TW515225B - Active radio frequency cavity amplifier - Google Patents

Active radio frequency cavity amplifier Download PDF

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Publication number
TW515225B
TW515225B TW90129652A TW90129652A TW515225B TW 515225 B TW515225 B TW 515225B TW 90129652 A TW90129652 A TW 90129652A TW 90129652 A TW90129652 A TW 90129652A TW 515225 B TW515225 B TW 515225B
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Taiwan
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cavity
input
output
power
radio frequency
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TW90129652A
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Chinese (zh)
Inventor
Bernard R Cheo
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Aria Microwave Systems Inc
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Abstract

An active radio frequency cavity amplifier (ARFCA) is provided having a housing defining an input cavity and an output cavity; a plurality of transistors mounted to said housing, each of the plurality of transistors having an input lead and an output lead; a first RF power coupling mechanism disposed within the housing in proximity to the input cavity for coupling RF power from a source into the input cavity to generate an RF field; a first conducting assembly having a plurality of conductors each configured to contact a respective input lead of each of the plurality of transistors for coupling the RF field in the input cavity to the input leads of the plurality of transistors; a second conducting assembly having a plurality of conductors each configured to contact a respective output lead of the plurality of transistors for coupling the amplified RF power from the output leads of the plurality of transistors to the output cavity; and a second RF power coupling mechanism disposed within the housing in proximity to the output cavity for coupling amplified RF power from the output cavity to a load.

Description

M ^225M ^ 225

優先權 、本申請案主張於200年12月13日向美國專利商標局提出 之名稱為“主動射頻空腔放大器,,申請案之優先權,該案所 賦之序號為6〇/255,276,納入本申請案以供參考。 發明背景 1 .發明蓺圚 本發明乃關於射頻電磁場諧振空腔,質言之,乃關於在 此等空腔中達成高度射頻功率輸出者。 2 .相關工藝說明 吾人皆知在空腔中產生高頻電磁場以供諸如線性加速器 等射頻加速器中帶電粒子束之加速。在典型之線性加速器 結構中,射頻功率及由以高壓(數萬伏特)操作之真空管放 大器所提供,經放大之射頻功率利用同軸電纜等自射頻真 空官傳輸至2腔而於空腔内形成振盪電磁場。普通型線性 加速器如漂移真空管線性加速器含有一系列漂移真空管, 配置於空腔内以由電場將粒子加速而形成所要之粒子束。 有若干應用或潛在應用,其需較輕且易運輸之射頻空腔 或線性加速器。此等應用包括地球軌道為主之應用,分散 依要求之醫用同位素生產以及高功率射頻放大器等。不 過,必要之射頻真2管,咼壓電力供應,電力調節裝備及 其相關組件等之重量與尺寸實對此等用途採用射頻空腔或 線性加速器方面構成相當大阻碍。 克服上述射頻S腔缺點之建4性解決方法顯示於a%年3 月5曰頒發之美國第5,497,050號,專利案圖*中,其複製為 _r4- 本紙張尺度適用中國國家標準(CNS) A4規格(210 x 297公釐)Priority, this application claims that the name filed with the US Patent and Trademark Office on December 13, 200, is "Active RF Cavity Amplifier." The priority of the application, the serial number assigned in this case is 60 / 255,276, which is incorporated herein. The application is for reference. BACKGROUND OF THE INVENTION 1. The invention relates to a radio-frequency electromagnetic field resonance cavity. In other words, it relates to those who achieve high RF power output in these cavities. 2. The relevant process description is well known to everyone A high-frequency electromagnetic field is generated in the cavity to accelerate the charged particle beam in a radio-frequency accelerator such as a linear accelerator. In a typical linear accelerator structure, the RF power and power are provided by a vacuum tube amplifier operating at high voltage (tens of thousands of volts). The amplified RF power is transmitted from the RF vacuum official to the 2 cavity using a coaxial cable and the like. An oscillating electromagnetic field is formed in the cavity. A common linear accelerator such as a drift vacuum tube linear accelerator contains a series of drift vacuum tubes, which are arranged in the cavity to remove particles by an electric field Accelerate to form the desired particle beam. There are several applications or potential applications that require lighter and more transportable RF Cavity or linear accelerator. These applications include applications based on Earth orbit, decentralized on-demand medical isotope production, and high-power RF amplifiers. However, the necessary RF true 2 tubes, pressure power supply, power conditioning equipment and The weight and size of related components and other components constitute a considerable obstacle to the use of RF cavities or linear accelerators for these purposes. The solution to overcome the shortcomings of the RF S cavity mentioned above is shown in the United States No. 5,497,050, in the patent case map *, it is reproduced as _r4- This paper size applies to China National Standard (CNS) A4 (210 x 297 mm)

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裝 本申請案之圖1,顯示由壁(112)所界定之射頻空腔(no), ” 有導私性内表面(i丨4 )。壁(1 12 )分成上下兩圓筒部分 (120)及(122),且在該兩部分間裝設環形列(124)之固態功率 放大器模件(126)。各模件(126)皆具有輸入終端,連接至 低功率射頻激勵信號源。正性直流終端(140)連接至上部分 (120 )外表面,同樣負性直流終端(146 )經由四分之一波長扼 流圈接點連接至下部分(122)。用做放大器時,射頻空腔 (110)包含波導管(160)或同軸電纜輸出連接器,以將高功 率電磁波自空腔(11〇 )中導出。 訂Figure 1 containing this application shows the RF cavity (no) defined by the wall (112), "with a private inner surface (i 丨 4). The wall (1 12) is divided into two upper and lower cylindrical portions (120 ) And (122), and a solid state power amplifier module (126) of a ring array (124) is installed between the two parts. Each module (126) has an input terminal connected to a low-power RF excitation signal source. The negative DC terminal (140) is connected to the outer surface of the upper part (120), and the negative DC terminal (146) is also connected to the lower part (122) through a quarter-wave choke contact. When used as an amplifier, the RF cavity is (110) Contains a waveguide (160) or a coaxial cable output connector to guide high-power electromagnetic waves from the cavity (11).

在权作中,施加至放大器模件(126 )終端之射頻激勵輸入 功率,其頻率與空腔(11〇)之所要求諧振模式對應。在輸入 ;放勵之控制下,放大器模件(126 )感應一大射頻電流,其蓁 值在數千安培於壁(112)之内表面(114)處流動以建立所要 之電磁場幅度。由於集膚效應,此電流循空腔壁内表面流 動,深度僅達數微米。通過模件之直流電流流經壁(ιΐ2)絕 大部分。屬低阻抗之放大器才莫件(126)於高電流低電壓操 作,而沿空腔(11〇)轴所產生之粒子束則於高電壓低電流操 作,代表一高阻抗負載。故射頻空腔(11〇)此時即充任放大 為模件(126 )之功率併合器及匹配變壓器之功能。 模件(126)結構簡單,其所需包裝極少,緣空腔㈠1〇)之 壁(112)充任電晶體的散熱之用。系統全部冷却預算未增 加,而且省去構成電晶體射頻功率系統最重部分包=之^ 大部分。同時由於傳統式射頻線性加速器所需之真空管2 非加速器空腔(110)所必備,故亦免去地球執道中高; -5- 515225 A7 B7 五、發明説明(3 ) 備之故障問題。尤其空腔(110 )之電源供應排除傳統加速器 之射頻功率傳輸損失,從而達成更高效率。 美國第5,497,050號專利案中所發表之空腔用做線性加速 器,其效率固屬頗高,就有效操作而言尚欠缺放大器之結 構。第一,該空腔僅顯示空腔輸出口之波導管,却未述及 接受待放大射頻功率之輸入口。第二,就涉及諧振空腔之 射頻裝置而言,必須具頻率調諧功能,始可於所要頻率上 磷當操作。因此,該專利案中之以前射頻空腔既未說明亦 未顯示放大器所需調諧之方法。 發明概要 本發明之目的在於提供一個高功率射頻空腔,其易於轉 換成有效率之高功率放大器。 本發明之另一目的在於提供一個具分立輸入口及輸出口 之高功率放大器。 本發明之再一目的在於提供一個具有頻率調諧能力之高 功率放大器。 根據本發明,上述諸目的乃以提供主動射頻空腔放大器 而達成。此放大器包含一個界定兩獨立調諧式諧振空腔之 外殼。每一空腔大致呈圓筒形並含有導電性壁。第一空腔 亦即輸入空腔之導電結構將輸入空腔内之射頻場耦合至多 個功率電晶體之輸出引線。 輸入空腔含一柱塞組合,將低射頻功率自其源處耦合入 輸入S腔。輸出空腔亦含一柱塞組合,將放大後射頻功率 耦合至外部負載。各空腔之柱塞組合並用做調諧空腔至與 _- 6 -_ 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)In the right operation, the RF excitation input power applied to the terminal of the amplifier module (126) has a frequency corresponding to the required resonance mode of the cavity (110). Under the control of input and excitation, the amplifier module (126) induces a large RF current, and its threshold value flows at thousands of amps on the inner surface (114) of the wall (112) to establish the desired amplitude of the electromagnetic field. Due to the skin effect, this current flows through the inner surface of the cavity wall to a depth of only a few microns. The direct current through the module flows through most of the wall (ιΐ2). The amplifier with low impedance can only operate at high current and low voltage (126), and the particle beam generated along the axis of the cavity (110) operates at high voltage and low current, representing a high impedance load. Therefore, the RF cavity (11) is now functioning as a power combiner and matching transformer that is amplified into a module (126). The module (126) has a simple structure and requires very little packaging. The wall (112) of the edge cavity (10) is used for heat dissipation of the transistor. The overall cooling budget of the system has not been increased, and the most important part of the RF power system of the transistor is eliminated. At the same time, because the vacuum tube 2 required by the traditional RF linear accelerator is not necessary for the accelerator cavity (110), it also avoids the earth's high and medium-duty; -5- 515225 A7 B7 V. Description of the invention (3) The problem of failure. In particular, the power supply of the cavity (110) eliminates the RF power transmission loss of traditional accelerators, thereby achieving higher efficiency. The cavity published in U.S. Patent No. 5,497,050 is used as a linear accelerator, and its efficiency is relatively high, and the structure of the amplifier is still lacking in terms of effective operation. First, the cavity only shows the waveguide of the cavity output port, but it does not mention the input port that receives the RF power to be amplified. Second, for RF devices that involve resonant cavities, they must have a frequency tuning function that starts with phosphorus at the desired frequency. Therefore, the previous RF cavity in this patent neither describes nor shows the method of tuning required by the amplifier. SUMMARY OF THE INVENTION The object of the present invention is to provide a high-power RF cavity which can be easily converted into an efficient high-power amplifier. Another object of the present invention is to provide a high-power amplifier with discrete input and output ports. Another object of the present invention is to provide a high power amplifier having a frequency tuning capability. According to the present invention, the above objects are achieved by providing an active radio frequency cavity amplifier. This amplifier contains a housing that defines two independently tuned resonant cavities. Each cavity is generally cylindrical and contains a conductive wall. The first cavity, that is, the conductive structure of the input cavity, couples the RF field in the input cavity to the output leads of multiple power transistors. The input cavity contains a plunger assembly that couples low RF power from its source into the input S cavity. The output cavity also contains a plunger assembly that couples the amplified RF power to an external load. The plunger combination of each cavity is used to tune the cavity to _- 6 -_ This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)

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k 515225 A7 B7 五、發明説明(4 ) 所要工作頻率諧振之裝置。 本發明之主動射頻空腔放大器及屬相當輕裝置,採用低 壓直流電源供給射頻功率電晶體。輸入空腔之功用對多個 射頻功率電晶體而言為一功率分配器及匹配變壓器。輸出 空腔用做電晶體輸出之功率併合器及匹配變壓器。空腔壁 可充任散熱器,達到高度效率。 依據本發明之一端,主動射頻空腔放大器中電晶體之併 合乃一次完成,故無傳統式多級串聯方法併合大批裝置之 累積損失及相位差。此外,各空腔固有之損耗性遠低於傳 統方法所採用之帶狀線結構,故主動射頻空腔放大器之效 率與增益可達所使用各個電晶體之效率與增益。 依據本發明之另一端,主動射頻空腔放大器不需真空且 無複雜之電極,電路或窗口等,故各結構部分可用標準之 電腦數控機量產。且由於以空腔達成併合及阻抗匹配,故 主動射頻空腔放大器不需其它分立之無源電子組件,從而 增進其可靠性。 附圖之簡單說明 自下述配合附圖之詳細說明中,本發明之以上與其它目 的,特徵及優點當會一目了然,附圖為: 圖1為先前技藝射頻空腔之透視圖; 圖2為本發明主動射頻空腔放大器部分分離出之透視 圖; 圖3為圖2主動射頻空腔放大器所用一般電晶體包之頂視 圖; 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)k 515225 A7 B7 V. Description of the invention (4) The device whose resonance frequency is required to work. The active radio frequency cavity amplifier of the present invention is a relatively light device and uses a low-voltage DC power source to supply radio frequency power transistors. The function of the input cavity is a power splitter and matching transformer for multiple RF power transistors. The output cavity is used as a power combiner and matching transformer for transistor output. The cavity wall can be used as a radiator for high efficiency. According to one aspect of the present invention, the combination of the transistors in the active RF cavity amplifier is completed at one time, so there is no cumulative loss and phase difference of the traditional multi-stage series method combined with a large number of devices. In addition, the inherent loss of each cavity is much lower than the stripline structure used in traditional methods, so the efficiency and gain of the active RF cavity amplifier can reach the efficiency and gain of each transistor used. According to the other end of the present invention, the active RF cavity amplifier does not need a vacuum and has no complicated electrodes, circuits or windows, so each structural part can be mass-produced by a standard computer numerical control machine. And because the cavity is used to achieve merging and impedance matching, the active RF cavity amplifier does not need other discrete passive electronic components, thereby improving its reliability. Brief description of the drawings From the following detailed description in conjunction with the drawings, the above and other objects, features and advantages of the present invention will be apparent at a glance. The drawings are: Figure 1 is a perspective view of a prior art radio frequency cavity; Figure 2 is A perspective view of a part of the active RF cavity amplifier of the present invention; FIG. 3 is a top view of a general transistor package used in the active RF cavity amplifier of FIG. 2; The paper size is applicable to China National Standard (CNS) A4 (210 X 297 mm (Centimeter)

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部 圖4 A為圖2中沿線4 A - 4 A所見之主動射 分線路调; 頻空腔放大器之 腔放大器 圖4B為圖4A之放大部分圖,顯示主動射頰空 輸入/輸出空腔之導杆耦合至一電晶體:及 圖4 C為本發明上耦合裝置之側面圖。 較佳具體實例之詳細 本發明之較佳具體實例將參考附圖說明於下。下述說明 中凡熟知之功能或結構皆從略以免模糊焦點。 、請參考圖2 ,賦予參考號數(10)者為本發明之主動射頻 空腔放大器。此放大器包含兩個獨立調諧式諧振空腔 (12,14)。兩空腔由裝有多個電晶體(18)之中心板(16)結 合在一起。空腔(12)耦合至電晶體(1 8)之輸入線,故稱為 輸入空腔。同時,空腔(1 4)耦合至電晶體(18)之輸出線而 稱為輸出空腔。 如圖2所示,兩空腔(1 2,14)就其内維持諧振射頻場言 之大致對稱相同,但由於電晶體輸入輸出所需阻抗匹配互 異而要求不同匹配。為簡化起見’茲僅就輸入空腔(丨2 )之 結構詳細說明於後,蓋空腔(丨4)之結構與空腔(丨2 )之結構 類似。 第一空腔(12)由一大致圓筒狀外殼(20)所界定,含有一 開口端(2 2 ),閉合端(2 4 )及中心板(1 6)。空腔(1 2 )由圓 筒外殼(2 0 )内之第一圓筒壁(2 6 )限定。外殼(2 0 )所界定環 狀空腔(3 0 )構成之第二圓筒壁(2 8 )環繞筒壁(2 6 )做為射頻 扼流圈,以防止操作期間電晶體(丨8 )射頻輸入發生短路。 ______-8- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)Fig. 4A is the active line branching line seen along line 4A-4A in Fig. 2; cavity amplifier of the frequency cavity amplifier Fig. 4B is an enlarged part of Fig. 4A, showing the active cheek cavity input / output cavity The guide rod is coupled to a transistor: and FIG. 4C is a side view of the coupling device of the present invention. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A preferred embodiment of the present invention will be described below with reference to the drawings. All the well-known functions or structures in the following description are omitted to avoid blurring the focus. Please refer to FIG. 2, and the reference number (10) is the active RF cavity amplifier of the present invention. This amplifier contains two independently tuned resonant cavities (12, 14). The two cavities are joined together by a central plate (16) containing a plurality of transistors (18). The cavity (12) is coupled to the input line of the transistor (18), so it is called the input cavity. At the same time, the cavity (14) is coupled to the output line of the transistor (18) and is called the output cavity. As shown in Figure 2, the two cavities (12, 14) are roughly the same in terms of maintaining the resonant RF field, but different matching is required because of the impedance matching required for the input and output of the transistor. For the sake of simplicity, only the structure of the input cavity (丨 2) is described in detail later. The structure of the cover cavity (丨 4) is similar to the structure of the cavity (丨 2). The first cavity (12) is defined by a substantially cylindrical shell (20), and includes an open end (2 2), a closed end (2 4), and a center plate (16). The cavity (1 2) is defined by a first cylindrical wall (2 6) inside the cylindrical casing (20). The second cylindrical wall (2 8) formed by the annular cavity (30) defined by the casing (20) surrounds the cylindrical wall (2 6) as a radio frequency choke to prevent the transistor (丨 8) from operating during operation. The RF input is shorted. ______- 8- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)

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▲ 515225 A7 B7 五、發明説明(6 第二圓筒壁(2 8 )亦可採其它型式充任射頻扼流圈,諸如第 二圓筒壁(28)自筒壁(26)向外延伸而不向垂直彎曲者是。 筒壁(28)含一圓邊(32),以將外殼(20)之開口端(22)與 中心板(16)連接。圓筒外殼(20)係以導電材料,諸如銅, 銘或其它導電或超導材料製成。▲ 515225 A7 B7 V. Description of the invention (6 The second cylindrical wall (2 8) can also be used as another type of RF choke, such as the second cylindrical wall (28) extending outward from the cylindrical wall (26) without Those that are bent vertically are: The cylinder wall (28) contains a rounded edge (32) to connect the open end (22) of the casing (20) with the center plate (16). The cylindrical casing (20) is made of a conductive material such as Made of copper, metal or other conductive or superconducting material.

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外殼(2 0 )之閉合端(2 4 )界定一孔眼(3 4 )以容納柱塞組合 (36)。此柱塞組合(36)包括一導體圓盤(3 8),一介質圓盤 (40)及一導體柱塞(42),共同構成一耦合電容器。請參考 圖4A,其顯示柱塞組合(36)之線路方塊圖。柱塞組合(36) 另含由通道(44)及具匹配部分(48)之中心導體(46)所構成 之同軸部分(41)以輸入及/或輸出射頻功率,例如輸入主 動射頻放大器(1 0 )之低輸入功率及自放大器輸出之放大後 功率。亦即第一或輸入空腔(12)之結構(3 8, 40, 42, 46) 將外部來源之低射頻功率耦合入第一空腔(丨2 ),而第二或 輸出2腔(1 4)之相同結構則將放大後射頻功率幸禺合至空腔 外部之負載。 柱墓組合(3 6 )可在其孔眼(3 4 )内以人工或由螺紋移動至 所要諧振頻率之位置。就所要之操作頻率而言,柱塞組合 (36)在孔眼(3 4)中之移動量可約略為預知者。 中心板(16)呈大致圓形,包含上部環狀板(5〇)界定第一 空腔(12)之界限,並含下部環狀板(52)界定第二空腔(14) 之界限。該上下兩環狀板(5 0,5 2 )由一圓形結構(5 4 )將之 結合,其上配置多個呈環列之電晶體(1 。 圖3為諸電晶體(1 8)所選用一般電晶體包之頂視圖。下 -9 - 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 515225 A7 B7 五、發明説明(7 ) 表係依特殊電晶體型式辨識其引線(18 X,18y)及安裝突緣 (18F) ’其電性兼通用於輸入及輸出,並將電晶體(18)内 部產生之熱傳導至充任散熱器之空腔(12,14)之壁上〇 BJT共基極 BJT共射極 場效電晶體 18x 集極 集極 汲極 18y 射極 基極 閘極 18F 基極 射極 源極 在操作中,直流電力經導杆(62a)及導線(60a)施加至電 晶體引線(1 8 X, 1 8 y)(圖1及圖4 C )。由於直流電須加至每 一電晶體(1 8 ),故可在各電晶體(1 8 )汲極或集極電源供應 電路中採用諸如鐵氧墊圈等元件以確保穩定操作。 施加至各輸入線(1 8 X)之偏電壓可單獨調整,以克服所 用電晶體間不一致之問題。外殼(2 0 )及中心板(1 6 )係於直 流之地電位以保主動射頻空腔放大器(1 〇 )之安全操作。如 圖4C中所示,在導杆(62&)與各電晶體輸入線(18\)間乃 由含螺釘(64a) ’彈黃(66a)及絕緣部分(68a)之上部鎮合 裝置(55a)施加至導杆(62a)上之壓力而使之保持接觸。請 注意’該上部搞合裝置(55a)乃配置於每一電晶體(18) 者。必要時,亦可將導杆(62a,b)焊接至電晶體引線(18x, y)以保持接觸。 同時含與上部耦合裝置(5 5 b)相同結構之下部耦合裝置 (55b)以壓力加至導杆(62b)上。亦即下部耦合裝置(55b) 含有導杆(62b)以同軸耦合電容器而與各電晶體輸出線 -10- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 515225The closed end (2 4) of the housing (20) defines an eyelet (3 4) to accommodate the plunger assembly (36). The plunger combination (36) includes a conductor disc (38), a dielectric disc (40), and a conductor plunger (42), which together constitute a coupling capacitor. Please refer to FIG. 4A, which shows a block circuit diagram of the plunger assembly (36). The plunger combination (36) additionally includes a coaxial portion (41) composed of a channel (44) and a central conductor (46) with a matching portion (48) for inputting and / or outputting RF power, such as an active RF amplifier (1 0) low input power and amplified power output from the amplifier. That is, the structure of the first or input cavity (12) (3 8, 40, 42, 46) couples low RF power from an external source into the first cavity (丨 2), and the second or output 2 cavity (1 4) The same structure combines the amplified RF power to a load outside the cavity. The tomb assembly (3 6) can be moved to the desired resonance frequency position manually or by screwing in the eyelet (3 4). As far as the desired operating frequency is concerned, the amount of movement of the plunger assembly (36) in the eyelet (34) can be approximately predicted. The central plate (16) is substantially circular, and includes an upper annular plate (50) defining the boundary of the first cavity (12), and a lower annular plate (52) defining the boundary of the second cavity (14). The upper and lower annular plates (50, 5 2) are combined by a circular structure (54), and a plurality of transistors (1 in a row) are arranged thereon. Figure 3 shows the transistors (1 8). Top view of the selected general transistor package. Bottom -9-This paper size applies to China National Standard (CNS) A4 (210X 297 mm) 515225 A7 B7 V. Description of the invention (7) The watch is identified by the special transistor type Its leads (18 X, 18y) and mounting flanges (18F) are used for both input and output, and conduct heat generated inside the transistor (18) to the cavity (12, 14) serving as a radiator. 〇BJT common base BJT common emitter field effect transistor 18x collector collector drain 18y emitter base gate 18F base emitter source In operation, DC power is passed through the guide rod (62a) and the wire (60a) is applied to the transistor leads (1 8 X, 1 8 y) (Figures 1 and 4 C). Since direct current must be applied to each transistor (1 8), it can be drawn in each transistor (1 8) Components such as ferrite washers are used in the pole or collector power supply circuit to ensure stable operation. The bias voltage applied to each input line (1 8 X) can be adjusted independently In order to overcome the inconsistency between the transistors used. The casing (20) and the central plate (16) are connected to the ground potential of the DC to ensure the safe operation of the active RF cavity amplifier (10). As shown in Figure 4C It is shown that between the guide rod (62 &) and each transistor input line (18 \), a ballast-containing device (55a) containing screws (64a) 'elastic yellow (66a) and an insulating portion (68a) is applied to the guide The pressure on the rod (62a) keeps it in contact. Please note that 'the upper engaging device (55a) is arranged on each transistor (18). If necessary, the guide rods (62a, b) can also be welded To the transistor leads (18x, y) to maintain contact. At the same time, the lower coupling device (55b) with the same structure as the upper coupling device (5 5b) is pressurized to the guide rod (62b). That is, the lower coupling device ( 55b) Coaxial coupling capacitors with guide rods (62b) are connected to the output lines of each transistor-10- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) 515225

(18y)接觸;該電容器係由導杆(62b),介質套管(70b)及 外導( 7 2 b )通過輸出空腔(丨4 )基座處之間隙而形成,將 各私日曰把(1 8 )之輸出射頻功率經由導杆(6 2 b )耦合至輸出 二心(1 4 )自各廷晶體所併合之輸出射頻功率大於自來源 輸入t射頻功率,緣其已由每一電晶體(丨8)放大故也。請 /王思,下部耦合裝置(5 5 b )配於每一電晶體(1 8 )上。 易言之’在每一電晶體(18)處,結構(62a,70a,72a) 或輸入2腔(12)之同軸耦合電容器將輸入空腔(12)中之射 頻場耦合至電晶體輸入線(丨8 χ),而結構(6 2 b,7 〇 b,7 2 b ) 或輸出空腔(14)之同軸耦合電容器則將輸出空腔(14)中之 射頻場耦合至電晶體輸出線(18y)。在低頻應用中,可採 用集片式電容器以取代同軸耦合電容器。在所要之空腔模 式例如‘‘ TM01〇 ”模式中之射頻場乃自空腔(丨4)經空腔(丨4 ) 柱塞組合(36)之耦合電容器組件耦合至負載。此等組件包 括導電圓盤(3 8) ’介質圓盤(4〇)及導電圓筒柱塞(42)之底 表面。 如上所述,柱塞組合(3 6 )之功能為將柱塞(4 2 )伸入各空 腔不同冰度以调1皆各空腔之諧振頻率。深度可由人工或以 自動控制裝置加以改變。由柱塞組合(3 6 )之通道(4 4 )所構 成之同軸部分(4 1)及含匹配部分(4 8)之中心導體(46),即 將放大後之射頻功率經由一標準同軸連接器耦合出空腔。 在輸入的一邊,射頻功率之流向與輸出邊者相反。亦即· 射頻功率自柱塞組合(3 6 )上所裝之輸入連接器,經由同轴 通道及耦合電容器,並通過輸入空腔(12)基座處間隙‘‘,, § -11 - 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐)(18y) contact; the capacitor is formed by the guide rod (62b), the dielectric sleeve (70b) and the outer guide (7 2b) through the gap at the base of the output cavity (丨 4). The output RF power of (1 8) is coupled to the output core (1 4) through the guide rod (6 2 b). The output RF power combined from each crystal is greater than the input RF power from the source. The crystal (丨 8) is enlarged. Please / Wang Si, the lower coupling device (5 5 b) is equipped on each transistor (1 8). In other words, at each transistor (18), the structure (62a, 70a, 72a) or the coaxial coupling capacitor of the input 2 cavity (12) couples the RF field in the input cavity (12) to the transistor input line (丨 8 χ), and the coaxial coupling capacitor of the structure (6 2 b, 7 〇b, 7 2 b) or the output cavity (14) couples the RF field in the output cavity (14) to the transistor output line (18y). In low frequency applications, a chip capacitor can be used instead of a coaxial coupling capacitor. The RF field in the desired cavity mode, such as "TM01〇" mode, is coupled from the cavity (丨 4) to the load through the coupling capacitor component of the cavity (丨 4) plunger combination (36). These components include The conductive disc (38) 'the bottom surface of the dielectric disc (40) and the conductive cylinder plunger (42). As mentioned above, the function of the plunger assembly (36) is to extend the plunger (42). Enter the different ice degrees of each cavity to adjust the resonant frequency of each cavity. The depth can be changed manually or by an automatic control device. The coaxial portion (4) formed by the channel (4 4) of the plunger assembly (3 6) 1) and the center conductor (46) with the matching part (48), the amplified RF power is coupled out of the cavity through a standard coaxial connector. On the input side, the flow of RF power is opposite to that on the output side. That is, the input connector installed on the RF power from the plunger assembly (3 6) passes through the coaxial channel and the coupling capacitor and passes through the gap at the base of the input cavity (12) ", § -11-This paper Standards apply to China National Standard (CNS) A4 specifications (210X297 mm)

裝 訂Binding

k 515225 A7 B7 五、發明説明( :同軸耦合電苳器之組件(62a,70a,72a),而抵達電晶 月五(18)之輸入引線(18x)。輸出空腔(14)中之組件及輸入 2腔(12)中對應之組件,其結構及用途均屬類似。 n 主動射頻芝腔放大器中絕大多數之導電組件彼 二屬良好熱觸點’因此而成為熱單元體。可裝設有效塵 力氣冷之散熱片。亦可於中心板或導電性外殼中他處建冷 劑通道而輕易地完成液冷。 本發明固已參考一定之較佳具體實例加以展示並說明, 但對嫻於工藝技術者而言,會做各種形式及細節之改變而 未離所附申請專利範圍之本發明原理者。 1 - 12 - 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐)k 515225 A7 B7 V. Description of the invention (: The components (62a, 70a, 72a) of the coaxial coupling electric appliance, and the input lead (18x) of the electric crystal moon (18). The components in the output cavity (14) And the corresponding components in the input 2 cavity (12), their structures and uses are similar. N Most of the conductive components in the active radio frequency cavity amplifier are good thermal contacts, so they become thermal unit bodies. Can be installed It is provided with an effective dust-cooled heat sink. It is also possible to easily complete liquid cooling by establishing a refrigerant channel in the center plate or in the conductive shell. The present invention has been shown and described with reference to certain specific examples. Those skilled in the arts will make various changes in form and details without departing from the principles of the invention of the attached patent. 1-12-This paper size applies to China National Standard (CNS) A4 (210X 297) %)

Claims (1)

515225 8 8 8 8 A B c D 六、申請專利範圍 1. 一種主動射頻空腔放大器,其包含: 界定輸入與輸出空腔之外殼; 安裝於外殼上之多個電晶體,每一電晶體皆含有一輸 入引線及一輸出引線; 第一射頻功率耦合裝置,配置於外殼内鄰近輸入空腔 處,將射頻功率自其源耦合入輸入空腔以產生射頻場; 第一導電組合,具有多個導體,各經佈置與電晶體之 各輸入引線接觸以將輸入空腔中之射頻場耦合至電晶體 之輸入引線; 第二導電組合,具有多個導體,各經佈置與電晶體之 各輸出引線接觸,將輸出空腔中之射頻場耦合至電晶體 之輸出引線以放大來自源之射頻功率;及 第二射頻功率耦合裝置,配置於外殼内鄰近輸出空腔 處,將放大後之射頻功率自輸出空腔耦合至負載。 2. 如申請專利範圍第1項之主動射頻空腔放大器,其中外 殼呈圓筒狀並界定圍繞輸入空腔之環形空腔及圍繞輸出 空腔之環形空腔。 3. 如申請專利範圍第2項之主動射頻空腔放大器,其中環 形空腔經配置做為射頻扼流圈,以防止放大之射頻功率 發生短路。 4. 如申請專利範圍第1項之主動射頻空腔放大器,其中外 殼係由導電材料製成。 5. 如申請專利範圍第1項之主動射頻空腔放大器,其中第 一及第二雨射頻功率耦合裝置各含一柱塞組合,組合中 -13- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 515225 A8 B8 C8 D8 六、申請專利範圍 .配有一柱塞於外殼内移動。 6. 如申請專利範圍第5項之主動射頻空腔放大器,其中第 一射頻功率耦合裝置之柱塞組合乃配置以供調諧輸入空 腔之諧振頻率,而第二射頻功率耦合裝置之柱塞則供調 諧輸出空腔之諧振頻率。 7. 如申請專利範圍第5項之主動射頻空腔放大器,其中柱 塞組合包含: 一耦合電容器,其含具有第一及第二兩端之導電圓筒 柱塞,至少一個介質圓盤與第二端結合;及 一同軸部分,其含有一中心導體及配置於圓筒柱塞通 道中之匹配部分。 8. —種放大射頻功率之方法,其包括以下步驟: 將射頻功率耦合至含界定輸入空腔及輸出空腔之外殼 的主動射頻空腔放大器,以於輸入空腔内產生射頻場; 且於輸入及輸出空腔鄰近處裝設多個電晶體,每一電晶 皆具有一輸入引線及一輸出引線; 調諧輸入空腔之諧振頻率及輸出空腔之諧振頻率; 將輸入空腔中之射頻場耦合至電晶體之輸入引線; 將輸出空腔中之射頻場耦合至電晶體之輸出引線,以 放大來自源之射頻功率;以及 將放大後之射頻功率自輸出空腔耦合出。 9. 一種射頻功率放大器,其包含: 將射頻功率耦合至含界定輸入空腔及輸出空腔之外殼 的主動射頻空腔放大器之器具;該耦合器具於輸入空腔 -14- 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐)515225 8 8 8 8 AB c D 6. Scope of patent application 1. An active RF cavity amplifier, comprising: a housing defining input and output cavities; a plurality of transistors mounted on the housing, each of which contains An input lead and an output lead; a first radio frequency power coupling device disposed in the housing adjacent to the input cavity to couple radio frequency power from its source into the input cavity to generate a radio frequency field; a first conductive combination having a plurality of conductors , Each arranged to contact each input lead of the transistor to couple the RF field in the input cavity to the input lead of the transistor; a second conductive combination having a plurality of conductors, each arranged to contact each output lead of the transistor , Coupling the RF field in the output cavity to the output lead of the transistor to amplify the RF power from the source; and a second RF power coupling device, which is arranged near the output cavity in the housing and outputs the amplified RF power from the output The cavity is coupled to a load. 2. For example, the active RF cavity amplifier of the scope of patent application, wherein the outer shell is cylindrical and defines a circular cavity surrounding the input cavity and a circular cavity surrounding the output cavity. 3. For example, the active RF cavity amplifier of the patent application No. 2 in which the annular cavity is configured as an RF choke coil to prevent short circuit of the amplified RF power. 4. For the active RF cavity amplifier of item 1 of the patent application, wherein the outer shell is made of a conductive material. 5. For example, the active RF cavity amplifier of the first patent application range, where the first and second rain RF power coupling devices each contain a plunger combination, the combination is -13- This paper size applies to China National Standard (CNS) A4 Specifications (210 X 297 mm) 515225 A8 B8 C8 D8 6. Scope of patent application. Equipped with a plunger to move inside the casing. 6. For the active RF cavity amplifier of item 5 of the patent application, wherein the plunger combination of the first RF power coupling device is configured to tune the resonant frequency of the input cavity, and the plunger of the second RF power coupling device is Resonant frequency for tuning output cavity. 7. The active RF cavity amplifier according to item 5 of the patent application, wherein the plunger combination includes: a coupling capacitor including a conductive cylinder plunger having first and second ends, at least one dielectric disc and the first The two ends are combined; and a coaxial portion containing a central conductor and a matching portion arranged in the cylindrical plunger channel. 8. A method of amplifying radio frequency power, comprising the steps of: coupling radio frequency power to an active radio frequency cavity amplifier including a housing defining an input cavity and an output cavity to generate a radio frequency field in the input cavity; and Multiple transistors are installed near the input and output cavity, each transistor has an input lead and an output lead; the resonant frequency of the input cavity and the resonant frequency of the output cavity are tuned; the radio frequency in the input cavity Field coupling to the input lead of the transistor; coupling the RF field in the output cavity to the output lead of the transistor to amplify the RF power from the source; and coupling the amplified RF power from the output cavity. 9. A radio frequency power amplifier comprising: an appliance for coupling radio frequency power to an active radio frequency cavity amplifier including a housing defining an input cavity and an output cavity; the coupling device is in the input cavity-14- This paper is for China National Standard (CNS) A4 specification (210X297 mm) 裝 訂Binding 515225 A8 B8 C8 D8 六、申請專利範圍 •内產生射頻場,於輸入空腔及輸出空腔附近裝設多個電 晶體,每一電晶體皆具有輸入引線及輸出引線;及 將輸入空腔中之射頻場耦合至電晶體之輸入引線及將 輸出空腔中之射頻場耦合至電晶體輸出引線之器具。 10. 如申請專利範圍第9項之射頻功率放大器,其另含: 調諧輸入空腔諧振頻率及輸出空腔諧振頻率之器具; 以及 將放大後射頻功率自輸出空腔耦合出之器具。 11. 一種射頻功率放大器,其包含: 將射頻功率耦合至含有界定輸入空腔及輸出空腔之外 殼的主動射頻空腔放大器具;該耦合器具於輸入空腔内 產生射頻場,於輸入空腔及輸出空腔附近裝設多個電晶 體’每一電晶體皆含有一輸入引線及一輸出引線;及 調諧輸入空腔諧振頻率及輸出空腔諧振頻率之器具。 12. 如申請專利範圍第1 1項之射頻功率放大器,其另含: 將輸入空腔中之射頻場耦合至電晶體之輸入引線及將 輸出空腔中之射頻場耦合至電晶體輸出引線之器具;以 及 將放大後之射頻功率自輸出空腔耦合出之器具。 -15- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)515225 A8 B8 C8 D8 VI. Patent application scope • Generate RF field, install multiple transistors near the input cavity and output cavity, each transistor has input leads and output leads; and put the input cavity into the input cavity A radio frequency field is coupled to the input lead of the transistor and a device for coupling the radio frequency field in the output cavity to the transistor output lead. 10. If the RF power amplifier of item 9 of the patent application scope includes: an apparatus for tuning the input cavity resonance frequency and an output cavity resonance frequency; and an apparatus for coupling the amplified RF power from the output cavity. 11. A radio frequency power amplifier, comprising: an active radio frequency cavity amplifier that couples radio frequency power to a housing that defines an input cavity and an output cavity; the coupling device generates a radio frequency field in the input cavity and an input cavity And a plurality of transistors are installed near the output cavity; each transistor includes an input lead and an output lead; and a device for tuning the input cavity resonant frequency and the output cavity resonant frequency. 12. For example, the RF power amplifier in the scope of patent application No. 11 further includes: coupling the RF field in the input cavity to the input lead of the transistor and coupling the RF field in the output cavity to the output lead of the transistor Appliances; and appliances that couple amplified RF power from the output cavity. -15- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
TW90129652A 2000-12-13 2001-11-30 Active radio frequency cavity amplifier TW515225B (en)

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