Klystron
阅读说明:本技术 速调管 (Klystron ) 是由 阿武俊郎 大久保良久 于 2017-12-25 设计创作,主要内容包括:速调管(10)包括电子枪部(A)、多个共振空腔(14a~14j)、收集极(15)以及多根漂移管(16a~16k)。多个共振空腔(14a~14j)包括沿着来自电子枪部(A)的电子(11)的行进方向依次定位的输入空腔(19)、多个中间空腔(21b~21i)以及输出空腔(20)。多个中间空腔(21b~21i)包括多个二次谐波空腔(23d、23g)。收集极(15)对经过多个共振空腔(14a~14j)的电子(11)进行捕捉。多根偏移管(16a~16k)设置在电子枪部(A)与输入空腔(19)之间、多个共振空腔(14a~14j)之间以及输出空腔(20)与收集极(15)之间。(The klystron (10) includes an electron gun section (A), a plurality of resonant cavities (14 a-14 j), a collector (15), and a plurality of drift tubes (16 a-16 k). The plurality of resonant cavities (14 a-14 j) include an input cavity (19), a plurality of intermediate cavities (21 b-21 i), and an output cavity (20) that are positioned in order along the direction of travel of electrons (11) from the electron gun section (A). The plurality of intermediate cavities (21 b-21 i) include a plurality of second harmonic cavities (23d, 23 g). The collector (15) captures electrons (11) that have passed through the plurality of resonant cavities (14 a-14 j). A plurality of offset tubes (16 a-16 k) are provided between the electron gun section (A) and the input cavity (19), between the plurality of resonance cavities (14 a-14 j), and between the output cavity (20) and the collector (15).)
1. A klystron, comprising:
an electron gun part that emits electrons;
a plurality of resonant cavities including an input cavity, a plurality of intermediate cavities, and an output cavity positioned in sequence along a direction of travel of electrons from the electron gun portion, the plurality of intermediate cavities including a plurality of second harmonic cavities;
a collector that captures electrons passing through the plurality of resonant cavities; and
a plurality of drift tubes disposed between the electron gun portion and the input cavity, between the plurality of resonant cavities, and between the output cavity and the collector.
2. A klystron as set forth in claim 1,
the total number of the plurality of resonant cavities is more than ten.
3. A klystron as set forth in claim 1,
the plurality of intermediate cavities are arranged along a traveling direction of electrons,
two or more intermediate cavities are provided between the second harmonic cavity located on the upstream side and the second harmonic cavity located on the downstream side in the traveling direction of electrons,
a plurality of intermediate cavities of the plurality of intermediate cavities other than the plurality of second harmonic cavities includes the two or more intermediate cavities.
4. A klystron as set forth in claim 1,
the diameter of the drift tube adjacent to the second harmonic cavity is equal to or less than half of the diameter of the second harmonic TE11 mode, at which the electromagnetic wave has a cutoff frequency.
5. The klystron of any one of claims 1 to 4,
each of the plurality of resonant cavities has a gap in communication with the interior of the drift tube,
the interval between the centers of the gaps of a pair of adjacent resonant cavities in the plurality of resonant cavities is 0.05-0.08 times of the plasma wavelength of the electrons.
6. A klystron as set forth in claim 1,
setting the total number of the plurality of resonant cavities to n,
counting from the side close to the electron gun part,
setting the diameter of the drift tube between the n-th resonance cavity and the n-1 st resonance cavity as Dn,
Setting the diameter of the drift tube between the n-1 th resonance cavity and the n-2 nd resonance cavity as Dn-1,
Setting the diameter of the drift tube between the n-2 th resonance cavity and the n-3 rd resonance cavity as Dn-2,
Setting the diameter of the offset tube between the n-th resonant cavity and the collector to Dc,
Satisfies the following conditions: dn-2<Dn-1<Dn<Dc。
7. The klystron of any one of claims 1 to 6,
the output cavity is composed of three or more cavity units electrically coupled to each other through a diaphragm provided in a longitudinal direction of the drift tube or a coupling hole provided in a wall surface of the cavity unit.
8. A klystron as set forth in claim 7,
the total number of the cavity units is three.
Technical Field
Embodiments of the present invention relate to a klystron.
Background
A klystron is an electron tube for amplifying high-frequency power, and includes an electron gun portion for emitting electrons, an input portion and an output portion for high-frequency power, a harmonic interaction portion, and a collector for capturing used electrons. The harmonic wave interaction portion is composed of a plurality of resonant cavities arranged in the traveling direction of electrons. The resonant cavity includes an input cavity to which the high-frequency power is input, an output cavity to which the high-frequency power is output, and a plurality of intermediate cavities between the input cavity and the output cavity. The electron gun part and the harmonic interaction part, the plurality of resonance cavities constituting the harmonic interaction part, and the harmonic interaction part and the collector part are connected by drift tubes, respectively.
In the klystron having the above-described configuration, electrons emitted from the electron gun portion pass through the input cavity and are clustered by interacting with the plurality of intermediate cavities located in front of the input cavity. The kinetic energy of the clustered electrons is applied to the high-frequency wave input from the input cavity, so that the clustered electrons are decelerated at the output cavity, thereby being extracted from the output portion as high-frequency power amplified to a target output.
In addition, in order to improve the electron clustering effect and increase the efficiency, a klystron is provided in which one of a plurality of intermediate cavities is used as a second harmonic cavity.
However, there are technical problems in the klystron as follows: the clustered electrons are easily repelled from each other by space charges and thus easily diffused in the traveling direction, and further, because there is a difference in the velocity of the electrons, the electrons cannot be uniformly decelerated at the input cavity, and the conversion efficiency into high-frequency power is difficult to improve.
Disclosure of Invention
Technical problem to be solved by the invention
The invention provides a klystron which improves the conversion efficiency of converting to high-frequency power.
Technical scheme for solving technical problem
The klystron of an embodiment includes:
an electron gun part that emits electrons;
a plurality of resonant cavities including an input cavity, a plurality of intermediate cavities, and an output cavity positioned in sequence along a direction of travel of electrons from the electron gun portion, the plurality of intermediate cavities including a plurality of second harmonic cavities;
a collector that captures electrons passing through the plurality of resonant cavities; and
a plurality of drift tubes disposed between the electron gun portion and the input cavity, between the plurality of resonant cavities, and between the output cavity and the collector.
Drawings
Fig. 1 is a sectional view showing the structure of a klystron according to a first embodiment.
Fig. 2 is a cross-sectional view showing a part of the tube container of the klystron shown in fig. 1, and shows a second harmonic cavity and the like.
Fig. 3 is a cross-sectional view showing a part of the tube container of the klystron shown in fig. 1, and is a view for explaining the intervals of the resonant cavities.
Fig. 4 is a sectional view showing a tube container and a collector of a klystron of the second embodiment, and is a view for explaining the diameter of a drift tube.
Fig. 5 is a sectional view showing a tube container and a collector of a klystron according to a third embodiment, and shows a cavity unit and the like.
Fig. 6 is a sectional view showing a tube container and a collector of a klystron according to a fourth embodiment, and shows a cavity unit and the like.
Detailed Description
Hereinafter, a first embodiment will be described with reference to fig. 1 to 3.
Fig. 1 is a sectional view showing a schematic structure of a klystron 10. As shown in fig. 1, the klystron 10 includes an electron gun portion a that emits electrons 11. The electron gun section a includes a cathode 12a for generating the electrons 11, an anode 12b for accelerating the electrons 11, and the like.
A harmonic interaction part B is provided in the traveling direction of the electrons 11, i.e., in front of the electron gun part a. The harmonic interaction portion B includes a
A
The electron gun section a and the harmonic interaction section B, the plurality of resonant cavities 14a to 14j, and the harmonic interaction section B and the
Further, of the plurality of resonant cavities 14a to 14j constituting the harmonic interaction portion B, an input portion 17 for inputting high-frequency power is connected to the resonant cavity 14a located on the electron gun portion a side, and an
Of the plurality of resonant cavities 14a to 14j constituting the high-frequency interaction portion B, the resonant cavity 14a located on the electron gun portion a side is an input cavity 19, the
According to the above description, the drift tube 16a is provided between the electron gun section a and the input cavity 19. The
The intermediate cavities 21b to 21i include a plurality of
In the present embodiment, the following case is shown: the number of resonant cavities 14a to 14j is ten, the number of intermediate cavities 21b to 21i is eight, and the number of second
Fig. 2 is a sectional view showing a part of the
Fig. 3 is a cross-sectional view showing a part of the
As shown in fig. 1, in the klystron 10 configured as described above, the electrons 11 emitted from the electron gun portion a pass through the resonant cavity 14a (input cavity 19) of the output portion 17 having high-frequency power, which is located on the electron gun portion a side, and are clustered by interacting with the plurality of resonant cavities 14b to 14j (the plurality of intermediate cavities 21b to 21i and the output cavity 20) located in front of the resonant cavity. The clustered electrons 11 are decelerated at the
When the electrons 11 are clustered by the interaction between the electrons 11 and the plurality of resonant cavities 14b to 14j, since the plurality of second
Here, in the case of, for example, grouping electrons using five resonant cavities, since the degree of grouping of electrons at each resonant cavity is large, the grouped electrons are repelled by space charges, and the electrons are easily diffused in the traveling direction thereof, and further, since there is a difference in the velocity of the electrons, the electrons cannot be uniformly decelerated at the resonant cavity (output cavity) connected to the output portion, and it is difficult to improve the conversion efficiency into high-frequency power.
In contrast, in the present embodiment, the electrons 11 can be gradually clustered by, for example, ten resonance cavities 14a to 14 j. This suppresses the diffusion of the clustered electrons 11 in the traveling direction thereof, thereby making the speed uniform and improving the conversion efficiency into high-frequency power. In order to gradually cluster the electrons 11, the total number of the resonant cavities 14a to 14j is preferably ten or more.
Further, by using, for example, the ten resonant cavities 14a to 14j, the intermediate cavities 21b to 21i can include the plurality of second-
The plurality of intermediate cavities 21b to 21i are arranged along the traveling direction of the electrons 11. Two or more intermediate cavities 21 are provided between the second harmonic cavity 23 located on the upstream side and the second harmonic cavity 23 located on the downstream side in the traveling direction of the electrons 11. The plurality of intermediate cavities 21 (fundamental wave cavities 22) other than the plurality of second harmonic cavities 23 among the plurality of intermediate cavities 21b to 21i include the two or more intermediate cavities 21.
In the present embodiment, of the positions of the intermediate cavities 21b to 21i, the second
By providing the second
As shown in fig. 1 and 2, in order to prevent the second harmonics generated in the second
As shown in fig. 1 and 3, when the dilatational wave of the bunched electrons 11 propagates in the traveling direction, the arrangement of the resonant cavities 14a to 14j can be optimized by setting the interval L between the centers of the
It is arbitrary which of the resonant cavities 14a to 14j is the second harmonic cavity 23, and three or more may be used as the second harmonic cavities 23. When the plurality of intermediate cavities 21 include three or more second harmonic cavities 23, it is preferable that two or more intermediate cavities 21 (fundamental wave cavities 22) are provided between a pair of adjacent second harmonic cavities 23.
Next, referring to fig. 4, the klystron 10 of the second embodiment will be described. The same reference numerals are given to the same components as those of the first embodiment, and the description of the components and their operational effects will be omitted.
Fig. 4 is a sectional view showing the
As shown in FIG. 4, the total number of resonant cavities 14a to 14j is n, and the diameter D of a
Dn-2<Dn-1<Dn<Dc… … type (1)
For example, if the diameters of the offset
Furthermore, the
The drift tube 16 is not limited to the
Next, referring to fig. 5, the klystron 10 of the third embodiment will be described. The same reference numerals are given to the same components as those in the embodiments, and the description of the components and their operational effects will be omitted.
Fig. 5 is a sectional view showing the
As shown in fig. 5, the
Further, by using the
Next, referring to fig. 6, the klystron 10 of the fourth embodiment will be described. The same reference numerals are given to the same components as those in the embodiments, and the description of the components and their operational effects will be omitted.
Fig. 6 is a cross-sectional view showing the
As shown in fig. 6, the
Further, the
According to at least one embodiment described above, diffusion of the electrons 11 clustered by the resonant cavities 14a to 14j in the traveling direction is suppressed, the speed is uniform, and the conversion efficiency into high-frequency power can be improved by the klystron 10.
While the embodiments of the present invention have been described above, the embodiments are merely examples and do not limit the scope of the present invention. These new embodiments may be implemented in other various ways, and various omissions, substitutions, and changes may be made without departing from the scope of the technical idea of the present invention. These embodiments and modifications thereof are included in the scope or gist of the invention, and are included in the invention described in the claims and the equivalent scope thereof.