阅读说明：本技术 光调制装置 (Light modulation device ) 是由 蔡坤廷 庄荣敏 于 2020-05-25 设计创作，主要内容包括：一种光调制装置,包含一分光器、一光相位调制器,及一光结合器。该分光器将一输入光信号以一分光比进行分光,以产生一第一分光信号及一第二分光信号,该光相位调制器将所述第一及第二分光信号进行相位调制,以分别产生一第一调制光信号及一第二调制光信号,该光结合器将所述第一及第二调制光信号以一结合比进行结合,以产生一具有一啁啾的输出光信号,该结合比等于该分光比,该结合比的一比值为正数,且该比值为小于一及大于一的二者其中之一。(An optical modulation device includes an optical splitter, an optical phase modulator, and an optical combiner. The optical splitter splits an input optical signal by a splitting ratio to generate a first splitting signal and a second splitting signal, the optical phase modulator phase-modulates the first splitting signal and the second splitting signal to generate a first modulated optical signal and a second modulated optical signal respectively, the optical combiner combines the first modulated optical signal and the second modulated optical signal by a combining ratio to generate an output optical signal with chirp, the combining ratio is equal to the splitting ratio, a ratio of the combining ratio is a positive number, and the ratio is one of less than one and more than one.)

1. A light modulation device, comprising:

the optical splitter is used for receiving an input optical signal and splitting the input optical signal by a splitting ratio to generate a first split optical signal and a second split optical signal;

an optical phase modulator coupled to the optical splitter to receive the first optical splitting signal and the second optical splitting signal, and perform phase modulation on the first optical splitting signal and the second optical splitting signal to generate a first modulated optical signal and a second modulated optical signal, respectively; and

an optical combiner coupled to the optical phase modulator to receive the first modulated optical signal and the second modulated optical signal and combine the first modulated optical signal and the second modulated optical signal with a combination ratio to generate an output optical signal with a chirp, wherein the combination ratio is equal to the splitting ratio, a ratio of the combination ratio is positive, and the ratio is one of less than one and greater than one.

2. The optical modulating device of claim 1, wherein the optical phase modulator comprises:

a first waveguide coupled between the optical splitter and the optical combiner for receiving the first optical signal from the optical splitter and generating the first modulated optical signal accordingly,

a second waveguide coupled between the optical splitter and the optical combiner, receiving the second split optical signal from the optical splitter, and generating the second modulated optical signal accordingly,

a first electrode disposed corresponding to the first waveguide and configured to receive a first modulation voltage, a phase of the first modulated optical signal varying with a variation of the first modulation voltage, an

And the second electrode is arranged corresponding to the second waveguide and is used for receiving a second modulation voltage, and the phase of the second modulation optical signal is changed along with the change of the second modulation voltage.

3. The optical modulation device of claim 2, wherein the chirp is a variable, the optical phase modulator further comprising:

and a bias electrode arranged corresponding to the second waveguide and the second electrode and used for receiving a bias signal, wherein the chirp of the output optical signal is changed along with the change of the bias signal.

4. The optical modulation device according to claim 2, wherein the first modulation voltage and the second modulation voltage are different in phase by 180 degrees, and the first modulation voltage and the second modulation voltage have the same amplitude.

5. The light modulating device of claim 1 wherein the beam splitter and the light combiner are each a Y-branch waveguide.

6. The light modulating device of claim 1, wherein the beam splitter and the light combiner are each a light directional coupler.

7. The light modulating device of claim 1, wherein the beam splitter and the light combiner are each a multimode interferometer.

8. The light modulating device of claim 1, wherein the splitting ratio and the combining ratio are both constant.

9. The light modulation device of claim 1, further comprising:

a ratio adjuster for receiving a variable DC voltage and adjusting the ratio of the splitting ratio to the combining ratio according to the DC voltage.

10. The light modulating device of claim 9, wherein the proportional regulator comprises

A first electrode disposed corresponding to the beam splitter and for receiving the DC voltage, an

A second electrode corresponding to the optical combiner and used for receiving the DC voltage.

Technical Field

The present invention relates to an apparatus, and more particularly, to an optical modulation apparatus.

Background

In optical fiber communication systems, fiber dispersion is a phenomenon in which light waves are dispersed into spectral components of different wavelengths due to the dependence of the wave velocity on its wavelength. When an optical signal or pulse emitted by the optical modulation device is projected into, for example, the optical fiber channel, its envelope propagates along the optical fiber channel at the group velocity to the optical receiving device. Since the pulse contains a series of spectral components, each spectral component travels at a different Group velocity, causing Group Velocity Dispersion (GVD), intramode dispersion (intramodal), or simply fiber dispersion. This dispersion phenomenon is also commonly referred to as pulse spreading. As the pulses travel along the fiber, the spectral components are continuously dispersed in space and time, such that the pulses become too wide, and the leading edge of one pulse overlaps the trailing edge of the previous pulse, Inter Symbol Interference (ISI) occurs and bit ambiguity results, which causes the optical receiver to be unable to distinguish the difference between the "0" bit and the "1" bit when receiving the optical signal and demodulating it accordingly, resulting in demodulation errors. Furthermore, the dispersion of an optical fiber is proportional to the length of the optical fiber, that is, the transmission distance of an optical signal is limited by the dispersion of the optical fiber. In addition, the demodulation accuracy of the optical receiver is also affected by the signal-to-noise ratio (SNR) of the optical signal received by the optical receiver.

As a result, the signal-to-noise ratio and the optical fiber dispersion of the optical signal become one of the important factors affecting the signal quality of the optical fiber communication. Therefore, how to avoid the optical signal with too low signal-to-noise ratio and the optical fiber dispersion from seriously affecting the optical fiber communication system to increase the optical transmission distance is a subject to be improved by the related communication manufacturers.

Disclosure of Invention

It is therefore an object of the present invention to provide a light modulation device that overcomes the disadvantages of the prior art.

Thus, the optical modulation device of the present invention includes an optical splitter, an optical phase modulator, and an optical combiner.

The optical splitter is used for receiving an input optical signal and splitting the input optical signal by a splitting ratio to generate a first split optical signal and a second split optical signal.

The optical phase modulator is coupled to the optical splitter to receive the first and second split optical signals, and performs phase modulation on the first and second split optical signals to generate a first modulated optical signal and a second modulated optical signal, respectively.

The optical combiner is coupled to the optical phase modulator to receive the first and second modulated optical signals and combine the first and second modulated optical signals with a combining ratio to generate an output optical signal with a chirp, wherein the combining ratio is equal to the splitting ratio, a ratio of the combining ratio is a positive number, and the ratio is one of less than one and more than one.

The invention has the technical effects that: the light splitting ratio is equal to the optical combining ratio, so that the output optical signal has a better signal-to-noise ratio, and an optical receiving device receiving the output optical signal has better demodulation accuracy when demodulating the output optical signal.

Drawings

Other features and technical effects of the present invention will be apparent from the embodiments with reference to the accompanying drawings, in which:

FIG. 1 is a plan view illustrating a first embodiment of an optical modulating device in accordance with the present invention;

FIG. 2 is a simulation diagram illustrating the variation of a first value in a combining ratio to a first value in a splitting ratio when the chirp of an output optical signal of the first embodiment is different values;

fig. 3 is a simulation diagram illustrating a change of an optical modulation amplitude of the output optical signal to a first value in the splitting ratio when the chirp of the output optical signal of the first embodiment is different in value; and

FIG. 4 is a plan view of a light modulating device according to a second embodiment of the present invention.

Description of reference numerals:

1-light modulating device

11. the optical splitter

111. 112. input terminal

12. the optical phase modulator

121. first waveguide

122. a second waveguide

123. first electrode

124. second electrode

125. bias electrode

13. DEG. optical combiner

131. 132. the output terminal

14. ratio regulator

141. a first electrode

142. second electrode

V1. first modulation voltage

V2. second modulation voltage

Vb. DEG. bias signal

Vdc. dc-voltage

Oin. the input optical signal

Output optical signal

Om1 DEG A first modulated optical signal

Om 2. second modulated optical signal

Os 1. first spectroscopic signal

Os 2. second tap signal

OMA. The optical modulation amplitude

First value of the ε 1. the spectroscopic ratio

First value of the ε 2. cndot

α, chirp of the structure

Detailed Description

Before the present invention is described in detail, it should be noted that in the following description, like elements are represented by like reference numerals.

< first embodiment >

Referring to fig. 1, an embodiment of an optical modulation device 1 according to the present invention is suitable for use in an optical communication system (not shown). The optical communication system includes an optical fiber (not shown) and an optical receiving device (not shown). The optical modulation device 1 is used for modulating an input optical signal Oin in the form of a Continuous wave (Continuous wave) to generate and emit an output optical signal Oout having a chirp (chirp), and transmitting the output optical signal Oout to the optical receiving device through the optical fiber. The optical receiving device demodulates the received output optical signal Oout.

The optical modulation device 1 of the present embodiment includes an optical splitter 11, an optical phase modulator 12, and an optical combiner 13. The optical modulation device 1 is a Mach-Zehnder modulator (MZM) made of one of a lithium niobate-based (LiNbO3-based), a Silicon (Silicon), and an indium phosphide (Inp).

The optical splitter 11 is configured to receive the input optical signal Oin and split the input optical signal Oin with a splitting ratio (i.e., ∈ 1 (1- ε 1), where 0< ε 1<1), to generate a first split optical signal Os1 and a second split optical signal Os 2. It should be noted that, in the present embodiment, the Optical splitter 11 is an Optical directional coupler (Optical directional coupler) and only receives the input Optical signal Oin, but is not limited thereto. In other embodiments, one input 111 of the optical splitter 11 receives the input optical signal Oin and the other input 112 receives another input optical signal. The beam splitter 11 may be a Y-branch waveguide (Y-branch waveguide) or a multi-mode interferometer (multi-mode interferometer).

The optical phase modulator 12 is coupled to the optical splitter 11 to receive the first and second optical split signals Os1, Os2, and performs phase modulation on the first and second optical split signals Os1, Os2 to generate a first modulated optical signal Om1 and a second modulated optical signal Om2, respectively. In the present embodiment, the optical phase modulator 12 includes a first waveguide 121, a second waveguide 122, a first electrode 123, a second electrode 124, and a bias electrode 125.

The first waveguide 121 is coupled between the optical splitter 11 and the optical combiner 13, receives the first optical splitting signal Os1 from the optical splitter 11, and accordingly generates the first modulated optical signal Om 1. The second waveguide 122 is coupled between the optical splitter 11 and the optical combiner 13, receives the second split optical signal Os2 from the optical splitter 11, and accordingly generates the second modulated optical signal Om 2. The first electrode 123 is disposed corresponding to the first waveguide 121 and is configured to receive a first modulation voltage V1. The second electrode 124 is disposed corresponding to the second waveguide 122 and is configured to receive a second modulation voltage V2. In detail, the first and second electrodes 123 and 124 are respectively disposed on the upper surfaces of the first and second waveguides 121 and 122. The first and second electrodes 123, 124 respectively generate a change in the refractive index of the first and second waveguides 121, 122 according to the first and second modulation voltages V1, V2 (for example, but not limited to, a change in the refractive index of the first and second waveguides 121, 122 according to heat generated by the first and second modulation voltages V1, V2), respectively), so that the propagation speeds of the first and second split optical signals Os1, Os2 propagated by the first and second waveguides 121, 122, respectively, are changed (i.e., a phase difference (phase modulation) is generated between light propagated in the first and second waveguides 121, 122), and the first and second modulated optical signals Om1, Om2 are generated, respectively. As a result, the phases of the first and second modulated optical signals Om1, Om2 change with changes in the first and second modulation voltages V1, V2, respectively.

The bias electrode 125 is disposed corresponding to the second waveguide 122 and the second electrode 124 (or the bias electrode 125 is disposed corresponding to the first waveguide 121 and the first electrode 123), and is configured to receive a bias signal Vb.

In detail, the polarity of the chirp of the output optical signal Oout is related to the positive or negative slope of a Transfer Function (Transfer Function) in which the optical modulation device 1 operates, and the magnitude of the chirp of the output optical signal Oout is related to the offset between a bias point of the optical modulation device 1 and an orthogonal point of the Transfer Function. Therefore, the present embodiment adjusts the optical modulation device 1 to operate at the positive slope or the negative slope of the transfer function by making the optical phase modulator 12 controlled by the bias signal Vb to change the polarity of the chirp, and deviates the bias point from the orthogonal point of the transfer function by the bias signal Vb to change the magnitude of the chirp, so that the chirp of the output optical signal Oout changes with the change of the bias signal Vb.

The optical combiner 13 is coupled to the optical phase modulator 12 to receive the first and second modulated optical signals Om1, Om2 and combine the first and second modulated optical signals Om1, Om2 at a combination ratio (i.e., ∈ 2 (1- ε 2), 0< ε 2<1) to generate the output optical signal Oout. It should be noted that the combination ratio and the splitting ratio are both constant. The binding ratio is equal to the splitting ratio (i.e., ∈ 1: (1- ε 1) ═ ε 2: (1- ε 2)), a ratio of the binding ratios is positive, and the ratio is one of less than one and greater than one. In addition, in the present embodiment, the optical combiner 13 is an optical directional coupler and only outputs the output optical signal Oout, but is not limited thereto. In other embodiments, one output 131 of the optical combiner 13 outputs the output optical signal Oout, and the other output 132 outputs another output optical signal. The output optical signal Oout and the further output optical signal may have different chirps. The optical combiner 13 may be a Y-branch waveguide or a multimode interferometer.

In the present embodiment, the amplitudes of the first and second modulation voltages V1, V2 are the same, and the phases of the first and second modulation voltages V1, V2 are different by 180 degrees. An Optical Modulation Amplitude (OMA) of the output Optical signal Oout can be obtained by the following formula (1):

wherein, the parameter OMA is the optical modulation amplitude, the parameters Po, max, Po, min are a maximum optical power and a minimum optical power of the output optical signal Oout, the parameter e 1 is a first value in the splitting ratio, the parameter e 2 is a first value in the combining ratio, and the parameter Pin is an optical power of the input optical signal Oin, respectively. According to the formula (1), it can be known that the optical modulation amplitude OMA of the output optical signal Oout is related to the optical splitting ratio and the combining ratio, so that when the wavelength and the transmission distance of the input optical signal Oin are determined and an optical fiber dispersion amount corresponding thereto is known, the chirp of the output optical signal Oout is selected according to the optical fiber dispersion amount, the required chirp is obtained by adjusting the bias signal Vb, and the optical splitting ratio and the combining ratio are preset in a manner such that the optical modulation amplitude OMA is maximized while the output optical signal Oout has the chirp. Therefore, the output optical signal Oout still has a good signal-to-noise ratio (SNR) when transmitted to the optical receiving device through the optical fiber.

Referring to fig. 2 and 3, fig. 2 illustrates the relationship between the first value e 1 in the splitting ratio and the first value e 2 in the combining ratio under different chirp conditions (in the figure, a parameter α is used as the chirp of the output optical signal Oout). Fig. 3 illustrates the relationship between the first value e 1 in the splitting ratio and the optical modulation amplitude OMA of the output optical signal Oout under different chirp conditions. As can be seen from fig. 2 and 3, under different chirp conditions, when the first value e 1 of the splitting ratio is equal to the first value e 2 of the combining ratio (i.e., e 1 ═ e 2), the optical modulation amplitude OMA of the output optical signal Oout has a maximum value. Therefore, the present invention determines the required chirp, and obtains a corresponding and same splitting ratio and combining ratio to preset the Optical modulation apparatus 1, so that the Optical modulation amplitude OMA is maximized while the output Optical signal Oout has the chirp, thereby improving the Optical link budget (Optical link budget).

< second embodiment >

Referring to fig. 4, a second embodiment of the light modulation device 1 of the present invention is similar to the first embodiment, except that in the second embodiment: (1) the split ratio and the coupling ratio are not constant (i.e., not preset); and (2) the light modulation device 1 further comprises a scale adjuster 14.

The ratio adjuster 14 is configured to receive a variable dc voltage Vdc and adjust the ratio of the splitting ratio to the combining ratio according to the dc voltage Vdc. In the present embodiment, the proportional regulator 14 includes a first electrode 141 and a second electrode 142. The first electrode 141 is disposed corresponding to and adjacent to the optical splitter 11 and is configured to receive the dc voltage Vdc. The second electrode 142 is disposed corresponding to and adjacent to the optical coupler 13 and is used for receiving the dc voltage Vdc. In detail, the first and second electrodes 141 and 142 generate heat according to the dc voltage Vdc, respectively, so as to adjust the ratio of the splitting ratio to the combining ratio corresponding to each electrode. In this embodiment, the combination ratio is also equal to the splitting ratio, the ratio of the combination ratio is positive, and the ratio is one of less than one and greater than one.

In summary, the optical modulation apparatus 1 of the present invention makes the splitting ratio equal to the optical combining ratio, so that the output optical signal Oout output by the optical modulation apparatus has a larger optical modulation amplitude OMA, so that the output optical signal Oout still has a better signal-to-noise ratio when being transmitted to the optical receiving apparatus through the optical fiber, so that the optical receiving apparatus has a better demodulation accuracy when performing demodulation according to the output optical signal Oout. In addition, the optical modulation device 1 can reduce the influence of dispersion caused by the optical fiber on the transmission of the output optical signal Oout by enabling the output optical signal Oout to have the optimized chirp, thereby improving the transmission performance of the optical communication system and increasing the optical transmission distance.

The above description is only an example of the present invention, and the scope of the present invention should not be limited thereby, and all the simple equivalent changes and modifications made according to the claims and the contents of the patent specification should be included in the scope of the present invention.