JP2000349690A - Code division multiple connection communication method - Google Patents

Code division multiple connection communication method

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Publication number
JP2000349690A
JP2000349690A JP2000092754A JP2000092754A JP2000349690A JP 2000349690 A JP2000349690 A JP 2000349690A JP 2000092754 A JP2000092754 A JP 2000092754A JP 2000092754 A JP2000092754 A JP 2000092754A JP 2000349690 A JP2000349690 A JP 2000349690A
Authority
JP
Japan
Prior art keywords
signal
carrier frequency
wave
correlation value
sequence
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.)
Granted
Application number
JP2000092754A
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Japanese (ja)
Other versions
JP3686817B2 (en
Inventor
Toshio Hayashi
俊夫 林
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.)
NEC Engineering Ltd
Original Assignee
NEC Engineering Ltd
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Filing date
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Priority to JP2000092754A priority Critical patent/JP3686817B2/en
Publication of JP2000349690A publication Critical patent/JP2000349690A/en
Application granted granted Critical
Publication of JP3686817B2 publication Critical patent/JP3686817B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To provide a transceiver in a simple processing procedure and also in a simple device constitution to suppress the non-desired waves having higher signal levels than a desired wave and to extract only the desired wave by offsetting the carrier frequency of a signal to be multiplexed by an amount equivalent to the symbol transmission frequency. SOLUTION: In a data communication method using a spread spectrum modulation system of a direct spread type, the carrier frequency is offset by an amount equivalent to 1/n symbol transmission frequency to the carrier frequency of another series to be multiplexed if an integrating section where the mutual correlation value is calculated is set in an n-symbol cycle (n: an integer of 2 or more) of a spread code. In a code division multiplex communication system, for example, a transmitter multiplexes and transmits a transmitting signal I of a system 1 and a transmitting signal Q of a system 2 after spreading them. Under such conditions, the non-desired waves of the system 1 belong to the system 2 with the non-desired waves of the system 2 belonging to the system 1 respectively. Thus, it is possible to approximate the mutual correlation value set between the desired and non-desired waves to zero by offsetting the carrier frequency.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明はスペクトラム拡散通
信方式に関し、特に直接拡散方式におけるチャンネル間
干渉を抑えた符号分割多重接続通信に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a spread spectrum communication system, and more particularly, to a code division multiple access communication system which suppresses interference between channels in a direct spread system.

【0002】[0002]

【従来の技術】スペクトラム拡散通信方式は、伝送する
信号のスペクトラム成分を広範な周波数帯域に拡散して
通信を行う方式で、直接拡散方式はPN(Pseudo
random Noise)系列と呼ばれる特殊な波形
を用いて信号の拡散を行う。図2は、直接拡散方式を用
いた2組の符号分割多重接続通信系のブロック図であ
る。送信機においては、2系統の送信信号I及びQを有
し、各々の送信信号を拡散器にてPN系列発生器からの
波形によって拡散し、変調器で変調された両系統の変調
信号を多重器にて多重し、送信アンテナ8から放射され
る。なお、PN系列IとPN系列Qは相異なるPN系列
である。受信機においては、送信機からの送信信号を受
信アンテナ9で受信し、分配器10で2分配された後、
各系統の復調器で復調された信号は、逆拡散器でPN系
列発生器からの波形によって逆拡散されて、受信信号I
及びQが再生されることになる。
2. Description of the Related Art A spread spectrum communication system is a system for performing communication by spreading a spectrum component of a signal to be transmitted over a wide frequency band, and a direct spread system is a PN (Pseudo) system.
The signal is spread using a special waveform called a "random noise" sequence. FIG. 2 is a block diagram of two sets of code division multiple access communication systems using the direct spreading method. The transmitter has two transmission signals I and Q. Each transmission signal is spread by a spreader with a waveform from a PN sequence generator, and the modulated signals of both systems modulated by the modulator are multiplexed. And radiated from the transmission antenna 8. Note that the PN sequence I and the PN sequence Q are different PN sequences. In the receiver, after the transmission signal from the transmitter is received by the receiving antenna 9 and split by the splitter 10,
The signal demodulated by the demodulator of each system is despread by the despreader by the waveform from the PN sequence generator, and the received signal I
And Q will be reproduced.

【発明が解決しようとする課題】しかし、それぞれの逆
拡散器で逆拡散される信号には、逆拡散しようとする希
望波以外の非希望波も重畳されている。逆拡散は希望波
のPN系列の自己相関最大値を取ることで行われるが、
希望波のPN系列と非希望波のPN系列の相互相関値が
常にゼロとなるPN系列の組み合わせは存在しないた
め、この相互相関は非希望波による干渉となる。従来技
術においては、このような特性を考慮し、相互相関がゼ
ロに十分近いPN系列を使用して多重化するため、希望
波と非希望波の信号レベルが同程度であれば、非希望波
による干渉の影響はほとんどない。しかし、近年の利用
形態においては、送信側で希望波の信号レベルよりも大
きい信号レベルの非希望波が重畳される場合等があり、
受信側の再生処理では、希望波どうしの自己相関値より
も、希望波と非希望波の相互相関値のほうが大きくなる
可能性がある。こうなると、希望波を正しく逆拡散する
ことができないため、受信信号に誤りが生じる。従っ
て、多重化する信号レベルに差がある場合は、大きな信
号レベルの信号が小さい信号に好ましくない影響を与え
る可能性があるため、逆拡散器において非希望波による
干渉を抑制する必要があるが従来技術では解決すること
ができない。そこで、本発明においては、希望波よりも
信号レベルが大きい非希望波による干渉を抑制し、希望
波のみを抽出できる送受信機を、簡易な処理手順及び装
置構成により実現することを目的する。
However, undesired waves other than the desired wave to be despread are also superimposed on the signals despread by the respective despreaders. Despreading is performed by taking the maximum value of the autocorrelation of the PN sequence of the desired signal.
Since there is no PN sequence combination in which the cross-correlation value between the PN sequence of the desired wave and the PN sequence of the undesired wave is always zero, the cross-correlation is interference by the undesired wave. In the prior art, in consideration of such characteristics, multiplexing is performed using a PN sequence whose cross-correlation is sufficiently close to zero. There is almost no interference effect. However, in recent usage forms, there is a case where a non-desired wave having a signal level higher than the signal level of the desired wave is superimposed on the transmitting side,
In the reproduction process on the receiving side, there is a possibility that the cross-correlation value between the desired wave and the non-desired wave becomes larger than the auto-correlation value between the desired waves. In this case, the desired signal cannot be correctly despread, and an error occurs in the received signal. Therefore, if there is a difference in signal levels to be multiplexed, a signal having a large signal level may have an undesired effect on a small signal. The conventional technology cannot solve it. Therefore, an object of the present invention is to realize a transceiver capable of extracting only a desired wave by suppressing interference caused by a non-desired wave having a signal level higher than that of the desired wave, with a simple processing procedure and a simple device configuration.

【0003】[0003]

【課題を解決するための手段】本発明の符号分割多重通
信は、非希望波からの干渉を抑制する。より具体的に
は、多重化する信号の搬送波周波数をシンボル伝送周波
数分ずつオフセットすることで実現される。また、2シ
ンボル区間以上にわたって相関値を求めるための積算を
行う場合にも適用できることを特徴とする。具体的には
数式8で示すようなオフセット量を与えればよい。これ
により、多重化する搬送波周波数をシンボル伝送周波数
分ずつオフセットすることで、希望波と非希望波間の相
互相関値がPN系列等に関係なくゼロになる。また、積
分区間の延長に伴い、相互相関値をゼロにするための搬
送波周波数オフセット量が小さくなる。
The code division multiplex communication of the present invention suppresses interference from undesired waves. More specifically, this is realized by offsetting the carrier frequency of the signal to be multiplexed by the symbol transmission frequency. Further, the present invention is characterized in that the present invention can be applied to a case where integration for obtaining a correlation value is performed over two or more symbol sections. Specifically, an offset amount as shown in Expression 8 may be given. By offsetting the carrier frequency to be multiplexed by the symbol transmission frequency, the cross-correlation value between the desired wave and the undesired wave becomes zero regardless of the PN sequence or the like. Further, with the extension of the integration section, the carrier frequency offset amount for making the cross-correlation value zero becomes smaller.

【0004】[0004]

【発明の実施の形態】次に、本発明の実施の形態につい
て図面を参照して詳細に説明する。図1は、本発明の実
施の一形態である符号分割多重通信系のブロック図であ
る。拡散方式は直接拡散方式、多重化数は2組とし、変
調方式はPSK方式とする。送信機は、乗算器21、I
用PN系列発生器22、乗算器23、発振器24、乗算
器25、Q用PN系列発生器26、乗算器27、発振器
28、加算器29、送信アンテナ30から構成され、系
1の送信信号Iと系2の送信信号Qを拡散した後、多重
して送信する。系1と系2の伝送レートは同一であっ
て、拡散処理に際しては、各々の系列に用意されたPN
系列発生器によって、1シンボルを1周期のPNパター
ン系列により拡散を行う。受信機は、受信アンテナ3
1、乗算器32、発振器33、乗算器34、I用PN系
列発生器35、LPF(Low Pass Filte
r)36、乗算器37、発振器38、乗算器39、Q用
PN系列発生器40、LPF41から構成されている。
なお、図中の文字変数の意味は以下の通りである。a1
(t)は、送信信号α、c1(t)はI用PN系列、f1は
I用変調波周波数、ω1はI用変調波角周波数で、ω2は
Q用変調波角周波数で、τは送信信号Iと送信信号Q間
の時間差、σ1は発振器33とI用PN系列発振器35
間の時間差、σ2は発振器38とQ用PN系列発生器4
0間の時間差を示す。またf1とf2は、f2=f1+Δf
(Δfはオフセット周波数である)の関係にある。送信
機における系1では、I用PN系列発生器22によって
発生したI用PN系列を送信信号Iに乗積して拡散し、
発振器24で生成した正弦波(cosω1t)とその拡散
波とを乗算器23で乗積して変調する。送信機における
系2でも同様な処理が行われ、送信信号QはQ用PN系
列で拡散、正弦波(cosω2t)で変調される。 この
2つの変調波を加算器29によって多重化し、送信アン
テナ30から放射する。送信アンテナ30から放射され
る信号は、以下の式で表される。
Next, embodiments of the present invention will be described in detail with reference to the drawings. FIG. 1 is a block diagram of a code division multiplex communication system according to an embodiment of the present invention. The spreading method is a direct spreading method, the number of multiplexing is two, and the modulation method is a PSK method. The transmitter comprises a multiplier 21, I
PN sequence generator 22, multiplier 23, oscillator 24, multiplier 25, PN sequence generator 26 for Q, multiplier 27, oscillator 28, adder 29, and transmission antenna 30. After the transmission signal Q of the system 2 is spread, it is multiplexed and transmitted. The transmission rates of the system 1 and the system 2 are the same, and the PN prepared for each system is used for the spreading process.
One symbol is spread by a sequence generator using a PN pattern sequence of one cycle. The receiver is receiving antenna 3
1, multiplier 32, oscillator 33, multiplier 34, PN sequence generator 35 for I, LPF (Low Pass Filter)
r) 36, a multiplier 37, an oscillator 38, a multiplier 39, a PN sequence generator 40 for Q, and an LPF 41.
The meanings of the character variables in the figure are as follows. a1
(T) is a transmission signal α, c1 (t) is a PN sequence for I, f1 is a modulation wave frequency for I, ω1 is a modulation wave angular frequency for I, ω2 is a modulation wave angular frequency for Q, and τ is a transmission signal. The time difference between the signal I and the transmission signal Q, σ1 is the oscillator 33 and the PN sequence oscillator for I 35
The time difference σ 2 between the oscillator 38 and the Q PN sequence generator 4
Indicates the time difference between 0. F1 and f2 are given by f2 = f1 + Δf
(Δf is an offset frequency). In the system 1 in the transmitter, the PN sequence for I generated by the PN sequence generator for I 22 is multiplied by the product of the transmission signal I and spread,
The sine wave (cos ω1t) generated by the oscillator 24 and its spread wave are multiplied by the multiplier 23 and modulated. Similar processing is performed in the system 2 in the transmitter, and the transmission signal Q is spread with a Q PN sequence and modulated with a sine wave (cos ω2t). The two modulated waves are multiplexed by the adder 29 and radiated from the transmission antenna 30. The signal radiated from the transmitting antenna 30 is represented by the following equation.

【数1】 受信アンテナ31で受信した変調波が、受信機の系1と
系2に分配される。受信アンテナ31で受信した変調波
が、受信機の系1と受信機の系2に分配される。受信機
の系1では、発振器33によって生成された正弦波(c
osω1t)と変調波を乗算器32で乗積して復調し、I
用PN系列発生器35によって発生されたI用PN系列
とその復調波とを乗算器34で乗積することで逆拡散す
る。逆拡散された信号はLPF36を通過し、受信信号
Iとなる。 受信機の系2でも同様な処理が行われ、正
弦波(cosω2t)で復調、Q用PN系列で逆拡散され
た信号がLPF41を通過して、受信信号Qとなる。
系1において、復調・逆拡散された信号の式は、
(Equation 1) The modulated wave received by the receiving antenna 31 is distributed to the systems 1 and 2 of the receiver. The modulated wave received by the receiving antenna 31 is distributed to the system 1 of the receiver and the system 2 of the receiver. In system 1 of the receiver, the sine wave (c
osω1t) and the modulated wave are multiplied and multiplied by the multiplier 32 and demodulated.
The PN sequence for I generated by the PN sequence generator 35 for I and the demodulated wave are multiplied by the multiplier 34 to despread. The despread signal passes through the LPF 36 and becomes a received signal I. Similar processing is performed in the receiver system 2, and a signal demodulated with a sine wave (cos ω2t) and despread with a PN sequence for Q passes through the LPF 41 to become a received signal Q.
In the system 1, the equation of the demodulated and despread signal is

【数2】 となる。ここで、f1>>Δfと考えると、(Equation 2) Becomes Here, considering that f1 >> Δf,

【数3】 のように近似できる。また、ω2τは定数である。co
s2ω1tに関する項は後段のLPFにおいて除去される
ので、最終的な系1での受信信号の式は、
(Equation 3) Can be approximated as follows. Ω2τ is a constant. co
Since the term relating to s2ω1t is removed in the subsequent LPF, the equation of the received signal in the final system 1 is:

【数4】 となる。数式4を1シンボル周期にわたって積分すれ
ば、系1での相関値が得られる。シンボル伝送周波数を
fs、1シンボル周期をTs(=1/fs)とすると、
相関値は以下のようになる。すなわち、数式4の前半を
1シンボル周期にわたって積分すると、数式5に示す自
己相関が得られる。ここで、t0は、任意の積分開始時
点を示す。
(Equation 4) Becomes By integrating Equation 4 over one symbol period, a correlation value in the system 1 is obtained. Assuming that the symbol transmission frequency is fs and the symbol period is Ts (= 1 / fs),
The correlation value is as follows. That is, when the first half of Equation 4 is integrated over one symbol period, the autocorrelation shown in Equation 5 is obtained. Here, t0 indicates an arbitrary integration start time.

【数5】 スペクトラム拡散通信の初期同期捕捉は主に、同じシン
ボルが連続する特有の区間で行われるが、このとき、I
用PN系列の自己相関はPN系列の位相が一致してσ1
=0となった時点で最大となる。なお、この区間ではa1
(t)がどの時間においても定数となる。次ぎに、数式4
の後半を1シンボル周期にわたって積分すると、数式6
に示す相互相関が得られる。
(Equation 5) Initial synchronization acquisition of spread spectrum communication is mainly performed in a specific section where the same symbol is continuous.
Auto-correlation of the PN sequence for
It becomes the maximum when it becomes = 0. In this section, a1
(t) is a constant at any time. Next, Equation 4
Is integrated over one symbol period, Equation 6
Are obtained.

【数6】 先述した初期同期捕捉のための特有区間では、a2(t+τ)
がどの時間においても定数となるので、数式6はc1と
c2の相互相関と正弦関数の積を1シンボル周期にわた
って積分する式と考えられる。c1とc2のPN符号はΔ
fよりも短い周期でノイズ的にランダム変化する信号で
あるから、一定区間を切り出したパタンは、切り出し開
始時点によらずほぼ同様なパタンとなる。非希望波の信
号レベルが希望波の信号レベルよりも大きい場合、相互
相関値はレベル差に比例して大きくなるため、信号レベ
ルが等しい場合には無視できていた相互相関が無視でき
なくなるが、ここで、
(Equation 6) In the specific section for initial synchronization acquisition described above, a2 (t + τ)
Is a constant at any time, and Equation 6 can be considered as an equation for integrating the product of the cross-correlation between c1 and c2 and the sine function over one symbol period. The PN code of c1 and c2 is Δ
Since the signal is a signal that randomly changes in a noise cycle with a period shorter than f, the pattern obtained by cutting out a certain section is almost the same regardless of the cutout start time. If the signal level of the undesired wave is higher than the signal level of the desired wave, the cross-correlation value increases in proportion to the level difference, so that if the signal levels are equal, the cross-correlation that could be ignored cannot be ignored. here,

【数7】 として周波数オフセット量をfsとすれば、正弦関数の
1シンボル周期の積分はゼロとなるため、結果的に数式
6の積分はゼロに近い値となる。なお、この系1では、
非希望波が系2である。また、系2においても、同様に
計算を行うと数式7の条件を得ることができる。なお、
非希望波は系1となる。以上のことから、数式7を満た
す周波数オフセットを与えた場合、非希望波と希望波間
の干渉による相互相関値がゼロに近い値となり、干渉の
影響を最低限に抑制することができる。さらに、一連の
処理内容は基本的なスペクトラム拡散通信方式に従うも
のであり、特殊な処理や特別な装置を必要としない。
(Equation 7) Assuming that the frequency offset amount is fs, the integral of one cycle of the sine function becomes zero, and as a result, the integral of Expression 6 becomes a value close to zero. In this system 1,
The undesired wave is system 2. Also, in the system 2, if the calculation is performed similarly, the condition of Expression 7 can be obtained. In addition,
The undesired wave becomes system 1. From the above, when a frequency offset that satisfies Equation 7 is given, the cross-correlation value due to the interference between the undesired wave and the desired wave becomes a value close to zero, and the influence of the interference can be suppressed to the minimum. Further, the series of processing contents follow the basic spread spectrum communication method, and does not require special processing or a special device.

【発明の他の実施の形態】上記の証明では、相関値を求
める積分区間を1シンボル周期としたが、積分区間をn
シンボル周期に拡張した場合の搬送波周波数オフセット
量は、
In the above proof, the integral interval for obtaining the correlation value is one symbol period, but the integral interval is n.
The carrier frequency offset amount when extended to the symbol period is

【数8】 で与えられる。従って、積算区間を大きくすると、オフ
セットする周波数は小さくなる。多重化数を増やす場合
は、必要な分ずつ発振周波数をオフセットした発振器を
多重化する数だけ用意すればよい。本明細書での図では
送信機内で多重化を行っているが、独立した送信機から
の信号を衛星等で多重化して通信する場合にも、同様に
適用できる。
(Equation 8) Given by Therefore, when the integration period is increased, the offset frequency is reduced. When increasing the number of multiplexes, it is sufficient to prepare the number of multiplexed oscillators whose oscillation frequencies are offset by a necessary amount. Although the multiplexing is performed in the transmitter in the figures in this specification, the same can be applied to a case where signals from independent transmitters are multiplexed and communicated by a satellite or the like.

【0005】[0005]

【発明の効果】第1の効果は、希望波よりも大きな信号
レベルの非希望波による干渉の影響を抑制できることで
ある。その理由は、搬送波周波数をオフセットすること
で希望波と非希望波との相互相関値をゼロに近づけるこ
とができるためである。第2の効果は、特殊な処理や追
加装置を必要としないことである。その理由は、一般的
なスペクトラム拡散通信に必要な構成物のみで系を組む
ことができるためである。また、積分区間をnとするこ
とにより、前記オフセット周波数を1/nとすることが
できるため、限られた周波数帯域を有効利用することが
できる。
The first effect is that the influence of interference by undesired waves having a signal level higher than the desired wave can be suppressed. The reason is that by offsetting the carrier frequency, the cross-correlation value between the desired wave and the undesired wave can be made closer to zero. The second effect is that no special processing or additional equipment is required. The reason is that a system can be formed only with components necessary for general spread spectrum communication. Further, by setting the integration interval to n, the offset frequency can be reduced to 1 / n, so that a limited frequency band can be effectively used.

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

【図1】本発明の一実施の形態にかかる符号分割多重接
続通信系のブロック図。
FIG. 1 is a block diagram of a code division multiple access communication system according to one embodiment of the present invention.

【図2】従来技術における直接拡散方式を用いた符号分
割多重接続通信系のブロック図。
FIG. 2 is a block diagram of a code division multiple access communication system using a direct spreading method according to the related art.

【符号の説明】[Explanation of symbols]

1 拡散器 2 I用PN系列発生器 3 変調器 4 拡散器 5 Q用PN系列発生器 6 変調器 7 多重器 8 送信アンテナ 9 受信アンテナ 10 分配器 11 復調器 12 逆拡散器 13 I用PN系列発生器 14 復調器 15 逆拡散器 16 Q用PN系列発生器 21 乗算器 22 I用PN系列発生器 23 乗算器 24 発振器 25 乗算器 26 Q用PN系列発生器 27 乗算器 28 発振器 29 加算器 30 送信アンテナ 31 受信アンテナ 32 乗算器 33 発振器 34 乗算器 35 I用PN系列発生器 36 LPF 37 乗算器 38 発振器 39 乗算器 40 Q用PN系列発生器 41 LPF Reference Signs List 1 spreader 2 PN sequence generator for I 3 modulator 4 spreader 5 PN sequence generator for Q 6 modulator 7 multiplexer 8 transmitting antenna 9 receiving antenna 10 distributor 11 demodulator 12 despreader 13 PN sequence for I Generator 14 Demodulator 15 Despreader 16 PN sequence generator for Q 21 Multiplier 22 PN sequence generator for I 23 Multiplier 24 Oscillator 25 Multiplier 26 PN sequence generator for Q 27 Multiplier 28 Oscillator 29 Adder 30 Transmitting antenna 31 Receiving antenna 32 Multiplier 33 Oscillator 34 Multiplier 35 PN sequence generator for I 36 LPF 37 Multiplier 38 Oscillator 39 Multiplier 40 PN sequence generator for Q 41 LPF

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 直接拡散型のスペクトラム拡散変調方式
を用いたデータ通信方法において、相互相関値を算出す
る積分区間を拡散符号のnシンボル周期(nは2以上の
整数とする)とした場合に、搬送周波数を、多重化する
他系列の搬送周波数に対して1/nシンボル伝送周波数
分だけオフセットしたことを特徴とする符号分割多重接
続通信方法。
1. A data communication method using a direct spread type spread spectrum modulation method, wherein an integration interval for calculating a cross-correlation value is n symbol periods of a spreading code (n is an integer of 2 or more). Wherein the carrier frequency is offset by 1 / n symbol transmission frequency with respect to the carrier frequency of another stream to be multiplexed.
JP2000092754A 1999-03-30 2000-03-30 Code division multiple access communication method Expired - Fee Related JP3686817B2 (en)

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Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP11-89649 1999-03-30
JP8964999 1999-03-30
JP2000092754A JP3686817B2 (en) 1999-03-30 2000-03-30 Code division multiple access communication method

Publications (2)

Publication Number Publication Date
JP2000349690A true JP2000349690A (en) 2000-12-15
JP3686817B2 JP3686817B2 (en) 2005-08-24

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Country Link
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Also Published As

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JP3686817B2 (en) 2005-08-24

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