JP3412776B2 - Optical time division separation circuit - Google Patents

Description

Detailed Description of the Invention

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention is used in an optical repeater, an optical terminal unit in ultrahigh-speed optical communication, or a time division demultiplexing circuit for high speed time division multiplexed digital optical signals required in optical signal processing.

[0002]

2. Description of the Related Art A conventional optical time division demultiplexing circuit will be described below with reference to the drawings.

FIG. 5 shows the configuration of a conventional optical time division demultiplexing circuit. This conventional optical time division demultiplexing circuit includes a signal light incident port 11 to which signal light is input, and a voltage controlled oscillator (VCO) that generates a timing signal for time division demultiplexing.
12, a low-frequency oscillator 13 that generates a low-frequency signal,
A microwave band mixer 14 for mixing the output of the VCO 12 and the output of the low frequency oscillator 13, an optical clock pulse generator 15 for outputting an optical pulse train of wavelength λclk controlled by the output of the mixer 14, and a voltage controlled oscillator 12 A control optical pulse generator 16 that outputs an optical pulse train of wavelength λcont controlled by the output of the optical signal, an optical demultiplexer 18 that branches the input signal light, and a signal that is branched from the output light of the optical clock pulse generator 15. The optical combiner 17 for combining the light, the optical combiner 19 for combining the output light of the control light pulse generator 16 and the branched signal light, and the light combined by the optical combiner 17 are input. A traveling-wave type semiconductor laser amplifier 20 for applying a nonlinear optical effect, a time-division demultiplexing circuit 21 for inputting the light multiplexed by the optical multiplexer 19 and outputting a demultiplexed optical time-division signal to an optical output port 25, Traveling wave type semiconductor laser amplifier 20
Optical bandpass filter (BPF) 22 that allows the light of wavelength λclk to pass from the output of the optical path and a light receiving circuit 23 that converts the light that has passed through the optical bandpass filter 22 into an electrical signal.
And a phase comparator 24 for performing phase comparison between the converted electric signal and the signal of the low frequency oscillator 13. In addition,
A frequency multiplier 26 is arranged between the low frequency oscillator 13 and the phase comparator 24.

As described above, in the conventional receiving system using all-optical signal processing, the optical signal is divided into two by the optical demultiplexer 18, one of which is a timing extraction circuit and the other of which is a time division demultiplexing circuit 21. Was typing in.

For details of this conventional circuit, see [1] S. Kawawanishi et al., "100 Gbit / s, 200 km optical.
transmission experiment using extremely low jitter
PLL timing extraction and all-optical demultiplex
ing based on polarization insensitive four-wave mi
xing, "Electron. Lett., 1994, 301, pp. 800-801.

First, the operation of timing extraction in the circuit shown in FIG. 5 will be described. The signal light pulse incident from the signal light incident port 11 is branched by the optical demultiplexer 18,
One is input to the traveling wave type semiconductor laser amplifier 20 through the optical clock generated from the optical clock pulse generator 15 and the optical multiplexer 17. In the traveling-wave type semiconductor laser amplifier 20, the nonlinear optical effect of the amplifier causes the amplifier to generate light of the third wavelength proportional to the product of the intensities of the signal light and the clock light. Examples of the non-linear optical effect for generating the light of the third wavelength include four-wave mixing and sum frequency light generation.

FIG. 6 shows the relationship between the wavelength λsig of the incident signal light and the wavelength λclk of the clock light in the case of four-wave mixing as an example. Here, the wavelength λclk of the four-wave mixed light generated.
The relationship of 1 / λclk. _FWM = 2 / λsig −1 / λclk (1) is established between the _FWM and the input light wavelength. In the case of sum frequency light generation, wavelength Ramudaclk of the generated sum frequency light. The relationship between the input light wavelength of the _SAM, which is _{1 / λclk. SAM = 1 /} λsig + 1 / λclk (2). Here, the third wavelength generated by appropriately selecting the wavelength λsig of the signal light and the wavelength λclk of the clock light.
Only the light of the wavelength of can be extracted by the optical bandpass filter 22. In fact, if the wavelength difference between adjacent lights is about 10 nm or more, they can be separated by using a wavelength separation filter currently on the market. The light separated by the optical bandpass filter 22 is received by the light receiving circuit 23 through the optical bandpass filter 22 and input to one of the phase comparators 24.

Next, the oscillation frequency of the voltage controlled oscillator 12 is set to f ₀ . As the value of f ₀ , the signal light incident port 11
It is set so that the bit rate of the signal light input from is nf ₀ (n is an integer of 1 or more). The output of the voltage controlled oscillator 12 is frequency-shifted by the low frequency oscillator 13 and the mixer 14, and the optical clock pulse generator 15
And the repetition frequency is f ₀ + Δf (or f ₀ −
An optical clock pulse of Δf or f ₀ ± Δf) is generated. In the all-optical time division demultiplexing circuit targeted by the present invention, the waveform of the optical clock pulse is not a sine wave,
It is necessary that the pulse width is narrow and that it contains harmonic components.

Now, the time waveform Pc of the optical pulse train to be generated
If (t) is Gaussian, it is expressed by the following equation (3).

[0010]

[Equation 1] Here, A and α are constants and T = 1 / (f ₀ + Δf). Expanding this Pc (t) into a Fourier series gives the following (4)
It becomes like a formula.

[0011]

[Equation 2] Looking at this equation (4), the n-th harmonic component n
It can be seen that (f ₀ + Δf) exists. This n-th harmonic component decreases as the coefficient increases as n increases, but when the pulse width is narrow (α is small), the coefficient increases to generate the n-th harmonic of sufficient strength. Is possible.

In order to generate a correlation signal of a sufficient level for signal light of high bit rate, it is necessary that the pulse width of the generated clock pulse is narrow. At present, it is relatively easy to generate an optical pulse having a pulse width of 5 ps or less by using a gain switch semiconductor laser or a mode-locked laser as an ultrashort optical pulse light source. Correlation detection can be performed for optical signals of s or more.

For simplicity, assume that the envelopes of the optical signal pulse and the optical clock are sine waves, and Ps (t) and Ps respectively.
Let c (t) be expressed as in the following equations (5) and (6).

Ps (t) = Ps {1 + sin n (2πf ₀ t + φ (t))} (5) Pc (t) = Pc {1 + sin 2nπ (f ₀ + Δf) t} (6) where Ps and Pc are It is a constant. Further, φ (t) is a phase difference (relative time difference between pulse positions) between the optical signal pulse and the optical clock, and this amount is an amount that should be controlled to 0 or a constant value by the PLL.

The photocurrent Os (t) when the correlation signal generated by inputting these two lights to the optical correlation detector is input to the light receiving circuit (eg PIN-PD) is expressed by the following equation (7). .

[0016]

[Equation 3] Here, e is the charge of the electron, η is the quantum efficiency of PIN-PD, and hν is the energy of the photon. The last term of the equation (7) is the nΔf component generated by the correlation with the optical clock. As is clear, the relative fluctuation φ (t) of the phase difference between the optical signal pulse and the optical clock pulse is
It is replaced with the phase fluctuation nφ (t) included in the f component. The output of this Δf component and the original low frequency oscillator 1
If the phase comparator 24 compares the Δf signal output of No. 3 with the output multiplied by n by the frequency multiplier 26, the change of the phase φ (t), that is, the phase difference component is detected. By feeding back to the oscillator 12, PL
L motion is achieved.

When n = 1, that is, when the clock frequency and the signal light bit rate are the same, the frequency multiplier 26 is unnecessary.

The control light pulse generator 16 is driven by the clock whose timing is extracted as described above, and this control light pulse is incident on the time division demultiplexing circuit 21 through the optical multiplexer 19 to perform time division demultiplexing of the signal light. Done.

[0019]

In such a configuration of the conventional example, the power of the optical signal is branched in the receiving system and is input to the PLL circuit and the optical time division demultiplexing circuit. In this conventional configuration, it is necessary to separately prepare an optical branching device, a timing extracting circuit, and an optical time division demultiplexing circuit as an optical branching unit in the receiving system, which not only complicates the entire receiving system but also reduces the signal light. There is a problem that the light receiving sensitivity is deteriorated due to the loss of light caused by the branching.

An object of the present invention is to solve the above-mentioned problems and to prevent a loss of light in the light receiving system, and to use a single nonlinear optical element using a nonlinear optical medium in the light receiving system to provide a timing extraction circuit, An object of the present invention is to provide a configuration for realizing both functions of the optical time division demultiplexing circuit at the same time.

Another object of the present invention is to provide an optical time division demultiplexing circuit having both functions of timing extraction and time division demultiplexing easily by using a semiconductor laser amplifier or an optical fiber known as a non-linear optical medium. To provide.

Another object of the present invention is to provide an optical time division demultiplexing circuit that is small in size and can realize ultrahigh speed operation and can use ultrahigh speed optical communication and optical signal processing.

[0023]

The present invention is directed to a first optical pulse light source for generating an optical pulse train of a first wavelength, a second optical pulse light source for generating an optical pulse train of a second wavelength, and an optical light source. A nonlinear medium, means for inputting the input signal light of the third wavelength, the optical pulse train of the first wavelength and the optical pulse train of the second wavelength to the optical nonlinear medium, and the nonlinearity of the optical nonlinear medium Output light of the first optical pulse light source and the second optical pulse light source, means for separating the light of the fourth and fifth wavelengths generated by the optical effect, and timing extraction from the light of the fourth wavelength Means for controlling the timing of the pulse, the light of the fourth wavelength is a signal proportional to the product of the intensity of the optical pulse of the first wavelength and the signal light, the light of the fifth wavelength Is the optical pulse of the second wavelength and the signal light A signal proportional to the product of the intensity, wherein the fifth wavelength light is output as a time division demultiplexing signals.

The frequency of the output optical pulse train of the first optical pulse light source is preferably set to a value deviating from the frequency corresponding to the bit rate of the signal light by Δf.

Further, the first wavelength and the second wavelength are such that the light of the first wavelength and the light of the third wavelength to the fourth wavelength are the optical nonlinearity with respect to the third wavelength. 4 in the medium
It is preferable that the wavelength relationship that is generated by light wave mixing and that the light of the second wavelength and the light of the third wavelength to the light of the fifth wavelength are generated by the four light wave mixing in the optical nonlinear medium is set. .

Further, the first wavelength and the second wavelength are such that the light of the first wavelength and the light of the third wavelength to the fourth wavelength are the optical nonlinearity with respect to the third wavelength. Generated as sum frequency light in the medium, the light of the second wavelength and the light of the third wavelength to the light of the fifth wavelength are set in a wavelength relationship in which they are generated as sum frequency light in the optical nonlinear medium. It is preferable that

Further, the means for controlling the timing of the output light pulse of the first light pulse light source and the second light pulse light source comprises the timing signal extracted from the separated light of the fourth wavelength and the first light pulse. A loopback control circuit for feedback-controlling the output timing of the first optical pulse light source and the second optical pulse light source so that the phase error becomes smaller by comparing with the timing signal of the optical pulse light source. preferable.

The optical nonlinear medium may be a semiconductor laser amplifier or an optical fiber.

Further, it is preferable to provide an optical bandpass filter for passing the light of the fourth and fifth wavelengths, respectively, after the means for separating the light of the fourth and fifth wavelengths.

[0030]

A signal light pulse and a control light pulse of two wavelengths are made incident on a nonlinear optical medium, and the fourth wavelength and the fifth wavelength generated between the two control light pulses and the signal light pulse by the nonlinear optical effect. One of the wavelengths is used for timing extraction and the other for time division separation. The timing extracted signal is fed back to the voltage controlled oscillator,
Is configured.

As a result, it is not necessary to branch the signal light into the time division demultiplexing circuit and the timing extraction circuit using the optical branching device, and no optical loss occurs in the light receiving system. Moreover, since two signals can be separated by a single nonlinear optical medium, the number of constituent elements of the circuit can be reduced and the size can be reduced.

[0032]

Embodiments of the present invention will be described below with reference to the drawings.

FIG. 1 is a diagram showing the configuration of the first embodiment of the present invention. The all-optical time division demultiplexing circuit according to the first embodiment includes a signal light incident port 101 and a control light pulse generator 102.
, Optical clock pulse generator 103, and optical multiplexer 10
5, 106, the optical nonlinear medium 107, and the optical demultiplexer 108
, Timing extraction circuit 109, and optical output port 110
It has a configuration including and. Regarding the connection, the control optical pulse generator 102 and the optical clock pulse generator 10 will be described.
The output light of No. 3 is input to the optical multiplexer 105. Optical multiplexer 1
The output of 05 and the signal light incident port 101 are connected to the optical multiplexer 106.
Is connected to the input side of. The output of the optical multiplexer 106 is input to the optical nonlinear medium 107, and the output of the optical nonlinear medium 107 is input to the optical demultiplexer 108. Optical demultiplexer 108
One of the outputs is input to the timing extraction circuit 109,
The output of the timing extraction circuit 109 is input to the control light pulse generator 102. The control light pulse generator 102
And the optical clock pulse generator 103 operate in synchronization with each other. The other output of the optical demultiplexer 108 is guided to the optical output port 110.

In the configuration of FIG. 1, an optical bandpass filter 111 is provided between the optical demultiplexer 108 and the timing extraction circuit 109, and an optical bandpass filter 111 is provided between the optical demultiplexer 108 and the optical output port 110. A pass filter 114 is provided.

The features of the first embodiment are that an optical clock pulse generator 103 which is a first optical pulse light source for generating an optical pulse train of a first wavelength (λclk) and a second wavelength (λcont). ), A control light pulse generator 102 which is a second light pulse light source for generating a light pulse train, an optical nonlinear medium 107, a signal light of a third wavelength and a first wavelength input from the signal light incident port 101. Optical pulse trains and the optical pulse trains of the second wavelength are incident on the optical nonlinear medium 107, and the fourth and fifth wavelengths generated by the nonlinear optical effect of the optical nonlinear medium 107. Demultiplexer 10 as a means for separating the light of
8 and the timing extraction from the light of the fourth wavelength, the control optical pulse generator 102 and the optical clock pulse generator 1
And a timing extraction circuit 109 as a means for controlling the timing of the output optical pulse of 03, the light of the fourth wavelength is a signal proportional to the product of the intensities of the optical pulse of the first wavelength and the signal light, The light of the fifth wavelength is a signal proportional to the product of the intensities of the optical pulse of the second wavelength and the signal light, and the light of the fifth wavelength is output from the optical output port 110 as a time-division separated signal. There is something to do.

Next, the operation of the first embodiment will be described.

First, a signal light pulse is incident from the signal light incident port 101 and enters the optical multiplexer 106. On the other hand, the control light pulse having the wavelength λcont generated from the control light pulse generator 102 is input to the optical nonlinear medium 107 through the optical multiplexers 105 and 106. Further, an optical clock pulse having a wavelength λclk synchronized with the repetition of the control optical pulse is generated from the optical clock pulse generator 103, and the optical multiplexer 10
The light is input to the optical nonlinear medium 107 through 5 and 106. Here, reference numeral 104 connecting the control optical pulse generator 102 and the optical clock pulse generator 103 indicates a signal line for synchronizing both.

The frequency of the control light pulse generated by the control light pulse generator 102 is set to f ₀ / N which is an integral fraction of the frequency f ₀ corresponding to the bit rate of the incident signal. However, N is an integer of 1 or more, and corresponds to the demultiplexing number of the time division demultiplexing by the circuit of this embodiment.

In the optical nonlinear medium 107, due to the nonlinear optical effect of the optical nonlinear medium, the fourth and fifth proportional to the product of the intensities of the signal light and the clock light and the product of the intensity of the signal light and the control light in the medium. Emits light. Examples of the nonlinear optical effect for generating the fourth and fifth lights include four-wave mixing and sum frequency light generation described in the related art.

Now, here, the wavelength of the signal light λ sig, the black
Difference between the wavelength λclk of the control light and the wavelength λcont of the control light
By appropriately selecting the generated wavelength λ^*cont.
Fourth light and wavelength λ^*clk by the optical demultiplexer 108
Setting so that each can be taken out separately
You can The wavelength input to this optical nonlinear medium 107
The relationship between the output wavelengths is shown in FIG. actually,
λ^*cont. and λ^* Clk wavelength difference is about 10 nm or more
If so, the wavelength separation filters currently on the market
It can be used as the wave device 108. This wavelength separation filter
Of the light separated by the optical demultiplexer 108 that uses a filter,
Fourth wavelength component generated by signal light and clock light
λ^*clk is guided to the timing extraction circuit 109. This
Then the fourth wavelength component λ^*Spontaneous emission light mixed in clk
And timing extraction circuit 1 to remove other wavelength components
The optical bandpass filter 111 may be used before 09.
Yes. In addition, the fifth wave separated by the optical demultiplexer 108
Long component λ^*cont. is the time-division separated signal output.
Optical bandpass filter 114 is used as necessary.
To remove the noise component and guide it to the optical output port 110.
Therefore, a time division separated output can be obtained.

FIG. 3 is a time chart of the signal light, the control light, and the four-wave mixed light pulse. As shown in FIG. 3, it can be seen that the four-wave mixing output, that is, the demultiplexing output is generated only at the position where the time positions of the signal light pulse and the control light pulse overlap.

The optical non-linear medium 107 may be any optical circuit element exhibiting a non-linear optical effect, such as an optical fiber, a semiconductor laser amplifier, or an optical waveguide made of other inorganic or organic optical material having a non-linear optical effect. Etc. can be used.

Next, a second embodiment of the present invention will be described with reference to FIG.

FIG. 4 shows the configuration of the second embodiment of the present invention. The optical time division demultiplexing circuit of the second embodiment includes a signal light incident port 401 and a voltage controlled oscillator (oscillates at a frequency (f ₀ / N) of 1 / N of a frequency f ₀ corresponding to the bit rate of the signal light. VCO) 402, a low-frequency oscillator 403 that oscillates at a frequency Δf, and a mixer 404 that mixes the output of the voltage-controlled oscillator 402 and the output of the low-frequency oscillator 403.
A control optical pulse generator 405 which outputs an optical pulse of wavelength λcont by the output of the voltage controlled oscillator 402, an optical clock pulse generator 406 which outputs an optical pulse of wavelength λclk by the output of the mixer 404, and a control optical pulse generation An optical multiplexer 407 for multiplexing the optical output of the optical device 405 and the optical output of the optical clock pulse generator 406, and this optical multiplexer 40
An optical multiplexer 408 for multiplexing the optical output of 7 and the signal light input from the signal light incident port, and a traveling wave type semiconductor laser amplifier 409 to which the output of the optical multiplexer 408 is input,
The traveling wave type semiconductor laser output amplifier 409 is input signal light and Ramudacont and wavelength is four-wave mixed light of the light λclk λclk. _FWM and wavelength Ramudacont. Optical demultiplexer and outputting the separated _FWM light 410, an optical bandpass filter 411 that allows the light of the wavelength λclk. _FWM to pass therethrough, and a light receiving circuit 412 that converts the light of the passed wavelength λclk. _FWM into an electrical signal.
And a phase comparator 413 which compares the converted clock signal with the output of the low frequency oscillator 403 and gives the comparison result as a control signal to the voltage controlled oscillator 402, and the wavelength λ cont. _FWM separated by the optical demultiplexer 410. An optical bandpass filter 414 that passes the light and an optical output port 4 that outputs the output of the optical bandpass filter 414 as an optical time division separation output.
15 is provided.

The operation of the second embodiment of the present invention will be described.

First, a signal light pulse is incident from the signal light incident port 401 and enters the optical multiplexer 408. On the other hand, the output of the voltage controlled oscillator 402 is divided into two, and one of them drives the control light pulse generator 405. The oscillation frequency of the voltage-controlled oscillator 402 is set to f ₀ / N which is an integral fraction of the frequency f ₀ corresponding to the bit rate of the incident signal. However,
N is an integer of 1 or more and corresponds to the demultiplexing number of the time division demultiplexing by this circuit. The control light pulse generated from the control light pulse generator 405 is input to the traveling wave type semiconductor laser amplifier 409 through the optical multiplexers 407 and 408. On the other hand, the other output of the voltage-controlled oscillator 402 divided into two is
Input to mixer 404 where low frequency generator 403
The frequency is mixed with (frequency Δf) and the frequency is shifted by Δf (f ₀ / N−Δf) or (f ₀ / N + Δf)
Alternatively, both frequency components are generated. The output of the mixer 404 is used to drive the optical clock pulse generator 406, and the generated optical clock is supplied to the optical multiplexers 407 and 40.
It is inputted to the traveling wave type semiconductor laser amplifier 409 through 8. In the traveling wave type semiconductor laser amplifier 409,
Due to the nonlinear optical effect of the traveling wave type semiconductor laser amplifier 409, a four-wave mixing output is generated in the medium as in the case of FIG. Here, 1 / λcont. _FWM = 2 / λsig −1 / λcont (8) 1 / λclk. _FWM = 2 / λsig −1 / λclk between the wavelength of the generated four-wave mixed light and the input light wavelength. The relationship of (9) is established.

Now, by appropriately selecting the wavelength difference between the wavelength λsig of the signal light, the wavelength λclk of the clock light and the wavelength λcont of the control light, the generated four-wave mixed light λcont.
_FWM and λclk. _FWM are set so that they can be taken out separately by the optical demultiplexer 410 composed of an optical filter. In fact, if the wavelength difference between λcont. _FWM and λclk. _FWM is about 10 nm or more, the wavelength separation filter currently on the market can be used. This optical demultiplexer 4
Of the lights separated by 10, the four-wave mixing component λclk. _FWM generated by the signal light and the clock light is converted into an electric signal by the light receiving circuit 412. At this time, 4
An optical bandpass filter 411 can be used before the light receiving circuit 412 to remove spontaneous emission light and other wavelength components mixed in the light wave mixing component λ clk. _FWM . The output of the light receiving circuit 412 is input to a phase comparator 413 that performs phase comparison based on an electrical signal, where it is phase-compared with the output of the low-frequency oscillator 403. The operation is realized. For details of the operation of this PLL circuit, see [2] O.
Kamatani et al., "Prescaled 6.3 GHz clock recovery
from 50 Gbit / s TDM optical signal with 50 GHz PLL u
suing four-wave mixing in a traveling-wave laser
diode optical amplifier, "Electron.Lett. vol.30, p
p.807-809, 1994.

The other λcont. _FWM components separated by the optical demultiplexer 410 are time-division separated signal outputs, and the optical bandpass filter 414 is used to remove noise components as necessary. By directing to the optical output port 415, a time division separated output is obtained.

[0049]

As described above, according to the present invention,
By using four-wave mixing or sum frequency light generation by the ultrafast nonlinear optical effect in a traveling wave type semiconductor laser amplifier or other optical nonlinear medium, a clock synchronized with the ultrafast time division multiplexed signal is regenerated, and this clock is further reproduced. It can be used to perform all-optical time division separation.

Further, since no optical branching means is required in the receiving system, it is possible to perform all-optical time division separation without causing optical loss in the receiving system and causing no deterioration in receiving sensitivity.

Moreover, since four-wave mixing or sum frequency light generation can be performed by a single nonlinear optical element, the circuit configuration is simple and an all-optical time division demultiplexing circuit can be realized without complicating the receiving system. Since it is compact and can realize ultra-high-speed operation, its effect is great when used in the fields of ultra-high-speed optical communication and optical signal processing.

Further, since a simple optical multiplexing circuit can be used as the structure for making the signal light, the control light and the clock light incident on the optical nonlinear medium, the circuit structure can be simplified.

Since an optical fiber or a semiconductor laser amplifier having a known characteristic of nonlinear optical effect is used as the optical nonlinear medium, it is easy to handle and can easily output four-wave mixed light or sum frequency light by the nonlinear optical effect. You can

Further, it is possible to shift the optical clock pulse from the frequency of the bit rate of the signal light by Δf and to perform phase comparison with the extracted timing signal, so that the accuracy of timing control can be improved. In addition, a PLL circuit can extract an accurate timing signal.

Also, the spontaneous emission light and other wavelength components can be removed by passing the optical output after separating the light of the fourth and fifth wavelengths generated by the non-linear optical effect through the optical bandpass filter, and the sensitivity can be improved. In addition, the accuracy can be improved.

[Brief description of drawings]

FIG. 1 is a diagram showing the configuration of a first embodiment of the present invention.

FIG. 2 is a diagram showing a relationship between a wavelength λsig of signal light, a wavelength λclk of clock light, and a wavelength λcont of control light which are incident on a traveling wave semiconductor laser amplifier.

FIG. 3 is a diagram showing a time chart of signal light, control light, and separated light pulses.

FIG. 4 is a diagram showing the configuration of a second embodiment of the present invention.

FIG. 5 is a diagram showing a configuration of a conventional technique.

FIG. 6 shows a wavelength λsig of incident signal light in the case of four-wave mixing,
The figure which shows the relationship of wavelength (lambda) clk of clock light.

[Explanation of symbols]

11, 101, 401 Signal light incident port 12, 402 Voltage controlled oscillator 13, 403 Low frequency oscillator 14, 404 Mixer 15, 103, 406 Optical clock pulse generator 16, 102, 405 Control optical pulse generator 17, 19, 105 , 106, 407, 408 Optical multiplexer 18, 108, 410 Optical demultiplexer 20, 409 Traveling wave type semiconductor laser amplifier 21 Time division demultiplexing circuit 22, 111, 114, 411, 414 Optical bandpass filter 23, 412 Light receiving circuit 24, 413 Phase comparator 25, 110, 415 Optical output port 26 Frequency multiplier 104 Synchronization signal line

Continuation of the front page (56) Reference JP-A-6-281975 (JP, A) JP-A-6-303216 (JP, A) (58) Fields investigated (Int.Cl. ⁷ , DB name) G02F 1 / 35-1/39 G02F 2/00 H04B 10/00-10/18 JISST file (JOIS)

Claims (7)

(57) [Claims] 1. A first for generating an optical pulse train of a first wavelength
Light pulse source of Light of the second wavelength in synchronization with the optical pulse train of the first wavelength
A second light pulse light source for generating a pulse train, An optical nonlinear medium, The input signal light of the third wavelength and the optical signal of the first wavelength are input.
The pulse train and the optical pulse train of the second wavelength.
Means for entering a linear medium, The fourth optical effect caused by the nonlinear optical effect of the optical nonlinear medium
And means for separating the light of the fifth wavelength, Timing extraction is performed from the light of the fourth wavelength,
Output of one light pulse light source and said second light pulse light source
And means for controlling the timing of the pulse, The abovesecondThe bit rate of the optical pulse train with the wavelength of
Bit rate of signal light (f₀) 1 / N (N isTwoMore than
Integer),The frequency of the output optical pulse train of the first optical pulse light source is
Frequency f corresponding to the bit rate of signal light ₀ From 1 / N
It is set to a value shifted by Δf, The light of the fourth wavelength is the light pulse of the first wavelength and
It is a signal proportional to the product of the intensity with the signal light, The light of the fifth wavelength is the same as the light pulse of the second wavelength.
It is a signal proportional to the product of the intensity with the signal light, The light of the fifth wavelength is output as a time-division separated signal.
An optical time division demultiplexing circuit characterized by being 2. The first wavelength and the second wavelength are the third wave.
For the length, the light of the first wavelength and the third wavelength
From the four wavelengths of light in the optical nonlinear medium
Generated by mixing, the light of the second wavelength and the first
From the light of the third wavelength to the light of the fifth wavelength in the optical nonlinear medium
2. The optical time division demultiplexing circuit according to claim 1, wherein the wavelength relationship generated by four-wave mixing is set . 3. The first wavelength and the second wavelength are the light of the first wavelength and the light of the third wavelength to the fourth wavelength with respect to the third wavelength. Sum frequency in medium
And the light generated, the sum the second light from the light and the third wavelength light of the fifth wavelength of wavelength in the optical nonlinear medium
Optical time division demultiplexing circuit of claim 1 Symbol <br/> mounting set in the wavelength relationship that occurs with frequency light. 4. A first optical pulse light source and a second optical pulse source.
The means for controlling the timing of the output light pulse of the light source is
Timin extracted from the separated fourth wavelength light
And a timing signal of the first optical pulse light source
In order to reduce the phase error in comparison, the first
Output timing of light pulse light source and second light pulse light source
2. A loopback control circuit for feedback controlling the loop is included.
4. The optical time division demultiplexing circuit according to any one of 3 to 3 . 5. An optical nonlinear medium is a semiconductor laser amplifier.
Optical time division demultiplexing circuit according to any one of claims 1 to 4 is. 6. The optical nonlinear medium is an optical fiber請<br/> Motomeko 1 to the optical time division demultiplexing circuit according to any one of 4. 7. Separation of light of fourth and fifth wavelengths
The fourth and fifth wavelengths of light are respectively transmitted after the means.
The optical time-division demultiplexing circuit according to any one of claims 1 to 6 , wherein an optical bandpass filter is provided .