with electrons emitted from the electron source and that have passed through the electron passage. The electron passage has a conical shape having a cross-sectional area that increases from an outlet on the target side toward an inlet on the electron source side. A material of the target is molybdenum, tantalum, or tungsten. The atomic number of a material of the electron reflector is greater than or equal to the atomic number of the material of the target.
With the present invention, the efficiency in generating X-rays with the target can be increased, and thereby a micro-focus X-ray generation apparatus having a high X-ray output power can be provided.
Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.
Hereinafter, an embodiment of the present invention will be described with reference to the drawings. In the present embodiment, X-rays are used as radiation. Alternatively, neutron radiation or gamma rays may be used.
An electron reflector 13 includes a tapered electron passage 15 extending from an electron inlet port to the target 11. The electron reflector 13 is disposed on a side (first side) of the target portion 16 on which electrons are incident (on the inner side of the target portion 16). The electron reflector 13 is made of a material having an atomic number that is greater than or equal to the atomic number of the material of the target 11. Because the electron reflectivity of a material is positively correlated with the atomic number of the material, when such a combination of materials is used, the electron reflectivity of the electron reflector 13 is greater than or equal to that of the target 11. Tungsten or gold is used as the material of the electron reflector 13, when the material of the target 11 is tungsten. Tantalum, tungsten, or gold is used as the material of the electron reflector 13, when the material of the target 11 is tantalum. Molybdenum, silver, gold, tantalum, or tungsten is used as the material of the electron reflector 13, when the material of the target 11 is molybdenum. In the present embodiment, the material of the target 11 may be the same as the material of the electron reflector 13. The material of both of the target 11 and the electron reflector 13 may be tungsten or tantalum.
The electron passage 15 has a conical shape having a cross-sectional area that increases from an outlet on the target side 11 toward an inlet on the electron source side. Because the electron passage 15 has a conical shape, electrons that are not directly incident on the target 11 from the electron source can be guided to the target 11 by making the electrons be bounced and reflected multiple times by the wall of the electron passage 15. The length of the conical shape is in the range of 5 to 10 mm. The diameter of an inlet opening, through which electrons enter, is in the range of 1 to 5 mm. The diameter of an outlet opening, through which electrons exit, is in the range of 10 to 500 μm. (The diameter of the outlet opening is selected in accordance with the size of a focal spot that is required.) The diameter L of the inlet opening may be greater than the beam diameter φ of an incident electron beam (which is, for example, in the range of 0.5 to 1.0 mm), and the diameter M of the outlet opening may be less than or equal to the beam diameter (I). The diameter L of the inlet opening and the beam diameter φ, and the diameter M of the outlet opening and the beam diameter φ may have the following relationships.
2≦L/φ≦5, 0.01≦M/φ≦1.0
When the electron passage 15 has a taper angle θ1 that satisfies 5≦tan θ1≦60, electrons reflected in the electron passage can be efficiently incident on the target. It is preferable that the taper angle θ1 satisfy 10≦tan θ1≦55. The same effect can be obtained when the electron passage 15 has, instead of a conical shape, a pyramidal shape having a rectangular or polygonal cross section, as long as the conditions for the taper angle θ1 are satisfied.
An X-ray shield 14 is disposed on another side (second side) of the target portion 16 so as to face the electron reflector 13 with the target portion 16 therebetween (on the outer side of the target portion 16). The X-ray shield 14 includes an X-ray passage 17 that is tapered in a direction opposite from the tapering of the electron passage 15. That is, expressed in another way, the X-ray passage 17 increases its sectional area outward from the target portion 16 to an outlet port thereof. The length of the X-ray passage 17 is in the range of 10 to 50 mm. The diameter of an opening on the substrate 12 side is in the range of 1 to 5 mm. The diameter of an outer opening, which is opposite to the opening on the substrate 12 side, is in the range of 3 to 10 mm. The X-ray shield 14 limits the scattering angle of X-rays radiated from the target 11. The X-ray shield 14 may be made of a material having a high absorption rate for X-rays and a high thermal conductivity, such as tungsten or tantalum. For medical application, the X-ray passage 17 may have a taper angle θ2 that satisfies 2≦tan θ2≦20.
The ratio of the diameter of the opening of the X-ray shield 14 on the substrate 12 side (the target 11 side) to the diameter of the outlet opening of the electron passage 15 may be in the range of 10 to 100. In this manner, even with a small focal spot size and a sufficiently large amount of X-rays can be achieved.
The target 11, the electron reflector 13, and the X-ray shield 14 may be made of the same material, such as tungsten, or similar materials. In this case, the efficiency in X-ray radiation, the efficiency in use of reflected electrons, and an effect of blocking unnecessary X-rays can be simultaneously increased. Moreover, in this case, the process of manufacturing the anode unit 10 is simplified.
The envelope 23 may have a sufficiently high strength as a container and high heat dissipation capability. The envelope 23 may be made of a metal material, such as brass, steel, or a stainless steel.
The insulating liquid 8 may be an electrically insulating oil (such as a silicone oil or a mineral oil), which can serve as a coolant for cooling the X-ray tube 21.
The envelope 23 has a window 28, through which X-rays can pass and through which radiation is emitted to the outside of the envelope 23. The window 28 is made of glass or aluminium.
The electron source 25 is disposed in the vacuum vessel 24 so as to face the target portion 16. The electron source 25 includes a hot cathode (for example, tungsten filament) or a cold cathode (for example, a carbon nanotube), an extraction electrode, and a lens electrode. The extraction electrode generates an electric field that causes electrons to be emitted, the lens electrode focuses the electrons onto the target 11, and thereby X-rays are generated. Between the electron source 25 and the target 11, an acceleration voltage Va in the range of 40 to 150 kV (kilo volts) is applied.
The vacuum vessel 24, which maintains a vacuum in the X-ray tube 21, is made of glass or ceramic. The degree of vacuum in the vacuum vessel 24 is in the range of 10−4 to 10−8 Pa. A getter may be disposed in the vacuum vessel 24 to maintain a vacuum. At the opening portion of the vacuum vessel 24, the X-ray shield 14 having the X-ray passage 17 is disposed in such a way that at least a part of the X-ray shield 14 protrudes toward the envelope 23. The anode unit 10 is joined to the periphery of the opening portion using silver solder.
While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2012-089700 filed Apr. 10, 2012, which is hereby incorporated by reference herein in its entirety.
Number | Date | Country | Kind |
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2012-089700 | Apr 2012 | JP | national |