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JP3568366B2 - Optical pulse generator - Google Patents
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JP3568366B2 - Optical pulse generator - Google Patents

Optical pulse generator Download PDF

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Publication number
JP3568366B2
JP3568366B2 JP18215597A JP18215597A JP3568366B2 JP 3568366 B2 JP3568366 B2 JP 3568366B2 JP 18215597 A JP18215597 A JP 18215597A JP 18215597 A JP18215597 A JP 18215597A JP 3568366 B2 JP3568366 B2 JP 3568366B2
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JP
Japan
Prior art keywords
optical modulator
optical
pulse generator
frequency
capacitor
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
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JP18215597A
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Japanese (ja)
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JPH1124018A (en
Inventor
佐藤  憲史
勇 小高
紘一 脇田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NTT Inc
NTT Inc USA
Original Assignee
Nippon Telegraph and Telephone Corp
NTT Inc USA
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
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Priority to JP18215597A priority Critical patent/JP3568366B2/en
Publication of JPH1124018A publication Critical patent/JPH1124018A/en
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  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
  • Semiconductor Lasers (AREA)

Description

【0001】
【発明の属する技術分野】
本発明は、高周波帯で高速変調を行う光パルス発生装置に関するものである。
【0002】
【従来の技術】
図5(a)は従来の光パルス発生装置を示す概念図である。図に示すように、1は半導体利得部、2は光変調器であり、半導体利得部1は外部DC電流源3から一定電流が注入され、光出力を発生する。光変調器2は、外部高周波電源4からバイアスティー6を介して、高周波電圧を伝搬するためのストリップ線路7と、インダクタンスを有する金線ワイヤ8で接続され、光変調器2に高周波電圧を加えることにより光強度が変調される。また、バイアスティー6を介して外部電圧源5からバイアス電圧を加えることができる。半導体利得部1と光変調器2より構成される光共振器において光往復時間の逆数で決まる周波数で光変調器2を変調すると、いわゆる能動モード同期により短いパルス光出力が得られる。9はストリップ線路7とのインピーダンス整合をとるための抵抗(通常50オーム)であり、光変調器2と並列に接続される。図5(b)はその等価回路であり、光変調器2は抵抗とコンデンサより構成されるというモデルを用いている。図6に光変調器2の応答と反射損失の周波数特性の計算結果を示した。
【0003】
【発明が解決しようとする課題】
しかし、このような従来の光パルス発生装置においては、周波数が高くなるに伴い電気的な反射が増大し、高周波電力が有効に光変調器2に供給されず、効果的に光パルスが得られにくいという問題があった。
【0004】
本発明は上述の課題を解決するためになされたもので、高周波帯で変換効率が高く、電気的な反射が少ない光パルス発生装置を提供することを目的とする。
【0005】
【課題を解決するための手段】
高周波電圧を加えることにより光の強度あるいは位相を変調する光変調器を含む光パルス発生装置において、上記高周波電圧を伝搬する線路と上記光変調器とをインダクタンスを有する第1の導体で接続し、上記光変調器とコンデンサとをインダクタンスを有する第2の導体で接続し、上記コンデンサの他方の電極を直接接地し、かつ、上記第2の導体の長さを上記光変調器の長さの5倍以下とする。
【0008】
【発明の実施の形態】
図1(a)は本発明に係る光パルス発生装置の実施の形態を示す概念図である。図に示すように、半導体利得部1は外部DC電流源3より一定電流が注入され光出力を発生する。約100ミクロン長の光変調器2は、外部高周波電源4からバイアスティー6を介して、高周波電圧を伝搬するためのストリップ線路7とインダクタンスを有する約250ミクロン長の金線ワイヤ8(第1の導体)で接続され、かつ、光変調器2の近傍に配置された約250ミクロン角のチップコンデンサ11の一方の電極とインダクタンスを有する約300ミクロン長の金線ワイヤ10(第2の導体)で接続され、コンデンサ11の他方の電極は直接接地されている。光変調器2にはバイアスティー6を介して外部DC電圧源5からバイアス電圧を加え、さらに外部高周波電源4からの高周波電圧を重畳することにより光強度が変調される。半導体利得部1と光変調器2より構成される光共振器において光往復時間の逆数で決まる周波数で光変調器2を変調すると、いわゆる能動モード同期により短いパルス光出力が得られる。光変調器2に接続されたコンデンサ11により、バイアスティー6を介して外部DC電圧源5からバイアス電圧を加えることが可能となる。コンデンサ11は直流成分を通さないために設けている。
【0009】
図1(b)はその等価回路であり、ストリップ線路7の特性インピーダンスは50オーム、金線ワイヤ8のインダクタンスLは180pH、光変調器2の直列抵抗Rは10オーム、容量Cは0.27pF、金線ワイヤ10のインダクタンスLは220pH、コンデンサ11の容量は100pFとしている。図2に光変調器2の応答と反射損失の周波数特性の計算結果を示した。図に示すように、26GHz近傍で反射が急激に低下し、変調応答も16GHzから26GHz近傍で大きくなることがわかる。反射が最小となる周波数は光変調器2の容量Cと金線ワイヤ10のインダクタンスLによってほぼ決まり、容量CとインダクタンスLが低下すると周波数が増大する。光変調器2の帯域はほぼその長さに比例しており、また、インダクタンスLは金線ワイヤ10の長さに比例しているため、光変調器2の帯域において反射を減らすためには、金線ワイヤ10の長さを小さくする必要がある。
【0010】
反射が最小となる周波数はおおよそ、fres=1/(2π√(LC))で与えられる。一方、変調器帯域はおおよそ、f=1/(πRC)で与えられる。ここでRは伝送路の特性インピーダンスであり通常50オームである。反射が最小となる周波数と変調器帯域をほぼ等しくする条件から、L=R C/4という関係が導出される。光変調器2の容量Cは光変調器2の長さ100μmあたり0.2〜0.4pFであり、前式からLは125〜250pHと算出される。一方、金線ワイヤ10のインダクタンスLは100μmあたり50〜100pHである。これらの結果から金線ワイヤ10の長さを光変調器2の長さのおおよそ5倍以下にすることにより、高周波で反射が少なく、変調効率の高い回路構成が実現できる。
【0011】
以上の回路構成は光変調器単体やレーザと集積化された光変調器においても同様に有効である。
【0012】
図3(a)は本発明に係る光パルス発生装置の参考例を示す概念図である。図に示すように、図1(a)と同一の構成に加えて、光変調器2とコンデンサ11との間に抵抗50オーム程度のチップ状の抵抗9を直列に接続しており、反射の少ない帯域が拡大する構成となっている。その等価回路を図3(b)に示した。図4には光変調器2の応答と反射損失の周波数特性の計算結果を示した。図に示すように、実施の形態の場合と同様に、高周波帯で反射が少なく、変調効率の高い回路構成が実現できる。なお、抵抗9はコンデンサ11とアースとの間に挿入しても同様の効果が得られる。
【0013】
以上の回路構成は光変調器単体やレーザと集積化された光変調器においても同様に有効である。
【0014】
【発明の効果】
以上説明したように、本発明に係る光パルス発生装置においては、光変調器の5倍以下の長さの導体とコンデンサを光変調器に接続することにより、高周波帯で変調効率が高く、電気的な反射損失の少ない光パルス発生装置が実現できる。
【図面の簡単な説明】
【図1】(a)は本発明に係る光パルス発生装置の実施の形態を示す概念図、(b)はその等価回路である。
【図2】図1の光変調器の応答と反射損失の周波数特性の計算結果である。
【図3】(a)は本発明に係る光パルス発生装置の参考例を示す概念図、(b)はその等価回路である。
【図4】図3の光変調器の応答と反射損失の周波数特性の計算結果である。
【図5】(a)は従来の光パルス発生装置を示す概念図、(b)はその等価回路である。
【図6】図5の光変調器の応答と反射損失の周波数特性の計算結果である。
【符号の説明】
1 半導体利得部
2 光変調器
3 DC電流源
4 高周波電源
5 DC電圧源
6 バイアスティー
7 ストリップ線路
8 金線ワイヤ
9 抵抗
10 金線ワイヤ
11 コンデンサ
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to an optical pulse generator that performs high-speed modulation in a high frequency band.
[0002]
[Prior art]
FIG. 5A is a conceptual diagram showing a conventional optical pulse generator. As shown in the figure, reference numeral 1 denotes a semiconductor gain unit, and 2 denotes an optical modulator. The semiconductor gain unit 1 receives a constant current from an external DC current source 3 to generate an optical output. The optical modulator 2 is connected to a strip line 7 for transmitting a high-frequency voltage from an external high-frequency power supply 4 via a bias tee 6 via a gold wire 8 having an inductance, and applies a high-frequency voltage to the optical modulator 2. This modulates the light intensity. Also, a bias voltage can be applied from the external voltage source 5 via the bias tee 6. When the optical modulator 2 is modulated at a frequency determined by the reciprocal of the optical round-trip time in the optical resonator including the semiconductor gain unit 1 and the optical modulator 2, a short pulse light output is obtained by so-called active mode locking. Reference numeral 9 denotes a resistor (normally 50 ohms) for impedance matching with the strip line 7, and is connected in parallel with the optical modulator 2. FIG. 5B shows an equivalent circuit thereof, which uses a model in which the optical modulator 2 includes a resistor and a capacitor. FIG. 6 shows the calculation results of the frequency characteristics of the response and the return loss of the optical modulator 2.
[0003]
[Problems to be solved by the invention]
However, in such a conventional optical pulse generator, as the frequency increases, the electrical reflection increases, and high-frequency power is not effectively supplied to the optical modulator 2, and an optical pulse can be obtained effectively. There was a problem that it was difficult.
[0004]
The present invention has been made to solve the above-described problems, and has as its object to provide an optical pulse generator having high conversion efficiency in a high frequency band and low electrical reflection.
[0005]
[Means for Solving the Problems]
In an optical pulse generator including an optical modulator that modulates the intensity or phase of light by applying a high-frequency voltage, a line that propagates the high-frequency voltage and the optical modulator are connected by a first conductor having an inductance, The optical modulator and the capacitor are connected by a second conductor having inductance, the other electrode of the capacitor is directly grounded, and the length of the second conductor is set to 5 times the length of the optical modulator. Double or less.
[0008]
BEST MODE FOR CARRYING OUT THE INVENTION
FIG. 1A is a conceptual diagram showing an embodiment of an optical pulse generator according to the present invention. As shown in the figure, a constant current is injected from an external DC current source 3 into a semiconductor gain section 1 to generate an optical output. The optical modulator 2 having a length of about 100 microns has a strip line 7 for transmitting a high-frequency voltage from an external high-frequency power supply 4 via a bias tee 6 and a gold wire 8 having a length of about 250 microns having inductance. And a metal wire 10 (second conductor) having a length of about 300 microns having an inductance with one electrode of a chip capacitor 11 having a size of about 250 microns arranged near the optical modulator 2. Connected, and the other electrode of the capacitor 11 is directly grounded. The light intensity is modulated by applying a bias voltage from the external DC voltage source 5 to the optical modulator 2 via the bias tee 6 and superimposing a high frequency voltage from the external high frequency power supply 4. When the optical modulator 2 is modulated at a frequency determined by the reciprocal of the optical round-trip time in the optical resonator including the semiconductor gain unit 1 and the optical modulator 2, a short pulse light output is obtained by so-called active mode locking. The capacitor 11 connected to the optical modulator 2 makes it possible to apply a bias voltage from the external DC voltage source 5 via the bias tee 6. The capacitor 11 is provided to prevent a DC component from passing.
[0009]
1 (b) is an equivalent circuit, the characteristic impedance of the strip line 7 50 ohms, the inductance L 1 of the gold wire 8 180PH, series resistance R of the optical modulator 2 is 10 ohms, the capacitor C 0. 27pF, the inductance L 2 of the gold wire 10 is 220PH, capacitance of the capacitor 11 is set to 100 pF. FIG. 2 shows a calculation result of the frequency characteristics of the response and the return loss of the optical modulator 2. As shown in the figure, it can be seen that the reflection sharply drops around 26 GHz and the modulation response also increases from 16 GHz to around 26 GHz. Frequency reflection is minimized substantially determined by the inductance L 2 of the capacitor C and the gold wire wire 10 of the optical modulator 2, the frequency is increased the capacitance C and the inductance L 2 is decreased. Band of the optical modulator 2 is substantially proportional to its length, also the inductance L 2 is proportional to the length of the gold wire 10, in order to reduce the reflection in the band of the optical modulator 2 It is necessary to reduce the length of the gold wire 10.
[0010]
The frequency at which the reflection is minimized is approximately given by f res = 1 / (2π√ (L 2 C)). On the other hand, the modulator band is approximately given by f m = 1 / (πR Z C). Here, RZ is the characteristic impedance of the transmission line, which is usually 50 ohms. The condition of L 2 = R Z 2 C / 4 is derived from the condition that the frequency where the reflection is minimized and the modulator band are almost equal. The capacity C of the optical modulator 2 is 0.2 to 0.4 pF per 100 μm of the length of the optical modulator 2, and L2 is calculated to be 125 to 250 pH from the above equation. On the other hand, the inductance L 2 of the gold wire 10 is 50~100pH per 100 [mu] m. From these results, by setting the length of the gold wire 10 to be approximately five times or less the length of the optical modulator 2, a circuit configuration with low reflection at high frequency and high modulation efficiency can be realized.
[0011]
The above circuit configuration is similarly effective for an optical modulator alone or an optical modulator integrated with a laser.
[0012]
FIG. 3A is a conceptual diagram showing a reference example of the optical pulse generator according to the present invention. As shown in the figure, in addition to the same configuration as in FIG. 1A, a chip-shaped resistor 9 having a resistance of about 50 ohms is connected in series between the optical modulator 2 and the capacitor 11 to provide a reflection. The configuration is such that a small band is expanded. The equivalent circuit is shown in FIG. FIG. 4 shows the calculation results of the frequency characteristics of the response and the return loss of the optical modulator 2. As shown in the figure, as in the case of the embodiment, a circuit configuration with little reflection in a high frequency band and high modulation efficiency can be realized. The same effect can be obtained by inserting the resistor 9 between the capacitor 11 and the ground.
[0013]
The above circuit configuration is similarly effective for an optical modulator alone or an optical modulator integrated with a laser.
[0014]
【The invention's effect】
As described above, in the optical pulse generator according to the present invention, by connecting a conductor and a capacitor having a length of 5 times or less of the optical modulator to the optical modulator, the modulation efficiency is high in the high frequency band, An optical pulse generator with a small reflection loss can be realized .
[Brief description of the drawings]
FIG. 1A is a conceptual diagram showing an embodiment of an optical pulse generator according to the present invention, and FIG. 1B is an equivalent circuit thereof.
FIG. 2 is a calculation result of a frequency characteristic of a response and a return loss of the optical modulator of FIG. 1;
3A is a conceptual diagram illustrating a reference example of an optical pulse generator according to the present invention, and FIG. 3B is an equivalent circuit thereof.
FIG. 4 is a calculation result of a frequency characteristic of a response and a return loss of the optical modulator of FIG. 3;
5A is a conceptual diagram showing a conventional optical pulse generator, and FIG. 5B is an equivalent circuit thereof.
FIG. 6 is a calculation result of a frequency characteristic of a response and a return loss of the optical modulator of FIG. 5;
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 Semiconductor gain part 2 Optical modulator 3 DC current source 4 High frequency power supply 5 DC voltage source 6 Bias tee 7 Strip line 8 Gold wire 9 Resistance 10 Gold wire 11 Capacitor

Claims (1)

高周波電圧を加えることにより光の強度あるいは位相を変調する光変調器を含む光パルス発生装置において、上記高周波電圧を伝搬する線路と上記光変調器とがインダクタンスを有する第1の導体で接続され、上記光変調器とコンデンサとがインダクタンスを有する第2の導体で接続され、上記コンデンサの他方の電極が直接接地され、かつ、上記第2の導体の長さが上記光変調器の長さの5倍以下であることを特徴とする光パルス発生装置。In an optical pulse generator including an optical modulator that modulates the intensity or phase of light by applying a high-frequency voltage, a line that propagates the high-frequency voltage and the optical modulator are connected by a first conductor having an inductance, The optical modulator and the capacitor are connected by a second conductor having inductance, the other electrode of the capacitor is directly grounded, and the length of the second conductor is 5 times the length of the optical modulator. An optical pulse generator characterized in that the number is not more than twice.
JP18215597A 1997-07-08 1997-07-08 Optical pulse generator Expired - Lifetime JP3568366B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18215597A JP3568366B2 (en) 1997-07-08 1997-07-08 Optical pulse generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18215597A JP3568366B2 (en) 1997-07-08 1997-07-08 Optical pulse generator

Publications (2)

Publication Number Publication Date
JPH1124018A JPH1124018A (en) 1999-01-29
JP3568366B2 true JP3568366B2 (en) 2004-09-22

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4640733B2 (en) * 1999-11-30 2011-03-02 Okiセミコンダクタ株式会社 Semiconductor device
JP3975786B2 (en) 2002-03-12 2007-09-12 日本電気株式会社 Optical modulator excitation circuit
JP2007096928A (en) * 2005-09-29 2007-04-12 Oki Electric Ind Co Ltd Frequency signal combining / separating circuit, optical wireless fusion transmission system using the circuit, optical modulation module, and optical communication system

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