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JPH0642655B2 - Asynchronous spread spectrum communication method - Google Patents
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JPH0642655B2 - Asynchronous spread spectrum communication method - Google Patents

Asynchronous spread spectrum communication method

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Publication number
JPH0642655B2
JPH0642655B2 JP2003343A JP334390A JPH0642655B2 JP H0642655 B2 JPH0642655 B2 JP H0642655B2 JP 2003343 A JP2003343 A JP 2003343A JP 334390 A JP334390 A JP 334390A JP H0642655 B2 JPH0642655 B2 JP H0642655B2
Authority
JP
Japan
Prior art keywords
spread spectrum
frequency
code
signal
transmitted
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
Application number
JP2003343A
Other languages
Japanese (ja)
Other versions
JPH03209940A (en
Inventor
忠夫 笠井
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.)
NEW TEKU KK
NYUUTEKU KK
Original Assignee
NEW TEKU KK
NYUUTEKU KK
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Filing date
Publication date
Application filed by NEW TEKU KK, NYUUTEKU KK filed Critical NEW TEKU KK
Priority to JP2003343A priority Critical patent/JPH0642655B2/en
Publication of JPH03209940A publication Critical patent/JPH03209940A/en
Publication of JPH0642655B2 publication Critical patent/JPH0642655B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は無線伝送方法の一形態であるスペクトラム拡散
通信方法に係り、特にスペクトラム拡散通信の実行にお
いて最も困難な部分とされる同期捕捉、同期維持の為の
回路を全く必要としない、完全非同期なスペクトラム拡
散通信方法に関するものである。
Description: TECHNICAL FIELD The present invention relates to a spread spectrum communication method which is one form of a wireless transmission method, and in particular, synchronization acquisition and synchronization, which are considered to be the most difficult part in execution of spread spectrum communication. The present invention relates to a completely asynchronous spread spectrum communication method which requires no maintenance circuit.

[従来の技術] スペクトラム拡散(Spread Spectrum )通信方法は拡散
の方法により、直接拡散( Direct Sequence)方法と、
周波数ホッピング(Frequency Hopping)方法に大別さ
れ、各々固有の特徴を有するが、共通点としては従来の
一般的通信方法に比して妨害や干渉に強く、且つ秘匿性
に優れた性質を利用して、主に軍事通信分野に於いて広
く普及発達した通信方法である。手段の差異は有るが基
本構成としては、送信電力の分布幅を、PN符号を用い
て従来の通信方法とは比較にならない程に拡大し、狭帯
域で評価した場合の平均電力密度を著しく低下せしめ
る。故に、従来の通信方法で受信した場合、単に雑音レ
ベルが増加した程度の影響しか与えない。該信号を受
信、復調する為には、送信時のPN符号と完全に等し
く、且つ、位相も一致したPN符号を用いて逆拡散を行
ない、伝送すべき情報を含んだコヒーレント(連続し
た)信号を収斂した後、復調を行なう。この過程に於い
て、受信装置の基準信号は、受信されるPN符号に対し
て、符号パターンの位置及び符号速度の両面で正確に同
期していなければならない。この為の同期技術、すなわ
ち同期捕捉技術及び同期維持技術こそは、スペクトラム
拡散通信の有効性を支配するものであり、最も多くの開
発力が投下され、各種の同期方法が考案されている。
[Prior Art] A spread spectrum communication method is a direct sequence method according to a spread method.
They are roughly classified into frequency hopping methods and each have their own unique characteristics, but the common point is that they are more resistant to interference and interference and superior in confidentiality than the conventional general communication methods. It is a communication method that has been widely spread and developed mainly in the field of military communication. Although there are differences in the means, the basic configuration is that the distribution width of the transmission power is expanded to the extent that it cannot be compared with the conventional communication method using the PN code, and the average power density when evaluated in a narrow band is significantly reduced. Excuse me. Therefore, when the signal is received by the conventional communication method, the noise level is merely increased. In order to receive and demodulate the signal, a coherent (continuous) signal including information to be transmitted is obtained by despreading using a PN code that is exactly the same as the PN code at the time of transmission and has the same phase. Is converged and then demodulated. In this process, the reference signal of the receiving device must be accurately synchronized with the received PN code in terms of both the position of the code pattern and the code rate. The synchronization technology for this purpose, that is, the synchronization acquisition technology and the synchronization maintenance technology, dominates the effectiveness of spread spectrum communication, and the greatest amount of development power has been invested, and various synchronization methods have been devised.

[発明が解決しようとする問題点] 上記のごとく、スペクトラム拡散通信技術における同期
技術は最大の研究課題であり、同期技術無くしてはスペ
クトラム拡散通信は成立し得ない。
[Problems to be Solved by the Invention] As described above, the synchronization technology in the spread spectrum communication technology is the greatest research subject, and spread spectrum communication cannot be established without the synchronization technology.

更に、同期の為の回路は主として一連のアルゴリズムに
従って動作する論理回路の依り構成されるのが通例であ
り、装置の主要部分を占有する為、装置の小型化、低価
格化には、現在の技術では困難を伴う。
Furthermore, the circuit for synchronization is usually composed mainly of a logic circuit that operates according to a series of algorithms, and since it occupies the main part of the device, it is necessary to reduce the size and cost of the device at present. Technology is difficult.

[問題点を解決する手段] 本発明は、同期の簡略化を行なう為の開発に端を発し、
結果として、スペクトラム拡散通信が有する特徴の内、
処理利得(プロセスゲイン)効果は減少するものの、基
本的特徴である、他通信への低干渉、低妨害性、および
通常の通信方法に対する強力な秘匿性を有し、且つ、全
く同期回路を要しない完全非同期なスペクトラム拡散通
信方法を提供し得るものである。
[Means for Solving Problems] The present invention originates from development for simplifying synchronization,
As a result, among the features of spread spectrum communication,
Although the processing gain effect is reduced, it has the basic features of low interference with other communications, low interference, and strong concealment with respect to ordinary communication methods, and requires no synchronization circuit. It is possible to provide a completely asynchronous spread spectrum communication method.

当該方法は、第一の周波数帯における伝送すべき情報を
含まないスペクトラム拡散信号と、第一の周波数帯及び
その高調波周波数関係に有る周波数帯以外の任意の第二
の周波数帯における、第一のスペクトラム拡散信号と特
定の相間関を有し、且つ伝送すべき情報を含んだ第二の
スペクトラム拡散信号の二波を、非能動素子を用いて合
成し、同時に送出する送信装置と、当該二波のスペクト
ラム拡散信号を同時に受信し、乗算器で掛け合わせた
後、その出力を更に二乗する事に依り発生する複数の周
波数成分の内、第一及び第二のスペクトラム拡散信号周
波数の中間に位置する計算上の周波数の二倍の周波数を
抽出し(この過程でコヒーレント信号が得られる)、こ
れを復調し得る機能を有する受信装置を備えてなる、完
全非同期なスペクトラム拡散通信方法である。
The method includes a spread spectrum signal that does not include information to be transmitted in a first frequency band and a first frequency band in any second frequency band other than a frequency band having a harmonic frequency relationship with the first frequency band. A second spread spectrum signal that has a specific correlation with the spread spectrum signal and that contains information to be transmitted, is synthesized by using an inactive element, and is transmitted at the same time; Wave spread spectrum signal is received at the same time, after being multiplied by the multiplier, the output is further squared, and among the multiple frequency components generated, it is located in the middle of the first and second spread spectrum signal frequencies. A completely asynchronous spectrum equipped with a receiver capable of extracting twice the calculated frequency (coherent signal is obtained in the process) and demodulating this. It is a non-diffusion communication method.

[作用] 本方法の動作原理を数式を用いて説明する。[Operation] The operation principle of this method will be described using mathematical expressions.

送信装置に於いて、第一のスペクトラム拡散信号f1を得
る手段として、まず第一の搬送波 fc1(fc1 =Ec・cos ω
1tただし、Ecは搬送波の振幅、ωは搬送波の角周波
数)を、PN符号 fp (fp=Ep・cos ptただし、EpはPN
符号の振幅、pはPN符号の瞬時角周波数)で振幅変調
すると、出力e1は以下で示される。
In the transmitter, as a means for obtaining the first spread spectrum signal f 1 , first the first carrier wave f c1 (f c1 = Ec · cos ω
1 t However, Ec is the amplitude of the carrier, ω 1 is the angular frequency of the carrier, and PN code fp (fp = Ep · cos pt where Ep is PN
When the amplitude of the code, p is the instantaneous angular frequency of the PN code) is amplitude-modulated, the output e 1 is shown below.

e1=(Ec+Ep・cos pt)・cos ω1t =Ec・cos ω1t+Ep・cos pt・cos ω1t =Ec・cos ω1t+(Ep/2)・cos(ω1+p)t+ (Ep/2)・cos(ω1-p)t…… 式の第2項の成分を帯域通過フィルターで取り出し、
これを第一のスペクトラム拡散信号f1とする。すなわ
ち、 f1=E・cos (ω1+p)t ただしE=Ep/2 …… 第二のスペクトラム拡散信号f2を得る手段として、第二
の搬送波 fc2(fc2=Ec・cos(ω2+Δf)tただし、Ecは搬送
波の振幅で、fc1の振幅と同等、ωは搬送波の角周波
数、Δf は伝達すべき情報の瞬時角周波数)を、前出の
PN符号fpで振幅変調すると、出力e2は以下で示され
る。
e 1 = (Ec + Ep ・ cos pt) ・ cos ω 1 t = Ec ・ cos ω 1 t + Ep ・ cos pt ・ cos ω 1 t = Ec ・ cos ω 1 t + (Ep / 2) ・ cos (ω 1 + p) t + (Ep / 2) ・ cos (ω 1 -p) t …… Extracts the second term component of the equation with a bandpass filter,
This is the first spread spectrum signal f 1 . That is, f 1 = E ・ cos (ω 1 + p) t, where E = Ep / 2 …… As a means to obtain the second spread spectrum signal f 2 , the second carrier f c2 (f c2 = Ec ・ cos ( ω 2 + Δf) t where Ec is the amplitude of the carrier and is equal to the amplitude of f c1 , ω 2 is the angular frequency of the carrier, Δf is the instantaneous angular frequency of the information to be transmitted), and the PN code fp With amplitude modulation, the output e 2 is shown below.

e2=(Ec+Ep・cos pt)・cos(ω2+Δf)t =Ec・cos(ω2+Δf)t +Ep・cos pt・cos(ω2+Δf)t =Ec・cos(ω2+Δf)t+(Ep/2)cos(ω2+Δf+p)t+ (Ep/2)cos(ω2+Δf)-p)t …… 式の第3項の成分を帯域通過フィルターで取り出し、
これを第二のスペクトラム拡散信号f2とする。すなわ
ち、 f2=E・cos((ω2+Δf)-p)t ただしE=Ep/2 …… 上記手段に依り得られたf1及びf2は、各々独立して所定
の電力まで増幅した後、非能動素子で構成される電力合
成器に依り合成された後、適切な空中線より空間に放射
される。ここで、特に注意しなければならない事は、電
力合成器には能動素子を用いてはならない事である。な
ぜならば、完全な直線性を有する能動素子は実際上存在
せず、何らかの非直線領域を持つため、この非直線領域
をf1及びf2が同時に通過すると、後出の受信装置におい
て説明するところのコヒーレント成分が生成される可能
性があり、本方法の特徴の1つである秘匿性が少なから
ず損なわれるからである。
e 2 = (Ec + Ep ・ cos pt) ・ cos (ω 2 + Δf) t = Ec ・ cos (ω 2 + Δf) t + Ep ・ cos pt ・ cos (ω 2 + Δf) t = Ec ・ cos ( ω 2 + Δf) t + (Ep / 2) cos (ω 2 + Δf + p) t + (Ep / 2) cos (ω 2 + Δf) -p) t …… The band-pass filter for the third term component of the equation Take out with
This is the second spread spectrum signal f 2 . That is, f 2 = E ・ cos ((ω 2 + Δf) -p) t, where E = Ep / 2 ...... f 1 and f 2 obtained by the above means are independently amplified to a predetermined power. Then, after being combined by a power combiner composed of non-active elements, it is radiated into space from an appropriate antenna. Here, it should be noted that the power combiner should not use active elements. Because there is practically no active element having perfect linearity and has some non-linear area, if f 1 and f 2 pass through this non-linear area at the same time, the explanation will be given in the later-described receiver. This is because the coherent component of 1 may be generated, and the confidentiality, which is one of the characteristics of the present method, is considerably deteriorated.

受信装置は、f1及びf2を、各々独立した選択増幅器に依
り所定の振幅まで増幅した後、乗算し、更にそれを2乗
する。この乗算及び2乗の処理は高周波アナログ・マル
チプライヤー(以下、端に高周波乗算器という)で、完
全実時間の内に行なわれる。以下に、その過程を数式を
用いて説明する。
The receiving device amplifies f 1 and f 2 to a predetermined amplitude by independent selection amplifiers, multiplies them, and then squares them. This multiplication and squaring process is performed by a high frequency analog multiplier (hereinafter referred to as a high frequency multiplier at the end) within a complete real time. The process will be described below using mathematical expressions.

f1及びf2が高周波乗算器内で受ける変化は、以下の式で
示される。
The change that f 1 and f 2 undergo in the high frequency multiplier is shown by the following equation.

(f×f2)2 …… 式に式及び式を代入して展開する。(f 1 × f 2 ) 2 …… Expands expressions by substituting them into the equation.

(f×f2)2 =E2・cos1+p)t・E2・cos2((ω2+Δf)-p)t =E4・(1/2)・(1+cos2(ω1+p)t× (1/2)・(1+・cos2((ω2+Δf)-p)t) =(E4/4)・{1+cos2(ω1+p)t+ cos2((ω2+Δf)-p)t)cos2(ω1+p)t+ cos2((ω2+Δf)-p)t} =(E4/4)・{1+cos2(ω1+p)t+ cos2((ω2+Δf)-p)t+(1/2)・ cos2((ω2+Δf)+ω1)t+ (1/2)・cos2((ω2+Δf)-ω1-2p)t} = E4・(1/4)+ E4・(1/4)cos2 (ω1+p)t+ E4・(1/4)cos2((ω2+Δf)-p)t+ E4・(1/8)cos2((ω2+Δf)+ω1)t+ E4・(1/8)cos2((ω2+Δf)-ω1-2p)t …… 式の内、第1項は直流成分、第2項はf1の2倍の周波
数成分、第3項はf2の2倍の周波数成分第4項は第一の
搬送波と第二の搬送波の和の2倍の成分で、PN符号の
瞬時角周波数pを含まないコヒーレント成分、第5項は
第一、第二搬送波の差から、2倍のPN符号の瞬時角周
波数を引いたものの2倍の成分である。
(f 1 × f 2 ) 2 = E 2・ cos 21 + p) t ・ E 2・ cos 2 ((ω 2 + Δf) -p) t = E 4・ (1/2) ・ (1 + cos2 (ω 1 + p) t × (1/2) · (1+ · cos2 ((ω 2 + Δf) -p) t) = (E 4/4) · {1 + cos2 (ω 1 + p ) t + cos2 ((ω 2 + Δf) -p) t) cos2 (ω 1 + p) t + cos2 ((ω 2 + Δf) -p) t} = (E 4/4) · {1 + cos2 (ω 1 + p) t + cos2 ((ω 2 + Δf) -p) t + (1/2) ・ cos2 ((ω 2 + Δf) + ω 1 ) t + (1/2) ・ cos2 ((ω 2 + Δf) -ω 1 -2p) t} = E 4・ (1/4) + E 4・ (1/4) cos2 (ω 1 + p) t + E 4・ (1/4) cos2 ((ω 2 + Δf) -p) t + E 4・ (1/8) cos2 ((ω 2 + Δf) + ω 1 ) t + E 4・ (1/8) cos2 ((ω 2 + Δf) -ω 1 -2p) t ...... In the equation, the first term is the direct current component, the second term is the frequency component twice f 1 , the third term is the frequency component twice f 2 , and the fourth term is the first carrier wave and the second carrier wave. A coherent component that is twice the sum and does not include the instantaneous angular frequency p of the PN code. The fifth term is twice the difference between the first and second carrier waves minus the instantaneous angular frequency of the PN code. Is a component of.

すなわち、第1項は直流分でコヒーレントであるが伝達
すべき情報を持たず、第2、第3、第5項は、いずれも
PN符号の瞬時角周波数pを含んだ、いわゆるスペクト
ラム拡散信号と同義なものである。唯一、第4項のみ
が、PN符号の瞬時角周波数pを含まず、単に第一及び
第二の搬送波のみで決定されるコヒーレント波となる。
このコヒーレント波には、第二の搬送波に含まれている
伝達すべき情報Δfが存在しており、当該第4項の成分
をフィルターで選択抽出すれば、以後の処理は一般的受
信機の構成手法を用いて、容易に伝達すべき情報Δfを
復調する事ができる。
That is, the first term is coherent in the direct current component but has no information to be transmitted, and the second, third and fifth terms are all so-called spread spectrum signals including the instantaneous angular frequency p of the PN code. They are synonymous. Only the fourth term is a coherent wave that does not include the instantaneous angular frequency p of the PN code and is determined only by the first and second carriers.
This coherent wave has the information Δf contained in the second carrier to be transmitted. If the component of the fourth term is selected and extracted by the filter, the subsequent processing is performed by the general receiver configuration. The method can be used to easily demodulate the information Δf to be transmitted.

当該作用の説明において、第一及び第二のスペクトラム
拡散信号に対して、各々独立した空中線を使用し得る環
境下にあっては、電力合成器を要しない事は明白である
が、第一及び第二のスペクトラム拡散信号を各々効率良
く放射し得る。一体の空中線を用いる場合には、非能動
素子で構成される電力合成器を使用する必要が有る事
に、注意を払わねばならない。
In the explanation of the operation, it is obvious that the power combiner is not required under the environment where independent antennas can be used for the first and second spread spectrum signals, respectively. Each of the second spread spectrum signals can be efficiently radiated. It should be noted that when using an integral antenna, it is necessary to use a power combiner composed of inactive elements.

[実施例] ここでは、繁雑さを回避する為、単に一つの実施例の説
明にとどめるが、本発明は、前出作用で説明したとお
り、当該動作原理を用いれば、その実施方法は極めて多
岐に渡って存在することは言を待たない。
[Embodiment] Here, in order to avoid complexity, only one embodiment will be described. However, as described in the above-mentioned operation, the present invention has a wide variety of implementation methods by using the operation principle. It doesn't wait to exist over the world.

本発明の動作原理に基ずき、伝達すべき情報を音声と
し、第二の搬送波に一次変調する方法をFM方法とし、
PN符号で拡散する方法をFH方法としたもので、送信
装置のブロックダイヤグラムを第1図に、送信装置各部
における周波数スペクトラムを第2図に、送信装置各部
における周波数スペクトラムを第3図に示す。
Based on the operation principle of the present invention, the information to be transmitted is voice, and the method of performing primary modulation on the second carrier wave is the FM method,
The FH method is used as the method of spreading with a PN code. A block diagram of the transmitter is shown in FIG. 1, a frequency spectrum in each part of the transmitter is shown in FIG. 2, and a frequency spectrum in each part of the transmitter is shown in FIG.

第1図を参照して送信装置の構成と動作を説明する。The configuration and operation of the transmitter will be described with reference to FIG.

入力された音声は増幅器1で増幅された後、通常のFM
送信と同様にして周波数変換回路2により第二搬送発生
回路3からの第二搬送波(fc2)をFM変調する。
The input voice is amplified by the amplifier 1 and then the normal FM
Similarly to the transmission, the frequency conversion circuit 2 FM-modulates the second carrier wave (fc2) from the second carrier generation circuit 3.

PN符号発生回路4で白色雑音を発生させ、第三搬送波
発生回路5からの第三搬送波をFH信号発生回路6でF
M変調する。この時点でFH符号と等価のPN符号が得
られ、且つ拡散帯域は白色雑音とFM変調度により一義
的に決定される。このPN符号(fc3)は分配器7によ
り分配され、音声入力回路の平衡変調回路8及び第一搬
送波用の平衡変調回路10に導かれる。
White noise is generated by the PN code generation circuit 4, and the third carrier wave from the third carrier wave generation circuit 5 is F by the FH signal generation circuit 6.
M-modulate. At this point, a PN code equivalent to the FH code is obtained, and the spreading band is uniquely determined by the white noise and the FM modulation degree. The PN code (fc3) is distributed by the distributor 7, and is guided to the balanced modulation circuit 8 of the voice input circuit and the balanced modulation circuit 10 for the first carrier.

第二搬送波(fc2)を平衡変調回路8においてPN符号
(fc3)で平衡変調すると、第3図(a)に示すスペク
トラムが得られるので、帯域通過波回路11により下
側波帯(f2)のみを取り出す(第3図(b)参照)。
When the second carrier wave (fc2) is balanced-modulated by the PN code (fc3) in the balanced modulation circuit 8, the spectrum shown in FIG. 3 (a) is obtained, so that only the lower sideband (f2) is generated by the bandpass wave circuit 11. Are taken out (see FIG. 3 (b)).

第一搬送波からの変調を掛けない第一搬送波(fc3)を
平衡変調回路10においてPN符号(fc3)で平衡変調
すると、第三図(c)に示すスペクトラムが得られるの
で、帯域通過波回路12により下側波帯(f1)のみを
取り出す(第3図(d)参照)。
When the first carrier (fc3) that is not modulated from the first carrier is balanced-modulated by the PN code (fc3) in the balanced modulator 10, the spectrum shown in FIG. To take out only the lower sideband (f1) (see FIG. 3 (d)).

f1及びf2は、各々電力増幅回路13、14により増幅さ
れ、低域通過波回路15、16で不要な高調波を取り
除いた後、電力合成回路17で合成され(第3図(e)
参照)、送信空中線より放射される。
f1 and f2 are amplified by the power amplifier circuits 13 and 14, respectively, and unnecessary harmonics are removed by the low-pass wave circuits 15 and 16 and then combined by the power combiner circuit 17 (FIG. 3 (e)).
), Emitted from the transmitting antenna.

次にこの信号を受信する受信装置の構成と動作を第2図
に関連して説明する。
Next, the configuration and operation of the receiving device for receiving this signal will be described with reference to FIG.

受信空中線より入力された信号は、分配器20によりf1
及びf2それぞれを通過する帯域通過波回路21、22
に分配され、高周波増幅回路23、24で増幅後、高周
波乗算器25で実時間演算される。これにより得られる
複数の周波数成分の内、(f1+f2)成分のみ通過する
帯域通過波回路26を通すと、既に説明したコヒーレ
ント波が得られる(第3図(f)参照)。
The signal input from the reception antenna is f1 by the distributor 20.
, F2 and band-pass wave circuits 21, 22 respectively
And is amplified by the high frequency amplifier circuits 23 and 24, and then calculated in real time by the high frequency multiplier 25. When the band-pass wave circuit 26 that passes only the (f1 + f2) 2 component of the plurality of frequency components thus obtained is passed, the coherent wave already described is obtained (see FIG. 3 (f)).

以下、局部発振回路28からの局部発振信号を用いて周
波数変換回路27により復調し、増幅回路29で増幅す
るなどの通常のFM受信装置で伝達されるべき情報であ
る音声を復調することが出来る。
Hereinafter, it is possible to demodulate the voice, which is information to be transmitted by a normal FM receiving device, such as demodulation by the frequency conversion circuit 27 using the local oscillation signal from the local oscillation circuit 28 and amplification by the amplification circuit 29. .

[発明の効果] 以上述べたように、本発明による、当該方法にあって
は、伝達すべき情報を第二の搬送波に一次変調する方法
について、AM、FM、FSKその他の変調形式を問わ
ず、又、PN符号で拡散する方法もDS方法、FH方法
いずれも可能であり、送信装置及び受信装置の構成も従
来の技術で構築でき、特別な素子(コンボルバー、マッ
チドフィルター等)や、複雑な同期装置を全く必要とし
ない為、極めて実用性、汎用性の高いスペクトラム拡散
方法を提供する事ができる。
[Effects of the Invention] As described above, according to the method of the present invention, the method of performing the primary modulation of the information to be transmitted on the second carrier wave is not limited to AM, FM, FSK and other modulation formats. Also, both the PN code spreading method, the DS method and the FH method are possible, and the structure of the transmitter and the receiver can be constructed by the conventional technique, and special elements (convolver, matched filter, etc.) and complicated Since a synchronizer is not required at all, it is possible to provide a spread spectrum method that is extremely practical and versatile.

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

第1図は本発明の方法を実施する実施例における送信装
置のブロック図であり、第2図は本発明の方法を実施す
る実施例における受信装置のブロック図であり、第3図
は上記送信及び受信装置の所定箇所の信号波形を示す。
FIG. 1 is a block diagram of a transmitter in an embodiment for carrying out the method of the present invention, FIG. 2 is a block diagram of a receiver in an embodiment for carrying out the method of the present invention, and FIG. 3A and 3B show signal waveforms at predetermined locations of the receiver.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】伝送すべき情報を含まずかつ特定の周波数
で変調した第一のスペクトラム拡散信号と、伝送すべき
情報を含みかつ前記特定の周波数で変調した第二のスペ
クトラム拡散信号とを、そのまま同時に又は非能動素子
を用いて合成して同時に送信する送信装置と、第一及び
第二のスペクトラム拡散信号を同時に受信した後、乗算
器で掛け合わせ、その出力を更に二乗する事により得ら
れる複数の周波数成分の内より、第一のスペクトラム拡
散信号と第二のスペクトラム拡散信号の中間に位置する
周波数の二倍の周波数を抽出し復調する事で伝送すべき
情報を得る事のできる受信装置で構成される、同期捕
捉、同期維持の為の回路を要しない、非同期型スペクト
ラム拡散通信方法。
1. A first spread spectrum signal that does not contain information to be transmitted and is modulated at a specific frequency, and a second spread spectrum signal that contains information to be transmitted and is modulated at the specific frequency. It can be obtained by receiving the first and second spread spectrum signals at the same time as they are at the same time or by combining them using inactive elements and transmitting at the same time, and then multiplying by the multiplier and squaring the output. A receiver capable of obtaining information to be transmitted by extracting and demodulating a frequency twice as high as a frequency located between the first spread spectrum signal and the second spread spectrum signal from a plurality of frequency components A non-synchronous spread spectrum communication method that does not require a circuit for synchronization acquisition and synchronization maintenance.
【請求項2】第一のスペクトラム拡散信号は、単一なス
ペクトラムを有する第一の搬送周波数を第一のPN(擬
似雑音)符号で変調を掛けたものであり、第二のスペク
トラム拡散信号は、伝送すべき情報で一次変調を受けた
第二の搬送周波数を第二のPN符号で変調を掛けたもの
である、特許請求の範囲第1項に記載の、非同期型スペ
クトラム拡散通信方法。
2. The first spread spectrum signal is the first carrier frequency having a single spectrum modulated by a first PN (pseudo noise) code, and the second spread spectrum signal is The asynchronous spread spectrum communication method according to claim 1, wherein the second carrier frequency, which has undergone primary modulation with information to be transmitted, is modulated with a second PN code.
【請求項3】第一のPN符号と第二のPN符号は同一の
ものであるが、第一及び第二のスペクトラム拡散信号と
化した状態において、第一のスペクトラム拡散信号と第
二のスペクトラム拡散信号の中間に位置する計算上の周
波数を原点として対称に分布し、且つ対称に瞬時偏移す
る様配置されたものである、特許請求の範囲第2項に記
載の、非同期型スペクトラム拡散通信方法。
3. The first PN code and the second PN code are the same, but the first spread spectrum signal and the second spectrum are in the state of being converted into the first and second spread spectrum signals. The asynchronous spread spectrum communication according to claim 2, wherein the asynchronous frequencies are distributed symmetrically with respect to the origin of a calculated frequency located in the middle of the spread signal and symmetrically shifted instantaneously. Method.
JP2003343A 1990-01-12 1990-01-12 Asynchronous spread spectrum communication method Expired - Lifetime JPH0642655B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2003343A JPH0642655B2 (en) 1990-01-12 1990-01-12 Asynchronous spread spectrum communication method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2003343A JPH0642655B2 (en) 1990-01-12 1990-01-12 Asynchronous spread spectrum communication method

Publications (2)

Publication Number Publication Date
JPH03209940A JPH03209940A (en) 1991-09-12
JPH0642655B2 true JPH0642655B2 (en) 1994-06-01

Family

ID=11554714

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2003343A Expired - Lifetime JPH0642655B2 (en) 1990-01-12 1990-01-12 Asynchronous spread spectrum communication method

Country Status (1)

Country Link
JP (1) JPH0642655B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4498381B2 (en) * 2007-04-26 2010-07-07 株式会社東芝 Wireless communication method, wireless transmission device, and wireless reception device

Also Published As

Publication number Publication date
JPH03209940A (en) 1991-09-12

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