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JPS585616B2 - Heterodyne relay method - Google Patents
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JPS585616B2 - Heterodyne relay method - Google Patents

Heterodyne relay method

Info

Publication number
JPS585616B2
JPS585616B2 JP52152624A JP15262477A JPS585616B2 JP S585616 B2 JPS585616 B2 JP S585616B2 JP 52152624 A JP52152624 A JP 52152624A JP 15262477 A JP15262477 A JP 15262477A JP S585616 B2 JPS585616 B2 JP S585616B2
Authority
JP
Japan
Prior art keywords
distortion
output
signal
relay
amplifier
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP52152624A
Other languages
Japanese (ja)
Other versions
JPS5484413A (en
Inventor
岡本栄晴
大山徹
野島俊雄
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NTT Inc
Original Assignee
Nippon Telegraph and Telephone Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP52152624A priority Critical patent/JPS585616B2/en
Publication of JPS5484413A publication Critical patent/JPS5484413A/en
Publication of JPS585616B2 publication Critical patent/JPS585616B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B7/00Radio transmission systems, i.e. using radiation field
    • H04B7/14Relay systems
    • H04B7/15Active relay systems
    • H04B7/155Ground-based stations

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
  • Cable Transmission Systems, Equalization Of Radio And Reduction Of Echo (AREA)
  • Radio Relay Systems (AREA)

Description

【発明の詳細な説明】 この発明は2個以上の中継装置を縦続接続した多中継ヘ
テロダイン中継方式に関し,特に各中継装置の送信用電
力増幅器で発生する非線形歪雑音を減少せしめる中継方
式に係わる。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a multi-relay heterodyne relay system in which two or more relay devices are connected in cascade, and particularly to a relay system that reduces nonlinear distortion noise generated in the transmission power amplifier of each relay device.

無線通信方式において従来から使用されているヘテロダ
イン中継方式に使用される中継装置は第1図に示すよう
に受信アンテナ11で受信された信号はダウンコンバー
タ12で搬送波信号源13からの搬送波帯の信号により
中間周波帯に周波数変換され.中間周波帯増幅器14で
増幅された後,再びアップコンバータ15で信号源13
からの信号により搬送波帯に周波数変換され進行波管増
幅器などの送信用電力増幅器16で高電力レベルに増幅
され送信用アンテナ17を通じて次の中継装置へ送信さ
れる。
As shown in FIG. 1, a relay device used in a heterodyne relay system conventionally used in wireless communication systems converts a signal received by a receiving antenna 11 into a carrier band signal from a carrier signal source 13 in a down converter 12. The frequency is converted to an intermediate frequency band by After being amplified by the intermediate frequency band amplifier 14, the signal source 13 is again transferred to the up converter 15.
The signal is frequency-converted into a carrier wave band, amplified to a high power level by a transmission power amplifier 16 such as a traveling wave tube amplifier, and transmitted to the next relay device via a transmission antenna 17.

従来のヘテロダイン中継方式においては各中継装置の構
成は同一とされている。
In the conventional heterodyne relay system, each relay device has the same configuration.

このため各中継装置の送信用電力増幅器16で発生する
歪雑音がほぼ同一振幅,同位相となり中継系全体の歪雑
音は各中継装置の送信用電力増幅器で発生する歪雑音の
電圧相加となる。
Therefore, the distortion noise generated in the transmission power amplifier 16 of each relay device has almost the same amplitude and the same phase, and the distortion noise of the entire relay system is the voltage addition of the distortion noise generated in the transmission power amplifier 16 of each relay device. .

従って中継装置の数をNとすると,受信端局では一つの
中継装置で発生する歪雑音電力よりも20logn〔d
B〕だけ増加した歪雑音が受信される欠点があった。
Therefore, if the number of relay devices is N, then at the receiving terminal station, the distortion noise power generated by one relay device is 20logn[d
There was a drawback that distortion noise increased by B] was received.

この発明はこの欠点を解決するため中継伝送系を構成す
る中継装置としてアツプコンバータ出力中の上側帯波を
とるものと,下側帯波をとるものとをそれぞれ少くとも
1つずつは使用し.例えばこれ等を交互に使用する構成
にすることにより中継装置の歪雑音相加の低減を実現す
ると同時に.中継系全体としての補償残留歪を抑圧する
ために非線形歪補償装置を受信端局などの中継装置に付
加する。
In order to solve this drawback, the present invention uses at least one relay device that takes the upper side band of the output of the up converter and one that takes the lower side band as the relay device constituting the relay transmission system. For example, by creating a configuration in which these are used alternately, it is possible to reduce the addition of distortion noise in the repeater, and at the same time. A nonlinear distortion compensator is added to a relay device such as a receiving terminal station in order to suppress compensation residual distortion in the entire relay system.

第2図はこの発明によるヘテロダイン中継方式の一例を
示し,第1図と対応する部分には同一符号を付けてあり
送信入力端子18からの信号は搬送波信号源19からの
搬送波信号によりアップコンバータ21において上側帯
波の搬送波帯に周波数変換され、送信用電力増幅器22
にて増幅されて送信用アンテナ23を通じて中継装置の
受信アンテナ11へ送出される。
FIG. 2 shows an example of a heterodyne relay system according to the present invention, in which parts corresponding to those in FIG. The frequency is converted to the carrier wave band of the upper side band in the transmission power amplifier 22.
The signal is amplified and sent to the receiving antenna 11 of the relay device via the transmitting antenna 23.

中継装置のアップコンバータ15は下側帯波を用いて搬
送波帯の周波数に変換される。
The upconverter 15 of the repeater uses the lower side band to convert the frequency to the carrier band.

またこの例では中間周波増幅器14とアップコンバータ
15との間に中間周波帯非線形歪補償装置24が直列に
挿入される。
Further, in this example, an intermediate frequency band nonlinear distortion compensator 24 is inserted in series between the intermediate frequency amplifier 14 and the up converter 15.

先ず中間周波帯非線形歪補償装置24が使用されてなく
.中間周波増幅器14の出力はアップコンバータ15へ
直接供給されるものとして説明する。
First, the intermediate frequency band nonlinear distortion compensator 24 is not used. The description will be made assuming that the output of intermediate frequency amplifier 14 is directly supplied to upconverter 15.

いま送信用電力増幅器16,22の各入力電圧をx(t
)、出力電圧をy(t)とすれば送信用電力増幅器の入
出力特性は基本周波数に関する出力信号に着目して y(t)=a1x(t)−a3x3(t)(1)のよう
に近似できる。
Now, each input voltage of the transmission power amplifiers 16 and 22 is expressed as x(t
), and the output voltage is y(t), the input/output characteristics of the transmitting power amplifier can be expressed as y(t) = a1x(t) - a3x3(t) (1), focusing on the output signal related to the fundamental frequency. Can be approximated.

ここにtは時間を表わす変数、a1は実定数、a3は複
素定数である。
Here, t is a variable representing time, a1 is a real constant, and a3 is a complex constant.

この場合3乗項の係数に位相項を有する複素数a3をと
ることにより入出力振幅非線形と位相非線形(AM−P
M変換)とが同時に表現できる。
In this case, input/output amplitude nonlinearity and phase nonlinearity (AM-P
M transformation) can be expressed simultaneously.

送信端のアップコンバータ21が上側帯波を使用し.端
子18からの中間周波信号の角周波数をωo,搬送波信
号源19の搬送波角周波数をωcとすると送信用電力増
幅器22の入力信号x1(t)はx1(t)=acos
(ωc+ωo)t(2)とおける。
The upconverter 21 at the transmitting end uses the upper sideband. If the angular frequency of the intermediate frequency signal from the terminal 18 is ωo, and the carrier angular frequency of the carrier signal source 19 is ωc, then the input signal x1(t) of the transmission power amplifier 22 is x1(t)=acos
(ωc+ωo)t(2).

ここにaは定数である。送信用電力増幅器22の出力電
圧y1(t)は基本周波数成分に関して(1)式及び(
2)式から ただしψ”=arg(a3) となる。
Here a is a constant. The output voltage y1(t) of the transmission power amplifier 22 is expressed by equation (1) and (
From equation 2), ψ”=arg(a3).

(3)式において右辺第2項が3次歪成分である。In equation (3), the second term on the right side is the third-order distortion component.

この出力信号はつぎの中継装置に送出され,受信ダウン
コンバータ12の出力電圧y11(t)はとなる。
This output signal is sent to the next relay device, and the output voltage y11(t) of the receiving down converter 12 becomes.

Aは伝搬損失などを表わす定数である。y11(t)は
中間周波帯増幅器14で送信端局での電カレベルと同一
のレベルまで増幅された後,アップコンバータ15によ
り再び搬送波帯に周波数変換されるが,この周波数変換
において使用する側帯波によりアップコンバータ15の
出力信号x2(t)はそれぞれ次のように3次歪の位相
項が異なったものになる。
A is a constant representing propagation loss and the like. After y11(t) is amplified by the intermediate frequency band amplifier 14 to the same level as the power level at the transmitting terminal station, it is frequency-converted again to the carrier band by the up-converter 15, but the sideband wave used in this frequency conversion is Therefore, the output signals x2(t) of the up-converter 15 have different phase terms of third-order distortion as follows.

即ち上側帯波の場合は下側帯波の場合は となる。In other words, in the case of the upper sideband, and in the case of the lower sideband, becomes.

(5)式(6)式の右辺第2項で分母にa1が在るのは
第1項の信号成分の振幅が(1)式の送信信号x1(t
)の振幅に増幅器14で利得調整したためである。
(5) The presence of a1 in the denominator in the second term on the right side of equation (6) means that the amplitude of the signal component in the first term is the transmission signal x1(t
This is because the gain was adjusted by the amplifier 14 to the amplitude of ).

これ等x2u(t)、x2L(t)が送信用電力増幅器
16で増幅されると新たに3次歪雑音が付加され.それ
ぞれの場合の出力信号y2u(t)、y2L(t)は(
5)式(6)式をそれぞれ(1)式に代入してa9の項
はa<<1なので無視し,又基本周波数成分のみに着目
していることから角周波数3(ωc+ωo)と3(ωc
−ωo)の項を消去すると(7)、(8)式が得られる
When these x2u(t) and x2L(t) are amplified by the transmission power amplifier 16, third-order distortion noise is newly added. The output signals y2u(t) and y2L(t) in each case are (
5) Substitute equation (6) into equation (1) and ignore the term a9 since a<<1, and since we are focusing only on the fundamental frequency component, the angular frequencies 3(ωc+ωo) and 3( ωc
-ωo), equations (7) and (8) are obtained.

ここでは前述のように増幅器16において歪成分の入力
により発生する歪成分はa<<1なる条件を考慮して最
小項として省略した。
Here, as mentioned above, the distortion component generated by the input of the distortion component in the amplifier 16 is omitted as the minimum term in consideration of the condition that a<<1.

式(8)について以下に第3図のベクトル図を使用して
説明する。
Equation (8) will be explained below using the vector diagram shown in FIG.

図中のベクトル25は送信用電力増幅器16の出力にお
ける主信号(歪のない信号)ベクトル26は送信用電力
増幅器16においてベクトル25の主信号出力に付随し
て発生する3次歪成分である。
A vector 25 in the figure is a main signal (undistorted signal) at the output of the transmission power amplifier 16, and a vector 26 is a third-order distortion component generated in the transmission power amplifier 16 along with the main signal output of the vector 25.

まず進行波管増幅器の如きマイクロ波帯増幅器の出力が
第3図のようなベクトル図で表現できることを説明する
First, it will be explained that the output of a microwave band amplifier such as a traveling wave tube amplifier can be expressed by a vector diagram as shown in FIG.

よく知られているようにマイクロ波帯増幅器は入出力の
飽和特性の他に入出力信号間の位相が入力レベルに依存
して変化するAM−PM変換と呼ばれる位相非線形を示
す。
As is well known, microwave band amplifiers exhibit not only input/output saturation characteristics but also phase nonlinearity called AM-PM conversion in which the phase between input and output signals changes depending on the input level.

このような振輻と位相非線形を示す増幅器の入出力特性
は(1)式の如き複素係数のべき級数で近似できること
が知られている。
It is known that the input/output characteristics of an amplifier exhibiting such vibration and phase nonlinearity can be approximated by a power series of complex coefficients as shown in equation (1).

いま単一周波数の入力信号x(t)= acosωc1
を考えれば基本周波数に着目した出力y(t)は(3)
式を得た如く次式で与えられる。
Now single frequency input signal x(t) = acosωc1
Considering this, the output y(t) focusing on the fundamental frequency is (3)
As we obtained the formula, it is given by the following formula.

この式は増幅器の出力信号が入力に線形比例した出力a
1acos(ωc+ωo)tとそれに対して入力の大き
さaと無関係に特定の位相差180°−ψを有する3次
歪成分に分解できることを意味している。
This formula shows that the output signal of the amplifier is the output a which is linearly proportional to the input.
1 acos(ωc+ωo)t, which means that it can be decomposed into third-order distortion components having a specific phase difference of 180°-ψ, regardless of the input magnitude a.

この状態を原理的に表示すると第7図の如きベクトル図
が得られる。
If this state is expressed in principle, a vector diagram as shown in FIG. 7 can be obtained.

第7図で(H)は位相遅れを示し, F(y)は出力y
(t)の軌跡を示す。
In Figure 7, (H) shows the phase delay, and F(y) is the output y
(t) shows the trajectory.

険40は線形出力成分.41は3次歪出力成分、そして
42は40と41のベクトル和で与えられる出力y(t
)を示す。
40 is the linear output component. 41 is the cubic distortion output component, and 42 is the output y(t
) is shown.

図においては入力信号振幅aが2倍の場合を例にしてそ
の軌跡を示すように出力y(t)は入力レベルaの増加
と共に線形出力40から徐々に位相が遅れ,また振幅も
非線形に変化しはじめる。
In the figure, the output y(t) gradually lags in phase from the linear output 40 as the input level a increases, and the amplitude also changes non-linearly, as shown in the figure, taking as an example the case where the input signal amplitude a is doubled. begins to

即ちこの位相の変化する非線形がAM−PM変換であり
.振幅変化が飽和特性を代表とする増幅器の振幅非線形
に一致するものである。
In other words, this nonlinear phase change is AM-PM conversion. The amplitude change corresponds to the amplitude nonlinearity of the amplifier, which is represented by saturation characteristics.

ただし第7図の場合には3次項までしか考慮していない
ので振幅の飽和特性がよく表われていない。
However, in the case of FIG. 7, only the third-order term is taken into consideration, so the amplitude saturation characteristics are not clearly expressed.

このようにして振幅と位相という二つの面で非線形を有
する増幅器の入出力特性を第7図の如きベクトル図で直
観的に表現できる。
In this way, the input/output characteristics of an amplifier that is nonlinear in two aspects, amplitude and phase, can be intuitively expressed using a vector diagram as shown in FIG.

そこで第3図にもどって各増幅器の出力ベクトルの関係
を説明する。
Therefore, returning to FIG. 3, the relationship between the output vectors of each amplifier will be explained.

送信用電力増幅器16による送信用電力増幅において発
生する歪ベクトル26に対して,送信用電力増幅器22
が発生する3次歪成分は,前述のように(8)式の〔
〕内第2項で示される。
For the distortion vector 26 generated in the transmission power amplification by the transmission power amplifier 16, the transmission power amplifier 22
As mentioned above, the third-order distortion component generated by
] is shown in the second term.

従ってこの送信用電力増幅器22が発生する3次歪成分
は、第3図においてベクトル27で表わされる。
Therefore, the third-order distortion component generated by the transmission power amplifier 22 is represented by a vector 27 in FIG.

このようにして第3図において送信用電力増幅器16に
よる歪ベクトル26に対して送信用電力増幅器22が発
生する3次歪成分がベクトル的に加算され.そのベクト
ル和はベクトル28となる。
In this way, in FIG. 3, the third-order distortion component generated by the transmission power amplifier 22 is vectorially added to the distortion vector 26 caused by the transmission power amplifier 16. The vector sum becomes vector 28.

得られるベクトル28は(8)式の最終誘導式で明らで
表わされる。
The obtained vector 28 is clearly expressed by the final induction equation (8).

つまり周波数変換器21及び15における通過側帯波が
同一の場合送信用電力増幅器22及び16で発生する3
次歪は同一振幅.同位相となるため送信用電力増幅器1
6の出力における3次歪は(7)式で表わされるように
ベクトル26の2倍相当,つまり2つの増幅器22及び
16の歪が電圧相加されたものになる。
In other words, if the passing sidebands in the frequency converters 21 and 15 are the same, the 3
The next distortion has the same amplitude. Transmission power amplifier 1 to be in the same phase
The third-order distortion at the output of the amplifier 6 is equivalent to twice the vector 26, as expressed by equation (7), that is, the distortions of the two amplifiers 22 and 16 are added in voltage.

一方周波数変換器21及び15における通過側帯波が異
なる場合電力増幅器16の出力における3次歪は互に共
役なベクトル26及び27の和のベクトル28になる。
On the other hand, when the passing sidebands in the frequency converters 21 and 15 are different, the third-order distortion at the output of the power amplifier 16 becomes a vector 28 which is the sum of the mutually conjugate vectors 26 and 27.

(8)式における3次歪成分クトル28であらわされる
It is represented by the third-order distortion component vector 28 in equation (8).

即ちこのような構成をとることにより何ら付加回路を施
すことなく1個の増幅器から発生する歪成分をcosψ
倍に低減できることがわかる。
In other words, by adopting such a configuration, the distortion components generated from one amplifier can be reduced to cosψ without any additional circuitry.
It can be seen that it can be reduced by a factor of two.

進行波管などの位相非線形の大きい送信用電力増幅器で
は例えばψは80°〜85°の値をとるため3次歪成分
が15〜20dB抑圧されることになる。
In a transmitting power amplifier with large phase nonlinearity such as a traveling wave tube, ψ takes a value of 80° to 85°, so the third-order distortion component is suppressed by 15 to 20 dB.

つぎに第2図において中間周波帯非線形歪補償装置24
の作用について説明する。
Next, in FIG. 2, the intermediate frequency band nonlinear distortion compensator 24
The effect of this will be explained.

この中間周波帯非線形歪補償装置24は補償残の歪成分
(ベクトル28)を打ち消すような歪成分 する機能を有するものでこの結果送信用電力増幅器16
の出力信号中の3次歪成分は更に低減される。
This intermediate frequency band nonlinear distortion compensator 24 has a function of generating a distortion component that cancels out the compensation residual distortion component (vector 28), and as a result, the transmission power amplifier 16
The third-order distortion component in the output signal of is further reduced.

挿入する歪成分は非直線素子を使用して発生させ.スペ
クトルアナライザで監視しながら歪が打ち消されるよう
なレベルで挿入すればよい。
The distortion component to be inserted is generated using a nonlinear element. It is sufficient to insert the signal at a level that cancels out the distortion while monitoring it with a spectrum analyzer.

第9図はこのような非線形歪補償回路の具体例を示すも
のであり.この第9図において51は入力端子,52は
出力端子.53はダイオードの逆並列回路等で構成され
たx3素子.54は可変抵抗器,55は可変移送器であ
る。
Figure 9 shows a specific example of such a nonlinear distortion compensation circuit. In FIG. 9, 51 is an input terminal, and 52 is an output terminal. 53 is a x3 element composed of an anti-parallel circuit of diodes, etc. 54 is a variable resistor, and 55 is a variable transfer device.

このような回路を用いx3素子53で発生した歪成分を
信号に付加して補償残の歪成分を打ち消すようにする。
Using such a circuit, the distortion component generated by the x3 element 53 is added to the signal to cancel out the distortion component remaining after compensation.

なお非線形歪補償装置24は各中継装置の周波数変換器
に使用する側帯波の違いを利用した3次歪補償の残留歪
成分を打ち消すために使用されるもので付加する場所は
第2図に示したような中間周波帯にのみ限定されるもの
ではない。
The nonlinear distortion compensator 24 is used to cancel the residual distortion component of third-order distortion compensation that utilizes the difference in sideband waves used in the frequency converter of each repeater, and the location where it is added is shown in Figure 2. The present invention is not limited to only intermediate frequency bands such as the above.

即ち非線形歪補償装置24の使用法としては第4図に示
すように送信端局装置30及び各中継装置31に非線形
歪補償装置を具備する場合.第5図に示すように最後の
受信端局で総合の残留歪成分を打ち消すように受信端局
装置32に非線形歪補償装置を設け.送信端局装置33
及び中継装置34には非線形歪補償装置は設けない場合
.或は第6図に示すように全中継系での歪が減少するよ
うに中継系の任意の中継装置に非線形歪補償装置を設け
たものを使用する場合.など各種の例が考えられる。
That is, the method of using the nonlinear distortion compensator 24 is as shown in FIG. As shown in FIG. 5, a nonlinear distortion compensator is provided in the receiving end station device 32 so as to cancel out the total residual distortion component at the last receiving end station. Transmitting terminal device 33
and when the relay device 34 is not provided with a nonlinear distortion compensator. Alternatively, as shown in Fig. 6, a nonlinear distortion compensation device is used in any repeater in the repeater system so that distortion in all repeaters is reduced. Various examples can be considered.

多段中継において隣接する中継装置のアツプコンバータ
として上側帯波利用のものと.下側帯波利用のものとを
交互に設ける場合のみならず,特に順序を定めずに途中
継装置のほぼ半数が上側帯波利用のアップコンバータと
し,残りのほぼ半数が下側帯波利用のものでもよい。
One that uses the upper sideband as an up-converter for adjacent repeaters in multi-stage repeaters. This is not only the case when the relay devices are installed alternately with those that use the lower side band, but also the case where almost half of the relay devices are up converters that use the upper side band and the remaining half are those that use the lower side band, without specifying a particular order. good.

また全中継装置の中で少くとも1つが上側帯波利用のア
ツプコンバータであり.残りの少くとも1つが下側帯波
利用のアップコンバータであっても歪を減少させる効果
は或る程度はある。
In addition, at least one of all relay devices is an up converter that uses the upper sideband. Even if at least one of the remaining upconverters is an upconverter that utilizes the lower sideband, it is still effective in reducing distortion to some extent.

以上説明したようにこの発明を用いればヘテロダイン中
継方式における送信用電力増幅器の歪雑音を低減するこ
とが可能となり.しかも各中継器で発生する歪雑音の相
加を緩和せしめる効果があるので低歪多中継通信系を構
成できる利点がある。
As explained above, by using this invention, it is possible to reduce the distortion noise of the transmitting power amplifier in the heterodyne relay system. Moreover, since it has the effect of alleviating the addition of distortion noise generated in each repeater, there is an advantage that a low-distortion multi-relay communication system can be constructed.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は従来のヘテロダイン中継装置の構成例を示すブ
ロック図.第2図はこの発明による中継方式の一構成例
を示すブロック図,第3図は周波数変換器の通過側帯波
の違いと歪補償の原理を示すベクトル図.第4図乃至第
7図はそれぞれこの発明の実施による中継系の構成例を
示すブロック図,第7図は非線特性を示すベクトル図.
第8図は非線形歪補償装置の回路構成を示す図である。 11・・・・・・受信アンテナ、12・・・・・・周波
数変換器(ダウンコンバータ),13・・・・・・搬送
波信号源.14・・・・・・中間周波帯増幅器,15,
21・・・・・・周波数変換器(アツプコンバータ)、
16,22・・・・・・送信用電力増幅器、17・・・
・・・送信アンテナ、24・・・・・・非線形歪補償装
置.18・・・・・・送信入力端,31・・・・・・非
線形歪補償装置を具備した中継装置,34・・・・・・
非線形歪補償装置を具備しない中継装置。
Figure 1 is a block diagram showing an example of the configuration of a conventional heterodyne repeater. Fig. 2 is a block diagram showing an example of the configuration of a relay system according to the present invention, and Fig. 3 is a vector diagram showing the difference in sidebands passed by frequency converters and the principle of distortion compensation. 4 to 7 are block diagrams showing configuration examples of relay systems according to the present invention, and FIG. 7 is a vector diagram showing nonlinear characteristics.
FIG. 8 is a diagram showing the circuit configuration of the nonlinear distortion compensator. 11... Receiving antenna, 12... Frequency converter (down converter), 13... Carrier wave signal source. 14... intermediate frequency band amplifier, 15,
21... Frequency converter (up converter),
16, 22... Transmission power amplifier, 17...
...Transmission antenna, 24...Nonlinear distortion compensator. 18...Transmission input end, 31...Relay device equipped with a nonlinear distortion compensation device, 34...
A relay device that does not include a nonlinear distortion compensation device.

Claims (1)

【特許請求の範囲】[Claims] 1 2個以上の中継装置を縦続的に接続したヘテロダイ
ン多中継伝送系において,上記中継装置の少くとも1つ
は上側帯波を使用する周波数変換器を具備し.他の中継
装置の少くとも1つに上記上側帯波を使用する周波数変
換器と同数の下側帯波を使用する周波数変換器を具備し
.かつ少くとも1つの中継装置又は受信端局にのみ上記
上側帯波及び上記下側帯波を使用する周波数変換器の出
力信号中に存在する残留3次歪波を打ち消すような信号
を発生し,この信号を上記残留3次歪波に付加する非直
線歪補償装置を設けることを特徴とするヘテロダイン中
継方式。
1. In a heterodyne multi-relay transmission system in which two or more repeaters are connected in series, at least one of the repeaters is equipped with a frequency converter that uses an upper sideband. At least one of the other relay devices is equipped with the same number of frequency converters that use lower sideband waves as the frequency converters that use upper sideband waves. and generates a signal that cancels residual third-order distortion waves present in the output signal of a frequency converter that uses the upper side band wave and the lower side band wave only in at least one repeater or receiving terminal station, and A heterodyne relay system comprising a nonlinear distortion compensator that adds a signal to the residual third-order distorted wave.
JP52152624A 1977-12-19 1977-12-19 Heterodyne relay method Expired JPS585616B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP52152624A JPS585616B2 (en) 1977-12-19 1977-12-19 Heterodyne relay method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP52152624A JPS585616B2 (en) 1977-12-19 1977-12-19 Heterodyne relay method

Publications (2)

Publication Number Publication Date
JPS5484413A JPS5484413A (en) 1979-07-05
JPS585616B2 true JPS585616B2 (en) 1983-02-01

Family

ID=15544439

Family Applications (1)

Application Number Title Priority Date Filing Date
JP52152624A Expired JPS585616B2 (en) 1977-12-19 1977-12-19 Heterodyne relay method

Country Status (1)

Country Link
JP (1) JPS585616B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62137927A (en) * 1985-12-11 1987-06-20 Fujitsu Ltd Cross modulation compensating device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5628059A (en) * 1979-08-15 1981-03-19 Hamana Jidosha Kogyo Kk Mounting device for side gate board of truck

Also Published As

Publication number Publication date
JPS5484413A (en) 1979-07-05

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