The present invention relates to a cold cathode X-ray tube and a control method therefor.
Conventional X-ray tubes use a filament as an electron emission element and use thermoelectrons emitted from the filament as an electron source. On the other hand, there are recently proposed some X-ray tubes (cold cathode X-ray tubes) that use a cold cathode as an electron emission element (e.g., U.S. Pat. No. 7,778,391, U.S. Pat. No. 7,809,114, and U.S. Pat. No. 7,826,595).
As compared to the X-ray tubes that use a filament as an electron emission element, the cold cathode X-ray tubes have a property that the electron emission amount thereof is subject to cathode surface conditions. Therefore, in conventional cold cathode X-ray tubes, there may occur such a problem that a vacuum degree is lowered by gas generated during the operation of the X-ray tube to change the cathode surface conditions to cause temporal reduction in anode current. In order to solve this problem, there is known a method that gradually increases extraction voltage (e.g., Non-Patent Documents 1 and 2).
Non-Patent Document 3 describes, as an example of field emission display, that in a Spindt-type cold cathode array using a Mo material, temporal reduction in anode current occurs due to generation of oxidizing gas in a vacuum tube being in an operating state. Further, Non-Patent Document 4 describes that hydrogen gas is effective for preventing such reduction in anode current. In the technique described in Non-Patent Document 4, a metal hydride is disposed in the flow of electrons (primary electrons) directed from the cathode to anode, and hydrogen gas is generated when the electrons collide with the metal hydride.
Non-Patent Document 1 IVNC2013 P15 Stable, High Current Density Carbon Nanotube Field Emission Devices (D. Smith et. al). Proc. Of SPIE Vol.7622 76225M-1 Distributed source X-ray technology for Tomosynthesis imaging (F. Sprenger, et.al)
Non-Patent Document 2 Proc. Of SPIE Vol.7622 76225M-1 Distributed source X-ray technology for Tomosynthesis imaging (F. Sprenger, et.al)
Non-Patent Document 3 J. Vac. Sci. Technol. B 16, 2859 (1998) Effect of 02 on the electron emission characteristics of active molybdenum field emission cathode arrays (B. Chalamala, et.al)
Non-Patent Document 4 J. Vac. Sci. Technol. B 21, 1187 (2003) Gas-induced current decay of molybdenum field emitter arrays (R. Reuss, et.al)
However, it is difficult for the above-described conventional techniques to sufficiently suppress the temporal reduction in anode current generated in the cold cathode X-ray tube. That is, in the method that gradually increases the extraction voltage, discharge is generated when the extraction voltage becomes excessively high, so that the temporal reduction in anode current cannot be sufficiently covered. Further, in the method utilizing the hydrogen gas, it is necessary to apply coating of the metal hydride onto a target in order to dispose the metal hydride in the flow of electrons (primary electrons) directed from the cathode to anode; otherwise this method cannot be applied to the cold cathode X-ray tube. Hereinafter, this point will be described in greater detail.
In the X-ray tube, a target as an X-ray generation source is disposed on a part of the anode surface with which the flow of electrons (primary electrons) directed from the cathode to anode directly collides. Therefore, it is necessary to apply coating of the metal hydride to the target in order to dispose the metal hydride in the flow of electrons (primary electrons) directed from the cathode to anode.
However, the target needs to be subjected to high-temperature baking treatment. Application of such baking treatment will cause hydrogen to desorb from the metal hydride, so that it is difficult to apply coating of the metal hydride onto the target for the purpose of generating hydrogen gas. Further, the target has a high temperature even during the operation of the X-ray tube, so that even if the target can be coated with the metal hydride, film peeling or cracks may occur in the metal hydride due to high temperature during the operation, thus preventing the metal hydride from playing a role as a hydrogen gas supply source.
It is therefore an object of the present invention to provide a cold cathode X-ray tube capable of being driven stably over a long period of time by preventing temporal reduction in anode current.
A cold cathode X-ray tube according to the present invention includes; an electron emission part including an electron emission element using a cold cathode; an anode part disposed opposite to the electron emission part; a target disposed on a part of a surface of the anode part; a housing in which the electron emission part, the anode part, and the target are disposed; and a hydrogen generation part that is made of a material that generates hydrogen when receiving collision of electrons and disposed on a portion other than the surface of the target out of surfaces existing in the housing.
In the cold cathode X-ray tube, scattering electrons collide also with a part of the anode surface other than a part thereof with which the flow of electrons directed from the cathode to anode directly collides (including other surfaces existing inside the housing), so that according to the present invention, even though the hydrogen generation part is disposed on a portion other than the target surface, hydrogen gas can be generated while the X-ray tube is being operated. Thus, the temporal reduction in the anode current can be prevented, allowing a cold cathode X-ray tube capable of being driven stably over a long period of time to be provided.
Preferred embodiments of the present invention will be explained below in detail with reference to the accompanying drawings.
The housing 15 is a sealed member made of glass, ceramic, or stainless. Although not illustrated, a valve is provided in the housing 15, and exhaust of gas from the housing 15 and injection of gas into the housing 15 are performed as needed through the valve. For example, before the cold cathode X-ray tube 1 is operated under the control of the controller 2, a vacuum pump is used to exhaust the gas from the housing 15 to form a vacuum state, and, meanwhile, hydrogen gas or a mixture of hydrogen gas and nitrogen gas is injected into the housing 15 to adsorb the hydrogen gas to the hydrogen generation part 14. This is treatment for suitably generating the hydrogen gas from the hydrogen generation part 14.
The anode part 11 is a metal member having an anode surface 11a disposed opposite to the electron emission part 10 and, specifically, the anode part 11 is made of copper (Cu). The anode part 11 is connected with the positive side terminal of a power supply P. Thus, when the gate electrode 22 illustrated in
The target 12 is a member made of a material that generates an X-ray by receiving electrons and disposed so as to cover a part of the anode surface 11a with which the electrons emitted from the electron emission elements 21 directly collide. Since the target 12 is disposed on the anode surface 11a, some or all of the plurality of electrons that collide with the anode surface 11a pass through the target 12, and an X-ray is generated in the target 12 during the passage. The thus generated X-ray is radiated downward in the drawing due to inclination of the anode surface 11a.
The focus structure 13 is a structure having a function of correcting the trajectory of the electrons emitted from the electron emission part 10 and is disposed between the electron emission part 10 and the target 12 disposed on the anode surface 11a. The focus structure 13 has a window 13h. The electrons emitted from the electron emission part 10 are directed to the target 12 through the window 13h. The focus structure 13 is supplied with focus voltage Vf from the controller 2. The focus voltage Vf plays a role of controlling the amount of correction of the electron trajectory made by the focus structure 13. The focus structure 13 may be divided into two or more areas and, in this case, it is possible to adjust the focus position of an electron beam on the anode surface 11a by applying different focus voltages Vf to the respective areas.
The controller 2 is a processor that operates according to a previously written program or an external instruction and has functions of supplying the ground potential GND to the cathode part 20, supplying the gate voltage Vg to the gate electrode 22, and supplying the focus voltage Vf to the focus structure 13. The X-ray tube 1 is activated when the gate voltage Vg starts being supplied to the gate electrode 22 under the control of the controller 2 and starts X-ray emission.
The hydrogen generation part 14 is a member made of a material that generates hydrogen when receiving collision of electrons. Examples of such material include a silicon nitride film (SiN), a silicon carbide film (SiC), a silicon carbonitride film (SiCN), an amorphous carbon film (a-C), and a diamond-like carbon film (DLC).
The hydrogen generation part 14 is disposed on a portion other than the surface of the target 12 out of surfaces existing in the housing 15. Specifically, as illustrated in
The hydrogen generation part 14 is preferably formed by, e.g., plasma CVD (Plasma-Enhanced Chemical Vapor Deposition). The use of the plasma CVD allows the hydrogen generation part 14 to be constituted by a thin film covering a surface of a target. For example, when the hydrogen generation part 14 is constituted by a diamond-like carbon film (DLC), it is preferable to use plasma CVD using methane (CH4) as source gas to form a thin film of 1 □m at 1 Pa and at 200□C.
When the primary electrons emitted from the electron emission part 10 collide with the target 12 formed on the anode surface 11a, second electrons are emitted from the target 12 in addition to the X-ray. At least some of the secondary electrons go behind the target 12 and collide with the surface of the anode part 11. Since the hydrogen generation part 14 is disposed there, hydrogen gas is generated due to collision of the electrons. As a result, gas atmosphere (partial pressure) inside the housing 15 is adjusted, whereby the temporal reduction in the anode current can be prevented.
As described above, in the cold cathode X-ray tube 1 according to the present embodiment, the temporal reduction in the anode current can be prevented, allowing a cold cathode X-ray tube capable of being driven stably over a long period of time to be provided. Further, in the cold cathode X-ray tube 1 according to the present embodiment, the hydrogen generation part 14 is not formed on the surface of the target 12, so that it is possible to avoid that the hydrogen generation part 14 cannot accomplish its role as a hydrogen gas supply source due to occurrence of film peeling or cracks.
As illustrated in
According to the present modification, some of the electrons emitted from the electron emission part 10 that scatter in the horizontal direction (backscattering electrons) collide with the hydrogen generation part 14. Thus, hydrogen gas is generated as in the case of the above embodiment, so that the temporal reduction in the anode current can be prevented according to the present modification as well, allowing a cold cathode X-ray tube capable of being driven stably over a long period of time to be provided. Further, it is possible to avoid the problem in that the hydrogen generation part 14 cannot accomplish its role as a hydrogen gas supply source due to the occurrence of film peeling or cracks.
According to the present modification, some of the electrons emitted from the electron emission part 10 that scatter in the horizontal direction (backscattering electrons) collide with the hydrogen generation part 14. Thus, hydrogen gas is generated as in the case of the above embodiment and the first modification, so that the temporal reduction in the anode current can be prevented according to the present modification as well, allowing a cold cathode X-ray tube capable of being driven stably over a long period of time to be provided. Further, it is possible to avoid the problem in that the hydrogen generation part 14 cannot accomplish its role as a hydrogen gas supply source due to the occurrence of film peeling or cracks.
It is apparent that the present invention is not limited to the above embodiments, but may be modified and changed without departing from the scope and spirit of the invention.
Filing Document | Filing Date | Country | Kind |
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PCT/JP2019/002967 | 1/29/2019 | WO | 00 |
Number | Date | Country | |
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62624314 | Jan 2018 | US |