1. Field of the Invention
The present invention relates to semiconductor optical integrated devices.
2. Description of the Related Art
Patent Literature 1 (Japanese Unexamined Patent Application Publication No. 2008-010484) discloses a semiconductor optical device in which a laser section and an optical modulator section are monolithically integrated. In the semiconductor optical device of Patent Literature 1, the optical modulator region has a ridge waveguide structure buried with an organic insulating material. The laser section has a ridge waveguide structure in which peripheral regions of the mesa are not buried in an organic insulating material or a semiconductor, namely, the side surfaces of the ridge waveguide structure are exposed to air, Patent Literature 2 (Japanese Unexamined Patent Application Publication No. 2013-033892) discloses a wavelength-tunable laser. In wavelength-tunable lasers, the refractive index of optical waveguides is changed to tune the wavelength. In the laser section of Patent Literature 2, the refractive index is changed by, for example, controlling the temperature of the waveguides with heaters.
The wavelength-tunable laser of Patent Literature 2 is manufactured as an individual device without being integrated with an optical modulator. For example, the side surfaces of the waveguides of the wavelength-tunable laser of Patent Literature 2 are buried with semiconductor layers. On the other hand, waveguides of an optical modulator have to be made with a high dimensional accuracy and therefore it is preferable that the side surfaces of the waveguides be not buried with semiconductors. That is, wavelength-tunable lasers and optical modulators have a difference in terms of preferred waveguide structures. This difference becomes a barrier to monolithically integrating a wavelength-tunable laser and an optical modulator on a single substrate. In the wavelength-tunable laser of Patent Literature 2, the waveguides are subjected to temperature changes with heaters in order to alter wavelengths, On the other hand, waveguides of an optical modulator are preferably maintained at a constant temperature to perform stable modulation. This difference in waveguide temperature requirements obstructs the monolithic integration of a wavelength-tunable laser and an optical modulator on a single substrate.
A semiconductor optical integrated device according to an aspect of the present invention includes a substrate having a principal surface including a first area, a second area and a third area extending along a waveguiding direction; a laser portion disposed on the third area of the substrate, the laser portion including a laser waveguide that includes an active section configured to generate light and a passive section including a heater thereon; a semiconductor waveguide disposed on the second area of the substrate, the semiconductor waveguide including a core layer and a cladding layer disposed on the core layer; a Mach-Zehnder modulator portion disposed on the first area of the substrate, the Mach-Zehnder modulator portion including a first multi-mode interference (MMI) coupler, a first arm, a second arm, a second MMI coupler, a first electrode and a second electrode; a buried region embedding the laser waveguide, the semiconductor waveguide, and the first and second arms of the Mach-Zehnder modulator portion; a groove disposed on the second area of the substrate, the groove extending in a direction intersecting the waveguiding direction to across the semiconductor waveguide to the buried region; and a resin body disposed on the Mach-Zehnder modulator portion. The laser portion is optically coupled to the Mach-Zehnder modulator portion via the semiconductor waveguide. The groove has a bottom on a surface of the core layer of the semiconductor waveguide,
Objects, features and advantages of the present invention will be understood more easily based on the following detailed description illustrating preferred embodiments of the invention with reference to the accompanying drawings.
Some embodiments will be described hereinbelow.
A semiconductor optical integrated device according to an embodiment includes (a) a substrate having a principal surface including a first area, a second area and a third area arranged in a waveguiding direction; (b) a laser portion disposed on the third area of the substrate, the laser portion including a laser waveguide that includes an active section configured to generate light and a passive section including a heater thereon; (c) a semiconductor waveguide disposed on the second area of the substrate, the semiconductor waveguide including a core layer and a cladding layer disposed on the core layer; (d) a Mach-Zehnder modulator portion disposed on the first area of the substrate, the Mach-Zehnder modulator portion including a first MMI coupler, a first arm, a second arm, a second MMI coupler, a first electrode and a second electrode; (e) a buried region embedding the laser waveguide, the semiconductor waveguide, and the first and second arms of the Mach-Zehnder modulator portion; (f) a groove disposed on the second area of the substrate, the groove extending in a direction intersecting the waveguiding direction to across the semiconductor waveguide to the buried region; and (g) a resin body disposed on the Mach-Zehnder modulator portion. The laser portion is optically coupled to the Mach-Zehnder modulator portion via the semiconductor waveguide. The groove has a bottom on a surface of the core layer of the semiconductor waveguide.
In the semiconductor optical integrated device, the laser portion and the Mach-Zehnder modulator portion are monolithically integrated on the substrate. in the semiconductor optical integrated device, the semiconductor waveguide is disposed to provide an optical coupling between the laser portion and the Mach-Zehnder modulator portion, and the groove extends across the cladding layer of the semiconductor waveguide. The groove is disposed between the laser portion and the Mach-Zehnder modulator portion to separate the laser portion and the Mach-Zehnder modulator portion thermally from each other. The groove is disposed so as to across the semiconductor waveguide to the buried region. With this configuration, the heat propagating from the heater of the laser portion to the Mach-Zehnder modulator portion is decreased. The groove has the bottom on the surface of the core layer of the semiconductor waveguide. With this configuration, the optical coupling of the laser portion and the Mach-Zehnder modulator portion is maintained.
In an embodiment of the semiconductor optical integrated device, the first MIMI coupler may be optically coupled to one end of the first arm and one end of the second arm. The second MMI coupler may be optically coupled to the other end of the first arm and the other end of the second arm. The buried region may include a first trench and a second trench, the first trench and the second trench each defining one side surface and the other side surface of the first arm. The buried region may include a third trench and a fourth trench, the third trench and the fourth trench each defining one side surface and the other side surface of the second arm. The first electrode and the second electrode may be connected to the first arm and the second arm via a first opening and a second opening in the resin body, respectively.
In this semiconductor optical integrated device, electrical signals are applied to the first and second arms of the Mach-Zehnder modulator portion by the first and the second electrode. Because these arms are embedded in the buried region, the leak current relating to the side surfaces of the first and second arms are reduced. The buried regions include the trenches that define the side surfaces of the first and second arms. These trenches contribute to increase the uniformity of the thickness of the resin body formed on the first and second arms, Openings are formed in the resin body on the first and second arms. As the thickness of the resin body is uniform on the first and second arms, the first and second openings are formed uniformly. Thus, it is possible to produce a plurality of Mach-Zehnder modulators on a single wafer or with different production lots with high reproducibility.
In an embodiment of the semiconductor optical integrated device, the buried region is made of Fe-doped InP. According to this semiconductor optical integrated device, the Fe-doped InP contributes to reduce a dark current at the first and second arms,
In an embodiment of the semiconductor optical integrated device, the buried region on the side surfaces of the first and second arms has a thickness of 0.3 μm to 0.5 μm. According to this semiconductor optical integrated device, the thickness of 0.3 μm to 0.5 μm allows for both the reduction of dark current and the decrease in parasitic capacitance of the Mach-Zehnder modulator portion.
In an embodiment of the semiconductor optical integrated device, the first MMI coupler and the second MMI coupler of the Mach-Zehnder modulator portion are buried with the resin body. According to this semiconductor optical integrated device, the laser waveguides, the semiconductor waveguides, the first and second arms are embedded in the buried regions, whereas the first MMI coupler and the second MMI coupler are not embedded in the buried regions. This configuration makes it possible to prevent the dimensions of the MMI couplers from being out of the designs due to the buried region. That is, the dimensions of the MMI couplers are only dependent on the accuracy of dry etching. The MMI couplers having accurate dimensions maintain good optical characteristics. Further, good optical characteristics of the MMI couplers arc maintained because of the large difference in refractive index between the semiconductors constituting the MMI couplers and the resin body.
In an embodiment of the semiconductor optical integrated device, the bottom of the groove reaches an upper surface of the core layer of the semiconductor waveguide. According to this semiconductor optical integrated device, the groove is formed to a depth that reaches the core layer, but not intersects the core layer. The groove having this depth, the amount of heat propagating from the heater to the Mach-Zehnder modulator portion is decreased. In addition, the optical loss due to the groove can be suppressed,
In an embodiment of the semiconductor optical integrated device, the resin body has a lower refractive index than a refractive index of the core layer, the resin body has a lower thermal conductivity than a thermal conductivity of the buried regions, and the resin body is disposed in the groove. According to this semiconductor optical integrated device, the optical loss due to the presence of the groove is suppressed.
The findings according to the present invention are easily understood based on the following detailed description with reference to the accompanying drawings given as examples. Hereinbelow, embodiments of the semiconductor optical integrated devices of the invention will be described with reference to the accompanying drawings. Where possible, the same reference numerals will be used for equivalent features,
Mach-Zehnder modulator portion 15, the second region 11f includes the semiconductor waveguides 17, and the third region 11g includes the laser portion 19.
The laser portion 19 includes heaters 23 (23a, 23b, 23c, 23d, 23e and 23f), a segmented grating 25 (gratings 25a, 25b, 25e, 25d, 25e, 25f and 25g), electrodes 27 (27a, 27b, 27c and 27d), and laser waveguides 29. The laser waveguide 29 includes one or more active waveguide sections 31 (31a, 31b, 31c, and 31d), and one or more passive waveguide sections 33 (33a, 33b, 33c and 33d). The electrodes 27 (27a, 27b, 27e and 27d) of the laser portion 19 are connected to the active waveguide sections 31 of the laser waveguide 29. The active waveguide sections 31 (31a to 31d) generate light in response to current injection from the electrodes 27 (27a, 27h, 27c and 27d). The heaters 23 are disposed in contact with the surface of the passive waveguide sections 33 (33a, 33h, 33c and 33d). The passive waveguide sections 33 (33a, 33b, 33c and 33d) produce a refractive index change in response to heat generated by the heaters 23. For example, the heaters 23 include NiCrSi.
The third region 11g includes a sampled grating distributed feedback region (hereinafter, “SG-DFB region”) 11i and a chirped sampled grating distributed Bragg reflector region (hereinafter, “CSG-DBR region”) 11j. In an embodiment, the third region 11g includes a semiconductor optical amplifier region (hereinafter, “SOA region”) 11h. In the SG-DFB region 11i, the active waveguide sections 31 and the passive waveguide sections 33 are arranged alternately, and the SG-DFB region 11i has an optical gain. The SG-DFB region 11 provides a gain spectrum having periodic peaks with respect to wavelengths. The CSG-DBR region 11j constitutes a reflector in a cavity of the semiconductor laser. The CSG-DBR region 11j provides a reflection spectrum having periodic peaks with respect to wavelengths.
The grating 25 includes a plurality of sampled gratings 25a, 25b, 25e, 25d, 25e, 25f and 25g. The sampled gratings 25a to 25g are arranged along the laser waveguide 29 while being separate from one another, and are optically coupled to the active waveguide sections 31 and the passive waveguide sections 33. For example, the sampled gratings 25a to 25g may be corrugation gratings.
In the SG-DFB region 11i and the CSG-DBR region 11j, the sampled gratings 25a to 25g are disposed. The grating 25 in the SG-DFB region 11i and the CSG-DBR region 11j is composed of a plurality of segments. The segments include first segments 26a and second segments 26b. Each of the first segments 26a has a single sampled grating (any one of the sampled gratings 25a to 25g). The second segments 26b do not include sampled gratings, and each second segment 26b is interposed between the first segments 26a. The arrangement of the plurality of segments constitutes a reflector. The SG-DFB region 11i includes a plurality of segments, and the segments have an identical optical length. The CSG-DBR. region 11j includes a plurality of segments. The segments in the CSG-DBR region 11j have an optical length different from that of the segments in the SG-DFB region 11i. Thus, the sampled gratings 25a to 25g in the SG-DFB region 11i and the CSG-DBR region 11, are arranged to have a plurality of grating periods. The CSG-DBR region 11j can provide a reflection spectrum having periodic peaks with respect to wavelengths. More specifically, the CSG-DBR region 11j is such that the plurality of sampled gratings is arranged with chirped periods. As a result, a reflection spectrum of the CSG-DBR region shows a wavelength dependency in which a plurality of reflection peaks forms an envelope. The wavelengths of the reflection peaks in the reflection spectrum are changed depending on the heat generated by the heaters 23. Utilizing the Vernier effect between the change in the reflection spectrum and the gain spectrum, it becomes possible to alter the emission wavelength of the semiconductor laser.
An example of the structure of the SG-DFB region 11i is shown below. In the refractive index modifying regions, the lower cladding layer 35a is n-type InP, the upper cladding layer 35b is p-type InP, and the core layer 35c is an InGaAsP bulk layer (1.4 μm). In the optical gain regions, the lower cladding layer 35a is n-type InP, the upper cladding layer 35b is p-type InP, and, in the quantum well structures (alternate stacks of well layers and barrier layers) 35d, the well layers 35e are GaInAsP (thickness: 5 nm, Ga ratio: 0.32, In ratio: 0.68), and the barrier layers 35f are GaInAsP (thickness: 10 nm, Ga ratio: 0.22, In ratio; 0.78). The bandgap of the well layers 35e is smaller than the bandgap of the barrier layers 35f. The outermost barrier layer may be an optical confinement layer. The contact layer 35h is p-type GaInAs. in the refractive index modifying regions and the optical gain regions, the semiconductor substrate 13 is an n-type InP crystal substrate, the grating layer 35g is GaInAsP (bandgap wavelength: 1.3 μm), and the semiconductor layer 35i is undoped InP. The grating 25 is made using the difference in refractive index between the grating layer 35g and the lower cladding layer 35a. The refractive index modifying regions and the optical gain regions are connected to each other by butt-joint coupling. The semiconductor waveguides 17 include the core layer 35c disposed on the lower cladding layer 35a, and the upper cladding layer 35b is disposed on the core layer 35c. The sampled gratings 25a to 25g are optically coupled to the core layer 35c and the quantum well structures 35d.
The Mach-Zehnder modulator portion 15 includes a first multi-mode interference (first MMI) coupler 37a, a first arm waveguide (first arm) 37b, a second arm waveguide (second arm) 37c, a second multi-mode interference (second MMI) coupler 37d, a first modulating electrode 37e and a second modulating electrode 37f. The first MMI coupler 37a has ports for providing modulated light. These ports are optically coupled to output ports of the semiconductor optical integrated device 11. One end of the first arm 37b and one end of the second arm 37c are connected to the respective ports of the first MMI 37a. The other end of the first arm 37b and the other end of the second arm 37c are connected to the respective ports of the second MMI 37d. The second MMI 37d receives the laser light from the laser portion 19 via the semiconductor waveguides 17. The first electrode 37e and the second electrode 37f are connected to the first arm 37b and the second arm 37c, respectively.
The semiconductor optical integrated device 11 further includes buried semiconductor regions 39 disposed to bury the semiconductor waveguides 17 and the laser waveguides 29. In the buried regions 39, the laser waveguides 29 are buried, in the semiconductor optical integrated device 11, a groove 41 is disposed in the semiconductor waveguide 17 and the buried regions 39. The semiconductor waveguide 17 extends along the first direction Ax1. The groove 41 extends in a direction intersecting with the first direction Ax1, and across the semiconductor waveguide 17 to the buried region 39. In the present embodiment, the groove 41 extends across the upper cladding layer 35b of the semiconductor waveguide 17. For example, the buried regions 39 is made of Fe-doped InP.
The semiconductor optical integrated device 11 further includes a resin body 43 disposed on the Mach-Zehnder modulator portion 15. For example, the resin body 43 includes bisbenzocyclobutene (BCB) resin.
In the semiconductor optical integrated device 11, the Mach-Zehnder modulator portion 15 and the laser portion 19 are monolithically integrated on a single semiconductor substrate. In this semiconductor optical integrated device 11, the semiconductor waveguide 17 is disposed between the Mach-Zehnder modulator portion 15 and the laser portion 19. The semiconductor waveguide 17 optically couples the Mach-Zehnder modulator portion 15 and the laser portion 19 to each other. In addition, the semiconductor waveguide 17 provide a certain distance between the Mach-Zehnder modulator portion 15 and the laser portion 19. The distance contributes to reduces the propagation of heat from the heaters 23 of the laser portion 19 to the Mach-Zehnder modulator portion 15. Further, the groove 41 is disposed between the Mach-Zehnder modulator portion 15 and the laser portion 19. The groove 41 extends across the upper cladding layer 35b of the semiconductor waveguide 17. The groove 41 is disposed in the semiconductor waveguide 17 and the buried regions 39. The groove 41 reduces the propagation of heat from the laser portion 19. Thus, the change in the characteristics of the Mach-Zehnder modulator portion 15 by the heat is avoided. The groove 41 does not extend across the core layer 35c but does extend across the upper cladding layer 35b. With this configuration, the optical loss caused by the groove 41 is suppressed.
As illustrated in
In the semiconductor optical integrated device 11, the bottom surface of the groove 41 includes the upper surface of the core layer 35c of the semiconductor waveguide 17. The groove 41 has a depth that reaches the upper surface of the core layer 35c. As a result of the groove 41 having this depth, the amount of the heat propagating from the heaters 23 to the Mach-Zehnder modulator portion 15 may be decreased.
In the present embodiment, the resin body 43 is disposed in the groove 41. The resin body 43 has a lower refractive index than the core layer 35c. The resin body 43 has a lower thermal conductivity than the buried regions 39. According to this semiconductor optical integrated device 11, the resin body 43 in the groove 41 suppresses the increase in optical loss due to the absence of the cladding layer.
The first electrode 37e and the second electrode 37f are connected to the first arm 37b and the second arm 37c via a first opening 43a and a second opening 43b disposed in the resin body 43, respectively.
According to this semiconductor optical integrated device 11, electricity is applied to the laser waveguides 29 of the laser portion 19 and to the first arm 37b and the second arm 37e of the Mach-Zehnder modulator portion 15. These waveguides are buried in the buried regions 39, and therefore the side surfaces of the waveguides are protected. Further, the burying of these waveguides in the buried regions 39 reduces the leak current associated with their side surfaces. One side surface and the other side surface of the first 7s arm 37b are defined by the first trench 47a and the second trench 47b, respectively. One side surface and the other side surface of the second arm $7c are defined by the third trench 47c and the fourth trench 47d, respectively. These trenches are disposed in the buried regions 39. These trenches contribute to the uniformity of the thickness of the resin body formed by application on the first arm 37h and the second arm 37c. Because the resin body is formed with a uniform thickness on top of the arms, the first opening 43a on the first arm 37b and the second opening 43b on the second arm 37c are formed with uniformity. Thus, it is possible to ensure that a plurality of Mach-Zehnder modulator portions 15 produced on a single wafer or with different production lots have uniform high-frequency characteristics.
The laser waveguides 29, the semiconductor waveguides 17, the first arm 37h and the second arm 37c are buried in the buried regions 39, whereas the first MMI 37a and the second MMI 37d are not buried in the buried regions 39. This configuration makes it possible to prevent the optical characteristics of the MMI couplers from being out of the designs defined by the dry etching process.
The buried regions 39 on the side surfaces on both sides of the first arm 37b and on the side surfaces on both sides of the second arm 37c is made of Fe-doped InP The Fe-doped InP contributes to the reduction of dark current at the first arm 37b and the second arm 37c. The thickness of the buried regions 39 on the side surfaces of the first arm 37h and the second arm 37c is preferably in the range of 0.3 μm to 0.5 μm. The thickness of 0.3 μm to 0.5 μm allows for both the reduction of dark current and the decrease in parasitic capacitance.
A method for manufacturing the semiconductor optical integrated device will be described with reference to
Next, a tunable distributed amplification (TDA) region is formed. As illustrated in
MZI region, and a laser portion 19 is formed in the SOA region, the DFB region and the DBR region. In the SOA region and TDA region, active sections of the laser waveguide are formed from the butt-joint mesas 69a to 69d. Passive sections of the laser waveguide are formed from the semiconductor stacks 71.
Next, after the mask 67 is removed, as illustrated in
As illustrated in
Next, as illustrated in
After forming the mask 87, a wet etching is performed in order to remove a damaged layer generated during the dry etching of the semiconductor stack on the side surfaces of the waveguide mesas 85. The waveguide mesas 85 covered with the mask 87 are protected from this wet etching and thus maintain the shape and the dimensional accuracy defined by the dry etching, Specifically, the waveguide mesas 85 for MMI couplers are not exposed to the wet etching, whereas the waveguide mesas 85 for laser waveguides and arms are wet etched. After the wet etching, buried regions 89 are grown using the ° WIPE method, as illustrated in
Next, there will be described steps in which a groove is formed across the semiconductor waveguide 17. After the formation of the buried regions 89, as illustrated in 9A, a mask 91 is formed on the regions for the Mach-Zehnder modulator portion 15, the semiconductor waveguides 17 and the laser portion 19. The mask 91 has an opening 91a on the waveguide mesa 85 for the semiconductor waveguide 17 and the buried regions 89. The semiconductor waveguide 17 connects the waveguide mesa 85 for the laser portion 19 to the waveguide mesa 85 for the Mach-Zehnder modulator portion 15. The opening 91a extends across the waveguide mesa 85 for the semiconductor waveguide 17, specifically, extends from the buried region 89 (89a) on one side of the waveguide mesa 85 to the buried semiconductor region 89 (89b) on the other side. As illustrated in
After the formation of the buried regions 89, trenches are formed in the buried regions 89. The trenches extend along the arm waveguides of the Mach-Zehnder modulator portion 15. The formation of the trenches is described with reference to
As illustrated in
With reference to specific examples, there will be described the reasons why the variations of modulation frequency bands are reduced. When the widths of the trenches 96a and 96b on both sides of the waveguide mesas 85 are the same as or similar to each other, the thickness of resin bodies extending from the trench 96a to the trench 96b over the waveguide mesa 85 (the thickness from the upper surface of the waveguide mesa 85 as the reference) is allowed to be uniform between the arm waveguides and also between the Mach-Zehnder modulators. An opening is formed in the resin body on the arm waveguide for the establishment of an electrical connection to the arm waveguide. When the thickness of the resin bodies on the waveguide mesas is uniform, the openings are formed by etching so as to ensure small variations in the opening size. Thus, variations of bands between the arm waveguides and between the Mach-Zehnder modulators are reduced. Further, the buried semiconductor terraces 96c and 96d serve as a help to control the areas to be buried with the resin body. This control of the area can substantially eliminate the occurrence of the separation of the resin body. The buried semiconductor may be semi-insulating InP (Fe-doped 10). The use of semi-insulating InP makes it possible to decrease the influence of the buried semiconductor layers on high-frequency characteristics. Thus, the buried semiconductor terraces 96c and 96d may be disposed close to the waveguide mesa 85.
For example, the thickness of the covering layer 89c on the side surface of the waveguide mesa 85, namely, the buried width BW may be in the range of 0.3 μm to 0.5 μm. The semiconductor burying with a thickness of 0.3 μm or more reduces dark current.
Further, the semiconductor burying with a thickness of 0.5 μm or less ensures that an increase in parasitic capacitance is avoided.
After the formation of the trenches 96a and 96b, as illustrated in
The resin body 99 on the device area for the laser portion 19 is removed by photolithography and an etching technique. After the formation of the resin body 99, as illustrated in
Through the aforementioned steps, the semiconductor optical integrated devices are manufactured.
First, crystals are grown on an n-type InP substrate by an OMVPE method to form an n-type InP buffer layer and an n-type GaInAsp grating layer (bandgap wavelength: 1300 nm). Next, the n-type GaInAsP grating layer is treated by an interference exposure method or a nano-imprint method to form a pattern of gratings. The n-type GaInAsP grating layer is etched by dry etching using CH4/H2 gas. This processing results in sampled gratings. After this formation, the patterned n-type GaInAsp grating layer is buried with InP by crystal growth using an OMVPE method. Subsequently, an n-type GaInAsP optical confinement layer (bandgap wavelength: 1200 nm), an undoped GaInAsP quantum well multilayer structure, an undoped optical confinement layer (bandgap wavelength: 1200 nm) and an undoped InP cap layer are grown. The quantum well multilayer structure has a bandgap wavelength of 1.55 μm and includes well layers and barrier layers. For example, the well layers include undoped GaInAsP having a thickness of 5 nm, and the barrier layers include undoped GaInAsP having a thickness of 10 nm.
A mask for the formation of butt-joints is formed. The mask includes SiN. The SiN film is deposited by a chemical vapor deposition (CVD) method. The thickness of the SiN film is 200 nm. The mask pattern for the formation of butt-joints is formed by photolithography and wet etching. The wet etching is performed using buffered hydrofluoric acid (BHF). Butt-joint mesas are formed by HCl wet etching through the patterned SiN mask, During the etching of the n-type GaInAsp optical confinement layer, the InP buffer layer disposed under the n-type GaInAsp optical confinement layer serves as an etching-stop layer. Next, an n-type InP layer, an undoped GaInAsP layer (bandgap wavelength: 1400 nm) and an undoped InP layer are grown while the SiN mask used for the formation of butt-joint mesas is used as a selective growth mask. These layers are used as waveguides for a distributed Bragg reflector (DBR), waveguides for a tunable distributed amplification (TDA) region, and waveguides for a Mach-Zehnder (MZ) modulator.
After the SiN mask used for the formation of butt-joint mesas is removed with BHF, a p-type InP cladding layer (thickness: 1500 nm) and a p-type GaInAs contact layer (thickness: 300 nm) are grown.
After these layers are grown, a SiN film (thickness: 300 nm) is deposited by a CVD method. The SiN film is treated by photolithography and etching (RIE using CF4 gas) to form a SiN waveguide mask defining a pattern of waveguides. Through the SiN waveguide mask, RIE is performed using Cl2 gas to form semiconductor mesa stripes.
Without removing the SiN waveguide mask, a SiN film (thickness: 200 nm) is deposited by a CVD method over the entire surface. The SiN film is processed into a regrowth mask by photolithography and etching with BHF. The regrowth mask covers the entirety of the regions for MMI couplers of the MZ modulator. With use of the regrowth mask, selective growth is performed to bury the arm waveguides for the MZ modulator and the laser waveguides for the wavelength-tunable laser diode. To realize this burying, the regrowth mask has openings through which the side surfaces of the arm waveguides for the MZ modulator and the side surfaces of the laser waveguides for the wavelength-tunable laser diode are accessible. Here, the SiN waveguide mask is still disposed while covering the upper surface of these waveguides. Subsequently, a damaged layer that has been generated by the dry etching is removed by wet etching with an HCl etchant. After the treatment, Fe-InP is regrown by an OMVPE method to bury the semiconductor stacks. Subsequently, the regrowth mask is removed with BHF.
Subsequently, a SiN film (thickness: 300 nm) is formed by a CVD method. The SiN film is treated by photolithography and CF4 dry etching to form a SiN groove mask defining the shape of a groove. Through the SiN groove mask, the semiconductor waveguide and the Fe-InP buried regions are etched by RIE using Cl2 gas. As a result, a groove is formed in the semiconductor waveguide and the Fe-InP buried regions. This groove is provided to prevent the heat from the wavelength tunable. laser portion from affecting the MZ modulator. The etching is stopped when the groove reaches a depth immediately above the core layer in the semiconductor waveguide. Plasma monitoring is used to stop the etching at this depth. In the etching step, the wavelength-tunable laser portion and the MZ modulator region are covered with the SiN groove mask.
Trenches are formed in order to reduce the parasitic capacitance of the arm waveguides for the MZ modulator. For the formation of trenches, a SiN mask which defines the shape of the trench structures is formed by depositing a SiN film (thickness: 300 nm) over the entire surface by a CVD method and treating the SiN film by photolithography and CF4 dry etching. Through the SiN mask, the Fe-InP buried layers are etched by RIE using Cl2 gas to form trenches. During this step, the wavelength-tunable laser portion and the groove are covered with the SiN mask.
After the trenches are formed in the Fe-InP buried regions of the MZ modulator region, a silicon dioxide film (thickness: 300 nm) is deposited to passivate the entire device. Further, a BCB resin is applied over the entire surface of the device for planarization. Subsequently, the BCB resin in the wavelength-tunable laser portion is removed by photolithograph) and dry etching with CF4/O2 gas.
Contact openings are formed in the BCB resin on the arm waveguides for the MZ modulator by photolithography and dry etching with CF4/O2 gas. During this etching, the MIMI coupler regions, the wavelength-tunable laser portion and the groove are covered with a resist mask. In the contact openings, the contact layers for contact with ohmic electrodes are exposed. P-Side and n-side ohmic electrodes are formed on the arm waveguides for the MZI modulator and on the wavelength-tunable laser portion.
In this Example, the side surfaces of the arm waveguide mesas for the MZ modulator are buried in Fe-InP. Further, trenches are disposed in the Fe-InP buried regions in which the arm waveguides for the MZ modulator are buried. Furthermore, the trenches are buried with BCB resin. With this structure, the MZ modulator and the wavelength-tunable laser achieve high reliability and good high-frequency characteristics. Further, the groove disposed between the wavelength-tunable laser and the MZ modulator prevents the phase variations of the MZ modulator from being destabilized by the heat generated by the wavelength tuning of the wavelength-tunable laser.
While preferred embodiments have been discussed above while illustrating the principle of the present invention, those skilled in the art will appreciate that various modifications may be made to the configurations and the details discussed above without departing from the principle of the invention. The scope of the invention is not limited to any specific configurations disclosed in the embodiments. Therefore, the features defined in the appended claims and all modifications and alterations which are within the spirit of the invention are claimed.
Number | Date | Country | Kind |
---|---|---|---|
2014-099704 | May 2014 | JP | national |