CN110824731A - Distributed light intensity modulator - Google Patents
Distributed light intensity modulator Download PDFInfo
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- CN110824731A CN110824731A CN201911210442.8A CN201911210442A CN110824731A CN 110824731 A CN110824731 A CN 110824731A CN 201911210442 A CN201911210442 A CN 201911210442A CN 110824731 A CN110824731 A CN 110824731A
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/03—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
- G02F1/0305—Constructional arrangements
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/03—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
- G02F1/0305—Constructional arrangements
- G02F1/0316—Electrodes
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/03—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
- G02F1/0327—Operation of the cell; Circuit arrangements
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/03—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
- G02F1/035—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect in an optical waveguide structure
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Abstract
The application discloses distributed light intensity modulator includes: the optical device comprises a substrate, and a light splitting element, an optical waveguide and a light combining element which are arranged on the substrate and connected in sequence; the driving electrode is arranged on the substrate and comprises a plurality of sub driving electrodes which are arranged at intervals; the optical waveguide sequentially passes through the sub-driving electrodes; at least one voltage bias electrode at least partially spaced from the sub-driving electrodes. The length of each sub-drive electrode is much less than the total length of a conventional such modulator, and the optical signal propagates approximately synchronously with the electrical signal in each sub-drive electrode. Walk-off phenomena between the photo-electric signals are minimized. The voltage bias electrodes are arranged among the sub-driving electrodes and are used as a crosstalk prevention device for shielding crosstalk among the sub-driving electrodes, so that the modulator can synchronously improve the modulation bandwidth and reduce the driving voltage, and simultaneously, the zero drift phenomenon of the modulator is reduced, and the problem of crosstalk among the sub-driving electrodes caused by the improvement of the modulation bandwidth and the reduction of the driving voltage is prevented.
Description
Technical Field
The application relates to the technical field of light modulation, in particular to a distributed light intensity modulator.
Background
High-speed electro-optical modulation has a very wide and important application such as optical communication, microwave optoelectronics, laser beam deflection, wavefront modulation, and the like. The electro-optical modulator is a modulator made using the electro-optical effect of some electro-optical crystals, such as lithium niobate crystal (LiNb03), gallium arsenide crystal (GaAs), and lithium tantalate crystal (LiTa 03). The electro-optic effect, i.e., when a voltage is applied to the electro-optic crystal, the refractive index of the electro-optic crystal changes, resulting in a change in the characteristics of the light wave passing through the crystal, which effects modulation of the phase, amplitude, intensity, and polarization state of the optical signal.
However, in modulating light, it is difficult to achieve both low driving voltage and high modulation bandwidth modulation.
Disclosure of Invention
It is a primary object of the present application to provide a distributed light intensity modulator to achieve modulation of low drive voltage and high modulation bandwidth.
Based on this, this application embodiment provides a distributed light intensity modulator, includes: the optical device comprises a substrate, and a light splitting element, an optical waveguide and a light combining element which are arranged on the substrate and connected in sequence; the driving electrode is arranged on the substrate and comprises a plurality of sub driving electrodes which are arranged at intervals; the optical waveguide sequentially penetrates through the sub-driving electrodes; at least one voltage bias electrode at least partially spaced from the sub-driving electrodes.
Optionally, the drive electrode is a coplanar waveguide structure.
Optionally, the same electrical signal is applied to the sub-driving electrodes.
Optionally, the electrical signal applied to the adjacent sub-driving electrodes has a time delay, wherein the time duration of the time delay is the time duration required for the optical signal to be transmitted from the starting end of the previous sub-driving electrode to the starting end of the adjacent next sub-driving electrode.
Optionally, the optical waveguide includes a plurality of modulation portions and a plurality of bending portions connected between the modulation portions, wherein a bending direction of the bending portion is toward a previous modulation portion connected to the bending portion.
Optionally, the modulation unit includes a first sub-modulation unit and a second sub-modulation unit, wherein light propagation directions inside the first sub-modulation unit and the second sub-modulation unit are opposite.
Optionally, the first sub-modulation section passes through the sub-drive electrode and/or the voltage bias electrode; the second sub-modulation section passes through the voltage bias electrode and/or the sub-drive electrode.
Optionally, the first sub-modulation section is parallel to the second sub-modulation section, and propagation directions of optical signals in the first sub-modulation section and the second sub-modulation section are opposite.
Optionally, the voltage bias electrode comprises: a voltage bias electrode to which a bias voltage is applied, and a first ground electrode and a second ground electrode located at both sides of the voltage bias electrode; the driving electrode includes: a driving signal electrode to which a driving signal is applied, and a third ground electrode and a fourth ground electrode positioned at both sides of the driving signal electrode.
Optionally, the optical waveguide includes a first modulation arm and a second modulation arm, wherein the first modulation arm is disposed between the voltage bias electrode and the first ground electrode and disposed between the driving signal electrode and the third ground electrode, and the second modulation arm is disposed between the voltage bias electrode and the second ground electrode and disposed between the driving signal electrode and the fourth ground electrode.
The application has the following beneficial effects:
the driving electrodes are distributed, and since the driving electrodes are distributed, the length of the driving electrode of each part is much smaller than the total length of the equivalent conventional modulator, and the driving signal voltage of each part is also much smaller than that of the equivalent conventional modulator. In the driving electrode of each part, the propagation of the optical signal can be approximately synchronous with the propagation of the electric signal, even the propagation of the electric signal can be synchronous. The walk-off phenomenon between photoelectric signals is minimized, and the upper limit of the modulation bandwidth is improved. Meanwhile, as the driving electrodes are changed from the traditional one-section driving electrodes into the distributed multi-section driving electrodes, the driving voltage required to be applied to each electrode is greatly reduced. The voltage bias electrodes are arranged among the sub-drive electrodes, the voltage bias electrodes are different from the electric signals applied to the sub-drive electrodes, and the voltage bias electrodes comprise the ground wires, so that the voltage bias electrodes can be used as a crosstalk prevention device for shielding crosstalk between the sub-drive electrodes, and therefore, the modulator can synchronously improve the modulation bandwidth and reduce the drive voltage, simultaneously reduce the zero drift phenomenon and prevent the crosstalk problem between the sub-drive electrodes caused by improving the modulation bandwidth and reducing the drive voltage, and the modulation performance of the optical modulator is greatly improved.
The same electric signal is applied to each sub-driving electrode, and the same electric signal is applied to each part of the driving electrode, which is equivalent to resetting the electric signal when the electric signal is transmitted along each part of the driving electrode, thereby greatly reducing the loss of the electric signal and greatly improving the modulation efficiency. The ground line groups are respectively arranged between the sub-driving electrodes, wherein the sub-driving electrodes are arranged on the parallel parts with the same optical signal propagation direction, and the ground line groups are arranged on the parallel parts opposite to the optical signal propagation direction of the parallel parts provided with the sub-driving electrodes, so that the crosstalk between the sub-driving electrodes can be greatly reduced.
Drawings
The accompanying drawings, which are incorporated in and constitute a part of this application, serve to provide a further understanding of the application and to enable other features, objects, and advantages of the application to be more apparent. The drawings and their description illustrate the embodiments of the invention and do not limit it. In the drawings:
FIG. 1 is a schematic diagram of a distributed optical intensity modulator according to an embodiment of the present application;
FIG. 2 is a schematic partial cross-sectional view of a distributed optical intensity modulator according to an embodiment of the present application;
FIG. 3 is a schematic diagram of another distributed optical intensity modulator according to an embodiment of the present application.
Detailed Description
In order to make the technical solutions better understood by those skilled in the art, the technical solutions in the embodiments of the present application will be clearly and completely described below with reference to the drawings in the embodiments of the present application, and it is obvious that the described embodiments are only partial embodiments of the present application, but not all embodiments. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present application. Furthermore, the terms "comprising" and "having," as well as any variations thereof, are intended to cover non-exclusive inclusions.
It should be noted that the embodiments and features of the embodiments in the present application may be combined with each other without conflict. The present application will be described in detail below with reference to the embodiments with reference to the attached drawings.
As described in the background, there is often a trade-off between drive voltage and modulation bandwidth. The electro-optic effect is typically weak in the electro-optic medium, so low drive voltages require a sufficiently long waveguide to cumulatively produce a sufficient electro-optic effect. However, the inventor finds that there is a group velocity mismatch between the optical wave and the driving electrical signal, and a severe walk-off (walk-off) phenomenon occurs when the optical wave and the driving electrical signal are transmitted over a long distance, which severely limits the modulation bandwidth. In addition, the long optical waveguide also requires a long driving electrode, which results in a large microwave driving signal propagation loss due to the resistive loss of the electrode material, and ultimately limits the possibility of further lowering the driving voltage. This serious design tradeoff problem exists for almost all traveling wave based electro-optic modulators, severely limiting device performance.
In an ideal case, the lithium niobate modulator has no applied voltage and applied voltage representing the maximum and minimum output light intensity, i.e., signals 1 and 0, respectively. However, due to the material characteristics of the lithium niobate material, even in the absence of an applied voltage, the two arms of the mach-zehnder interferometer (MZI) have a phase difference, so that the output light intensity is between the maximum and minimum values under the applied voltage and the applied voltage, which is the zero point voltage drift phenomenon. Meanwhile, as the bandwidth increases, the problem of crosstalk between multiple signals becomes more and more significant. Eventually, it is difficult to further reduce the driving voltage.
Based on the research findings of the inventor, the embodiment of the invention provides a distributed light intensity modulator, as shown in fig. 1, the light modulator comprises: a substrate 60, and a light splitting element 10, an optical waveguide 20, and a light combining element 30, which are provided on the substrate 60 and connected in this order; a driving electrode 40 disposed on the substrate 60 and including a plurality of sub-driving electrodes 41 arranged at intervals, wherein the optical waveguide 40 sequentially passes through the sub-driving electrodes 41; at least one voltage bias electrode 50, at least a partial number of the voltage bias electrodes 50 in the voltage bias electrodes 50 are arranged at intervals from the sub-driving electrodes 41, specifically, at least one voltage bias electrode 50 may be arranged between two sub-driving electrodes 41, and the arrangement order of the voltage bias electrodes 50 and the sub-driving electrodes 41 may be any order.
Due to the group velocity mismatch between the optical wave and the driving electric signal, a serious optical wave-driving point signal walk-off phenomenon can be generated through long-distance transmission, and the driving voltage and the bandwidth are severely limited. Therefore, in the present embodiment, the driving electrodes 40 are distributed driving electrodes 40, and since the driving electrodes 40 are distributed, the length of each sub-driving electrode 41 is much smaller than the total length of the modulator, and in each sub-driving electrode 41, the optical signal can propagate approximately synchronously with the electrical signal, or even synchronously with the electrical signal. The walk-off phenomenon between photoelectric signals is minimized, the upper limit of the modulation bandwidth at a higher level is increased, and since the lithium niobate modulator has a zero drift phenomenon, a voltage bias electrode 50 is disposed between the sub-driving electrodes 41, and a bias voltage is applied to the voltage bias electrode 50 to modulate the phase difference on the modulation arm. As the modulation bandwidth increases, the problem of crosstalk between multiple signals becomes more and more significant, when the driving electrode 40 includes a plurality of sub-driving electrodes 41 arranged at intervals, the crosstalk problem exists not only between the signals of the channels but also between each electrode of each sub-electrode, in this embodiment, the voltage bias electrode 50 is disposed between each sub-driving electrode 41, the voltage bias electrode 50 is different from the electrical signal applied to each sub-driving electrode 41, and each voltage bias electrode 50 includes a bottom line, and thus can be used as a crosstalk prevention device for shielding crosstalk between the sub-driving electrodes 41, so that the modulator can reduce the zero drift phenomenon and prevent the crosstalk problem between the sub-driving electrodes 41 caused by increasing the modulation bandwidth and reducing the driving voltage simultaneously, thus, the modulation performance of the optical modulator is greatly improved.
As exemplary embodiments, the optical modulator may be a lithium niobate crystal (LiNb03) optical modulator, a gallium arsenide crystal (GaAs) optical modulator, or a lithium tantalate crystal (LiTa03) optical modulator. In this embodiment, a lithium niobate crystal optical modulator will be described as an example. As shown in fig. 2, the optical waveguide 20 and the driving electrode 40 are located on the surface of the substrate 60, and a bonding layer 70 may be further disposed between the substrate 60 and the optical waveguide 20 and the driving electrode 40.
As an exemplary embodiment, the voltage bias electrode 50 includes: a voltage signal electrode to which a bias voltage is applied, and a first ground electrode and a second ground electrode located at both sides of the voltage bias electrode; the driving electrode includes: a driving signal electrode to which a driving signal is applied, and a third ground electrode and a fourth ground electrode positioned at both sides of the driving signal electrode. The optical waveguide 20 includes a first modulation arm 24 and a second modulation arm 25, wherein the first modulation arm 24 is disposed between the voltage bias electrode and the first ground electrode and disposed between the driving signal electrode and the third ground electrode, and the second modulation arm 25 is disposed between the voltage bias electrode and the second ground electrode and disposed between the driving signal electrode and the fourth ground electrode.
As an exemplary embodiment, the light splitting element 10 may adopt a Y-branch splitting optical waveguide, the light combining element 30 may adopt a Y-branch combining optical waveguide, one end of the light splitting element 10 is connected to a single-mode optical fiber, the optical combiner is used for inputting optical signals, the Y branch at the other end is connected with the first modulation arm 24 and the second modulation arm 25 respectively, the Y branch at one end of the optical combiner 30 is connected with the first modulation arm 24 and the second modulation arm 25 respectively, the other end is connected with a single-mode fiber for outputting optical signals, specifically, the input optical signals are divided into two equal or similar beams at one Y branch after passing through a section of single-mode fiber and are transmitted through the first modulation arm 24 and the second modulation arm 25 respectively, the first modulation arm 24 and the second modulation arm 25 are made of electro-optical materials, the refractive index of the two optical signals changes with the magnitude of the applied voltage, so that the two optical signals reach the 2 nd Y branch to generate phase difference. If the optical path difference of the two optical signals is integral multiple of the wavelength, the coherence of the two optical signals is strengthened; if the optical path difference between the two optical signals is 1/2, the two optical signals are coherently cancelled, and the output of the modulator is small. The optical signal can be modulated by controlling the voltage of the electrical signal on the drive electrode 40.
As an exemplary embodiment, the driving electrode 40 includes N sub driving electrodes 41 arranged at intervals along the optical waveguide 20, where N ≧ 2. As shown in fig. 1. The drive electrode 40 is divided into N sections, each section having a shorter length L, the final effective drive length being N x L. In the present embodiment, the electrical signals applied to the sub-driving electrodes 41 are the same, and the same electrical signals are applied to each portion of the driving electrodes 40, which is equivalent to resetting the electrical signals when the electrical signals propagate along each portion of the driving electrodes 40, so that the loss of the electrical signals is greatly reduced, and the modulation efficiency is greatly improved.
In order to better match the electrical signals on the sub-driving electrodes 41, so that the modulation of the optical signal on each sub-driving electrode 41 is as same as possible, in the present embodiment, the electrical signals applied on the adjacent sub-driving electrodes 41 have a time delay, wherein the time duration of the time delay is the time duration required for the optical signal to be transmitted from the starting end of the previous sub-driving electrode 41 to the starting end of the adjacent next sub-driving electrode 41. As an exemplary embodiment, assume that the electrical signal applied to the first sub-driving electrode 41 is V1(T), the time required for the optical signal to travel from the nth sub-driving electrode 41 to the start of the (n + 1) th sub-driving electrode 41 is TnWhere N-1, 2, …, N-1 indicates that it is the second sub-driving electrode 41. The expression of the electric signal applied to each sub-drive electrode 41 is as follows:
due to the delay of the electrical signal and optical signal applied to the adjacent sub-driving electrodes 41 before the distributed driving electrode 40, the sub-driving electrodes 41 of each part have the same electrical signal, which is equivalent to resetting the electrical signal when the electrical signal propagates along each part of the sub-driving electrodes 41, so that the loss of the electrical signal is greatly reduced, and the modulation efficiency is greatly improved.
In this embodiment, the driving electrode 40 is a coplanar waveguide structure, which may be a GSG coplanar waveguide line as an example, or may be another radio frequency transmission line such as a CPW or CPWG coplanar waveguide line, where G is a ground electrode, and S is a signal electrode (the coplanar waveguide structure may use another phase modulation unit). The unmodulated constant-brightness light source is input from the inlet end, enters the light splitting element 10, and is divided into two beams of light with equal or approximate light intensity, and the two beams of light enter the first modulation arm 24 and the second modulation arm 25 respectively. The first modulation arm 24 and the second modulation arm 25 simultaneously pass through the region of the driving electrode 40 of the coplanar waveguide structure and the time for the optical signal to pass through the adjacent two sub driving electrodes 41 in the first modulation arm 24 and the second modulation arm 25 is the same, i.e. the lengths of the two sub driving electrodes 40 are equal. The sub-driving electrode 41 has one end that is an input region of an electrical signal and the other end that is coupled to an external microwave termination isolator (rftermination) or microwave termination circuit (on-chip circuit). After passing through the multiple segments of sub-driving electrodes 41, the first modulation arm 24 and the second modulation arm 25 are combined by one light combining element 30 into the same optical waveguide 20 and then output. As an exemplary embodiment, the impedance of the sub driving electrode 41 is the same as or similar to the impedance of the electric signal input terminal, for example, may be 50 Ω; the propagation speed of the electrical signal in the driving electrode 40 is the same as or similar to the speed of light in the optical waveguide 20; the resistance loss of the electric signal transmitted in the driving electrode 40 is as low as possible, and in this embodiment, the driving electrode 40 may be made of a high-conductivity low-resistance material such as gold, silver, copper, aluminum, graphene, or the like.
As an exemplary embodiment, the optical waveguide includes a plurality of modulation parts 21 and a plurality of bending parts 22 connected between the modulation parts 21, wherein a bending direction of the bending part 22 is toward a previous modulation part 21 connected to the bending part 22. Illustratively, the optical waveguide starts from the first modulation section 21, the bending direction of the first bending portion 22 connected to the first modulation section 21 is toward the first modulation section 21, so that the extending direction of the second modulation section 21 connected to the first bending portion 22 is toward the first modulation section 21, and the plurality of modulation sections 21 are connected to the plurality of bending portions 22 to form a shape of a substantially "S" shape or a "serpentine shape" extending back and forth. As an exemplary embodiment, the modulation section 21 includes a first sub-modulation section 211 and a second sub-modulation section 212, wherein light propagation directions inside the first sub-modulation section 211 and the second sub-modulation section 212 are different. For example, the extending direction of the first sub-modulation part 211 may be a "forward" direction of the optical waveguide, and the extending direction of the second sub-modulation part 212 may be a "backward" direction of the optical waveguide.
The first sub-modulation part 211 passes through the sub-driving electrode 41, and the second sub-modulation part 212 passes through the voltage bias electrode 50, it should be understood by those skilled in the art that the first sub-modulation part 211 may also pass through the voltage bias electrode 50, and the second sub-modulation part 212 may also pass through the sub-driving electrode 41. In the present embodiment, the arrangement positions of the voltage bias electrode 50 and the sub drive electrode 41 are not limited. Illustratively, as shown in fig. 1, the first sub-modulation section 211 and the second sub-modulation section 212 are disposed at intervals along the substrate surface Y direction, and the sub-driving electrode 41 is disposed at intervals from the voltage bias electrode 50. Because crosstalk exists between the sub-drive electrodes when the modulation bandwidth is synchronously improved and the drive voltage is reduced (a plurality of spaced sub-drive electrodes are adopted), and the voltage bias electrodes are arranged between the sub-drive electrodes at intervals along the Y direction of the surface of the substrate, the modulation bandwidth is synchronously improved and the drive voltage is synchronously reduced, the zero drift phenomenon of the modulator is reduced, the problem of crosstalk between the sub-drive electrodes caused by improvement of the modulation bandwidth and reduction of the drive voltage is solved, and the modulation performance of the optical modulator can be greatly improved.
As another exemplary embodiment, in order to prevent crosstalk between the sub driving electrodes, as shown in fig. 3, a ground line group 80 may be disposed between the sub driving electrodes, and in this embodiment, the ground line group 80 may include a first ground line, a second ground line, and a third ground line, wherein the first modulation arm 24 is located between the second ground line and the first ground line, and the second modulation arm 25 is located between the second ground line and the third ground line. Since there may be a crosstalk problem between each of the sub driving electrodes 41, adding three ground lines between two sub driving electrodes 41 can greatly reduce the crosstalk between the sub driving electrodes 41.
The above description is only a preferred embodiment of the present application and is not intended to limit the present application, and various modifications and changes may be made by those skilled in the art. Any modification, equivalent replacement, improvement and the like made within the spirit and principle of the present application shall be included in the protection scope of the present application.
Claims (10)
1. A distributed light intensity modulator, comprising:
the optical device comprises a substrate, and a light splitting element, an optical waveguide and a light combining element which are arranged on the substrate and connected in sequence;
the driving electrode is arranged on the substrate and comprises a plurality of sub driving electrodes which are arranged at intervals;
a voltage bias electrode disposed between the sub driving electrodes;
at least one voltage bias electrode at least partially spaced from the sub-driving electrodes.
2. The distributed optical intensity modulator of claim 1,
the driving electrode is a coplanar waveguide structure.
3. The distributed optical intensity modulator of claim 1,
the same electrical signal is applied to the sub-driving electrodes.
4. The distributed optical intensity modulator of claim 3,
the electrical signals applied to the adjacent sub-driving electrodes have time delays, wherein the time duration of the time delay is the time duration required for the optical signals to be transmitted from the starting end of the previous sub-driving electrode to the starting end of the adjacent next sub-driving electrode.
5. The distributed optical intensity modulator of any one of claims 1-4, wherein the optical waveguide comprises a plurality of modulating portions and a plurality of curved portions connected between the modulating portions, wherein a direction of curvature of the curved portions is toward a previous modulating portion connected to the curved portions.
6. The distributed optical intensity modulator of claim 5,
the modulation part comprises a first sub-modulation part and a second sub-modulation part, wherein the light propagation directions in the first sub-modulation part and the second sub-modulation part are opposite.
7. The distributed optical intensity modulator of claim 6,
the first sub-modulation part passes through the sub-driving electrode and/or the voltage bias electrode;
the second sub-modulation section passes through the voltage bias electrode and/or the sub-drive electrode.
8. The distributed optical intensity modulator of claim 6,
the first sub-modulation part is parallel to the second sub-modulation part, and the propagation directions of optical signals in the first sub-modulation part and the second sub-modulation part are opposite.
9. The distributed optical intensity modulator of claim 1,
the voltage bias electrode includes: a voltage bias electrode to which a bias voltage is applied, and a first ground electrode and a second ground electrode located at both sides of the voltage bias electrode;
the driving electrode includes: a driving signal electrode to which a driving signal is applied, and a third ground electrode and a fourth ground electrode positioned at both sides of the driving signal electrode.
10. The distributed optical intensity modulator of claim 9,
the optical waveguide comprises a first modulation arm and a second modulation arm, wherein the first modulation arm is arranged between the voltage bias electrode and the first grounding electrode in a penetrating mode and arranged between the driving signal electrode and the third grounding electrode in a penetrating mode, and the second modulation arm is arranged between the voltage bias electrode and the second grounding electrode in a penetrating mode and arranged between the driving signal electrode and the fourth grounding electrode in a penetrating mode.
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| CN201911210442.8A CN110824731A (en) | 2019-11-29 | 2019-11-29 | Distributed light intensity modulator |
| PCT/CN2020/071084 WO2021103294A1 (en) | 2019-11-29 | 2020-01-09 | Distributed light intensity modulator |
| EP20893527.0A EP4006630A4 (en) | 2019-11-29 | 2020-01-09 | Distributed light intensity modulator |
| US17/637,824 US20220283453A1 (en) | 2019-11-29 | 2020-01-09 | Distributed light intensity modulator |
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| CN201911210442.8A CN110824731A (en) | 2019-11-29 | 2019-11-29 | Distributed light intensity modulator |
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