JPH10213783A - Optical modulator - Google Patents

Abstract

PROBLEM TO BE SOLVED: To remove a dip that optical modulation characteristics of the optical modulator have by providing an air layer below a tapered part and a feed part of a progressive wave electrode and at their peripheries across an optical substrate. SOLUTION: A groove part 24 provided for a metallic housing 23 is a part which becomes the air layer when a substrate (optical substrate) 18 is fixed to the metallic housing 23. This groove part 24 is provided below the tapered part and feed part of the progressive wave electrode 16 provided on the substrate (optical substrate) 18 when the substrate (optical substrate) 18 is fixed to the metallic housing 23. When the air layer is thus provided, the gap between the progressive wave electrode 16 and metal housing 23 becomes wide, so almost all of lines of electric force in the substrate (optical substrate) 18 travel from the progressive wave electrode 16 to a ground electrode 17. At this time, the distance from the progressive wave electrode 16 to the metallic housing 23 needs to be made longer than the distance from the progressive wave electrode 16 to the ground electrode 17.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical modulator in optical communication, and more particularly, to a configuration of an optical modulator using a substrate having an electro-optical effect (optical substrate).

[0002]

2. Description of the Related Art In recent years, in the field of communication, optical communication systems have been rapidly developed with the increase in communication speed. A transmission module used in such an optical communication system generally includes a laser diode module 3, an optical isolator 2, and an optical modulator 1, as shown in the block diagram of FIG. When performing transmission using this transmission module, the laser light output from the laser diode module 3 passes through the optical isolator 2 and then passes through the optical modulator 1.
Then, the intensity of the modulated signal is modulated according to the modulated signal (electric signal) and sent to the trunk system.

Here, a laser diode joule 3 is used.
Is a module for generating laser light using a laser diode, an optical isolator 2 is an optical element for passing laser light in one direction, and an optical modulator 1 applies a modulation signal to the laser light. It is an optical element for mounting.

As a modulation method for applying a modulation signal to a laser beam, a direct modulation of directly inputting a modulated electric signal to a laser diode for outputting a laser beam, and a modulation of a laser beam output from the laser diode are applied. There is indirect modulation.

[0005] As an optical modulator for the indirect modulation,
2. Description of the Related Art An optical modulator using a semiconductor optical modulator using a semiconductor and a substrate (optical substrate) having an electro-optical effect represented by lithium niobate is known. These optical modulators are characterized by lower chirping than those using direct modulation. Among them, an optical modulator using a lithium niobate substrate (an optical modulator using the electro-optical effect) is a semiconductor optical modulator. It is also superior in terms of insertion loss (small insertion loss).

[Optical Modulator Utilizing Electro-Optical Effect] The configuration and operation of an optical modulator utilizing the electro-optical effect will be described with reference to FIGS. FIG.
FIG. 9 is a plan view showing a configuration of the optical modulator, FIG. 9 is a cross-sectional view showing an AA ′ cross section of FIG. 8, and FIG. 10 is an explanatory diagram showing an operation principle of the optical modulator.

In the optical modulator shown in FIGS. 8 and 9, a Mach-Zehnder type titanium diffused optical waveguide 11 is formed on the surface of a Z-cut lithium niobate substrate 18, and a buffer layer 19 made of silicon dioxide is provided thereon. Further, a traveling wave electrode 16 and a ground electrode 17 are further provided thereon.

Here, the Mach-Zehnder type titanium diffusion optical waveguide 11 is formed by thermally diffusing titanium on a lithium niobate substrate 18, and is branched into two pieces on the way to join again. When a modulation signal (microwave signal) is applied to the traveling wave electrode 11, an electric field 20 is generated between the traveling wave electrode 16 and the ground electrode 17, and the electric field 20 is applied to the two branched optical waveguides 11. It is applied in the opposite direction. In other words, when an electric field crosses one optical waveguide from top to bottom, the other optical waveguide crosses the electric field from bottom to top, and the material of the substrate (optical substrate) 18 on which the optical waveguide 11 is formed is made of a material. Some lithium niobate (LiNb
Since it has the electro-optical effect of O ₃ ), the refractive index in the optical waveguide 11 changes according to the applied electric field. When the direction of the applied electric field is reversed, the change in the refractive index is reversed, and the amount of the change is determined by the electro-optic constant inherent to the substrate (optical substrate) and the intensity of the applied electric field. The reason why a Z-cut substrate is used as the lithium niobate substrate 19 is as follows.
This is because in the case of a lithium niobate substrate, the largest change in refractive index is obtained when an electric field is applied in the Z-axis direction.
Also, the lithium niobate substrate 18 and the electrode (the traveling wave electrode 16)
And a buffer layer 19 formed between the gate electrode 17 and the ground electrode 17).
Are provided for the purpose of suppressing DC drift and the like.

When the refractive index of the optical waveguide 11 changes as described above, a phase change occurs in the laser light traveling through the optical waveguide 11. Since this phase change is different between the two branched optical waveguides 11, a phase difference occurs in the laser light traveling in the two optical waveguides. Then, since the laser light having a phase difference causes multiplex interference at the junction of the optical waveguide 11,
The laser light output from the optical modulator is intensity-modulated.

For example, as shown in FIG. 10, a laser beam having a constant intensity is input to the optical waveguide 11, and a modulation signal is applied so that the laser beams traveling in the two branched optical waveguides 11 have opposite phases. When the laser beam is applied (applied to the traveling wave electrode 11), the intensity of the laser light that has been multiplexed and interfered at the junction is reduced to zero and output.

[Regarding Traveling Wave Electrode and Grounding Electrode] Next, the traveling wave electrode and the grounding electrode will be described with reference to FIG.

The traveling wave electrode 16 has an electrode width capable of efficiently performing light modulation in the interaction portion 12 near the optical waveguide 11,
Specifically, the ground electrode 17 is formed with a gap between the electrodes of about 10 to 20 μm on both sides thereof in order to keep the characteristic impedance of the traveling wave electrode 16 at 50Ω. .

At both ends of the traveling wave electrode 16, a tapered portion 13 and a power supply portion 14 are provided to facilitate connection with an RF connector for inputting a modulation signal (microwave signal). Therefore, the modulation signal (microwave signal)
Is supplied (applied) to the interaction part 12 via the tapered part 13 and the feeding part 14.

Here, the electrode width of the traveling wave electrode 16 (5 to 1)
The reason for providing the tapered portion 13 that gradually widens the width (about 5 μm) to the electrode width (several hundred μm) of the power supply portion 14 is to maintain the characteristic impedance of the traveling wave electrode 16 at 50Ω.
In addition, the inter-electrode gap in the tapered portion 13 is reduced from the inter-electrode gap (10 to 20 μm) in the interaction portion 12 with an increase in the electrode width in order to keep the characteristic impedance of the traveling wave electrode 16 at 50Ω. It is gradually spread to several hundred μm.

The interaction portion 12 is a portion where an electric field generated by a modulation signal (microwave signal) affects the optical waveguide. As the length of the interaction portion 12 increases, the sensitivity of the optical modulator increases, and the driving voltage decreases. descend. Further, the light modulation characteristics of the light modulator are affected by the electric transmission characteristics (transmission loss) of the traveling wave electrode 16 with respect to the microwave signal which is a modulation signal.

By the way, the optical modulator is usually fixed directly to the grounded metal housing on the back surface of the substrate (optical substrate) 18. In this case, the traveling wave electrode 16 is resonated by microwave resonance. The transmission loss is a number d as shown in FIG.
A sharp dip of B (a sharp decrease in characteristics) occurs, and a similar dip occurs in the light modulation characteristics.

Conventionally, in order to suppress the dip caused by the transmission loss, the thickness or width of the substrate (optical substrate) is reduced or the substrate is reduced as shown in FIG. 12 and FIG. 13 (BB ′ sectional view in FIG. 12). (Optical substrate) An air layer 22 is provided between the metal housing 23 and the metal housing 23 (Japanese Patent Laid-Open No. 4-1604) to suppress the microwave resonance.

In the optical modulator disclosed in Japanese Patent Application Laid-Open No. 5-93892, the dielectric constant of glass or the like is low between a substrate (optical substrate) and a metal housing in order to suppress microwave resonance. A layer of material is provided.

[0019]

However, the optical modulator in which measures against the above-described microwave resonance are taken has the following problems.

(1) In the case of an optical modulator in which an air layer is provided between a substrate (optical substrate) and a metal housing, the mechanical strength is low because the substrate (optical substrate) is not reinforced by the metal housing. Weak
The handling and connection with the optical fiber were difficult.

(2) When glass or the like having a low thermal strength is used as a material having a low dielectric constant, it is not possible to perform a process of applying heat when fixing to a metal housing or connecting an RF connector.

Conventionally, it has not been sufficiently elucidated where the microwave resonance, which is the cause of the dip occurring in the transmission loss (electrical transmission characteristics) of the traveling wave electrode, occurs. It has been difficult to take appropriate measures against wave resonance.

Accordingly, the present invention is to clarify the portion where microwave resonance occurs and the cause thereof, and to take appropriate measures against such microwave resonance. It is an object of the present invention to provide an optical modulator which solves the above-mentioned problem while suppressing (a dip occurring in transmission loss (electrical transmission characteristics) of a traveling wave electrode).

According to the present invention, measures against microwave resonance can be taken in a simple and reliable manner.

[0025]

According to a first aspect of the present invention, there is provided an optical modulator, wherein an optical waveguide, a traveling wave electrode, and a ground electrode are formed on an optical substrate having an electro-optical effect, and the optical substrate is mounted on a metal housing. In the optical modulator fixed to the above, an air layer is provided below and around the tapered portion and the feed end portion of the traveling wave electrode via the optical substrate.

According to a second aspect of the present invention, there is provided an optical modulator in which an optical waveguide, a traveling-wave electrode, and a ground electrode are formed on an optical substrate having an electro-optical effect, and the optical substrate is fixed on a metal housing. In the modulator, a layer made of a material having a lower dielectric constant than the optical substrate is provided below and around the tapered portion and the feeding end portion of the traveling wave electrode via the optical substrate. It is.

According to a third aspect of the present invention, in the optical modulator according to the first or second aspect, the distance L1 from the traveling-wave electrode to the metal housing is set to a distance from the traveling-wave electrode to the ground electrode. When the distance is L2, L1 ≧ 1.5 × L2 is satisfied.

[0028]

BEST MODE FOR CARRYING OUT THE INVENTION

[Regarding Portion and Cause of Resonance of Microwave] Referring to FIGS. 14 and 15, a portion and cause of resonance of the microwave in the conventional optical modulator will be described.

The dip occurring in the optical modulation characteristic of the optical modulator (the dip occurring in the transmission loss (electrical transmission characteristic) of the traveling wave electrode) is caused by the resonance of the electromagnetic wave propagating in the substrate (optical substrate) 18. The resonance of this electromagnetic wave is shown in FIG.
As shown in (1), the electric field distribution is generated in the portion where the gap between the traveling wave electrode 16 and the ground electrode 17 is wide, that is, in the tapered portion 13 and the feeding portion 14.

FIG. 14 shows an electric field distribution (lines of electric force) in a substrate (optical substrate) at a tapered portion or a feeding portion of a traveling wave electrode of a conventional optical modulator. In the tapered portion or the feeding portion of the traveling wave electrode shown in FIG. 3, since the gap between the traveling wave electrode 16 and the ground electrode 17 is widened, the lines of electric force in the substrate (optical substrate) 18 are shown.
Most of them go from the traveling wave electrode 16 to the metal housing 23.

[0031] The electric field distribution (field distribution) is very close to the TE ₁₀ mode (see FIG. 8) when the electromagnetic wave propagates. The TE ₁₀ mode is a low-order mode and is the simplest electromagnetic field distribution in which an electromagnetic wave can propagate in the substrate (optical substrate) 18. The electromagnetic field distribution exists only in the vertical direction electric field component with respect to the traveling direction, the magnetic field is a mode that is present in the traveling direction, TE ₁₀ mode, the simplest electromagnetic field distribution in that mode Mode.

As described above, in the TE ₁₀ mode, a modulated signal (microwave signal) is applied to the traveling wave electrode 16 because the electromagnetic wave is the simplest electromagnetic field distribution that can propagate in the substrate (optical substrate) 18. Then, an electromagnetic wave propagating in the substrate (optical substrate) 18 is generated. Since this electromagnetic wave causes a resonance phenomenon in the substrate (optical substrate), the traveling wave electrode 1
A dip occurs in the transmission loss (electrical transmission characteristic) of No. 6 and a dip occurs in the light modulation characteristic of the optical modulator.

Therefore, a dip (transmission loss of the traveling wave electrode 16 (electrical transmission characteristic)) generated in the optical modulation characteristic of the optical modulator
To remove the dip) occurring in the, TE ₁₀ mode may be so as not to cause in the substrate (optical substrate).

[Configuration of Optical Modulator According to the Present Invention]
The TE ₁₀ mode is described the structure of an optical modulator according to the present invention measures that does not occur in the substrate (optical substrate) has been subjected.

FIG. 1 is an exploded view showing the configuration of an optical modulator according to the present invention. In the figure, a substrate (optical substrate) 18 and a metal housing 2 are shown to show the structure of the metal housing 23.
Although the substrate 3 is shown in a separated state, the substrate (optical substrate) 18 is actually fixed to a grounded metal housing 23 using a conductive adhesive or the like. Here, the groove portion 24 provided in the metal housing 23 is a portion that becomes an air layer when the substrate (optical substrate) 18 is fixed to the metal housing 23.

As shown in FIG. 2 (cross section CC ′ in FIG. 1), the groove 24
3, it is provided so as to be located below the tapered portion and the feeding portion of the traveling wave electrode 16 provided on the substrate (optical substrate) 18.

FIG. 3 shows an electric field distribution (lines of electric force) generated in the tapered portion or the feeding portion of the traveling wave electrode 16 when the air layer is provided. When the air layer is provided, the gap between the electrodes of the traveling wave electrode 16 and the metal casing 23 is widened. Therefore, when the lines of electric force in the substrate (optical substrate) 18 are shown, most of the lines of the traveling wave electrode 16 are shown. From ground electrode
Going to 17

Here, in order to increase the ratio of lines of electric force from the traveling wave electrode 16 to the ground electrode 17, the distance L 1 from the traveling wave electrode 16 to the metal casing 23 must be increased.
6 needs to be longer than the distance L2 from the ground electrode 17, and it is desirable to provide the groove 24 so that L1 ≧ 1.5 × L2 (1). However,
For the TE ₁₀ mode is to prevent the occurrence in the substrate (optical substrate) is sufficient L1 = 1.5 × L2 ··· (2 ), in consideration of the mechanical strength, less the L1 It is not preferable to make it longer. In addition, even when L1 is short (when Expression (1) is not satisfied), the dip occurring in the optical modulation characteristic of the optical modulator (the dip occurring in the transmission loss of the traveling wave electrode 16 (electrical transmission characteristic)) does not occur. The effect of removing is obtained. However, the effect is reduced.

The electric field distribution (electromagnetic field distribution) as shown in FIG. 3 is called a quasi-TEM mode (mode in which electric and magnetic field components exist only in a direction perpendicular to the traveling direction).
This mode is not propagated in contrast to the TE ₁₀ mode substrate (optical substrate), it does not cause resonance of microwaves in a substrate (optical substrate).

Incidentally, the optical waveguide in the optical modulator according to the present invention is not particularly limited, and a titanium diffusion type,
The present invention can be applied to an optical waveguide such as a ridge type.

[Regarding Groove] Next, the shape of the groove will be described.

The shape of the groove is not particularly limited, and the cross-sectional shape may be represented by a curve or an arc. Therefore, the shape of the groove can be freely determined in consideration of easiness of processing, reduction in the strength of the substrate (optical substrate), and the like.

For example, as shown in FIG.
May be provided with a step 25. In this case, the air layer is provided in a portion other than the tapered portion of the traveling wave electrode, the power supply portion, and the portion below the gap between the electrodes. Further, as shown in FIG. 5, a step may be provided using the metal block 26.

In the above description, the groove is formed as an air layer (when the groove is filled with air). However, the groove may be evacuated, or a fluorine resin (Teflon: ε = 2.6) or the like may be used. May be filled with a material having a low dielectric constant (which may be a gas). However, the material filling this groove must be a material having a lower dielectric constant than the substrate (optical substrate).

As described above, even if the groove is filled with a vacuum or a material having a low dielectric constant (which may be a gas), the same effect as when the groove is filled with air can be obtained.

[0046]

【Example】

Embodiment 1 Next, an embodiment of the optical modulator according to the present invention will be described. In this embodiment, an optical modulator having the configuration shown in FIGS. 1 and 2 was manufactured.

(1) First, as the substrate (optical substrate) 18, a Z having a thickness of 0.5 mm (typically about 0.2 to 0.8 mm) is used.
A cut Y-axis propagating lithium niobate substrate is prepared, and the width of the substrate (optical substrate) is 9 μm (typically about 6 to 12 μm).
A pattern of a titanium thin film having a thickness of 80 nm (generally about 40 to 120 nm) was formed. Here, an electron beam evaporation method was used to form the titanium thin film, and a lift-off method was used to form the pattern. Then, 950 to 110 is added to this substrate (optical substrate).
A thermal diffusion treatment was performed at 0 ° C. to produce a Mach-Zehnder type titanium diffusion optical waveguide.

(2) Next, on this substrate (optical substrate), as a buffer layer, a thickness of 1 μm (usually about 0.3 to 2 μm)
Silicon dioxide and (SiO ₂₎ thin film was formed by electron beam evaporation.

(3) Subsequently, an 8 μm thick traveling-wave electrode and a ground electrode made of gold were formed on the buffer layer by electroplating after forming a guide resist.

(4) Next, a metal casing made of brass was prepared, and a groove having a depth of 2 mm was formed by cutting in a portion below the tapered portion of the traveling wave electrode, the power supply portion, and the gap between the electrodes. .

(5) The substrate (optical substrate) 18 is fixed to the metal housing using a conductive adhesive, and an RF connector (for inputting microwaves to the optical modulator) provided on the metal housing. Of the traveling-wave electrode is soldered to the power supply portion of the traveling-wave electrode.

FIG. 6 shows the results of measuring the transmission loss (electrical transmission characteristics) of the traveling wave electrode 16 for the optical modulator manufactured as described above. As you can see from the figure,
It was confirmed that the dip caused by the transmission loss (electrical transmission characteristic) of the traveling wave electrode 16 was sufficiently removed.
Also, good light modulation characteristics of the light modulator were obtained.

Example 2 Next, an optical modulator in which a groove was filled with a fluororesin (Teflon) was manufactured in the same process as in Example 1. For this optical modulator, the transmission loss (electrical transmission characteristic) of the traveling wave electrode 16 was measured.
It was confirmed that the dip caused by the transmission loss (electrical transmission characteristic) of the traveling wave electrode 16 was sufficiently removed as in the case of (1). Also, good light modulation characteristics of the light modulator were obtained.

[0054]

As described above, according to the optical modulator of the present invention, an air layer or a material having a low dielectric constant is formed on the tapered portion of the traveling wave electrode, the feeding portion, and the portion under the gap between the electrodes. The following effects could be obtained by providing the layer consisting of

(1) The dip (dip caused by the transmission loss (electrical transmission characteristic) of the traveling wave electrode 16) generated in the optical modulation characteristic of the optical modulator can be removed. That is, the light modulation characteristics of the light modulator (the electrical transmission characteristics of the traveling wave electrode) can be improved.

(2) In portions other than the grooves of the metal housing, the substrate (optical substrate) is reinforced by the metal housing, so that the mechanical strength is hardly reduced.

(3) It is possible to easily cope with a design change only by changing the groove provided in the metal housing.

(4) When the groove of the metal housing is filled with air, when the groove is evacuated, or when the groove is filled with fluororesin (Teflon), there is no need to worry about the thermal strength. Therefore, it is possible to freely apply heat when fixing to the metal housing or connecting the RF connector.

[Brief description of the drawings]

FIG. 1 is an exploded view (perspective view) showing a configuration of an optical modulator according to the present invention.

FIG. 2 is a cross-sectional view (cross-section CC ′ in FIG. 1) illustrating the configuration of the optical modulator according to the present invention.

FIG. 3 shows a row wave electrode 16 in the optical modulator according to the present invention.
4 is a drawing showing an electric field distribution (lines of electric force) generated in a tapered portion or a power feeding portion of FIG.

FIG. 4 is an exploded view (perspective view) showing a configuration of an optical modulator according to the present invention.

FIG. 5 is an exploded view (perspective view) showing the configuration of the optical modulator according to the present invention.

FIG. 6 is a traveling wave electrode 1 in the optical modulator according to the present invention.
6 is a graph showing transmission loss (electrical transmission characteristics) of No. 6;

FIG. 7 is a block diagram illustrating a configuration of a transmission module.

FIG. 8 is a plan view showing a configuration of an optical modulator.

FIG. 9 is a cross-sectional view (AA ′ in FIG. 8) showing the configuration of the optical modulator;
Cross section).

FIG. 10 is a diagram for explaining an operation of the optical modulator.

FIG. 11 is a graph showing transmission loss (electrical transmission characteristics) of a traveling wave electrode 16 in a conventional optical modulator.

FIG. 12 is an exploded view (perspective view) showing a configuration of a conventional optical modulator.

FIG. 13 is a sectional view showing the configuration of a conventional optical modulator (FIG. 1);
2 BB ′ section).

FIG. 14 is a view showing an electric field distribution (lines of electric force) generated in a tapered portion or a feeding portion of a row wave electrode 16 in a conventional optical modulator.

15 is a diagram showing an electromagnetic field distribution of TE ₁₀ mode.

[Explanation of symbols]

 DESCRIPTION OF SYMBOLS 1 Optical modulator 2 Optical isolator 3 Laser diode module 11 Optical waveguide 12 Interaction part 13 Taper part 14 Feeding part 16 Traveling wave electrode 17 Ground electrode 18 Substrate (optical substrate) 19 Buffer layer 20 Electric field (line of electric force) 21 Dip 22 Air layer 23 Metal housing 24 Groove 25 Step 26 Metal block 27 RF connector

Claims (3)

[Claims] 1. An optical modulator in which an optical waveguide, a traveling-wave electrode, and a ground electrode are formed on an optical substrate having an electro-optic effect, and the optical substrate is fixed on a metal housing. An optical modulator, wherein an air layer is provided below and around a tapered portion and a feeding end portion of an electrode via the optical substrate. 2. An optical modulator in which an optical waveguide, a traveling-wave electrode, and a ground electrode are formed on an optical substrate having an electro-optic effect, and the optical substrate is fixed on a metal housing. An optical modulator characterized in that a layer made of a material having a lower dielectric constant than the optical substrate is provided below and around the tapered portion and the feeding end portion of the electrode via the optical substrate. 3. The optical modulator according to claim 1, wherein a distance L1 from the traveling wave electrode to the metal casing is a distance L2 from the traveling wave electrode to the ground electrode. An optical modulator characterized by satisfying ≧ 1.5 × L2.