JPH08201450A - Spectrum analyzer - Google Patents

Spectrum analyzer

Info

Publication number
JPH08201450A
JPH08201450A JP3162095A JP3162095A JPH08201450A JP H08201450 A JPH08201450 A JP H08201450A JP 3162095 A JP3162095 A JP 3162095A JP 3162095 A JP3162095 A JP 3162095A JP H08201450 A JPH08201450 A JP H08201450A
Authority
JP
Japan
Prior art keywords
frequency
sweep
vco
linearity
correction
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.)
Pending
Application number
JP3162095A
Other languages
Japanese (ja)
Inventor
Hirobumi Musha
博文 武者
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.)
Advantest Corp
Original Assignee
Advantest 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 Advantest Corp filed Critical Advantest Corp
Priority to JP3162095A priority Critical patent/JPH08201450A/en
Priority to PCT/JP1996/000131 priority patent/WO1996023232A1/en
Priority to DE19680092T priority patent/DE19680092C2/en
Publication of JPH08201450A publication Critical patent/JPH08201450A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R23/00Arrangements for measuring frequencies; Arrangements for analysing frequency spectra
    • G01R23/16Spectrum analysis; Fourier analysis
    • G01R23/173Wobbulating devices similar to swept panoramic receivers
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03BGENERATION OF OSCILLATIONS, DIRECTLY OR BY FREQUENCY-CHANGING, BY CIRCUITS EMPLOYING ACTIVE ELEMENTS WHICH OPERATE IN A NON-SWITCHING MANNER; GENERATION OF NOISE BY SUCH CIRCUITS
    • H03B23/00Generation of oscillations periodically swept over a predetermined frequency range
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03BGENERATION OF OSCILLATIONS, DIRECTLY OR BY FREQUENCY-CHANGING, BY CIRCUITS EMPLOYING ACTIVE ELEMENTS WHICH OPERATE IN A NON-SWITCHING MANNER; GENERATION OF NOISE BY SUCH CIRCUITS
    • H03B5/00Generation of oscillations using amplifier with regenerative feedback from output to input
    • H03B5/18Generation of oscillations using amplifier with regenerative feedback from output to input with frequency-determining element comprising distributed inductance and capacitance
    • H03B5/1882Generation of oscillations using amplifier with regenerative feedback from output to input with frequency-determining element comprising distributed inductance and capacitance the frequency-determining element being a magnetic-field sensitive resonator, e.g. a Yttrium Iron Garnet or a magnetostatic surface wave resonator
    • H03B5/1888Generation of oscillations using amplifier with regenerative feedback from output to input with frequency-determining element comprising distributed inductance and capacitance the frequency-determining element being a magnetic-field sensitive resonator, e.g. a Yttrium Iron Garnet or a magnetostatic surface wave resonator the active element in the amplifier being a semiconductor device
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03CMODULATION
    • H03C3/00Angle modulation
    • H03C3/02Details
    • H03C3/08Modifications of modulator to linearise modulation, e.g. by feedback, and clearly applicable to more than one type of modulator

Abstract

PURPOSE: To provide a further inexpensive oscillation source by performing the linear correction such that the voltage controlled oscillation frequency of a variable capacity diode generates a sweeping frequency of constant inclination. CONSTITUTION: The constitution of a sweep control section 70 is additionally provided with a linear correction section 78 thus providing an additional code data conversion processing for correcting the linearity of a varactor tuned voltage controlled oscillator(VCO) 20. The correcting section 78 is provided with a linearity correction table 79 prestored with correction values 79dal for determining the characteristic curve of control voltage 38uosc vs oscillation frequency. The correction value 79dal is read out using a code data 72cod , received from a ramp signal generating section 72, as an address. It is then multiplied by the data 72cod to produce a conversion code data 78cod subjected to linearity correction which is then fed to a DA converter 74. Consequently, the VCO 20 can oscillates a linear sweeping frequency having incremental inclination of a constant frequency. Since a local oscillator 30 can be constituted of a relatively inexpensive VCO circuit, a further inexpensive oscillation source can be obtained.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、局部発振器に使用さ
れる発振源を安価に構成するスペクトラムアナライザに
関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a spectrum analyzer for inexpensively constructing an oscillation source used for a local oscillator.

【0002】[0002]

【従来の技術】従来において、スペクトラムアナライザ
の局部発振器に使用される発振源として、YIG(Yttr
ium Iron Garnet)を用いたスペクトラムアナライザの
例がある。これについて、図4と図5と図6を参照して
説明する。本装置は、図4のブロック図に示すように、
周波数変換部50と、掃引制御部70と、検波部62
と、表示演算部64と、表示部68とで構成している。
2. Description of the Related Art Conventionally, as an oscillation source used for a local oscillator of a spectrum analyzer, YIG (Yttr
There is an example of a spectrum analyzer using (ium Iron Garnet). This will be described with reference to FIGS. 4, 5, and 6. This device, as shown in the block diagram of FIG.
Frequency converter 50, sweep controller 70, detector 62
And a display calculation section 64 and a display section 68.

【0003】周波数変換部50は、一般的なスペクトラ
ムアナライザの周波数変換部の原理構成であり、被測定
信号100を受けて、局部発振器で所望の周波数範囲を
掃引して一定の中間周波数に変換し、BPF(バンドパ
ス・フィルタ)で所望の帯域幅特性にフィルタした後、
検波部62に供給する。検波部62は、この掃引して得
られた信号を検波した後、デジタル信号に変換し、表示
演算部64に供給する。この周波数変換部50の中に、
掃引ランプ信号76sweepを受けて掃引する局部発振器
30がある。
The frequency conversion section 50 has the principle configuration of a frequency conversion section of a general spectrum analyzer. The frequency conversion section 50 receives a signal under test 100, sweeps a desired frequency range with a local oscillator, and converts it into a constant intermediate frequency. , BPF (bandpass filter) after filtering to the desired bandwidth characteristics,
It is supplied to the detection unit 62. The detection unit 62 detects the signal obtained by the sweeping, converts the signal into a digital signal, and supplies the digital signal to the display calculation unit 64. In this frequency conversion unit 50,
There is a local oscillator 30 that receives and sweeps a sweep ramp signal 76sweep.

【0004】掃引制御部70は、局部発振器30へ掃引
用のアナログランプ波形を供給するものであって、掃引
開始信号70sttを受けて、ランプ発生部72がスパン
周波数(掃引範囲周波数)区間に対応して一定の傾斜で
ランプ掃引するコードデータを、掃引速度に対応した時
間間隔で順次DA変換器74に供給してアナログ階段波
形に変換し、LPF(ローパスフィルタ)76で直線的
傾きにフィルタしたランプ信号76sweepを局部発振器
30へ供給する。
The sweep control unit 70 supplies a swept analog ramp waveform to the local oscillator 30, and upon receipt of the sweep start signal 70stt, the ramp generation unit 72 responds to a span frequency (sweep range frequency) section. Then, the code data for sweeping the ramp at a constant slope is sequentially supplied to the DA converter 74 at a time interval corresponding to the sweep speed, converted into an analog staircase waveform, and filtered by a LPF (low-pass filter) 76 into a linear slope. The ramp signal 76sweep is supplied to the local oscillator 30.

【0005】局部発振器30は、ランプ信号76sweep
を受けて、掃引周波数範囲を掃引する発振器であって、
この内部構成は、図5に示すように、分周器34、37
と、位相比較器36と、積分器35と、加算器38と、
YTO(YIG-tuned Oscillator)40とで構成してい
る。
The local oscillator 30 outputs a ramp signal 76sweep.
In response to this, an oscillator for sweeping a sweep frequency range,
As shown in FIG. 5, the internal configuration is such that the frequency dividers 34 and 37 are
, A phase comparator 36, an integrator 35, an adder 38,
It is composed of a YTO (YIG-tuned Oscillator) 40.

【0006】YTO40は、掃引する前時点で、PLL
(Phase Locked Loop)のロックループを形成させて掃
引周波数の中間値である中心周波数f0を発振して位相
ロックした状態にしておく。このときのランプ信号76
sweep電圧は0v状態にある。次に掃引開始するとき
に、積分器35の出力端のアナログ電位35voscを保持
状態に切り替え制御する。これによりPLLロックルー
プが解除されて中心周波数f0で発振するフリーラン状
態になる。この状態で掃引制御部70からのランプ信号
76sweepをアナログ加算器38の一端に供給してアナ
ログ電位35voscとを加算した結果の制御電圧38vosc
をYTO40に供給することで、ランプ掃引する発振周
波数を発生する。即ち、掃引時は、フリーラン状態にし
て電圧制御発振入力端にランプ信号76sweepを加算し
たアナログ電圧を与えて掃引する。この為、YTO40
としては入力されるアナログ電圧に比例した発振周波数
を発生する直線性の良い発振源が必要とされる。
The YTO 40 has a PLL before the sweep.
A locked loop of (Phase Locked Loop) is formed to oscillate the center frequency f0 which is the intermediate value of the sweep frequency, and the phase is locked. Lamp signal 76 at this time
The sweep voltage is in the 0v state. Next, when the sweep is started, the analog potential 35vosc at the output end of the integrator 35 is controlled to be switched to the holding state. As a result, the PLL lock loop is released and a free-run state in which the PLL lock loop oscillates at the center frequency f0 is established. In this state, the ramp signal 76sweep from the sweep control unit 70 is supplied to one end of the analog adder 38 to add the analog potential 35vosc to the control voltage 38vosc.
Is supplied to the YTO 40 to generate an oscillation frequency for sweeping the lamp. That is, at the time of sweeping, a free-run state is set and an analog voltage obtained by adding the ramp signal 76sweep is applied to the voltage-controlled oscillation input end to sweep. Therefore, YTO40
Therefore, an oscillation source with good linearity that generates an oscillation frequency proportional to the input analog voltage is required.

【0007】ここで、VCO(電圧制御発振器)である
YTO40について、内部回路構成を図6に示して説明
する。YTO40は、YIG共振器42を用いたVCO
であって、コイル42bに流す電流値と発振周波数値と
が比例関係にある直線性に優れた発振器である。上記加
算器38からの制御電圧38vosc信号を受けて、IV変
換器41で電流に変換した後コイル42bに供給してY
IG共振器42に磁界を与える。これによって、YIG
共振器42は、磁界に比例した同調周波数となる。これ
を共振回路として、トランジスタ43と直列フィードバ
ック素子44と出力マッチング・ネットワーク(MN)
とで構成する負性抵抗回路49によって発振回路を形成
する。この負性抵抗回路49は使用する発振周波数範
囲、例えば4〜8GHzの間で発振条件を満たす負性抵
抗となるように各素子のパラメータを与える。この発振
回路からの発振信号をバッファアンプ48で緩衝増幅し
た発振周波数信号40oscを出力している。このYIG
共振器を使うことにより、掃引時において、直線性精度
の良い掃引周波数を発生でき、スペクトラム測定の高い
周波数確度を維持している。
The internal circuit configuration of the YTO 40, which is a VCO (voltage controlled oscillator), will be described with reference to FIG. The YTO 40 is a VCO using the YIG resonator 42.
In addition, the oscillator having excellent linearity, in which the value of the current flowing through the coil 42b and the value of the oscillation frequency are in a proportional relationship. The control voltage 38vosc signal from the adder 38 is received, converted into a current by the IV converter 41, and then supplied to the coil 42b, and then Y
A magnetic field is applied to the IG resonator 42. By this, YIG
The resonator 42 has a tuning frequency proportional to the magnetic field. Using this as a resonance circuit, the transistor 43, the series feedback element 44, and the output matching network (MN)
An oscillation circuit is formed by the negative resistance circuit 49 configured by. The negative resistance circuit 49 gives parameters of each element so that the negative resistance satisfies the oscillation condition in the oscillation frequency range used, for example, in the range of 4 to 8 GHz. An oscillation frequency signal 40osc obtained by buffer-amplifying the oscillation signal from this oscillation circuit with a buffer amplifier 48 is output. This YIG
By using a resonator, a sweep frequency with good linearity accuracy can be generated during sweep, and high frequency accuracy of spectrum measurement is maintained.

【0008】[0008]

【発明が解決しようとする課題】上記説明のように、局
部発振器30としては、掃引時にフリーラン状態にして
電圧制御発振入力端にランプ信号76sweepを加算した
アナログ電圧で掃引する為、従来のスペクトラムアナラ
イザでは、VCOとして、入力されるアナログ電圧に比
例した発振周波数を発生する直線性の良いYIG素子を
用いたVCOで構成していた。しかし、このYIG素子
は比較的高価であり、製品原価費に占める割合が比較的
大きいという難点がある。
As described above, the local oscillator 30 is swept by the analog voltage obtained by adding the ramp signal 76sweep to the voltage-controlled oscillation input terminal in the free-run state at the time of sweeping. In the analyzer, a VCO using a YIG element having good linearity that generates an oscillation frequency proportional to the input analog voltage is used as the VCO. However, this YIG element is relatively expensive and has a drawback that it accounts for a relatively large proportion of the product cost.

【0009】そこで、本発明が解決しようとする課題
は、YIG共振器の変わりに比較的安価なVCO回路を
使用し、この直線性を補正して構成する局部発振器を構
成することで、より安価なスペクトラムアナライザの発
振源を実現することを目的とする。
Therefore, the problem to be solved by the present invention is to reduce the cost by using a relatively inexpensive VCO circuit instead of the YIG resonator and constructing a local oscillator that corrects this linearity. The purpose is to realize an oscillating source for various spectrum analyzers.

【0010】[0010]

【課題を解決する為の手段】上記課題を解決するため
に、本発明の構成では、上記可変容量ダイオード24の
電圧制御発振周波数を、一定傾きの掃引周波数を発生す
るように直線性補正する直線性補正部78手段を設ける
構成手段にする。これにより、マイクロ波用可変容量ダ
イオード24を使用して電圧制御発振器VCOを構成す
る局部発振器30を有して、アナログの掃引ランプ信号
76sweepを受けて直線性良く掃引する比較的安価なス
ペクトラムアナライザ用の局部発振器30を実現する。
In order to solve the above-mentioned problems, in the structure of the present invention, a straight line for correcting the voltage controlled oscillation frequency of the variable capacitance diode 24 so as to generate a sweep frequency having a constant slope. The property correction section 78 is provided as a constituent means. As a result, for a relatively inexpensive spectrum analyzer that has the local oscillator 30 that configures the voltage controlled oscillator VCO using the variable capacitance diode 24 for microwaves and sweeps with good linearity by receiving the analog sweep ramp signal 76sweep. The local oscillator 30 is realized.

【0011】具体的手段としては、掃引制御部70のラ
ンプ発生部72からのコードデータ72codを受けて、
電圧制御発振器の発振周波数を、ランプ掃引と比例した
一定周波数の増加傾きとなる直線性補正処理した変換コ
ードデータ78codを出力してアナログの掃引ランプ信
号76sweepによる掃引周波数を直線性補正する直線性
補正部78手段を設ける構成手段がある。
As a concrete means, by receiving the code data 72cod from the ramp generating section 72 of the sweep control section 70,
Linearity correction that outputs conversion code data 78cod that has undergone linearity correction processing in which the oscillation frequency of the voltage controlled oscillator has an increasing slope of a constant frequency that is proportional to the ramp sweep, and corrects the sweep frequency by the analog sweep ramp signal 76sweep. There is a constituent means for providing the means 78.

【0012】[0012]

【作用】直線性補正部78は、ランプ発生部72からの
コードデータ72codを受けて、バラクタチューンドV
CO20での発振周波数が、ランプ掃引と比例した一定
周波数の増加傾きとなるように直線性補正した変換コー
ドデータ78codを出力する作用がある。マイクロ波用
可変容量ダイオード24を可変同調素子としてVCOを
構成し、掃引制御部70の直線性補正部78で発振周波
数の掃引直線性を補正するコードデータに変換してラン
プ掃引する局部発振器30は、従来と同等レベルのスペ
クトラム測定の周波数確度を維持できる効果が得られ
る。
The linearity correction section 78 receives the code data 72cod from the ramp generation section 72 and receives the varactor tune V
The conversion code data 78cod is linearly corrected so that the oscillation frequency of the CO 20 has an increasing slope of a constant frequency proportional to the lamp sweep. A local oscillator 30 that configures a VCO using the variable capacitance diode for microwaves 24 as a variable tuning element, converts it into code data for correcting the sweep linearity of the oscillation frequency by the linearity correction unit 78 of the sweep control unit 70, and performs ramp sweep is used. , It is possible to obtain the effect of maintaining the frequency accuracy of spectrum measurement at the same level as the conventional one.

【0013】[0013]

【実施例】本発明の実施例は、局部発振器をバラクタチ
ューンドVCOで構成した場合の例である。これについ
て、図1と図2を参照して説明する。本装置全体の構成
は、図4に示す従来構成と同様の構成であるが、この中
で、周波数変換部50の局部発振器30と掃引制御部7
0の構成を変えている。局部発振器30では、図1に示
すように、YTO40の代わりにバラクタチューンドV
CO20の置き換えた構成としている。また、掃引制御
部70では、直線性補正部78をDA変換器74の前に
追加して設けた構成としている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The embodiment of the present invention is an example in which the local oscillator is composed of a varactor tuned VCO. This will be described with reference to FIGS. 1 and 2. The configuration of the entire apparatus is the same as the conventional configuration shown in FIG. 4, but in this, the local oscillator 30 of the frequency conversion unit 50 and the sweep control unit 7 are included.
The composition of 0 is changed. In the local oscillator 30, as shown in FIG. 1, instead of the YTO 40, a varactor tuned V
The configuration is such that CO20 is replaced. Further, the sweep control unit 70 has a configuration in which a linearity correction unit 78 is additionally provided in front of the DA converter 74.

【0014】バラクタチューンドVCO20の内部構成
は、図2に示すように、可変同調回路21と、負性抵抗
回路49と、バッファアンプ48とで構成していて、負
性抵抗回路49と、バッファアンプ48は従来と同様で
ある。可変同調回路21は、マイクロ波用可変容量ダイ
オード24を可変同調素子として使用したタンク回路
(Tank Circuit)であり、集中定数の等価共振用コイル
29と、等価共振用容量28としているが、実際にはマ
イクロ波帯である為、マイクロストリップラインの分布
定数でこれらを形成する。可変容量ダイオード24は、
例えばガリひ素(GaAs)を使用したチューニング用ダ
イオード素子(GaAs Tuning Diode chip)であり数GH
z帯まで適用可能な素子を使用する。可変容量ダイオー
ド24は、このタンク回路とコンデンサ26とで直列に
接続して、全体で共振回路を形成している。そして、直
流電圧である制御電圧38voscは、高抵抗22を通して
可変容量ダイオード24に印加している。
As shown in FIG. 2, the internal structure of the varactor tuned VCO 20 is composed of a variable tuning circuit 21, a negative resistance circuit 49, and a buffer amplifier 48. The negative resistance circuit 49 and the buffer amplifier 48 are provided. 48 is the same as the conventional one. The variable tuning circuit 21 is a tank circuit (Tank Circuit) using a microwave variable capacitance diode 24 as a variable tuning element, and includes a lumped constant equivalent resonance coil 29 and an equivalent resonance capacitance 28. Are in the microwave band, so they are formed by the distributed constants of the microstrip line. The variable capacitance diode 24 is
For example, it is a tuning diode element (GaAs Tuning Diode chip) using gallium arsenide (GaAs).
An element applicable to the z band is used. The variable capacitance diode 24 is connected in series with the tank circuit and the capacitor 26 to form a resonance circuit as a whole. The control voltage 38vosc, which is a DC voltage, is applied to the variable capacitance diode 24 through the high resistance 22.

【0015】ここで、可変容量ダイオード24に与える
制御電圧38voscに対する発振周波数の特性を、図3の
発振周波数の電圧感度特性曲線例に示す。可変容量ダイ
オードは、個々のサンプルA、サンプルB毎に異なった
非直線性曲線を有している。この為、掃引制御部70か
らの制御電圧38voscは、非直線性曲線を直線性補正の
補正変換された制御電圧38voscが供給される。
Here, the characteristic of the oscillation frequency with respect to the control voltage 38vosc given to the variable capacitance diode 24 is shown in an example of the voltage sensitivity characteristic curve of the oscillation frequency of FIG. The variable-capacitance diode has a different non-linear curve for each sample A and sample B. Therefore, the control voltage 38vosc from the sweep control unit 70 is supplied with the control voltage 38vosc obtained by correcting and converting the non-linear curve for linearity correction.

【0016】掃引制御部70の内部構成は、図1に示す
ように、ランプ発生部72と、直線性補正部78と、D
A変換器74と、LPF76とで構成していて、直線性
補正部78を追加して、バラクタチューンドVCO20
の直線性を補正するコードデータ変換処理を追加してい
る。内部の直線性補正テーブル79には、制御電圧38
voscに対する発振周波数特性曲線を求めておいた補正値
79datを、予め格納しておく。ランプ発生部72から
のコードデータ72codを受けて、これをアドレスとす
る直線性補正テーブル79の補正値79datを読みだし
て、コードデータ72codと乗算して直線性補正した変
換コードデータ78codをDA変換器74に供給する。
この結果、バラクタチューンドVCO20は一定周波数
の増加傾きとなる直線性のある掃引周波数を発振出力で
きる。ところで、ランプ発生部72からのコードデータ
全部に対する補正値を直線性補正テーブル79に設ける
のは大きなメモリ容量が必要となる。そこで、直線性補
正は±0.1%以下に収まれば十分なので、所望間隔毎
のコードデータ72codに対する補正値を格納してお
き、この区間のコードデータは直線補間手法により算出
して補正演算する。
The internal structure of the sweep control unit 70 is, as shown in FIG. 1, a ramp generation unit 72, a linearity correction unit 78, and a D
The varactor tuned VCO 20 includes an A converter 74 and an LPF 76, and a linearity correction unit 78 is added.
A code data conversion process to correct the linearity of is added. The internal linearity correction table 79 has a control voltage 38
The correction value 79dat for which the oscillation frequency characteristic curve for vosc has been obtained is stored in advance. Upon receiving the code data 72cod from the ramp generator 72, the correction value 79dat of the linearity correction table 79 having this as an address is read, and the conversion code data 78cod corrected by linearity by multiplication with the code data 72cod is DA converted. Supply to the container 74.
As a result, the varactor tuned VCO 20 can oscillate and output a sweep frequency having a linearity with a constant frequency increasing slope. By the way, providing a correction value for all the code data from the ramp generating section 72 in the linearity correction table 79 requires a large memory capacity. Therefore, it is sufficient for the linearity correction to be within ± 0.1%. Therefore, the correction value for the code data 72cod for each desired interval is stored, and the code data in this section is calculated by the linear interpolation method and the correction calculation is performed. .

【0017】上記実施例の説明では、直線性補正テーブ
ル79への補正値79datの格納を、予め求めておくと
して説明したが、局部発振器30の発振周波数を測定す
る周波数カウンタを内蔵するものにおいては、現在環境
で各コードデータ72codで発振させ、この発振周波数
を所望により随時測定し、これから補正値79datを算
出して直線性補正テーブル79に格納した後、掃引実施
するようにしても良く、同様にして実施できる。
In the above description of the embodiment, the correction value 79dat is stored in the linearity correction table 79 in advance. However, in the case where the frequency counter for measuring the oscillation frequency of the local oscillator 30 is built-in, the correction value 79dat is stored in advance. It is also possible to oscillate with each code data 72cod in the current environment, measure the oscillation frequency at any time as desired, calculate a correction value 79dat from this, store it in the linearity correction table 79, and then execute sweeping. Can be carried out.

【0018】[0018]

【発明の効果】本発明は、以上説明したように構成され
ているので、下記に記載されるような効果を奏する。掃
引制御部70の直線性補正部78は、バラクタチューン
ドVCO20の発振周波数の非直線性を補正して、掃引
周波数が一定周波数の増加傾きとなるように直線性補正
した掃引を可能にする効果が得られる。マイクロ波用可
変容量ダイオード24を可変同調素子としてVCOを構
成し、掃引制御部70の直線性補正部78で発振周波数
の掃引直線性を補正するコードデータに変換してランプ
掃引する局部発振器30は、従来と同等レベルのスペク
トラム測定の周波数確度を維持できる効果が得られる。
これらから、従来よりも安価なスペクトラムアナライザ
の発振源を実現できる効果が得られる。
Since the present invention is configured as described above, it has the following effects. The linearity correction unit 78 of the sweep control unit 70 has the effect of correcting the nonlinearity of the oscillation frequency of the varactor tuned VCO 20 to enable the linearity-corrected sweep so that the sweep frequency has an increasing slope of a constant frequency. can get. A local oscillator 30 that configures a VCO using the variable capacitance diode for microwaves 24 as a variable tuning element, converts it into code data for correcting the sweep linearity of the oscillation frequency by the linearity correction unit 78 of the sweep control unit 70, and performs ramp sweep is used. , It is possible to obtain the effect of maintaining the frequency accuracy of spectrum measurement at the same level as the conventional one.
From these, it is possible to obtain the effect of realizing an oscillation source of a spectrum analyzer which is cheaper than the conventional one.

【0019】[0019]

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

【図1】本発明の、局部発振器30と掃引制御部70の
構成図である。
FIG. 1 is a configuration diagram of a local oscillator 30 and a sweep control unit 70 of the present invention.

【図2】本発明の、バラクタチューンドVCO20の構
成図である。
FIG. 2 is a block diagram of a varactor tuned VCO 20 of the present invention.

【図3】可変容量ダイオード24の発振周波数の電圧感
度特性曲線の例である。
FIG. 3 is an example of a voltage sensitivity characteristic curve of an oscillation frequency of a variable capacitance diode 24.

【図4】従来の、局部発振器30の全体構成図である。FIG. 4 is an overall configuration diagram of a conventional local oscillator 30.

【図5】従来の、YTO40の構成図である。FIG. 5 is a configuration diagram of a conventional YTO 40.

【図6】[Figure 6]

【符号の説明】[Explanation of symbols]

20 バラクタチューンドVCO 21 可変同調回路 24 可変容量ダイオード 26 コンデンサ 28 等価共振用容量 29 等価共振用コイル 30 局部発振器 34、37 分周器 35 積分器 35vosc アナログ電位 36 位相比較器 38 加算器 38vosc 制御電圧 40 YTO(YIG-tuned Oscillator) 40osc 発振周波数信号 41 IV変換器 42 YIG共振器 42b コイル 43 トランジスタ 44 直列フィードバック素子 48 バッファアンプ 49 負性抵抗回路 50 周波数変換部 62 検波部 64 表示演算部 68 表示部 70 掃引制御部 70stt 掃引開始信号 72 ランプ発生部 72cod コードデータ 74 DA変換器 76sweep ランプ信号 76 LPF(ローパスフィルタ) 78 直線性補正部 78cod 変換コードデータ 79 直線性補正テーブル 100 被測定信号 20 varactor tuned VCO 21 variable tuning circuit 24 variable capacitance diode 26 capacitor 28 equivalent resonance capacitance 29 equivalent resonance coil 30 local oscillator 34, 37 frequency divider 35 integrator 35 vosc analog potential 36 phase comparator 38 adder 38 vosc control voltage 40 YTO (YIG-tuned Oscillator) 40osc Oscillation frequency signal 41 IV converter 42 YIG resonator 42b Coil 43 Transistor 44 Series feedback element 48 Buffer amplifier 49 Negative resistance circuit 50 Frequency conversion unit 62 Detection unit 64 Display operation unit 68 Display unit 70 Sweep control unit 70stt Sweep start signal 72 Ramp generation unit 72cod code data 74 DA converter 76 sweep ramp signal 76 LPF (low pass filter) 78 Linearity correction unit 78cod conversion code data 79 Linearity correction table 00 signal to be measured

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 マイクロ波用可変容量ダイオード(2
4)を使用して電圧制御発振器(VCO)を構成する局
部発振器(30)を有して、アナログの掃引ランプ信号
(76sweep)を受けて掃引する局部発振器(30)に
おいて、 上記可変容量ダイオード(24)の電圧制御発振周波数
を、一定傾きの掃引周波数を発生するように直線性補正
する直線性補正部(78)手段を設け、 以上を具備していることを特徴としたスペクトラムアナ
ライザ。
1. A variable capacitance diode for microwaves (2
4) using a local oscillator (30) which constitutes a voltage controlled oscillator (VCO), and which receives and sweeps an analog sweep ramp signal (76sweep), the variable capacitance diode (30) A spectrum analyzer characterized in that a linearity correction section (78) means for correcting the voltage-controlled oscillation frequency of 24) to generate a sweep frequency having a constant slope is provided.
【請求項2】 マイクロ波用可変容量ダイオード(2
4)を使用して電圧制御発振器(VCO)を構成する局
部発振器(30)を有して、アナログの掃引ランプ信号
(76sweep)を受けて掃引する局部発振器(30)に
おいて、 掃引制御部(70)のランプ発生部(72)からのコー
ドデータ(72cod)を受けて、電圧制御発振器の発振
周波数を、ランプ掃引と比例した一定周波数の増加傾き
となる直線性補正処理した変換コードデータ(78co
d)を出力してアナログの掃引ランプ信号(76sweep)
による掃引周波数を直線性補正する直線性補正部(7
8)手段を設け、 以上を具備していることを特徴としたスペクトラムアナ
ライザ。
2. A variable capacitance diode for microwaves (2
In the local oscillator (30) which has a local oscillator (30) which constitutes a voltage controlled oscillator (VCO) using 4) and which receives and sweeps an analog sweep ramp signal (76sweep), a sweep control unit (70) ) Received the code data (72cod) from the ramp generator (72), the conversion frequency of the voltage-controlled oscillator is converted into linearity correction processing that has an increasing slope of a constant frequency proportional to the ramp sweep (78cod).
d) is output to output an analog sweep ramp signal (76sweep)
Linearity correction unit (7
8) A spectrum analyzer provided with means and having the above.
JP3162095A 1995-01-27 1995-01-27 Spectrum analyzer Pending JPH08201450A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP3162095A JPH08201450A (en) 1995-01-27 1995-01-27 Spectrum analyzer
PCT/JP1996/000131 WO1996023232A1 (en) 1995-01-27 1996-01-25 Spectrum analyzer
DE19680092T DE19680092C2 (en) 1995-01-27 1996-01-25 Spectrum analyzer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3162095A JPH08201450A (en) 1995-01-27 1995-01-27 Spectrum analyzer

Publications (1)

Publication Number Publication Date
JPH08201450A true JPH08201450A (en) 1996-08-09

Family

ID=12336267

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3162095A Pending JPH08201450A (en) 1995-01-27 1995-01-27 Spectrum analyzer

Country Status (3)

Country Link
JP (1) JPH08201450A (en)
DE (1) DE19680092C2 (en)
WO (1) WO1996023232A1 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008193389A (en) * 2007-02-05 2008-08-21 Nippon Dempa Kogyo Co Ltd Synchronized sweep synthesizer
JP2014197764A (en) * 2013-03-29 2014-10-16 アンリツ株式会社 Magnetically tuned device driver, signal analysis device using the same, and method for driving magnetically tuned device

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102004054261A1 (en) * 2004-11-09 2006-05-11 Hameg Gmbh Spectrum analyzer and method for measuring frequency levels

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5223591B2 (en) * 1972-06-20 1977-06-25
US4129832A (en) * 1977-06-20 1978-12-12 Harris Corporation Method and means for linearizing a voltage controlled oscillator sweep generator
JP2704626B2 (en) * 1988-04-01 1998-01-26 株式会社アドバンテスト Frequency converter
JPH0373021U (en) * 1989-11-17 1991-07-23
US5347176A (en) * 1993-02-17 1994-09-13 Hewlett-Packard Company Analog ramp generator with digital correction

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008193389A (en) * 2007-02-05 2008-08-21 Nippon Dempa Kogyo Co Ltd Synchronized sweep synthesizer
JP2014197764A (en) * 2013-03-29 2014-10-16 アンリツ株式会社 Magnetically tuned device driver, signal analysis device using the same, and method for driving magnetically tuned device

Also Published As

Publication number Publication date
DE19680092C2 (en) 2000-10-26
DE19680092T1 (en) 1997-04-24
WO1996023232A1 (en) 1996-08-01

Similar Documents

Publication Publication Date Title
US4940950A (en) Frequency synthesis method and apparatus using approximation to provide closely spaced discrete frequencies over a wide range with rapid acquisition
Musch et al. A highly linear frequency ramp generator based on a fractional divider phase-locked-loop
US4374358A (en) Apparatus for measuring the oscillation frequency of a voltage controlled oscillator
JPS60203007A (en) Frequency modulator circuit
JPS63219225A (en) Clock signal generator
US5130670A (en) Phase-locking circuit for swept synthesized source preferably having stability enhancement circuit
JPH08292214A (en) Precise voltage measuring system
JPH08201450A (en) Spectrum analyzer
Helfrick Electrical spectrum and network analyzers: a practical approach
JPH01168122A (en) Frequency synthesizer
US4287469A (en) Process and circuit arrangement for the measuring of coefficients of message-transmission equipment
JP2010190836A (en) Frequency measuring device and inspection system
JPH07209351A (en) Local oscillator for spectrum analyzer
Musch et al. Fractional divider concepts with phase-lock-control for the generation of precise linear frequency ramps
JP4036636B2 (en) Phase-locked-loop oscillator with a function to compensate for the loop gain
Musch et al. Measurement of the ramp linearity of extremely linear frequency ramps using a fractional dual loop structure
JPH0718188Y2 (en) Phase locked loop circuit
Meniailo et al. Self-oscillator tracking filter with nonlinear feedback
JPH07113829A (en) Time/frequency measuring apparatus
JP3144501B2 (en) Frequency synthesizer
JPS5817710A (en) Sweep oscillator
SU1402955A2 (en) Devije for measuring the mean variation rate and linearity of modulation characteristics of frequency-modulated generators
US3609575A (en) Harmonic sensitive network for phase lock of an oscillator
Woo et al. A digital microwave frequency lock system
Alekseev Direct digital frequency synthesizers: Potentialities and limitations for microwave spectroscopy applications

Legal Events

Date Code Title Description
A02 Decision of refusal

Free format text: JAPANESE INTERMEDIATE CODE: A02

Effective date: 20030318