Embodiments described herein relate generally to an X-ray tube.
Generally, X-ray tubes are used for applications such as image diagnosis. A cathode of such an X-ray tube comprises two electron guns. Each of the electron guns includes a filament coil for emitting electrons and a focusing groove for focusing the emitted electrons. Two electron guns share one focusing electrode. The electrons emitted from each electron gun and then focused collide with a target surface of an anode target, and a focal spot is thereby formed on the target surface. Two electron guns are located with the focal spot in between so as to form a focal spot at the same position on the target surface, and are arranged so as to be inclined.
The target surface is inclined at an angle called a target angle in the main radiation direction. When viewed from a direction orthogonal to both the main radiation direction and the X-ray tube axis, the target surface and the surface on the side facing the target surface of the electron gun are inclined by approximately the target angle. Since the flight distance of electrons emitted from one of ends of the filament coil in the longitudinal direction and the flight distance of electrons emitted from the other end, are different from each other, the focal spot has a distorted shape. Therefore, in order to correct such distortion of the focal spot shape, a technique of inclining the whole electron gun to an appropriate angle with respect to the main radiation direction is known.
In general, according to one embodiment, there is provided an X-ray tube comprising:
an anode including a target surface radiating X-rays in a main radiation direction from a first focal spot formed by collision of an electron beam; and
a cathode arranged at a position opposite to the target surface of the anode, and including a first filament emitting the electron beam and a focusing electrode focusing the electron beam emitted from the first filament, the focusing electrode including a valley bottom part farthest (with the shortest distance longest) from the first focal spot, a first inclined plane obliquely rising from the valley bottom part in the anode direction, a first focusing groove opened to the first inclined plane, and a first housing groove opened to the bottom surface of the first focusing groove to accommodate the first filament,
wherein
if an axis passing through a center of the first focal spot and parallel to an X-ray tube axis is a reference axis, a plane including the reference axis and the main radiation direction is a first reference plane, and an angle formed inside by a first extending line and a second extending line intersecting on a side opposite to a side of radiating the X-rays to the reference axis is referred to as a first angle θ1, where the first extending line is a virtual straight line extending from a boundary straight line between the valley bottom part and the first inclined plane along the first reference plane, and the second extending line is a virtual straight line extending from the target surface along the first reference plane and the target surface,
θ1>0°
the first housing groove has a long axis, and
the other end part of the first housing groove is closer to the first reference plane than one end part of the first housing groove on the first extending line side.
Embodiments will be described hereinafter with reference to the drawings. The disclosure is merely an example, and proper changes in keeping with the spirit of the invention, which are easily conceivable by a person of ordinary skill in the art, come within the scope of the invention as a matter of course. In addition, in some cases, in order to make the description clearer, the widths, thicknesses, shapes and the like, of the respective parts are illustrated schematically in the drawings, rather than as an accurate representation of what is implemented. However, such schematic illustration is merely exemplary, and in no way restricts the interpretation of the invention. In addition, in the specification and drawings, the same elements as those described in connection with preceding drawings are denoted by like reference numbers, and detailed description thereof is omitted unless necessary.
As shown in
The anode 3 includes a target body 3a and an anode extending portion 3d connected to the target body 3a. The target body 3a includes a target layer 3b against which electrons collide. The surface of the target layer 3b on the side where electrons collide is a target surface 3c. The target body 3a is formed of a highly thermally conductive metal such as molybdenum (Mo), copper (Cu), an alloy thereof, or the like. The target layer 3b is formed of a metal having a melting point higher than that of the material used for the target body 3a. For example, the target body 3a is formed of copper or a copper alloy, and the target layer 3b is formed of a tungsten alloy. The anode extending portion 3d is formed in a columnar shape and uses copper or a copper alloy. The anode extending portion 3d fixes the target body 3a. The anode 3 emits X-rays as electrons emitted from the filament and focused by the focusing electrode impinge on the target surface 3c.
The vacuum envelope 4 includes a glass container 4a and a metal container 4b. The metal container 4b is airtightly connected to the glass container 4a on the one hand and airtightly connected to the anode 3 on the other. The glass container 4a is formed by using, for example, borosilicate glass. The glass container 4a can be formed by hermetically joining, for example, a plurality of glass members by melting. Since the glass container 4a has X-ray transparency, X-rays emitted from the anode 3 pass through the glass container 4a and are emitted to the outside of the vacuum envelope 4. The metal container 4b is airtightly fixed to at least one of the target body 3a and the anode extending portion 3d. The metal container 4b is airtightly connected to the target body 3a by brazing. In addition, the metal container 4b and the glass container 4a are airtightly connected by sealing. In the present embodiment, the metal container 4b is formed in an annular shape. In addition, the metal container 4b is formed by using Kovar.
The vacuum envelope 4 accommodates the cathode 2 and the target body 3a, and is formed such that the anode extending portion 3d is exposed. A plurality of pin assemblies 15 are airtightly attached to the vacuum envelope 4. Each of the pin assemblies 15 includes a cathode pin and the like and is located inside and outside the vacuum envelope 4.
The Z axis is an axis parallel to the X-ray tube axis A, the X axis is an axis orthogonal to the Z axis, and the Y axis is an axis orthogonal to both the X axis and the Z axis. A main radiation direction d of the X-rays which will be explained later is parallel to the X axis and the direction is opposite.
The voltage and current output from the power supply unit outside the X-ray tube 1 is supplied to the pin assembly 15 for filament and is consequently supplied to the filament. As a result, the filament emits electrons (thermal electrons). The power supply unit also supplies a predetermined voltage to the cathode 2 and the anode 3. In the present embodiment, a negative high voltage is applied to the cathode and a positive high voltage is applied to the anode 3. Since an X-ray tube voltage (tube voltage) is applied between the anode 3 and the cathode 2, the electrons emitted from the filament are accelerated and made incident on the target surface 3c as an electron beam. That is, the X-ray tube current (tube current) flows from the cathode 2 to the focal spot on the target surface 3c.
The focusing electrode serving as the cathode potential can focus electron beams (electrons) from the filament towards the anode 3.
The target surface 3c emits X-rays when an electron beam is made incident, and the X-rays emitted from the focal spot are transmitted through the vacuum envelope 4 and emitted to the outside of the X-ray tube 1.
As shown in
The front surface 10A is closest to the anode 3, in the cathode 2 (focusing electrode 10). In this embodiment, the front surface 10A is parallel to the X-Y plane. However, the front surface 10A and the valley bottom part M may not be parallel to the X-Y plane.
The first inclined plane 11 and the second inclined plane 12 are inclined from the X-Y plane such that the two electron guns can form the focal spot F at the same position. The valley bottom part M is located on the X-Z plane passing through the reference axis RA.
The distance from the focal spot F to the valley bottom part M is longest of distances from the focal spot F to the first inclined plane 11 or the second inclined plane 12.
The first focusing groove 21 opens in the first inclined plane 11. The first housing groove 31 opens in the bottom surface 21b of the first focusing groove 21 and accommodates the filament coil 5. The second focusing groove 22 opens in the second inclined plane 12. The second housing groove 32 opens in the bottom surface 22b of the second focusing groove 22 and accommodates the filament coil 6.
The first inclined plane 11 is parallel to the bottom face 21b and the second inclined plane 12 is parallel to the bottom face 22b. For this reason, an opening 310 of the first housing groove 31 is parallel to an opening 210 of the first focusing groove 21, and an opening 32o of the second housing groove 32 is parallel to an opening 22o of the second focusing groove 22. The filament coil 5 extends along a virtual plane parallel to the opening 31o. The filament coil 6 extends along a virtual plane parallel to the opening 32o.
Of the focal spots F formed on the target surface 3c, a focal spot at which electrons emitted from the filament coil 5 are made incident on the target surface 3c and thereby irradiate X-rays in the main radiation direction is referred to as a first focal spot F1. On the other hand, a focal spot at which electrons emitted from the filament coil 6 are made incident on the target surface 3c to emit X-rays in the main radiation direction is referred to as a second focal spot F2. In the present embodiment, the center position of the first focal spot F1 and the center position of the second focal spot F2 are the same as each other. However, the dimension of the first focal spot F1 is different from the dimension of the second focal spot F2. This is because two electron guns are different in structure from each other, in the present embodiment. As will be explained later, for example, the dimensions of the filament coil 5 are different from the dimensions of the filament coil 6.
The reference axis RA is an axis passing through the center of the first focal spot F1 and parallel to the X-ray tube axis A. In the present embodiment, the reference axis RA is also an axis passing through the center of the second focal spot F2 and parallel to the X-ray tube axis A since the central positions of the first focal spot F1 and the second focal spot F2 are the same as each other. In addition, a plane including the reference axis RA and the main radiation direction is referred to as a first reference plane S1. A virtual plane located on the same plane as the front surface 10A is referred to as a second reference plane S2.
As shown in
In the present embodiment, the long axis of each of the first housing groove 31 and the filament coil 5 is not parallel to the first reference plane S1. The long axis of each of the second housing groove 32 and the filament coil 6 is not parallel to the first reference plane S1.
The first focusing groove 21 has one end part 21e1 and the other end part 21e2. The first housing groove 31 has one end part 31e1 and the other end part 31e2. The filament coil 5 has one end part 5e1 and the other end part 5e2.
In addition, the second focusing groove 22 has one end part 22e1 and the other end part 22e2. The second housing groove 32 has one end part 32e1 and the other end part 32e2. The filament coil 6 has one end part 6e1 and the other end part 6e2.
The main radiation direction is a direction on the X-Z plane passing through the reference axis RA and a direction along the central axis of the available X-ray flux. In the present embodiment, the main radiation direction is perpendicular to the reference axis RA. In general, the shape of the focal spot formed on the target surface 3c as viewed from the outside of the X-ray tube 1 along the main radiation direction d which passes through the center of the focal spot and perpendicularly intersects the reference axis RA is called an effective focal spot.
As shown in
θ1>0°. In the present embodiment, the first angle θ1 is an acute angle (0°<θ1<90°). That is, the front surface 10A and the valley bottom part M are not parallel to the target surface 3c.
A plane including the reference axis RA and orthogonal to the first reference plane S1 is referred to as a third reference plane S3.
As shown in
Similarly, the other end part 32e2 of the second housing groove 32 is closer to the first reference plane S1 than the one end part 32e1 of the second housing groove 32 on the side of the first extending line E1. In addition, the other end part 6e2 of the filament coil 6 is closer to the first reference plane S1 than the one end part 6e1 of the filament coil 6 on the side of the first extending line E1.
As shown in
θ2>0°. In the present embodiment, the second angle θ2 is an acute angle (0°<θ2<90°).
Similarly, an angle formed by a fifth extending line E5 and a sixth extending line E6 intersecting on the side viewed beyond the cathode 2 and the anode 3 from the reference axis RA is referred to as a third angle θ3. The fifth extending line E5 is a virtual straight line extending from the second inclined plane 12 along the third reference plane S3 and the second inclined plane 12. The sixth extending line E6 is a virtual straight line extending from the target surface 3c along the third reference plane S3 and the target plane 3c.
θ3>0°. In the present embodiment, the third angle θ3 is an acute angle (0°<θ3<90°).
As shown in
As shown in
As shown in
As shown in
In the perpendicular projection view of
As shown in
In the perpendicular projection view of
Next, results of simulations executed by the present inventors for emitting X-rays on the assumption that the X-ray tube 1 according to the present embodiment is used will be described. At this time, only the filament coil 5 of the plurality of filament coils was driven. For this reason, the focal spot formed on the target surface 3c was the first focal spot F1 and was a single focal spot. In addition, the simulation was executed under the same conditions.
More specifically, only the filament coil 5 was driven. The electrons emitted from the filament coil 5 are made incident on the target surface 3c as an electron beam. The electron beam is focused by the action of the electric field formed by the first focusing groove 21 of the focusing electrode 10. The positions and dimensions of a main focal spot formed by the electrons emitted from the upper surface (the surface on the target surface 3c side) of the filament coil 5 and the sub-focal spot formed by the electrons emitted from the side surface of the filament coil 5 substantially overlapped.
Various angles and distances are as follows.
θ1=16°
θ2=25°
θ4=2°
D1=13.3 mm
D2=16.7 mm
As can be understood from
As shown in
According to the X-ray tube 1 of the embodiment configured as described above, the X-ray tube 1 comprises a cathode 2 and an anode 3. The cathode 2 includes a filament coil 5, and a focusing electrode 10 including a front surface 10A, a first inclined plane 11, a first focusing groove 21 and a first housing groove 31. The anode 3 has a target surface 3c.
θ1>0° and θ2>0°. The filament coil 5, the first housing groove 31, and the first focusing groove 21 are located on the third extending line E3 side from the first reference plane S1. The other end part 31e2 of the first housing groove 31 is closer to the first reference plane S1 than the one end part 31e1 on the first extending line E1 side of the first housing groove 31.
The distortion of the shape of the first focal spot F1 can be thereby corrected. That is, the distortion of the shape of the first focal spot F1 can be suppressed as compared with a case where θ4=0°. In this case, the above effect can be obtained without increasing the outer diameter of the focusing electrode 10. In addition, the above effect can be obtained without tilting the long axis of the first focusing groove 21. Based on the above, the X-ray tube 1 which is small in size and can reduce the distortion of the focal spot shape can be obtained.
Next, results of investigations on the fourth angle θ4 and the fifth angle θ5 executed by the present inventors will be explained.
As shown in
When θ2=25° and θ1=20°, it is desirable that θ4=4.4°.
When θ2=25° and θ1=5°, it is desirable that θ4=1.0°.
When θ2=25° and θ1=2.5°, it is desirable that θ4=0.5°.
Next, attention is paid to the first angle θ1, the third angle θ3, and the fifth angle θ5.
When θ3=25° and θ1=20°, it is desirable that θ5=5.2°.
When θ3=25° and θ1=5°, it is desirable that θ5=1.3°.
When θ3=25° and θ1=2°, it is desirable that θ5=0.5°.
The second angle θ2 depends on the length of the first straight-line distance D1, the length of the second straight-line distance D2, and the size of the first focusing groove 21. The third angle θ3 depends similarly to the second angle θ2. The case where each of the second angle θ2 and the third angle θ3 is 25° has been explained as an example, but the angles are not limited to these and can be variously modified. For example, the second angle θ2 and the third angle θ3 may be approximately 20°.
Based on the above, the fourth angle θ4 becomes smaller as the second angle θ2 is smaller. The fifth angle θ5 becomes smaller as the third angle θ3 is smaller. In addition, the fourth angle θ4 becomes larger as the first focusing groove 21 is larger. The fifth angle θ5 becomes larger as the second focusing groove 22 is larger.
An optimum value of the fourth angle θ4 exists depending on the magnitude of the first angle θ1, the magnitude of the second angle θ2, the length of the first straight-line distance D1, the length of the second straight-line distance D2, and the size of the first focusing groove 21. Similarly, an optimum value of the fifth angle θ5 exists depending on the magnitude of the first angle θ1, the magnitude of the third angle θ3, the length of the third straight-line distance D3, the length of the fourth straight-line distance D4, and the size of the second focusing groove 22. For example, each of the fourth angle θ4 and the fifth angle θ5 is desirably selected from the range of 0.5° to 5°.
The upper limit value of the fourth angle θ4 is a value at which the first housing groove 31 interferes with the first focusing groove 21. For example, in
Next, the X-ray tube of a comparative example will be explained for comparison with the X-ray tube 1 according to the above embodiment.
As shown in
As can be understood from
As shown in
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel embodiments described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the embodiments described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the inventions.
For example,
If the X-ray tube 1 includes a plurality of electron guns, the housing groove (filament coil) of at least one electron gun of the X-ray tube 1 may be inclined as shown in
For this reason, the X-ray tube 1 may be provided with a housing groove (filament coil) which is not inclined as shown in
In addition, the example that the valley bottom part M is linear is explained in the above embodiment, but the valley bottom part M may be a flat surface perpendicular to the first reference plane S1. In this case, the flat valley bottom part M may be provided with a non-inclined focusing groove and a non-inclined housing groove (filament coil) as shown in
Furthermore, the example that the focusing electrode 10 includes the flat front surface 10A is explained in the above embodiment, but the flat front surface 10A may not be present.
Embodiments of the present invention are not limited to the above-explained stationary anode X-ray tube 1 but can be applied to various types of stationary anode X-ray tubes, rotation anode X-ray tubes, and other X-ray tubes.
Number | Date | Country | Kind |
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2016-121669 | Jun 2016 | JP | national |
This application is a Continuation Application of PCT Application No. PCT/JP2017/021449, filed Jun. 9, 2017 and based upon and claiming the benefit of priority from Japanese Patent Application No. 2016-121669, filed Jun. 20, 2016, the entire contents of all of which are incorporated herein by reference.
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Number | Date | Country | |
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20190180970 A1 | Jun 2019 | US |
Number | Date | Country | |
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Parent | PCT/JP2017/021449 | Jun 2017 | US |
Child | 16227273 | US |