JPH0369206B2 - - Google Patents
Info
- Publication number
- JPH0369206B2 JPH0369206B2 JP58083332A JP8333283A JPH0369206B2 JP H0369206 B2 JPH0369206 B2 JP H0369206B2 JP 58083332 A JP58083332 A JP 58083332A JP 8333283 A JP8333283 A JP 8333283A JP H0369206 B2 JPH0369206 B2 JP H0369206B2
- Authority
- JP
- Japan
- Prior art keywords
- loop
- signal
- correlation
- reference signal
- slc
- 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 - Lifetime
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q3/00—Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system
- H01Q3/26—Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture
- H01Q3/2605—Array of radiating elements provided with a feedback control over the element weights, e.g. adaptive arrays
- H01Q3/2611—Means for null steering; Adaptive interference nulling
Landscapes
- Radar Systems Or Details Thereof (AREA)
- Noise Elimination (AREA)
- Variable-Direction Aerials And Aerial Arrays (AREA)
Description
【発明の詳細な説明】
本発明はサイドローブ・キヤンセラ(以下SLC
と略記する)の相関ループ利得の改良に係るもの
である。[Detailed Description of the Invention] The present invention provides a sidelobe canceller (hereinafter referred to as SLC).
This relates to the improvement of the correlation loop gain of (abbreviated as).
従来のSLCは第1図のような構成であつた。図
においてu,xはそれぞれ主アンテナ及び補助ア
ンテナからの入力信号の搬送波をそれぞれ周波数
w1,w2(w1>w2)の中間周波数(IF)に変換し
た信号をあらわす(以下、u,xをそれぞれ主信
号、参照信号と呼ぶ。)。1は減算器、2,5はミ
キサ、3は中心周波数w1−w2の狭帯域通過形フ
イルタ、4は利得gの増幅器である。この構成に
おいて減算器1からミキサ2、ミキサ5を通つて
再び減算器1に至るループが存在する。これを相
関ループと呼ぶ。 A conventional SLC had a configuration as shown in Figure 1. In the figure, u and x are the carrier waves of the input signals from the main antenna and the auxiliary antenna, respectively.
It represents a signal converted to an intermediate frequency (IF) of w 1 and w 2 (w 1 >w 2 ) (hereinafter, u and x are called the main signal and reference signal, respectively). 1 is a subtracter, 2 and 5 are mixers, 3 is a narrow band pass filter with a center frequency of w 1 -w 2 , and 4 is an amplifier with a gain of g. In this configuration, there is a loop from subtracter 1 through mixer 2 and mixer 5 to subtracter 1 again. This is called a correlation loop.
次にこの装置の動作について説明する。補助ア
ンテナは無指向性であり、その利得は主アンテナ
のサイドローブの利得程度にとられるため、主ア
ンテナのメインローブより入射する電波について
は信号uの電力が信号xの電力よりも大きくな
る。これに対して主アンテナのサイドローブより
入射する電波に対しては、参照信号xの電力の方
が主信号uのそれよりも大きくなる。本装置はこ
れを利用し、主信号u中の成分で参照信号xと相
関を持つものを、参照信号xに対して制御荷重信
号wを乗じた信号yとして推定し、主信号uから
この推定信号yを引き去つた信号zを出力信号と
する構造を有し、主アンテナのメインローブから
入射する電波の影響のみを残すものである。SLC
からの出力信号zはミキサ2に入力されてフイー
ドバツクされる。ミキサ2の出力信号をv,vに
対して狭帯域フイルタ3、増幅器4を通過した後
の信号をwとするとwは中心周波数w1−w2の信
号となる。ミキサ5は信号wと補助アンテナ入力
信号xを掛け合わせ、信号yを出力する。以上の
過程を数式化すると、次のようになる。(信号成
分はすべて複素数で表現するものとする。)
まず、主アンテナ入力信号uと出力信号zとの
関係は
z=u−y (1)
である。次に狭帯域フイルタ3を時定数τ0の一次
遅れフイルタとすれば、増幅器4の出力信号であ
る制御荷重信号wに関して、次の微分方程式が成
り立つ。 Next, the operation of this device will be explained. Since the auxiliary antenna is omnidirectional and its gain is about the same as the gain of the side lobe of the main antenna, the power of the signal u is greater than the power of the signal x for radio waves incident from the main lobe of the main antenna. On the other hand, for radio waves incident from the side lobes of the main antenna, the power of the reference signal x is greater than that of the main signal u. This device uses this to estimate components in the main signal u that have a correlation with the reference signal x as a signal y obtained by multiplying the reference signal x by the control weight signal w, and estimates this from the main signal u. It has a structure in which the signal z obtained by subtracting the signal y is used as an output signal, and only the influence of the radio waves incident from the main lobe of the main antenna remains. SLC
The output signal z from the mixer 2 is input to the mixer 2 and fed back. If the output signals of the mixer 2 are v and v, and the signal after passing through the narrow band filter 3 and the amplifier 4 is w, then w becomes a signal with a center frequency w 1 -w 2 . Mixer 5 multiplies signal w and auxiliary antenna input signal x and outputs signal y. The above process can be expressed mathematically as follows. (All signal components are expressed as complex numbers.) First, the relationship between the main antenna input signal u and the output signal z is z=u−y (1). Next, if the narrowband filter 3 is a first-order lag filter with a time constant τ 0 , then the following differential equation holds true with respect to the control load signal w, which is the output signal of the amplifier 4.
τ0dw/dt+w=gzx* (2)
但しx*はxの共役複素数をあらわす。また、
ミキサ5に関しては、
y=wx (3)
となる。ここで(1),(2),(3)を用いると、
τ0dw/dt+(1+g|x|2)w=gux* (4)
となる。これは制御荷重信号wに関する一階の線
形微分方程式である。式(4)において|x|2の値
及びux*の包絡信号成分の変化がτ0に比較してゆ
るやかでほぼ一定値である場合には、式(4)は次の
ような解を持つ。 τ 0 dw/dt+w=gzx * (2) where x * represents the conjugate complex number of x. Also,
Regarding mixer 5, y=wx (3). If (1), (2), and (3) are used here, τ 0 dw/dt+(1+g|x| 2 )w=gux * (4). This is a first-order linear differential equation for the control load signal w. In Equation (4), if the value of |x| 2 and the envelope signal component of ux * change slowly and are almost constant compared to τ 0 , Equation (4) has the following solution. .
但し式(5)において、w0はt=0のときのwの
初期値であり、また、τ0,αは
T0=τ0/1+g|x|2 (6)
α=gux*/1+g|x|2 (7)
という値である。式(5)において制御荷重信号wの
値はtが十分大きくなれば値αに近づいてゆく。
第2図は制御荷重信号wの値の絶対値|w|が値
|α|に収束してゆく様子を示すものである。こ
の時の時定数はT0である。一方、出力信号zは、
図より
z=u−wx (8)
であるため、サイドローブ・キヤンセラによる信
号抑圧比(CR)を
CR=<(u/z)2>=<(u/u−wx)2> (9)
と定義すれば(但し<>は時間平均を示す。)、t
が十分大きくなつた場合には式(9)のwの代わりに
式(7)のαを代入して、
CR=(1+g|x|2)2 (10)
となる。式(10)より明らかなように信号抑圧比CR
は、参照信号電力|x|2の値に依存して参照信
号電力|x|2が大きくなれば大きくなる。この
関係を第3図に示す。 However, in formula (5), w 0 is the initial value of w when t=0, and τ 0 and α are T 0 =τ 0 /1+g|x| 2 (6) α=gux * /1+g The value is |x| 2 (7). In equation (5), the value of the control load signal w approaches the value α when t becomes sufficiently large.
FIG. 2 shows how the absolute value |w| of the value of the control load signal w converges to the value |α|. The time constant at this time is T 0 . On the other hand, the output signal z is
From the figure, z=u−wx (8), so the signal suppression ratio (CR) due to sidelobe canceller is CR=<(u/z) 2 >=<(u/u−wx) 2 > (9) If defined as (where <> indicates the time average), then t
When becomes sufficiently large, α in equation (7) is substituted for w in equation (9), resulting in CR=(1+g|x| 2 ) 2 (10). As is clear from equation (10), the signal suppression ratio CR
depends on the value of reference signal power |x| 2 and increases as reference signal power |x| 2 increases. This relationship is shown in FIG.
このように制御荷重電圧wの収束時定数T0及
びSLCによる信号抑圧比CRは増幅器のゲインg
と参照信号電力|x|2との積g|x|2に大きく
影響される。特に参照信号電力|x|2が小さい
値の時は増幅器4の利得gを大きくとらないと、
制御荷重電圧wの収束時定数T0が大きくなつて
しまう。ところが利得gを大きくとると参照信号
電力|x|2が大きい時にはループ利得が大きす
ぎて、回路の非線形要素のために発振が生じてし
まう。従来のSLCにおいては以上のような欠点が
あつた。 In this way, the convergence time constant T 0 of the control load voltage w and the signal suppression ratio CR due to SLC are determined by the amplifier gain g
and the reference signal power |x| 2 , which is the product g|x| 2 . Especially when the reference signal power |x| 2 is a small value, the gain g of the amplifier 4 must be set large.
The convergence time constant T 0 of the control load voltage w becomes large. However, when the gain g is large, the loop gain becomes too large when the reference signal power |x| 2 is large, and oscillation occurs due to the nonlinear elements of the circuit. Conventional SLC has the above-mentioned drawbacks.
本発明はこの欠点を克服するため、SLC回路に
改良を試みたものである。本発明のSLC回路を第
4図に示す。図においてもとのSLC回路に対して
追加されたものについて説明すると、6,7は異
なる減衰度a1,a2(1>a1>a2)を持つ減衰器、
8は比較器10の信号によつて制御される選択ス
イツチ、9はミキサである。ミキサ9の出力信号
は参照信号電力|x|2である。比較器10は|
x|2をあらかじめ設定された値p1,p2(p1<p2)
と比較し、スイツチ8において
|x|2<p1のときは端子S1を、
p1|x|2<p2のときは端子S2を、
p2|x|2のときは端子S3を、
それぞれ選択するものとする。このようにすると
増幅器4からスイツチ8の出力端に至るまでの等
価ゲインは
|x|2<p1のときg
p1|x|2<p2のときa1g
p2|x|2のときa2g
となり、参照信号の電力|x|2に応じて相関ル
ープのゲインが制御される。また、減衰度a1,a2
の設定法として
a1=p1/p2 (11)
a2=p1/pmax (12)
(但し、pmaxは参照信号電力|x|2の許容最
大値を示す)となるようにしておくと、相関ルー
プのゲインは第5図に示すようになる。このよう
に減衰度を決めておけばSLCの相関ループが発振
しなくなるような参照信号電力|x|2の許容範
囲が広がる。 The present invention attempts to improve the SLC circuit in order to overcome this drawback. The SLC circuit of the present invention is shown in FIG. To explain what has been added to the original SLC circuit in the figure, 6 and 7 are attenuators with different attenuation degrees a 1 and a 2 (1>a 1 >a 2 );
8 is a selection switch controlled by the signal from the comparator 10, and 9 is a mixer. The output signal of mixer 9 has reference signal power |x| 2 . The comparator 10 is |
x| 2 to preset values p 1 , p 2 (p 1 < p 2 )
In comparison, in switch 8, when |x| 2 < p 1 , terminal S 1 is connected, when p 1 | x | 2 < p 2 , terminal S 2 is connected, and when p 2 | 3 shall be selected respectively. In this way, the equivalent gain from amplifier 4 to the output terminal of switch 8 is: g p 1 when |x| 2 < p 1 ; a 1 when |x| 2 < p 2 ; g p 1 when |x| 2 a 2 g , and the gain of the correlation loop is controlled according to the power |x| 2 of the reference signal. Also, the attenuation degree a 1 , a 2
As a setting method, a 1 = p 1 / p 2 (11) a 2 = p 1 / pmax (12) (where pmax indicates the maximum allowable value of reference signal power |x| 2 ) Then, the gain of the correlation loop becomes as shown in FIG. By determining the degree of attenuation in this manner, the allowable range of reference signal power |x| 2 that prevents the SLC correlation loop from oscillating can be widened.
また、第6図には、この場合の相関ループにお
ける制御電圧wの収束する時定数T0の参照信号
電力|x|2との関係について示す。これによる
と時定数T0はτ0/(1+gp1)以上の値となる。
次に第7図にSLCの信号抑圧度CRと、参照信号
電力|x|2との関係を示す。図より信号抑圧度
CRは(1+gp1)2以下の値となる。このように、
たとえば|x|2<p1のとき|x|2がp1に近い
程、SLCの特性としては望ましいものになるが、
逆にp1よりも大きく離れる時にはSLCとしての特
性は悪化してゆく。 Furthermore, FIG. 6 shows the relationship between the time constant T 0 at which the control voltage w converges in the correlation loop in this case and the reference signal power |x| 2 . According to this, the time constant T 0 has a value greater than or equal to τ 0 /(1+gp 1 ).
Next, FIG. 7 shows the relationship between the SLC signal suppression degree CR and the reference signal power |x| 2 . From the figure, signal suppression degree
CR has a value of (1 + gp 1 ) 2 or less. in this way,
For example, when |x| 2 < p 1 , the closer |x| 2 is to p 1 , the more desirable the SLC characteristics are.
Conversely, when the distance is greater than p 1 , the characteristics as an SLC deteriorate.
以上のように本発明に係るSLCでは参照信号電
力|x|2の値によつて相関ループの等価ゲイン
を制御することができるため、参照信号電力|x
|2が低い場合にでもある程度抑圧度を維持させ
つつ、かつ相関ループが発振しないような参照信
号電力|x|2の許容範囲を広げることができる。 As described above, in the SLC according to the present invention, the equivalent gain of the correlation loop can be controlled by the value of the reference signal power |x| 2 .
Even when | 2 is low, the degree of suppression can be maintained to some extent, and the allowable range of reference signal power |x| 2 can be widened so that the correlation loop does not oscillate.
第1図は従来のサイドローブ・キヤンセラ
(SLC)の構成ブロツク図、第2図は第1図の
SLCにおける制御荷重電圧の絶対値が時間と伴に
所望の荷重値に収束してゆく様子を説明した図、
第3図は第1図のSLCにおける参照信号電力と信
号抑圧度との関係を示した説明図、第4図は本発
明の改良をほどこしたSLCの構成ブロツク図、第
5図は本発明のSLCの参照信号電力と相関ループ
のゲインとの関係を示す説明図、第6図は本発明
のSLCの参照信号電力と相関ループ収束の時定数
との関係を示す説明図、第7図は本発明のSLCに
おける参照信号電力と信号抑圧度との関係を示す
説明図である。
1……減算器、2,5,9……ミキサ、3……
狭帯域フイルタ、4……増幅器、6,7……減衰
器、8……スイツチ、10……比較器。なお、図
中同一あるいは相当部分には同一符号を付して示
してある。
Figure 1 is a block diagram of a conventional sidelobe canceller (SLC), and Figure 2 is a block diagram of a conventional sidelobe canceller (SLC).
A diagram explaining how the absolute value of the control load voltage in SLC converges to the desired load value over time,
FIG. 3 is an explanatory diagram showing the relationship between the reference signal power and the degree of signal suppression in the SLC of FIG. An explanatory diagram showing the relationship between the reference signal power of the SLC and the gain of the correlation loop, FIG. 6 is an explanatory diagram showing the relationship between the reference signal power of the SLC of the present invention and the time constant of correlation loop convergence, and FIG. FIG. 3 is an explanatory diagram showing the relationship between reference signal power and signal suppression degree in SLC of the invention. 1...Subtractor, 2, 5, 9...Mixer, 3...
Narrow band filter, 4... amplifier, 6, 7... attenuator, 8... switch, 10... comparator. It should be noted that the same or corresponding parts in the figures are indicated by the same reference numerals.
Claims (1)
波等の不要電波の受信々号を抑圧するための相関
ループを有し、別に補助アンテナより受信した不
要電波に対する参照信号との相関成分を抽出する
事により、主アンテナからの受信々号中の不要電
波成分を推定し、これを主アンテナの受信々号か
ら引き去る事によつて、不要電波成分を抑圧する
サイドローブ・キヤンセラにおいて相関ループ中
のループ利得を得るための増幅器の後段に複数端
子を持つ切換えスイツチと、この切換えスイツチ
の各端子に接続して異なる減衰度特性を有する減
衰器を並列に接続した回路をループ中に有し、更
に、これとは別に補助アンテナから受信した参照
信号の平均電力に比例した電圧を出力する回路を
有し、この電圧に応じて、相関ループ中の上記切
換えスイツチを制御することにより、相関ループ
のループ利得の調整を可能とした事を特徴とする
サイドローブ・キヤンセラ。1. It has a correlation loop for suppressing the received signals of unnecessary radio waves such as interference waves that enter from the side lobe of the main antenna, and also by extracting the correlation component between the reference signal and the unnecessary radio waves received from the auxiliary antenna. , the loop gain in the correlation loop in a sidelobe canceller that suppresses unnecessary radio wave components by estimating the unnecessary radio wave components in the received signals from the main antenna and subtracting them from the received signals from the main antenna. In the loop, there is a changeover switch with multiple terminals after the amplifier to obtain the same, and a circuit in which attenuators having different attenuation characteristics are connected to each terminal of this changeover switch in parallel. Separately, it has a circuit that outputs a voltage proportional to the average power of the reference signal received from the auxiliary antenna, and by controlling the changeover switch in the correlation loop according to this voltage, the loop gain of the correlation loop can be adjusted. A side lobe canceller that is adjustable.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58083332A JPS59208901A (en) | 1983-05-12 | 1983-05-12 | Side lobe cancelier |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58083332A JPS59208901A (en) | 1983-05-12 | 1983-05-12 | Side lobe cancelier |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59208901A JPS59208901A (en) | 1984-11-27 |
| JPH0369206B2 true JPH0369206B2 (en) | 1991-10-31 |
Family
ID=13799471
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58083332A Granted JPS59208901A (en) | 1983-05-12 | 1983-05-12 | Side lobe cancelier |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59208901A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4250522B2 (en) * | 2003-12-25 | 2009-04-08 | 株式会社東芝 | Antenna device |
-
1983
- 1983-05-12 JP JP58083332A patent/JPS59208901A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59208901A (en) | 1984-11-27 |
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