This application claims priority from Japanese Patent Application No. 2012-234010 filed on Oct. 23, 2012, the entire subject matter of which is incorporated herein by reference.
This disclosure relates to an electro-absorption semiconductor optical modulator that is used in an optical transmitter for optical fiber communication and the like.
As a light source of an optical transmitter for optical fiber communication for high speed/long distance, an optical modulator integrated semiconductor laser is useful in which a semiconductor laser and a semiconductor optical modulator are monolithically integrated. In an optical modulator unit of the optical modulator integrated semiconductor laser, an electro-absorption optical modulator is used. As a waveguide structure thereof, a high-mesa ridge type, where a core layer (optical waveguide layer) is provided at an inner side of a ridge, or a low-mesa ridge type, where a core layer is provided below a ridge is adopted (for example, refer to JP-A-2008-10484 (paragraphs [0038] to [0039] and FIG. 2 of JP-A-2008-10484)).
According to the electro-absorption optical modulator having the low-mesa ridge structure, a strong electric field is applied to the optical waveguide layer below the ridge by applying a negative voltage to an anode part. As a result, an optical-absorption coefficient of the optical waveguide layer is increased by the Quantum Confined Stark Effect, so that a light quenching operation is made. In this structure, since the optical waveguide layer also serves as an optical-absorption layer, the optical-absorption coefficient of the largest area of a light distribution is made to be largest. In general, the light has a property of propagating toward an area having a small optical-absorption coefficient while avoiding an area having a large optical-absorption coefficient. Accordingly, the unimodality of light that is propagated through the waveguide of the optical modulator breaks down, and then a shape of the laser light that is emitted from the optical modulator is not unimodal.
In view of the above, this disclosure provides at least a semiconductor optical modulator where a shape of emitted laser light is unimodal.
A semiconductor optical modulator of this disclosure includes: a substrate, which has a first conductivity type, and which includes a first electrode formed on a first main surface thereof; a first clad layer having the first conductivity type, a transparent waveguide layer, a second clad layer having the first conductivity type, an optical-absorption layer, and a third clad layer having a second conductivity type, which are sequentially laminated on a second main surface of the substrate from the substrate; a ridge part, which is formed by removing the third clad layer and a part of the second clad layer in a laminated direction, and a second electrode, which is formed on the ridge part and is connected to the third clad layer.
According to this disclosure, since an optical-absorption area exists at an end of a light distribution, it is possible to obtain a semiconductor optical modulator where a shape of emitted laser light is unimodal.
The foregoing and additional features and characteristics of this disclosure will become more apparent from the following detailed descriptions considered with the reference to the accompanying drawings, wherein:
A semiconductor optical modulator according to illustrative embodiments of this disclosure will be described with reference to the drawings. The same or corresponding elements are denoted with the same reference numerals and the overlapping descriptions may be omitted.
For comparison,
In the optical modulator of this disclosure, the transparent waveguide layer 4 is provided at the position of the optical-absorption layer 104 of the optical modulator of the background art, and the transparent waveguide layer 4 is sandwiched between the n-type semiconductor layers. Also, the optical-absorption layer 6 is positioned above the transparent waveguide layer 4 and is sandwiched between the n-type and p-type semiconductor layers (the second clad layer 5 and the third clad layer 7).
In order to manufacture the optical modulator of this illustrative embodiment, the first clad layer 3, the transparent waveguide layer 4, the second clad layer 5, the optical-absorption layer 6 and the third clad layer 7 are laminated and grown on the n-type InP substrate 2 by a MOCVD method. Then, the channel 9 is etched to form the ridge part 8 and the pedestal part 9 by a wet etching and the like. Subsequently, the insulation film 11, the n electrode 1 and the p electrode 12 are formed to manufacture the optical modulator.
In the below, operations are described. The laser light emitted from the semiconductor laser is incident (not shown) onto the transparent waveguide layer 4 from the rear of
Meanwhile, as shown in
On the other hand, according to the optical modulator of the background art, as shown in
According to this illustrative embodiment, since the optical-absorption area exists at the end of the light distribution propagating through the optical waveguide, it is possible to implement a light quenching operation without breaking down the unimodality of the light distribution 15. Therefore, it is possible to obtain the optical modulator where the shape of the emitted laser light 14 is kept unimodal.
In the second illustrative embodiment, the optical-absorption layer 26 is provided in the clad layer below the transparent waveguide 24 and is sandwiched between the n-type semiconductor (clad layer 21) and the p-type semiconductor (clad layer 22).
In order to manufacture the optical modulator of this illustrative embodiment, the n-type InP clad layer 21, the MQW optical-absorption layer 26 and the p-type InP clad layer 22 are laminated and grown on the n-type InP substrate 2 by the MOCVD method. Then, a ridge stripe pattern is formed by a wet etching and the like and the undoped InP buried layer 23 is buried and grown at both sides of the ridge stripe. Subsequently, the transparent waveguide layer 24 and the p-type InP clad layer 25 are laminated and grown by the MOCVD, and then the ridge part 8 is formed by the same method as the first illustrative embodiment.
Also in the optical modulator of this illustrative embodiment, the same effects as the first illustrative embodiment are obtained. Also, since a capacitance is reduced by the buried layer 23, it is possible to obtain the optical modulator having excellent high-speed responsiveness.
Meanwhile, in this illustrative embodiment, the buried layer 23 is used. However, as shown in
The optical modulator of this illustrative embodiment has a configuration where the arrangement of the p electrode 12 is changed in the modulator having a structure shown in
In the below, operations are described. The laser light emitted from the semiconductor laser is incident into the transparent waveguide layer 34 and propagates in the transparent waveguide layer 34 serving as a core layer. When a negative voltage is applied to the p electrode 36, the transparent waveguide layer 34 sandwiched between the n-type and p-type semiconductor layers (the clad layer 33 and the clad layer 35) is applied with an electric field and an optical-absorption coefficient is thus increased, so that the laser light is absorbed. At this time, the electric field is mainly applied to the transparent waveguide layer 34 just below the channel 9 and is not applied to the transparent waveguide layer 34 just below the ridge, so that the absorption area 18 is eccentrically distributed in the transparent waveguide layer 34 just below the channel 9. Therefore, as shown in FIG. 8B, the light is not absorbed at the center of the horizontal transverse mode 16, and the optical-absorption area 18 exists at both ends of the horizontal transverse mode 16. Accordingly, the unimodality of the light distribution 15 scarcely breaks down, so that the shape of the emitted laser light 14 is not degraded.
In the optical modulator of this illustrative embodiment, the electric field is mainly applied to the transparent waveguide layer 34 just below the pedestal 10 and is not applied to the transparent waveguide layer 34 just below the ridge, the absorption area 18 is eccentrically distributed in the transparent waveguide layer 34 just below the pedestal 10. Therefore, as shown in
Also, by independently controlling voltages to be applied to the three p electrodes, it is possible to obtain an effect of controlling the shape of the emitted laser light and an emission direction thereof.
In the above illustrative embodiments, the optical modulator integrated semiconductor laser has been exemplified. However, even when a single laser and a single semiconductor optical modulator are used, the same effects are obtained.
Although the n-type substrate has been exemplified, a p-type substrate may be also used. In this case, the conductivity types of the n-type and p-type may be reversed each other. Although the InP-based material has been exemplified as the semiconductor material, the other materials may be also used.
The configuration where the p electrode and the clad layer are directly connected has been illustrated. However, when the p electrode and the clad layer are connected with a contact layer being sandwiched between the p electrode and the clad layer, it is possible to form an ohmic electrode more securely.
Number | Date | Country | Kind |
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2012-234010 | Oct 2012 | JP | national |