WO2021022476A1 - Waveguide structure, integrated optical chip, and method for realizing electrical isolation - Google Patents

Waveguide structure, integrated optical chip, and method for realizing electrical isolation Download PDF

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Publication number
WO2021022476A1
WO2021022476A1 PCT/CN2019/099441 CN2019099441W WO2021022476A1 WO 2021022476 A1 WO2021022476 A1 WO 2021022476A1 CN 2019099441 W CN2019099441 W CN 2019099441W WO 2021022476 A1 WO2021022476 A1 WO 2021022476A1
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layer
doped layer
cavity
waveguide
doped
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PCT/CN2019/099441
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French (fr)
Chinese (zh)
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邵海峰
陈宏民
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华为技术有限公司
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Priority to PCT/CN2019/099441 priority Critical patent/WO2021022476A1/en
Priority to CN201980098441.0A priority patent/CN114128061A/en
Publication of WO2021022476A1 publication Critical patent/WO2021022476A1/en

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/06Arrangements for controlling the laser output parameters, e.g. by operating on the active medium

Definitions

  • This application relates to the field of semiconductor technology, in particular to a waveguide structure, an integrated optical chip, and a method for achieving electrical isolation.
  • optical communication technology is widely used in network data transmission to meet the requirements of network transmission performance.
  • the integrated optical chip plays an important role in optical communication.
  • the integrated optical chip uses a semi-insulating substrate to integrate active optical devices such as lasers, modulators, semiconductor optical amplifiers (SOA), and detectors, and these active devices are connected by optical waveguides.
  • active optical devices usually share the same conductive layer (such as N-type doped layer or P-type doped layer), and active optical devices need to apply corresponding work on the shared conductive layer in the area where the active optical device is located.
  • Voltage can achieve its own functions (such as modulation, amplification, detection, etc.).
  • different working voltages are usually applied, so that a voltage difference is formed between different regions of the shared conductive layer. There is current flowing between different areas of the shared conductive layer, which may increase the power consumption of the integrated optical chip, affect the normal operation of the integrated optical chip, and may also cause electrical crosstalk between two active optical devices with different working voltages .
  • the laser, semiconductor optical amplifier, modulator in the integrated optical chip, and the optical waveguide connecting these active optical devices share the N-type doped layer.
  • the modulator needs to be loaded with a forward voltage, such as +10V, on the N-type doped layer where the modulator is working, while the laser and optical amplifier need to be loaded with 0V voltage on the N-type doped layer when working, resulting in the modulator and the laser , There is a 10V voltage difference in the N-type doped layer between the amplifiers, which generates a lot of heat and power consumption.
  • This application provides a waveguide structure, an integrated optical chip, and a method for achieving electrical isolation, so as to solve the problem of electrical crosstalk in the integrated optical chip due to the different working voltages of different active optical devices in the integrated optical chip, and increase the power of the integrated optical chip.
  • the problem of consumption is a problem of consumption.
  • this application provides a waveguide structure, which is applied to an integrated optical chip.
  • the waveguide structure includes a substrate, a first doped layer, a second doped layer, and a first waveguide core layer stacked in sequence from bottom to top, and the first waveguide core layer covers a part of the upper surface of the second doped layer .
  • the second doped layer includes an upper barrier layer and a sacrificial layer, and the sacrificial layer is located between the upper barrier layer and the first waveguide core layer for supporting the upper barrier layer.
  • the first doped layer can be an N-type doped layer or a P-type doped layer.
  • the second doped layer is a P-type doped layer.
  • the second doped layer is an N-type doped layer, that is, the first doped layer and the second doped layer have opposite doping types.
  • the second doped layer of the waveguide structure has at least one cavity, and the thickness of the upper barrier layer directly above the cavity can be controlled to a smaller value according to actual requirements, the cavity can be increased.
  • the impedance of the upper barrier layer directly above reduces the current transmitted by the upper barrier layer directly above the cavity in the direction extending along the waveguide core layer.
  • the doping types of the first doped layer and the second doped layer are opposite, so that the waveguide structure is formed on opposite sides of the cavity and shares the substrate, the first doped layer and the second doped layer of the waveguide structure.
  • a PNP structure or an NPN structure is formed between the active optical devices of the layer, and the PNP structure or the NPN structure is reversely cut off when the active optical device is working, further suppressing the transmission of the second doped layer in the direction extending along the waveguide core layer ⁇ current. Therefore, the waveguide structure provided by the embodiments of the present application can effectively suppress the current transmitted by the second doped layer in the direction along the waveguide core layer, and thus can realize the active structure formed on opposite sides of the cavity of the waveguide structure in the integrated optical chip. Electrical isolation between optical devices.
  • the projection of the first waveguide core layer on the plane of the bottom wall of the cavity is located in the bottom wall of the cavity, wherein the bottom wall of the cavity is a partial area of the upper surface of the first doped layer .
  • the cavity is enclosed by the upper barrier layer, the sacrificial layer and the first doped layer.
  • target ions are implanted in the upper barrier layer directly above the cavity, and the target ions are used to increase the upper barrier layer directly above the cavity ⁇ impedance.
  • the target ions may be ions such as helium ions that can increase the resistance of the blocking layer on the portion directly above the cavity.
  • the thickness of the upper barrier layer in the waveguide structure can be controlled according to actual needs, usually the thickness of the upper barrier layer is small, so the energy required for ion implantation is lower, which can solve the electrical isolation effect caused by the limitation of ion implantation energy on ion implantation depth
  • the problem of poorness enables the target ions to be implanted as far as possible into the entire thickness range of the upper barrier layer directly above the cavity, thereby making the impedance of the upper barrier layer directly above the cavity larger, which can effectively isolate the electrical isolation .
  • the thickness of the upper barrier layer directly above the cavity is less than or equal to a set value, and the set value is the maximum depth at which target ions can be implanted into the upper barrier layer directly above the cavity, to The target ions can be implanted into the entire thickness range of the upper barrier layer directly above the cavity.
  • the waveguide structure further includes a third doped layer, the third doped layer is located above the first waveguide core layer, wherein the second doped layer is an N-type doped layer, and the third doped layer It is a P-type doped layer; or, the second doped layer is a P-type doped layer, and the third doped layer is an N-type doped layer.
  • the material of the third doped layer may be indium phosphide InP.
  • the first doped layer includes a buffer layer and a lower barrier layer, the buffer layer is located between the lower barrier layer and the substrate; the bottom wall of the cavity is a partial area of the upper surface of the lower barrier layer.
  • the present application also provides an integrated optical chip.
  • the integrated optical chip includes the waveguide structure, the first active component, and the second active component described in any one of the possible implementations of the first aspect.
  • the upper surface of the upper barrier layer is provided with a first active component and a second active component isolated from each other.
  • the first active component and the second active component are respectively located on opposite sides of the cavity. Just below is a part of the sacrificial layer, directly below the second active component is another part of the sacrificial layer, the sacrificial layer directly below the first active component and the sacrificial layer directly below the second active component are separated by the cavity Come.
  • the first active component includes a second waveguide core layer and a fourth doped layer stacked sequentially from bottom to top.
  • the second active component includes a third waveguide core layer and a fifth doped layer stacked sequentially from bottom to top.
  • the second waveguide core layer and the third waveguide core layer are respectively connected with the first waveguide core layer.
  • the second doped layer is an N-type doped layer
  • the fourth doped layer and the fifth doped layer are both P-type doped layers; alternatively, the second doped layer is a P-type doped layer, and the fourth doped layer And the fifth doped layer is an N-type doped layer.
  • the first active component and the part of the waveguide structure directly below the first active component (including the second doped layer directly below the first active component, the first doped layer and the substrate )
  • the second active component and the part of the waveguide structure directly below the second active component forms the second active optical device, that is, the first active optical device and the second active optical device share the substrate, the first doped layer and the second doped layer.
  • the voltage of the first active device is different from the voltage of the second active device.
  • the voltage on the second doped layer in the first active device is different from the voltage on the second doped layer.
  • the voltage on the second doped layer in the second active device is different.
  • the first active optical device may be a modulator
  • the second active optical device may be a laser, an optical amplifier, or an optical detector.
  • first The groove and the second groove, the first groove and the second groove all penetrate the second doped layer.
  • the first active optical device, the second active optical device and the isolation device are all located between the first groove and the second groove, and the isolation device includes a first waveguide core layer, a second doped layer, and a first doped The part of the impurity layer directly below the second doped layer and the part of the substrate directly below the second doped layer.
  • this application also provides a method of electrical isolation, which is used to achieve electrical isolation between active optical devices in an integrated optical chip.
  • the method includes: sequentially growing a first doped layer, a second doped layer, and a first waveguide core layer on a substrate, the first waveguide core layer covers a part of the upper surface of the second doped layer, and the second doping
  • the layer includes an upper barrier layer and a sacrificial layer, the sacrificial layer is located between the first doped layer and the upper barrier layer;
  • the first doped layer is an N-type doped layer, and the second doped layer is a P-type doped layer, or ,
  • the first doped layer is a P-type doped layer, the second doped layer is an N-type doped layer;
  • the first waveguide core layer is etched to form a waveguide trench, the depth of the waveguide trench is greater than The thickness of the first waveguide core layer;
  • the second doped layer exposed in the waveguide trench is etched to form at
  • the second doped layer exposed in the waveguide trench is etched to form at least one cavity in the second doped layer, which specifically includes the following steps: the upper barrier exposed in the waveguide trench The layer is etched to form at least one etch window; wherein the depth of the etch window is greater than the thickness of the upper barrier layer; an etchant is added to the at least one etch window to etch the sacrificial layer to form at least one cavity.
  • the second doped layer exposed in the waveguide trench is etched, and after at least one cavity is formed in the second doped layer, the method further includes: blocking the part directly above the cavity The target ions are implanted into the layer; wherein the target ions are used to increase the impedance of the barrier layer on the part directly above the cavity.
  • any of the integrated optical chips provided above includes the waveguide structure described in the first aspect, and any one of the foregoing methods for achieving electrical isolation can prepare the waveguide structure described in the first aspect.
  • the beneficial effects that can be achieved can refer to the beneficial effects in the corresponding waveguide structure provided in the first aspect, which will not be repeated here.
  • 1A is one of the three-dimensional schematic diagrams of a waveguide structure provided by an embodiment of the application.
  • FIG. 1B is one of the schematic cross-sectional views of a waveguide structure in the BB' direction according to an embodiment of the application;
  • FIG. 1C is one of the schematic cross-sectional views in the AA' direction of a waveguide structure according to an embodiment of the application;
  • FIG. 1D is the second cross-sectional schematic diagram of a waveguide structure in the AA' direction according to an embodiment of the application;
  • FIG. 2 is a schematic diagram of the relationship between a waveguide structure and an active optical device according to an embodiment of the application;
  • 3A is the second schematic diagram of a three-dimensional structure of a waveguide structure provided by an embodiment of this application.
  • 3B is a schematic cross-sectional view of a waveguide structure in the CC' direction according to an embodiment of the application;
  • 3C is the second schematic cross-sectional view of a waveguide structure in the BB' direction according to an embodiment of the application;
  • 4A is the third schematic diagram of a three-dimensional structure of a waveguide structure provided by an embodiment of this application.
  • 4B is the second schematic cross-sectional view of a waveguide structure in the AA' direction according to an embodiment of the application;
  • 4C is the third schematic cross-sectional view of a waveguide structure in the BB' direction according to an embodiment of the application;
  • 5A is a fourth schematic diagram of a three-dimensional structure of a waveguide structure provided by an embodiment of this application.
  • 5B is the third schematic cross-sectional view of a waveguide structure in the AA' direction according to an embodiment of the application;
  • FIG. 5C is the fourth cross-sectional schematic diagram of a waveguide structure in the BB' direction according to an embodiment of the application;
  • FIG. 6 is a fifth schematic diagram of a three-dimensional structure of a waveguide structure provided by an embodiment of this application.
  • FIG. 7A is one of the top schematic diagrams of an integrated optical chip provided by an embodiment of the application.
  • FIG. 7B is one of the schematic cross-sectional views in the AA' direction of an integrated optical chip according to an embodiment of the application;
  • FIG. 8 is a schematic structural diagram of a modulator provided by an embodiment of the application.
  • 9A is the second schematic top view of an integrated optical chip provided by an embodiment of the application.
  • FIG. 9B is one of the schematic cross-sectional views of an integrated optical chip in the BB' direction according to an embodiment of the application.
  • 10A is the third schematic top view of an integrated optical chip provided by an embodiment of this application.
  • 10B is a fourth schematic top view of an integrated optical chip provided by an embodiment of this application.
  • 10C is a fifth schematic top view of an integrated optical chip provided by an embodiment of the application.
  • FIG. 11 is a schematic flowchart of an electrical isolation method provided by an embodiment of the application.
  • FIG. 12 is a schematic diagram of the relationship between an ion implantation angle and the upper barrier layer provided by an embodiment of the application.
  • Active optical devices such as lasers, modulators, SOA, and detectors integrated in integrated optical chips usually share the same conductive layer (such as N-type doped layer or P-type doped layer), while active optical devices need to share conductive layers. Only when the corresponding working voltage is applied to the area where the active optical device on the layer is located can its own functions (such as modulation, amplification, detection, etc.) be realized. For active optical devices with different functions, it is usually necessary to apply different working voltages to form a voltage difference between different regions of the shared conductive layer (because different regions of the shared conductive layer are respectively provided with active optical devices with different working voltages), This leads to an increase in the power consumption of the integrated optical chip, which affects the normal operation of the integrated optical chip. In addition, electrical crosstalk may also occur between two active optical devices with different operating voltages.
  • helium ion implantation is usually used to form electrical isolation between different regions of the conductive layer of the integrated optical chip.
  • the conductive layer of the integrated optical chip is shared by multiple active optical devices, and the multiple active optical devices are located in different regions of the conductive layer.
  • the conductive layer shared by the active optical devices in the integrated optical chip is usually thicker, because when the conductive layer shared by the active optical devices in the integrated optical chip is thick, it has many benefits to the integrated optical chip, such as beneficial to the active optical chip.
  • the loading of the bias voltage (or working voltage) on the device can reduce the resistance of the shared conductive layer in the active optical device and can increase the bandwidth of the modulator.
  • the corresponding implantation depth is limited.
  • the implantation depth corresponding to the energy of 400keV is about 1.6um.
  • the greater the implantation depth the higher the energy required, and the higher the cost of ion implantation. Therefore, only using the helium ion implantation method, the electrical isolation effect between the regions where different active optical devices are located in the conductive layer shared by the active optical devices in the integrated optical chip is poor.
  • the active optical devices in the integrated optical chip are connected by optical waveguides (or waveguide core layers), that is, the active optical devices in the integrated optical chip are optically connected through the waveguide core layer on the shared conductive layer, which also increases The difficulty of electrical isolation in the direction in which the waveguide core layer extends (the direction of optical signal propagation) between the regions where different active optical devices are located in the conductive layer shared by the active optical devices.
  • the present application provides a waveguide structure for achieving electrical isolation between active optical devices in an integrated optical chip.
  • the waveguide structure 100 is applied to an integrated optical chip to realize the propagation direction of the optical signal of the active optical device in the integrated optical chip (that is, the optical waveguide in the integrated chip). Extension direction) electrical isolation.
  • the waveguide structure 100 includes a substrate 110, a first doped layer 120, a second doped layer 130, and a first waveguide core layer 140 that are sequentially stacked from bottom to top.
  • the first waveguide core layer 140 covers a partial area of the upper surface of the second doped layer 130.
  • the so-called upper surface of any layer refers to the surface of the layer (for example, the first doped layer 120) facing upward
  • any layer for example, The lower surface of the first doped layer 120 refers to the surface of the layer (for example, the first doped layer 120) facing downward.
  • the upper and lower surfaces of any layer are opposite.
  • upper and lower are a pair of relative concepts, and the upper and lower refer to the current placement orientation of the drawings of this application.
  • the first doped layer 120 is located above the substrate 110 and below the second doped layer 130
  • the first waveguide core layer 140 is located above the second doped layer 130.
  • the second doped layer 130 includes an upper barrier layer 131 and a sacrificial layer 132.
  • the sacrificial layer 132 is located between the upper barrier layer 131 and the first waveguide core layer 140 and is used to support the upper barrier layer 131.
  • a cross-sectional view of the waveguide structure 100 in the BB' direction (the extending direction of the cavity 133) is shown in FIG. 1B. It can be seen from FIG. 1B that the cavity 133 runs along the cavity.
  • the extending direction of the cavity 133 penetrates the second doped layer 130, the first waveguide core layer 140 is located directly above the cavity 133, and the extending direction of the cavity 133 and the extending direction of the first waveguide core layer 140 are perpendicular to each other.
  • FIG. 1C The cross-sectional view of the waveguide structure 100 in the AA' direction (the extension direction of the first waveguide core layer 140) is shown in FIG. 1C.
  • the cavity 133 is formed by the upper barrier layer 131, the sacrificial layer 132 and the first doped layer.
  • a part of the upper surface of the upper barrier layer 131 is the top wall of the cavity 133
  • the side of the sacrificial layer 132 facing the cavity 133 is the side wall of the cavity 133
  • the first doped layer 120 Part of the upper surface of the area is the bottom wall of the cavity 133.
  • the projection of the first waveguide core layer 140 on the plane of the bottom wall of the cavity 133 is located in the bottom wall of the cavity 133.
  • the sacrificial layer 132 When the second doped layer 130 has one cavity 133, the sacrificial layer 132 includes two parts, as shown in FIG. 1C, when the second doped layer 130 has two or more cavities 133, the sacrificial layer 132 includes at least three parts. For example, when there are two cavities 133 in the second doped layer 130, the sacrificial layer 132 includes three parts, as shown in FIG. 1D.
  • the first doped layer 120 may be an N-type doped layer or a P-type doped layer.
  • the second doped layer 130 is a P-type doped layer.
  • the second doped layer 130 is an N-type doped layer, that is, the doping types of the first doped layer 120 and the second doped layer 130 are opposite, so that the waveguide structure 100
  • the PNP structure or NPN structure is formed between the active optical devices that share the waveguide structure 100, the substrate 110, the first doped layer 120, and the second doped layer 130 formed on opposite sides of the cavity 133 (as shown in FIG.
  • the PNP structure or the NPN structure is reversely cut off when the active optical device is working, which can prevent the active device from conducting conduction through the first doped layer 120 in the waveguide structure 100.
  • the upper barrier layer 131 and the sacrificial layer 132 have the same doping type, that is, when the second doped layer 130 is a P-type doped layer, the upper barrier layer 131 and the sacrificial layer 132 are both P-type doped layers.
  • the second doped layer 130 is an N-type doped layer
  • the upper barrier layer 131 and the sacrificial layer 132 are both N-type doped layers.
  • the substrate 110 may be a semi-insulating (SI) substrate, and the material of the substrate 110 may be indium phosphide (InP).
  • the waveguide core layer 140 is used to transmit optical signals, and the waveguide core layer 140 may be etched to form one or more parallel optical waveguides to transmit optical signals.
  • the waveguide structure 100 mainly realizes the electrical isolation between the active optical devices in the integrated optical chip through the area where the cavity 133 is located.
  • the upper barrier layer 131 can be divided into a first part and a second part. There are two parts. The first part is the upper barrier layer 131 directly above the cavity 133, and the second part is the part directly above the sacrificial layer 132.
  • the upper barrier layer 131 is located in the cavity 133.
  • the upper part of the upper barrier layer 131 directly above may also be implanted with target ions, and the target ions are used to increase the impedance of the upper barrier layer 131 in the part directly above the cavity 133.
  • the target ions may be ions such as helium ions that can increase the resistance of the blocking layer 131 on the portion directly above the cavity 133.
  • the thickness of the upper barrier layer 131 in the waveguide structure 100 can be controlled according to actual requirements (for example, 2 ⁇ m-10 ⁇ m), usually the thickness of the upper barrier layer 131 is small (may be less than 2 ⁇ m), so the energy required for ion implantation is low, which can solve
  • the problem of poor electrical isolation caused by the limitation of ion implantation energy on the depth of ion implantation enables target ions to be implanted as far as possible into the entire thickness range of the upper barrier layer 131 located directly above the cavity 133, thereby making the cavity 133 positive.
  • the upper barrier layer 131 above has a relatively large impedance, which can effectively isolate the electrical isolation.
  • the thickness of the upper barrier layer 131 directly above the cavity 133 is less than or equal to a set value, and the set value is the maximum depth that target ions can be implanted into the upper barrier layer directly above the cavity 133 to The target ions can be implanted into the entire thickness range of the upper barrier layer 131 directly above the cavity 133.
  • the cavity 133 can be obtained by etching the sacrificial layer 132, that is, the reaction rate of the sacrificial layer 132 and the etchant is greater than the reaction rate of the upper barrier layer 131 and the etchant, so that the sacrificial layer 132 can be etched away , And the upper barrier layer 131 can be retained to form a cavity 133.
  • the size of the cavity 133 can be controlled by the dose of the etchant and the etching time (that is, by controlling the volume of the sacrificial layer 132 etched away) The size of the cavity 133).
  • etching windows 134 may be formed on the upper barrier layer 132, and these etching windows 134 are located Both sides of the waveguide core layer 140 or the same side. It should be noted that the embodiment of the present application does not limit the size, shape, and number of the etching window 134, and the etching window 134 may specifically be a rectangle, a rounded rectangle, a circle, or a triangle.
  • the material of the sacrificial layer 132 may be InGaAs, InAlAs, InAlAs, or three layers of InP, InAlAs, and InP.
  • the material of the upper barrier layer 131 may be
  • the sacrificial layer 132 is composed of three layers of InP, InAlAs, and InP
  • the material of the upper barrier layer 131 may be InGaAs, InAlAs or InGaAsP InGaAsP.
  • the refractive index of the waveguide core layer 140 is greater than the refractive index of the material around the waveguide core layer 140 (for example, the second doped layer 130), forming a certain refractive index difference to confine the optical signal in the waveguide core layer 140 Transmission, reducing the leakage of optical signals. Therefore, in a scenario where the refractive index of the upper barrier layer 131 is close to the refractive index of the waveguide core layer 140 (for example, the current lower cladding layer), the second doped layer 130 may also include a lower cladding layer 135, which is located in the waveguide. Between the core layer 140 and the upper barrier layer 131, compared to the lower cladding layer 135, the upper barrier layer 131 is thinner.
  • FIG. 4A a three-dimensional schematic diagram of the waveguide structure 100 is shown in FIG. 4A, a cross-sectional view of the waveguide structure 100 in the AA' direction As shown in FIG. 4B, the cross-sectional view of the waveguide structure 100 in the BB' direction is as shown in FIG. 4C.
  • the material of the under-cladding layer 135 may be InP.
  • the first doped layer 120 may include a buffer layer 121 and a lower barrier layer 122.
  • the buffer layer 121 is located between the lower barrier layer 1221 and the substrate 110.
  • FIG. 5A a three-dimensional schematic diagram of the waveguide structure 100 is shown in FIG. 5A.
  • the cross-sectional view of the waveguide structure 100 in the AA' direction is shown in FIG. 5B
  • FIG. 5C the cross-sectional view of the waveguide structure 10 in the BB' direction
  • FIG. 5C It can be seen from FIG. 5B that in the scenario where the first doped layer 120 includes the buffer layer 121 and the lower barrier layer 122, the bottom wall of the cavity 133 is a partial area of the upper surface of the lower barrier layer 122.
  • the buffer layer 121 is used to perform lattice matching on the substrate 110 to improve the quality of the material grown on the substrate 110.
  • the doping types of the buffer layer 121 and the lower barrier layer 122 are the same.
  • the doping types of the buffer layer 121 and the lower barrier layer 122 are also P-type doping.
  • the doping types of the buffer layer 121 and the lower barrier layer 122 are also N-type doping.
  • the material of the buffer layer 121 is usually InP
  • the material of the lower barrier layer 122 is usually the same as the material of the upper barrier layer 131, and may be InP, InGaAs, InAlAs, or the like. Therefore, the combination of materials used in the upper barrier layer 131, the sacrificial layer 132, and the lower barrier layer 122 includes but is not limited to any of the following: (1) the upper barrier layer 131 is InP, and the sacrificial layer 132 is InGaAs, The lower barrier layer 122 is InP; (2) the upper barrier layer 131 is InP, the sacrificial layer 132 is InAlAs, and the lower barrier layer 122 is InP; (3) the upper barrier layer 131 is InGaAs, and the sacrificial layer 132 is composed of InP, InAlAs, and It is composed of three layers of InP, the lower barrier layer 122 is InGaAs; (4) the upper barrier layer 131 is InAlAs,
  • the waveguide structure 100 may further include a third doped layer 150 formed on the waveguide core layer 140.
  • the third doped layer 150 is a P-type doped layer.
  • the third doped layer 150 is an N-type doped layer, that is, the second doped layer 130 and the third doped layer 150
  • the doping type is opposite.
  • the material of the third doped layer 150 may be InP.
  • the second doped layer 130 of the waveguide structure 100 has at least one cavity 133, and the thickness of the upper barrier layer 131 directly above the cavity 133 can be controlled to a smaller value according to actual requirements,
  • the impedance of the upper barrier layer 131 directly above the cavity 133 is increased, and the current transmitted by the upper barrier layer 131 directly above the cavity 133 in the direction along which the waveguide core layer 140 extends is reduced.
  • the first doped layer 120 and the second doped layer 130 have opposite doping types, so that the waveguide structure 100 is formed on opposite sides of the cavity 133 and shares the substrate 110 and the first doped layer of the waveguide structure 100.
  • a PNP structure or an NPN structure is formed between the active optical device of the layer 120 and the second doped layer 130.
  • the PNP structure or the NPN structure is reversely cut off, further suppressing the second doping layer 130 A current that travels in the direction in which the core of the waveguide extends. Therefore, the waveguide structure 100 provided by the embodiments of the present application can effectively suppress the current transmitted by the second doped layer 130 in the extending direction of the waveguide core layer, and then can realize the integrated optical chip through the waveguide structure 100 on opposite sides of the cavity 133.
  • the electrical isolation between the formed active optical devices can effectively suppress the current transmitted by the second doped layer 130 in the extending direction of the waveguide core layer, and then can realize the integrated optical chip through the waveguide structure 100 on opposite sides of the cavity 133.
  • the present application also provides an integrated optical chip 200.
  • a top view is shown in FIG. 7A.
  • the integrated optical chip 200 includes the waveguide structure 100 and the first active component 210 described in any one of the above possible embodiments. And second active component 220. As shown in FIG. 7A
  • the first active component 210 and the second active component 220 are disposed on the upper surface of the upper barrier layer of the waveguide structure 100, and the first active component 210 and the second active component 220 are respectively located in the cavity 133
  • the first active component 210 and the second active component 220 are respectively located in the cavity 133
  • just below the first active component is a part of the sacrificial layer 132
  • directly below the second active component 132 is another part of the sacrificial layer 132
  • the sacrificial layer 132 directly below the second active component 220 is separated by the cavity 133, that is, the sacrificial layer 132 is divided into at least two parts by the cavity 133.
  • the first active component 210 includes a second waveguide core layer 211 and a fourth doped layer 212 stacked sequentially from bottom to top.
  • the second active component 220 includes a third waveguide core layer 221 and a fourth doped layer stacked sequentially from bottom to top.
  • the fifth doped layer 222, the second waveguide core layer 211 and the third waveguide core layer 221 are respectively connected to the first waveguide core layer 140.
  • the second doped layer 130 is an N-type doped layer, and the fourth doped layer 212 and the fifth doped layer 222 are both P-type doped layers; or, the second doped layer 130 is a P-type doped layer, The fourth doped layer 212 and the fifth doped layer 222 are both N-type doped layers.
  • the first active component 210 and the part of the waveguide structure 100 directly below the first active component 210 forms the first active optical device 230, the second active component 220, and the portion of the waveguide structure 100 directly below the second active component 220 (including the second doping directly below the second active component 220).
  • the layer 130, the first doped layer 120 and the substrate 110) form a second active optical device, that is, the first active optical device 230 and the second active optical device 240 share the substrate 110, the first doped The layer 120 and the second doped layer 130.
  • the integrated optical chip 200 because when the integrated optical chip 200 is working, not all the active optical devices in the integrated optical chip 200 have a voltage difference between the second doped layers 130. Therefore, in order to save the cost of the integrated optical chip 200, and To reduce the processing complexity of the integrated optical chip 200, only active optical devices with a voltage difference between the second doped layers 130 during operation can be arranged on opposite sides of the cavity 133 and connected. That is to say, when the integrated optical chip 200 is working, the voltage of the first active device 230 is different from the voltage of the second active device 240, in particular, the voltage on the second doped layer 130 in the first active device 230 The voltage is different from the voltage on the second doped layer 130 in the second active device 240.
  • the first active optical device 230 may be a modulator
  • the second active optical device 240 may be a laser, an optical amplifier, or an optical detector.
  • the modulator sequentially includes a substrate 110, a first doped layer 120, a second doped layer 130, a second waveguide core layer 211, and a first doped layer.
  • the second doped layer 130 is provided with a first electrode 213, and the fourth doped layer 212 is provided with a second electrode 214.
  • the first doped layer 120 may be a P-type doped layer based on InP
  • the second doped layer 130 may be an InP-based N-type doped layer
  • the fourth doped layer 212 may be an InP-based P-type doped layer.
  • the voltage on the first electrode 213 is higher than the voltage on the second electrode 214
  • the second waveguide core layer 211 performs electro-optic modulation based on the quantum confined stark effect (QCSE) or other photoelectric effects.
  • QCSE quantum confined stark effect
  • the first waveguide structure 100 has first The groove 250 and the second groove 260, the first groove 250 and the second groove 260 both penetrate the second doped layer 130, so that current cannot pass between the active devices except for the extending direction of the first waveguide core layer 140.
  • the second doped layer 130 in the direction is transmitted.
  • the top view of the integrated optical chip 200 is shown in FIG. 9A, and the cross-sectional view of the integrated optical chip 200 in the AA′ direction is shown in FIG. 9B.
  • the isolation device 270 includes a first waveguide core layer 140, a second The doped layer 130, the portion of the first doped layer 120 directly below the second doped layer 130, and the portion of the substrate 110 directly below the second doped layer 130, as shown in FIG. 9B.
  • the isolation device 270 further includes the third doped layer 150 above the first waveguide core layer 140, that is, the isolation device 270 includes the third doped layer 150 above the first waveguide core layer 140.
  • the doped layer 150, the first waveguide core layer 140, the second doped layer 130, the portion of the first doped layer 120 directly below the second doped layer 130, and the substrate 110 is located directly on the second doped layer 130 The lower part.
  • the aforementioned waveguide structure 100 may be an isolation device 270.
  • first groove 250 and the second groove 260 may also penetrate the first doped layer 120 on the substrate 110.
  • the embodiments of the present application do not limit the number of first active devices and the number of second active devices. Since there is no voltage difference between the plurality of first active optical devices 230 or the plurality of second active optical devices 240 in the integrated optical chip 200, the plurality of first active optical devices 230 or the plurality of second active optical devices The devices 240 may be located on the same side of the cavity 133, that is, between the plurality of first active optical devices 230 or between the plurality of second active optical devices 240 may not be electrically isolated by the cavity 133. For example, as shown in FIG.
  • the modulator, laser, and optical amplifier included in the integrated optical chip 200 are located on opposite sides of the first cavity 133, and the modulator and the optical amplifier are located in the second cavity 133.
  • the modulator, laser, and optical amplifier included in the integrated optical chip 200 are respectively located on opposite sides of the cavity 133, the laser and the optical amplifier are located on the same side, by the integrated optical
  • the modulator, laser, and optical amplifier in the integrated optical chip 200 there is no voltage difference between the laser and the optical amplifier, so the laser and the optical amplifier do not need to be electrically isolated by the cavity 133;
  • Figure 10C the modulator, laser, and optical amplifier in the integrated optical chip 200
  • the optical detector, the modulator and the optical amplifier are located on opposite sides of the cavity 133, and the laser, the optical detector and the optical amplifier are on the same side.
  • the integrated optical chip 200 works, there is no space between the laser, the optical detector and the optical amplifier. Because of the voltage difference, the laser, the photodetector
  • the integrated optical chip 200 provided by the embodiment of the present application is a complete integrated optical chip, and also has the structure of a known integrated optical chip (such as a driving circuit of an active optical device).
  • a known integrated optical chip such as a driving circuit of an active optical device.
  • the related structure of the optical chip involved in realizing the electrical isolation of the common doped layer of the active device in the integrated optical chip will be described, and other structures will not be repeated.
  • this application also provides a method for realizing electrical isolation between active optical devices in an integrated optical chip, that is, a method for preparing the waveguide structure 100. As shown in Figure 11, the method mainly includes the following steps:
  • S1101 The first doped layer 120, the second doped layer 130, and the first waveguide core layer 140 are sequentially grown on the substrate 110.
  • the first waveguide core layer 140 covers a part of the upper surface of the second doped layer 130.
  • the second doped layer 130 includes an upper barrier layer 131 and a sacrificial layer 132.
  • the sacrificial layer 132 is located on the first doped layer 120 and above.
  • the first doped layer 120 may be an N-type doped layer or a P-type doped layer, when the first doped layer 120 is an N-type doped layer, the second doped layer 130 is a P-type Doped layer.
  • the second doped layer 130 is an N-type doped layer, that is, the doping type of the first doped layer 120 and the second doped layer 130 in contrast.
  • S1102 Etching the first waveguide core layer 140 to form a waveguide trench.
  • the depth of the waveguide groove is greater than the thickness of the first waveguide core layer 140 to expose the second doped layer 130 under the first waveguide core layer 140.
  • S1103 The second doped layer 130 exposed in the waveguide trench is etched, and at least one cavity 133 is formed in the second doped layer 130.
  • the sacrificial layer 132 remaining after etching is used to support the upper barrier layer 131, the cavity 133 penetrates the second doped layer 130 along the extending direction of the cavity 133, and the first waveguide core layer 140 is located directly above the cavity 133.
  • the extension direction of the cavity 133 and the extension direction of the first waveguide core layer 140 are perpendicular to each other.
  • etching the second doped layer 130 exposed in the waveguide trench to form at least one cavity 133 in the second doped layer 130 includes the following steps: i. Exposing the waveguide trench The upper barrier layer 131 is etched to form at least one etch window 134; wherein the depth of the etch window 134 is greater than the thickness of the upper barrier layer 131, so that the etchant can contact the sacrificial layer 132, and then to Etching is performed to form a cavity 133; ii, an etchant is added to at least one etching window to etch the sacrificial layer 132 to form at least one cavity 133. Specifically, when the second doped layer 130 exposed in the waveguide trench is etched, the area except for the etching window is protected by a mask.
  • the method further includes: implanting target ions into the upper barrier layer 131 directly above the cavity 133.
  • the target ions are used to increase the impedance of the blocking layer 131 on the portion directly above the cavity 133.
  • the portion of the upper barrier layer 131 directly above the cavity 133 directly below the first waveguide core layer 140 also be able to implant target ions, usually from a direction (ion The implantation angle) performs ion implantation, and selects appropriate ion implantation energy and dose according to the matching result of the implantation depth, ion implantation energy and dose, and implants target ions into the upper barrier layer 131 directly above the cavity 133.
  • the depth of ion implantation can be greater than or equal to So that the upper barrier layer 131 located directly above the cavity 133 and directly below the first waveguide core layer 140 is implanted with target ions.
  • the embodiments of the present application provide a waveguide structure, an integrated optical chip, and an electrical isolation method.
  • electrical isolation between active optical devices in the integrated optical chip can be achieved, thereby reducing
  • the power consumption and heat generation of the integrated optical chip ensure the normal operation of the integrated optical chip.

Abstract

A waveguide structure, an integrated optical chip, and a method for realizing electrical isolation, wherein same are used to solve the problems of electrical crosstalk generated in an integrated optical chip and an increase in the power consumption of the integrated optical chip due to the different working voltages of different active optical devices. The waveguide structure comprises a substrate, a first doped layer, a second doped layer and a first waveguide core layer stacked in sequence from bottom to top, wherein the first waveguide core layer covers a partial region of the upper surface of the second doped layer; the second doped layer comprises an upper barrier layer and a sacrificial layer; the sacrificial layer is located between the upper barrier layer and the first waveguide core layer, and is used for supporting the upper barrier layer; the second doped layer is internally provided with at least one cavity, and the cavity penetrates through the second doped layer along the direction of extension of the cavity; the first waveguide core layer is located right above the cavity, and the direction of extension of the cavity is perpendicular to the direction of extension of the first waveguide core layer; and the doping type of the first doped layer and that of the second doped layer are opposite.

Description

一种波导结构、集成光芯片及实现电学隔离的方法Waveguide structure, integrated optical chip and method for realizing electrical isolation 技术领域Technical field
本申请涉及半导体技术领域,尤其涉及一种波导结构、集成光芯片及实现电学隔离的方法。This application relates to the field of semiconductor technology, in particular to a waveguide structure, an integrated optical chip, and a method for achieving electrical isolation.
背景技术Background technique
随着互联网技术的高速发展,信息量呈现爆炸式增长,光通信技术广泛应用在网络数据传输中,以满足网络对传输性能的要求。With the rapid development of Internet technology, the amount of information has exploded, and optical communication technology is widely used in network data transmission to meet the requirements of network transmission performance.
集成光芯片作为光模块的核心器件,在光通信中发挥着重要的作用。集成光芯片采用半绝缘衬底将激光器、调制器、半导体光放大器(semiconductor optical amplifier,SOA)以及探测器等有源光器件集成在一起,这些有源器件之间通过光波导连接。这些有源光器件通常共享同一个导电层(如N型掺杂层或P型掺杂层),而有源光器件需要在共享导电层上的该有源光器件所在的区域施加相应的工作电压才能实现自身的功能(如调制、放大、探测等功能),对于不同功能的有源光器件,通常需要施加不同的工作电压,使得该共享导电层的不同区域之间形成电压差,进而在该共享导电层的不同区域之间有电流流过,这可能增加集成光芯片的功耗,影响集成光芯片正常工作,并且还可能导致工作电压不同的两个有源光器件之间产生电学串扰。As the core device of the optical module, the integrated optical chip plays an important role in optical communication. The integrated optical chip uses a semi-insulating substrate to integrate active optical devices such as lasers, modulators, semiconductor optical amplifiers (SOA), and detectors, and these active devices are connected by optical waveguides. These active optical devices usually share the same conductive layer (such as N-type doped layer or P-type doped layer), and active optical devices need to apply corresponding work on the shared conductive layer in the area where the active optical device is located. Voltage can achieve its own functions (such as modulation, amplification, detection, etc.). For active optical devices with different functions, different working voltages are usually applied, so that a voltage difference is formed between different regions of the shared conductive layer. There is current flowing between different areas of the shared conductive layer, which may increase the power consumption of the integrated optical chip, affect the normal operation of the integrated optical chip, and may also cause electrical crosstalk between two active optical devices with different working voltages .
例如,目前的相干光通信中,集成光芯片中的激光器、半导体光放大器、调制器,以及连接这些有源光器件的光波导共享N型掺杂层。其中,调制器工作时需要在调制器所在的N型掺杂层上加载正向电压,如+10V,而激光器、光放大器工作时需要在N型掺杂层加载0V电压,导致调制器与激光器、放大器之间的N型掺杂层存在10V电压差,进而产生大量的热及功耗。For example, in current coherent optical communication, the laser, semiconductor optical amplifier, modulator in the integrated optical chip, and the optical waveguide connecting these active optical devices share the N-type doped layer. Among them, the modulator needs to be loaded with a forward voltage, such as +10V, on the N-type doped layer where the modulator is working, while the laser and optical amplifier need to be loaded with 0V voltage on the N-type doped layer when working, resulting in the modulator and the laser , There is a 10V voltage difference in the N-type doped layer between the amplifiers, which generates a lot of heat and power consumption.
发明内容Summary of the invention
本申请提供了一种波导结构、集成光芯片及实现电学隔离的方法,以解决集成光芯片中由于不同有源光器件的工作电压不同,导致集成光芯片中产生电学串扰、增加集成光芯片功耗的问题。This application provides a waveguide structure, an integrated optical chip, and a method for achieving electrical isolation, so as to solve the problem of electrical crosstalk in the integrated optical chip due to the different working voltages of different active optical devices in the integrated optical chip, and increase the power of the integrated optical chip. The problem of consumption.
第一方面,本申请提供了一种波导结构,应用于集成光芯片中。该波导结构包括从下到上依次层叠设置的衬底、第一掺杂层、第二掺杂层以及第一波导芯层,第一波导芯层覆盖第二掺杂层的上表面的部分区域。其中,第二掺杂层包括上阻挡层和牺牲层,牺牲层位于上阻挡层和第一波导芯层之间,用于支撑上阻挡层。第二掺杂层内具有至少一个空腔,空腔沿着空腔的延伸方向贯穿第二掺杂层,第一波导芯层位于空腔的正上方,且空腔的延伸方向与第一波导芯层的延伸方向相互垂直。第一掺杂层可以为N型掺杂层或P型掺杂层,当第一掺杂层为N型掺杂层时,第二掺杂层为P型掺杂层,当第一掺杂层为P型掺杂层时,第二掺杂层为N型掺杂层,即第一掺杂层与第二掺杂层的掺杂类型相反。In the first aspect, this application provides a waveguide structure, which is applied to an integrated optical chip. The waveguide structure includes a substrate, a first doped layer, a second doped layer, and a first waveguide core layer stacked in sequence from bottom to top, and the first waveguide core layer covers a part of the upper surface of the second doped layer . Wherein, the second doped layer includes an upper barrier layer and a sacrificial layer, and the sacrificial layer is located between the upper barrier layer and the first waveguide core layer for supporting the upper barrier layer. There is at least one cavity in the second doped layer, the cavity penetrates the second doped layer along the extension direction of the cavity, the first waveguide core layer is located directly above the cavity, and the extension direction of the cavity is the same as that of the first waveguide. The extending directions of the core layers are perpendicular to each other. The first doped layer can be an N-type doped layer or a P-type doped layer. When the first doped layer is an N-type doped layer, the second doped layer is a P-type doped layer. When the layer is a P-type doped layer, the second doped layer is an N-type doped layer, that is, the first doped layer and the second doped layer have opposite doping types.
通过上述方案,由于波导结构的第二掺杂层中具有至少一个空腔,且位于空腔的正上方的上阻挡层的厚度可以根据实际需求控制到较小值,进而可以增大位于空腔的正上方的上阻挡层的阻抗,减小位于空腔的正上方的上阻挡层在沿波导芯层延伸的方向上传输的电流。另外,第一掺杂层与第二掺杂层的掺杂类型相反,使得在波导结构中在空腔相对两侧 形成的,共用波导结构的衬底、第一掺杂层以及第二掺杂层的有源光器件之间形成PNP结构或NPN结构,在上述有源光器件工作时该PNP结构或者NPN结构反向截止,进一步抑制第二掺杂层在沿波导芯层延伸的方向上传输的电流。因此,本申请实施例提供的波导结构能够有效抑制第二掺杂层在沿波导芯层延伸的方向上传输的电流,进而可以实现集成光芯片中通过波导结构空腔相对两侧形成的有源光器件之间的电学隔离。Through the above solution, since the second doped layer of the waveguide structure has at least one cavity, and the thickness of the upper barrier layer directly above the cavity can be controlled to a smaller value according to actual requirements, the cavity can be increased. The impedance of the upper barrier layer directly above reduces the current transmitted by the upper barrier layer directly above the cavity in the direction extending along the waveguide core layer. In addition, the doping types of the first doped layer and the second doped layer are opposite, so that the waveguide structure is formed on opposite sides of the cavity and shares the substrate, the first doped layer and the second doped layer of the waveguide structure. A PNP structure or an NPN structure is formed between the active optical devices of the layer, and the PNP structure or the NPN structure is reversely cut off when the active optical device is working, further suppressing the transmission of the second doped layer in the direction extending along the waveguide core layer的current. Therefore, the waveguide structure provided by the embodiments of the present application can effectively suppress the current transmitted by the second doped layer in the direction along the waveguide core layer, and thus can realize the active structure formed on opposite sides of the cavity of the waveguide structure in the integrated optical chip. Electrical isolation between optical devices.
一个可能的实施方式中,第一波导芯层在空腔的底壁所在平面上的投影位于空腔的底壁内,其中,空腔的底壁是第一掺杂层的上表面的部分区域。也就是说,空腔是由上阻挡层、牺牲层和第一掺杂层围合而成的。In a possible implementation manner, the projection of the first waveguide core layer on the plane of the bottom wall of the cavity is located in the bottom wall of the cavity, wherein the bottom wall of the cavity is a partial area of the upper surface of the first doped layer . In other words, the cavity is enclosed by the upper barrier layer, the sacrificial layer and the first doped layer.
一个可能的实施方式中,为了进一步增加波导结构的电学隔离效果,位于空腔正上方的部分上阻挡层中被注入有目标离子,该目标离子用于增加位于空腔正上方的部分上阻挡层的阻抗。其中,该目标离子可以为氦离子等能够增加被位于空腔正上方的部分上阻挡层阻抗的离子。In a possible embodiment, in order to further increase the electrical isolation effect of the waveguide structure, target ions are implanted in the upper barrier layer directly above the cavity, and the target ions are used to increase the upper barrier layer directly above the cavity的impedance. Wherein, the target ions may be ions such as helium ions that can increase the resistance of the blocking layer on the portion directly above the cavity.
由于波导结构中上阻挡层的厚度可以根据实际需求控制,通常上阻挡层的厚度较小,因此离子注入所需的能量较低,可以解决离子注入能量对离子注入深度的限制导致的电学隔离效果差的问题,使得目标离子能够尽可能注入到位于空腔正上方的上阻挡层的整个厚度范围内,进而使得位于空腔正上方的上阻挡层的阻抗均较大,能够有效隔进行电学隔离。Since the thickness of the upper barrier layer in the waveguide structure can be controlled according to actual needs, usually the thickness of the upper barrier layer is small, so the energy required for ion implantation is lower, which can solve the electrical isolation effect caused by the limitation of ion implantation energy on ion implantation depth The problem of poorness enables the target ions to be implanted as far as possible into the entire thickness range of the upper barrier layer directly above the cavity, thereby making the impedance of the upper barrier layer directly above the cavity larger, which can effectively isolate the electrical isolation .
一个可能的实施方式中,位于空腔正上方的上阻挡层的厚度小于或等于设定值,该设定值为目标离子能够注入到位于空腔正上方的上阻挡层中的最大深度,以使该目标离子能够注入到位于空腔正上方的上阻挡层的整个厚度范围内。In a possible embodiment, the thickness of the upper barrier layer directly above the cavity is less than or equal to a set value, and the set value is the maximum depth at which target ions can be implanted into the upper barrier layer directly above the cavity, to The target ions can be implanted into the entire thickness range of the upper barrier layer directly above the cavity.
一个可能的实施方式中,波导结构还包括第三掺杂层,第三掺杂层位于第一波导芯层的上方,其中,第二掺杂层为N型掺杂层,第三掺杂层为P型掺杂层;或者,第二掺杂层为P型掺杂层,第三掺杂层为N型掺杂层。进一步地,第三掺杂层的材料可以为磷化铟InP。In a possible embodiment, the waveguide structure further includes a third doped layer, the third doped layer is located above the first waveguide core layer, wherein the second doped layer is an N-type doped layer, and the third doped layer It is a P-type doped layer; or, the second doped layer is a P-type doped layer, and the third doped layer is an N-type doped layer. Further, the material of the third doped layer may be indium phosphide InP.
一个可能的实施方式中,第一掺杂层包括缓冲层和下阻挡层,缓冲层位于下阻挡层与衬底之间;空腔的底壁为下阻挡层的上表面的部分区域。In a possible embodiment, the first doped layer includes a buffer layer and a lower barrier layer, the buffer layer is located between the lower barrier layer and the substrate; the bottom wall of the cavity is a partial area of the upper surface of the lower barrier layer.
第二方面,本申请还提供了一种集成光芯片,集成光芯片包括上述第一方面任意一种可能的实施方式所述的波导结构、第一有源组件和第二有源组件。上阻挡层的上表面设置有相互隔离的第一有源组件和第二有源组件,第一有源组件和第二有源组件分别位于空腔的相对的两侧,第一有源组件的正下方为牺牲层的一部分,第二有源组件的正下方为牺牲层的另一部分,第一有源组件正下方的牺牲层与第二有源组件正下方的牺牲层,被空腔隔离开来。In a second aspect, the present application also provides an integrated optical chip. The integrated optical chip includes the waveguide structure, the first active component, and the second active component described in any one of the possible implementations of the first aspect. The upper surface of the upper barrier layer is provided with a first active component and a second active component isolated from each other. The first active component and the second active component are respectively located on opposite sides of the cavity. Just below is a part of the sacrificial layer, directly below the second active component is another part of the sacrificial layer, the sacrificial layer directly below the first active component and the sacrificial layer directly below the second active component are separated by the cavity Come.
其中,第一有源组件包括从下到上依次层叠的第二波导芯层和第四掺杂层第二有源组件包括从下到上依次层叠的第三波导芯层和第五掺杂层,第二波导芯层和第三波导芯层分别与第一波导芯层相连接。第二掺杂层为N型掺杂层,第四掺杂层以及第五掺杂层均为P型掺杂层;或者,第二掺杂层为P型掺杂层,第四掺杂层以及第五掺杂层均为N型掺杂层。Wherein, the first active component includes a second waveguide core layer and a fourth doped layer stacked sequentially from bottom to top. The second active component includes a third waveguide core layer and a fifth doped layer stacked sequentially from bottom to top. , The second waveguide core layer and the third waveguide core layer are respectively connected with the first waveguide core layer. The second doped layer is an N-type doped layer, the fourth doped layer and the fifth doped layer are both P-type doped layers; alternatively, the second doped layer is a P-type doped layer, and the fourth doped layer And the fifth doped layer is an N-type doped layer.
一个可能的实施方式中,第一有源组件和波导结构中位于第一有源组件正下方的部分(包括第一有源组件正下方的第二掺杂层、第一掺杂层和衬底)形成第一有源光器件,第二有源组件以及波导结构中位于第二有源组件正下方的部分(包括第二有源组件正下方的第二掺杂层、第一掺杂层和衬底)形成第二有源光器件,也就是说,第一有源光器件和第二有源光器件共用衬底、第一掺杂层以及第二掺杂层。In a possible embodiment, the first active component and the part of the waveguide structure directly below the first active component (including the second doped layer directly below the first active component, the first doped layer and the substrate ) To form the first active optical device, the second active component and the part of the waveguide structure directly below the second active component (including the second doped layer directly below the second active component, the first doped layer and The substrate) forms the second active optical device, that is, the first active optical device and the second active optical device share the substrate, the first doped layer and the second doped layer.
一个可能的实施方式中,集成光芯片工作时,第一有源器件的电压,与第二有源器件 的电压不同,尤其是,第一有源器件中的第二掺杂层上的电压与第二有源器件中的第二掺杂层上的电压不同。In a possible implementation, when the integrated optical chip is working, the voltage of the first active device is different from the voltage of the second active device. In particular, the voltage on the second doped layer in the first active device is different from the voltage on the second doped layer. The voltage on the second doped layer in the second active device is different.
一个可能的实施方式中,第一有源光器件可以为调制器,第二有源光器件可以为激光器、光放大器或光探测器。In a possible implementation, the first active optical device may be a modulator, and the second active optical device may be a laser, an optical amplifier, or an optical detector.
一个可能的实施方式中,为了实现第一有源光器件以及第二有源光器件在除第一波导芯层延伸方向外其他方向上的电学隔离,在波导结构的两侧的分别具有第一凹槽和第二凹槽,第一凹槽以及第二凹槽均贯穿第二掺杂层。其中,第一有源光器件、第二有源光器件和隔离器件均位于第一凹槽和第二凹槽之间,隔离器件包括第一波导芯层、第二掺杂层、第一掺杂层中位于第二掺杂层正下方的部分,以及衬底位于第二掺杂层正下方的部分。In a possible implementation manner, in order to achieve electrical isolation of the first active optical device and the second active optical device in directions other than the extending direction of the first waveguide core layer, there are first The groove and the second groove, the first groove and the second groove all penetrate the second doped layer. Wherein, the first active optical device, the second active optical device and the isolation device are all located between the first groove and the second groove, and the isolation device includes a first waveguide core layer, a second doped layer, and a first doped The part of the impurity layer directly below the second doped layer and the part of the substrate directly below the second doped layer.
第三方面,本申请还提供了一种电学隔离的方法,用于实现集成光芯片中有源光器件之间的电学隔离。该方法包括:在衬底上依次生长第一掺杂层、第二掺杂层以及第一波导芯层,第一波导芯层覆盖第二掺杂层的上表面的部分区域,第二掺杂层包括上阻挡层和牺牲层,牺牲层位于第一掺杂层与上阻挡层之间;第一掺杂层为N型掺杂层,述第二掺杂层为P型掺杂层,或者,所述第一掺杂层为P型掺杂层,所述第二掺杂层为N型掺杂层;对第一波导芯层进行刻蚀,形成波导沟槽,波导沟槽的深度大于第一波导芯层的厚度;对波导沟槽中露出的第二掺杂层进行刻蚀,在第二掺杂层中形成至少一个空腔,刻蚀后剩余的牺牲层用于支撑上阻挡层,空腔沿空腔的延伸方向贯穿第二掺杂层,第一波导芯层位于空腔的正上方,且空腔的延伸方向与第一波导芯层的延伸方向相互垂直。In the third aspect, this application also provides a method of electrical isolation, which is used to achieve electrical isolation between active optical devices in an integrated optical chip. The method includes: sequentially growing a first doped layer, a second doped layer, and a first waveguide core layer on a substrate, the first waveguide core layer covers a part of the upper surface of the second doped layer, and the second doping The layer includes an upper barrier layer and a sacrificial layer, the sacrificial layer is located between the first doped layer and the upper barrier layer; the first doped layer is an N-type doped layer, and the second doped layer is a P-type doped layer, or , The first doped layer is a P-type doped layer, the second doped layer is an N-type doped layer; the first waveguide core layer is etched to form a waveguide trench, the depth of the waveguide trench is greater than The thickness of the first waveguide core layer; the second doped layer exposed in the waveguide trench is etched to form at least one cavity in the second doped layer, and the remaining sacrificial layer after etching is used to support the upper barrier layer The cavity penetrates the second doped layer along the extending direction of the cavity, the first waveguide core layer is located directly above the cavity, and the extending direction of the cavity and the extending direction of the first waveguide core layer are perpendicular to each other.
一个可能的实施方式中,对波导沟槽中露出的第二掺杂层进行刻蚀,在第二掺杂层中形至少一个空腔,具体包括以下步骤:对波导沟槽中露出的上阻挡层进行刻蚀,形成至少一个刻蚀窗口;其中,刻蚀窗口的深度大于上阻挡层的厚度;将腐蚀剂加入至少一个刻蚀窗口中,对牺牲层进行腐蚀,形成至少一个空腔。In a possible implementation, the second doped layer exposed in the waveguide trench is etched to form at least one cavity in the second doped layer, which specifically includes the following steps: the upper barrier exposed in the waveguide trench The layer is etched to form at least one etch window; wherein the depth of the etch window is greater than the thickness of the upper barrier layer; an etchant is added to the at least one etch window to etch the sacrificial layer to form at least one cavity.
一个可能的实施方式中,对波导沟槽中露出的第二掺杂层进行刻蚀,在第二掺杂层中形至少一个空腔之后,还包括:向位于空腔正上方的部分上阻挡层中注入目标离子;其中,目标离子用于增加位于空腔正上方的部分上阻挡层的阻抗。In a possible implementation, the second doped layer exposed in the waveguide trench is etched, and after at least one cavity is formed in the second doped layer, the method further includes: blocking the part directly above the cavity The target ions are implanted into the layer; wherein the target ions are used to increase the impedance of the barrier layer on the part directly above the cavity.
可以理解地,上述提供的任一种集成光芯片包括上述第一方面所述的波导结构,上述任意一种实现电学隔离的方法可以制备得到上述第一方面所述的波导结构,因此,其所能达到的有益效果可参考第一方面所提供的对应的波导结构中的有益效果,此处不再赘述。It is understandable that any of the integrated optical chips provided above includes the waveguide structure described in the first aspect, and any one of the foregoing methods for achieving electrical isolation can prepare the waveguide structure described in the first aspect. The beneficial effects that can be achieved can refer to the beneficial effects in the corresponding waveguide structure provided in the first aspect, which will not be repeated here.
附图说明Description of the drawings
图1A为本申请实施例提供的一种波导结构的立体结构示意图之一;1A is one of the three-dimensional schematic diagrams of a waveguide structure provided by an embodiment of the application;
图1B为本申请实施例提供的一种波导结构在BB’方向上的剖面示意图之一;FIG. 1B is one of the schematic cross-sectional views of a waveguide structure in the BB' direction according to an embodiment of the application;
图1C为本申请实施例提供的一种波导结构在AA’方向上的剖面示意图之一;FIG. 1C is one of the schematic cross-sectional views in the AA' direction of a waveguide structure according to an embodiment of the application;
图1D为本申请实施例提供的一种波导结构在AA’方向上的剖面示意图之二;FIG. 1D is the second cross-sectional schematic diagram of a waveguide structure in the AA' direction according to an embodiment of the application;
图2为本申请实施例提供的一种波导结构与有源光器件的关系示意图;2 is a schematic diagram of the relationship between a waveguide structure and an active optical device according to an embodiment of the application;
图3A为本申请实施例提供的一种波导结构的立体结构示意图之二;3A is the second schematic diagram of a three-dimensional structure of a waveguide structure provided by an embodiment of this application;
图3B为本申请实施例提供的一种波导结构在CC’方向上的剖面示意图;3B is a schematic cross-sectional view of a waveguide structure in the CC' direction according to an embodiment of the application;
图3C为本申请实施例提供的一种波导结构在BB’方向上的剖面示意图之二;3C is the second schematic cross-sectional view of a waveguide structure in the BB' direction according to an embodiment of the application;
图4A为本申请实施例提供的一种波导结构的立体结构示意图之三;4A is the third schematic diagram of a three-dimensional structure of a waveguide structure provided by an embodiment of this application;
图4B为本申请实施例提供的一种波导结构在AA’方向上的剖面示意图之二;4B is the second schematic cross-sectional view of a waveguide structure in the AA' direction according to an embodiment of the application;
图4C为本申请实施例提供的一种波导结构在BB’方向上的剖面示意图之三;4C is the third schematic cross-sectional view of a waveguide structure in the BB' direction according to an embodiment of the application;
图5A为本申请实施例提供的一种波导结构的立体结构示意图之四;5A is a fourth schematic diagram of a three-dimensional structure of a waveguide structure provided by an embodiment of this application;
图5B为本申请实施例提供的一种波导结构在AA’方向上的剖面示意图之三;5B is the third schematic cross-sectional view of a waveguide structure in the AA' direction according to an embodiment of the application;
图5C为本申请实施例提供的一种波导结构在BB’方向上的剖面示意图之四;FIG. 5C is the fourth cross-sectional schematic diagram of a waveguide structure in the BB' direction according to an embodiment of the application;
图6为本申请实施例提供的一种波导结构的立体结构示意图之五;6 is a fifth schematic diagram of a three-dimensional structure of a waveguide structure provided by an embodiment of this application;
图7A为本申请实施例提供的一种集成光芯片的俯视示意图之一;FIG. 7A is one of the top schematic diagrams of an integrated optical chip provided by an embodiment of the application;
图7B为本申请实施例提供的一种集成光芯片在AA’方向上的剖面示意图之一;FIG. 7B is one of the schematic cross-sectional views in the AA' direction of an integrated optical chip according to an embodiment of the application;
图8为本申请实施例提供的调制器的结构示意图;FIG. 8 is a schematic structural diagram of a modulator provided by an embodiment of the application;
图9A为本申请实施例提供的一种集成光芯片的俯视示意图之二;9A is the second schematic top view of an integrated optical chip provided by an embodiment of the application;
图9B为本申请实施例提供的一种集成光芯片在BB’方向上的剖面示意图之一;FIG. 9B is one of the schematic cross-sectional views of an integrated optical chip in the BB' direction according to an embodiment of the application;
图10A为本申请实施例提供的一种集成光芯片的俯视示意图之三;10A is the third schematic top view of an integrated optical chip provided by an embodiment of this application;
图10B为本申请实施例提供的一种集成光芯片的俯视示意图之四;10B is a fourth schematic top view of an integrated optical chip provided by an embodiment of this application;
图10C为本申请实施例提供的一种集成光芯片的俯视示意图之五;10C is a fifth schematic top view of an integrated optical chip provided by an embodiment of the application;
图11为本申请实施例提供的一种电学隔离方法的流程示意图;FIG. 11 is a schematic flowchart of an electrical isolation method provided by an embodiment of the application;
图12为本申请实施例提供的一种离子注入角度与上阻挡层的关系示意图。FIG. 12 is a schematic diagram of the relationship between an ion implantation angle and the upper barrier layer provided by an embodiment of the application.
具体实施方式detailed description
集成光芯片中集成的激光器、调制器、SOA以及探测器等有源光器件通常共享同一个导电层(如N型掺杂层或P型掺杂层),而有源光器件需要在共享导电层上的该有源光器件所在的区域施加相应的工作电压才能实现自身的功能(如调制、放大、探测等功能)。对于不同功能的有源光器件,通常需要施加不同的工作电压,使得共享导电层的不同区域之间形成电压差(因为共享导电层的不同区域分别设有工作电压不同的有源光器件),导致集成光芯片的功耗增加,影响集成光芯片的正常工作,另外,工作电压不同的两个有源光器件之间还会因此而产生电学串扰。Active optical devices such as lasers, modulators, SOA, and detectors integrated in integrated optical chips usually share the same conductive layer (such as N-type doped layer or P-type doped layer), while active optical devices need to share conductive layers. Only when the corresponding working voltage is applied to the area where the active optical device on the layer is located can its own functions (such as modulation, amplification, detection, etc.) be realized. For active optical devices with different functions, it is usually necessary to apply different working voltages to form a voltage difference between different regions of the shared conductive layer (because different regions of the shared conductive layer are respectively provided with active optical devices with different working voltages), This leads to an increase in the power consumption of the integrated optical chip, which affects the normal operation of the integrated optical chip. In addition, electrical crosstalk may also occur between two active optical devices with different operating voltages.
现有技术中通常采用氦离子注入的方式,对集成光芯片的导电层的不同区域之间形成电学隔离。应当知道的是,该集成光芯片的导电层被多个有源光器件所共享,且多个有源光器件分别位于导电层的不同区域。但是,集成光芯片中有源光器件共享的导电层通常比较厚,因为当集成光芯片中有源光器件共享的导电层较厚时,对集成光芯片有诸多益处,例如有利于有源光器件上偏置电压(或称为工作电压)的加载,能够降低有源光器件中共享导电层的电阻以及能够提升调制器的带宽等。而氦离子注入时由于离子注入的能量有限,相对应的注入深度有限,例如400keV的能量对应的注入深度约为1.6um。相对应的,注入深度越大,需要的能量也越高,离子注入的成本也就越高。因此仅采用氦离子注入的方式,集成光芯片中有源光器件共享的导电层中不同有源光器件所在的区域之间的电学隔离效果较差。In the prior art, helium ion implantation is usually used to form electrical isolation between different regions of the conductive layer of the integrated optical chip. It should be known that the conductive layer of the integrated optical chip is shared by multiple active optical devices, and the multiple active optical devices are located in different regions of the conductive layer. However, the conductive layer shared by the active optical devices in the integrated optical chip is usually thicker, because when the conductive layer shared by the active optical devices in the integrated optical chip is thick, it has many benefits to the integrated optical chip, such as beneficial to the active optical chip. The loading of the bias voltage (or working voltage) on the device can reduce the resistance of the shared conductive layer in the active optical device and can increase the bandwidth of the modulator. However, due to the limited energy of ion implantation during helium ion implantation, the corresponding implantation depth is limited. For example, the implantation depth corresponding to the energy of 400keV is about 1.6um. Correspondingly, the greater the implantation depth, the higher the energy required, and the higher the cost of ion implantation. Therefore, only using the helium ion implantation method, the electrical isolation effect between the regions where different active optical devices are located in the conductive layer shared by the active optical devices in the integrated optical chip is poor.
另外,集成光芯片中的有源光器件之间通过光波导(或波导芯层)连接,即集成光芯片中有源光器件通过共享的导电层上的波导芯层实现光学连接,也增加了有源光器件共享的导电层中不同有源光器件所在的区域之间,在波导芯层延伸的方向上(光信号传播的方向)的电学隔离的难度。In addition, the active optical devices in the integrated optical chip are connected by optical waveguides (or waveguide core layers), that is, the active optical devices in the integrated optical chip are optically connected through the waveguide core layer on the shared conductive layer, which also increases The difficulty of electrical isolation in the direction in which the waveguide core layer extends (the direction of optical signal propagation) between the regions where different active optical devices are located in the conductive layer shared by the active optical devices.
为了解决上述问题,本申请提供了一种波导结构,用于实现对集成光芯片中有源光器件之间的电学隔离。In order to solve the above-mentioned problems, the present application provides a waveguide structure for achieving electrical isolation between active optical devices in an integrated optical chip.
需要说明的是,本申请中所涉及的多个,是指两个或两个以上。另外,需要理解的是,在本申请的描述中,“第一”或“第二”等词汇,仅用于区分描述,而不能理解为指示或暗示相对重要性,也不能理解为指示或暗示顺序。It should be noted that the multiple involved in this application refers to two or more. In addition, it should be understood that in the description of this application, words such as "first" or "second" are only used to distinguish the description, and cannot be understood as indicating or implying relative importance, nor can it be understood as indicating or implying order.
为了使本申请的目的、技术方案和优点更加清楚,下面将结合附图对本申请作进一步地详细描述。In order to make the objectives, technical solutions, and advantages of the present application clearer, the present application will be further described in detail below with reference to the accompanying drawings.
图1A为本申请提供的一种波导结构100的立体示意图,波导结构100应用于集成光芯片中,用于实现集成光芯片中有源光器件在光信号传播方向(即集成芯片中光波导的延伸方向)上的电学隔离。参阅图1A所示,波导结构100包括从下到上依次层叠设置的衬底110、第一掺杂层120、第二掺杂层130以及第一波导芯层140。第一波导芯层140覆盖第二掺杂层130的上表面的部分区域。1A is a three-dimensional schematic diagram of a waveguide structure 100 provided by this application. The waveguide structure 100 is applied to an integrated optical chip to realize the propagation direction of the optical signal of the active optical device in the integrated optical chip (that is, the optical waveguide in the integrated chip). Extension direction) electrical isolation. Referring to FIG. 1A, the waveguide structure 100 includes a substrate 110, a first doped layer 120, a second doped layer 130, and a first waveguide core layer 140 that are sequentially stacked from bottom to top. The first waveguide core layer 140 covers a partial area of the upper surface of the second doped layer 130.
需要说明的是,在本申请中,所谓的任一层(例如第一掺杂层120)的上表面是指该层(例如第一掺杂层120)朝向上方的表面,任一层(例如第一掺杂层120)的下表面是指该层(例如第一掺杂层120)朝向下方的表面。应当知道的是,任一层的上表面和下表面是相背离的。应当知道的是,在本申请中,上和下是一对相对的概念,并且上和下参考的是本申请的附图当前的放置方位,例如,如图1A所示,第一掺杂层120位于衬底110的上方,位于第二掺杂层130的下方,第一波导芯层140位于第二掺杂层130的上方。It should be noted that in this application, the so-called upper surface of any layer (for example, the first doped layer 120) refers to the surface of the layer (for example, the first doped layer 120) facing upward, and any layer (for example, The lower surface of the first doped layer 120) refers to the surface of the layer (for example, the first doped layer 120) facing downward. It should be understood that the upper and lower surfaces of any layer are opposite. It should be understood that in this application, upper and lower are a pair of relative concepts, and the upper and lower refer to the current placement orientation of the drawings of this application. For example, as shown in FIG. 1A, the first doped layer 120 is located above the substrate 110 and below the second doped layer 130, and the first waveguide core layer 140 is located above the second doped layer 130.
其中,第二掺杂层130包括上阻挡层131和牺牲层132,牺牲层132位于上阻挡层131和第一波导芯层140之间,用于支撑上阻挡层131。第二掺杂层130内具有至少一个空腔133,波导结构100在BB’方向(空腔133的延伸方向)上的剖面图如图1B所示,由图1B可知,空腔133沿着空腔133的延伸方向贯穿第二掺杂层130,第一波导芯层140位于空腔133的正上方,且空腔133的延伸方向与第一波导芯层140的延伸方向相互垂直。The second doped layer 130 includes an upper barrier layer 131 and a sacrificial layer 132. The sacrificial layer 132 is located between the upper barrier layer 131 and the first waveguide core layer 140 and is used to support the upper barrier layer 131. There is at least one cavity 133 in the second doped layer 130. A cross-sectional view of the waveguide structure 100 in the BB' direction (the extending direction of the cavity 133) is shown in FIG. 1B. It can be seen from FIG. 1B that the cavity 133 runs along the cavity. The extending direction of the cavity 133 penetrates the second doped layer 130, the first waveguide core layer 140 is located directly above the cavity 133, and the extending direction of the cavity 133 and the extending direction of the first waveguide core layer 140 are perpendicular to each other.
波导结构100在AA’方向(第一波导芯层140的延伸方向)上的剖面图如图1C所示,由图1C可知,空腔133是由上阻挡层131、牺牲层132和第一掺杂层120围合而成的,上阻挡层131的上表面的部分区域为空腔133的顶壁,牺牲层132朝向空腔133的侧面为空腔133的侧壁,第一掺杂层120的上表面的部分区域为空腔133的底壁。第一波导芯层140在空腔133的底壁所在平面上的投影位于空腔133的底壁内。当第二掺杂层130中具有一个空腔133时,牺牲层132包括两部分,如图1C所示,当第二掺杂层130中具有两个或两个以上空腔133时,牺牲层132包括至少三部分,例如,当第二掺杂层130中具有两个空腔133时,牺牲层132包括三部分,如图1D所示。The cross-sectional view of the waveguide structure 100 in the AA' direction (the extension direction of the first waveguide core layer 140) is shown in FIG. 1C. It can be seen from FIG. 1C that the cavity 133 is formed by the upper barrier layer 131, the sacrificial layer 132 and the first doped layer. A part of the upper surface of the upper barrier layer 131 is the top wall of the cavity 133, the side of the sacrificial layer 132 facing the cavity 133 is the side wall of the cavity 133, and the first doped layer 120 Part of the upper surface of the area is the bottom wall of the cavity 133. The projection of the first waveguide core layer 140 on the plane of the bottom wall of the cavity 133 is located in the bottom wall of the cavity 133. When the second doped layer 130 has one cavity 133, the sacrificial layer 132 includes two parts, as shown in FIG. 1C, when the second doped layer 130 has two or more cavities 133, the sacrificial layer 132 includes at least three parts. For example, when there are two cavities 133 in the second doped layer 130, the sacrificial layer 132 includes three parts, as shown in FIG. 1D.
第一掺杂层120可以为N型掺杂层或P型掺杂层,当第一掺杂层120为N型掺杂层时,第二掺杂层130为P型掺杂层,当第一掺杂层120为P型掺杂层时,第二掺杂层130为N型掺杂层,即第一掺杂层120与第二掺杂层130的掺杂类型相反,使得波导结构100中在空腔133相对两侧形成的,共用波导结构100的衬底110、第一掺杂层120以及第二掺杂层130的有源光器件之间形成PNP结构或者NPN结构(如图2所示),在上述有源光器件工作时该PNP结构或者NPN结构反向截止,能够防止上述有源器件通过波导结构100中的第一掺杂层120导电。其中,上阻挡层131与牺牲层132的掺杂类型性均相同,即当第二掺杂层130为P型掺杂层时,上阻挡层131与牺牲层132均为P型掺杂层,当第二掺杂层130为N型掺杂层时,上阻挡层131与牺牲层132均为N型掺杂层。The first doped layer 120 may be an N-type doped layer or a P-type doped layer. When the first doped layer 120 is an N-type doped layer, the second doped layer 130 is a P-type doped layer. When one doped layer 120 is a P-type doped layer, the second doped layer 130 is an N-type doped layer, that is, the doping types of the first doped layer 120 and the second doped layer 130 are opposite, so that the waveguide structure 100 The PNP structure or NPN structure is formed between the active optical devices that share the waveguide structure 100, the substrate 110, the first doped layer 120, and the second doped layer 130 formed on opposite sides of the cavity 133 (as shown in FIG. 2 (Shown), the PNP structure or the NPN structure is reversely cut off when the active optical device is working, which can prevent the active device from conducting conduction through the first doped layer 120 in the waveguide structure 100. Wherein, the upper barrier layer 131 and the sacrificial layer 132 have the same doping type, that is, when the second doped layer 130 is a P-type doped layer, the upper barrier layer 131 and the sacrificial layer 132 are both P-type doped layers. When the second doped layer 130 is an N-type doped layer, the upper barrier layer 131 and the sacrificial layer 132 are both N-type doped layers.
进一步地,衬底110可以是半绝缘(semi-insulating,SI)衬底,衬底110的材料可以为磷化铟(InP)。波导芯层140用于传输光信号,波导芯层140可以通过刻蚀形成一个或 多个平行光波导来传输光信号。Further, the substrate 110 may be a semi-insulating (SI) substrate, and the material of the substrate 110 may be indium phosphide (InP). The waveguide core layer 140 is used to transmit optical signals, and the waveguide core layer 140 may be etched to form one or more parallel optical waveguides to transmit optical signals.
波导结构100主要通过空腔133所在的区域实现集成光芯片中有源光器件之间的电学隔离,根据上阻挡层131与空腔133的位置关系,上阻挡层131可以划分为第一部分和第二部分两个部分,第一部分为位于空腔133的正上方的上阻挡层131,第二部分为位于牺牲层132正上方的部分,为了进一步增加波导结构100的电学隔离效果,位于空腔133正上方的部分上阻挡层131,即上阻挡才层的第一部分中还可以注入有目标离子,该目标离子用于增加位于空腔133正上方的部分上阻挡层131的阻抗。其中,该目标离子可以为氦离子等能够增加被位于空腔133正上方的部分上阻挡层131阻抗的离子。The waveguide structure 100 mainly realizes the electrical isolation between the active optical devices in the integrated optical chip through the area where the cavity 133 is located. According to the positional relationship between the upper barrier layer 131 and the cavity 133, the upper barrier layer 131 can be divided into a first part and a second part. There are two parts. The first part is the upper barrier layer 131 directly above the cavity 133, and the second part is the part directly above the sacrificial layer 132. In order to further increase the electrical isolation effect of the waveguide structure 100, the upper barrier layer 131 is located in the cavity 133. The upper part of the upper barrier layer 131 directly above, that is, the first part of the upper barrier layer, may also be implanted with target ions, and the target ions are used to increase the impedance of the upper barrier layer 131 in the part directly above the cavity 133. Wherein, the target ions may be ions such as helium ions that can increase the resistance of the blocking layer 131 on the portion directly above the cavity 133.
由于波导结构100中上阻挡层131的厚度可以根据实际需求控制(例如2μm~10μm),通常上阻挡层131的厚度较小(可以小于2μm),因此离子注入所需的能量较低,可以解决离子注入能量对离子注入深度的限制导致的电学隔离效果差的问题,使得目标离子能够尽可能注入到位于空腔133正上方的上阻挡层131的整个厚度范围内,进而使得位于空腔133正上方的上阻挡层131的阻抗均较大,能够有效隔进行电学隔离。Since the thickness of the upper barrier layer 131 in the waveguide structure 100 can be controlled according to actual requirements (for example, 2 μm-10 μm), usually the thickness of the upper barrier layer 131 is small (may be less than 2 μm), so the energy required for ion implantation is low, which can solve The problem of poor electrical isolation caused by the limitation of ion implantation energy on the depth of ion implantation enables target ions to be implanted as far as possible into the entire thickness range of the upper barrier layer 131 located directly above the cavity 133, thereby making the cavity 133 positive. The upper barrier layer 131 above has a relatively large impedance, which can effectively isolate the electrical isolation.
具体实施中,位于空腔133正上方的上阻挡层131的厚度小于或等于设定值,该设定值为目标离子能够注入到位于空腔133正上方的上阻挡层中的最大深度,以使该目标离子能够注入到位于空腔133正上方的上阻挡层131的整个厚度范围内。In a specific implementation, the thickness of the upper barrier layer 131 directly above the cavity 133 is less than or equal to a set value, and the set value is the maximum depth that target ions can be implanted into the upper barrier layer directly above the cavity 133 to The target ions can be implanted into the entire thickness range of the upper barrier layer 131 directly above the cavity 133.
进一步地,空腔133可以通过腐蚀牺牲层132得,也就是说,牺牲层132与刻蚀剂的反应速率大于上阻挡层131与刻蚀剂的反应速率,以使牺牲层132可以被腐蚀掉,而上阻挡层131可以保留下来,进而形成空腔133,空腔133的大小可以通过刻蚀剂的剂量以及刻蚀时间进行控制(即通过控制被刻蚀掉的牺牲层132的体积来控制空腔133的大小)。Further, the cavity 133 can be obtained by etching the sacrificial layer 132, that is, the reaction rate of the sacrificial layer 132 and the etchant is greater than the reaction rate of the upper barrier layer 131 and the etchant, so that the sacrificial layer 132 can be etched away , And the upper barrier layer 131 can be retained to form a cavity 133. The size of the cavity 133 can be controlled by the dose of the etchant and the etching time (that is, by controlling the volume of the sacrificial layer 132 etched away) The size of the cavity 133).
在具体实施中,为了对牺牲层132进行腐蚀以形成空腔133,需要先在上阻挡层131上刻蚀得到刻蚀窗口,刻蚀窗口的深度大于上阻挡层131的厚度,以从刻蚀窗口中注入刻蚀剂对牺牲层132进行刻蚀,因此,如图3A-图3C所示,在上阻挡层132上还可以形成有一个或多个刻蚀窗口134,这些刻蚀窗口134位于波导芯层140两侧或者同一侧。需要说明的是,本申请实施例并不对刻蚀窗口134的大小、形状以及个数进行限定,刻蚀窗口134具体可以为矩形、圆角矩形、圆形或者三角形等形状。In a specific implementation, in order to etch the sacrificial layer 132 to form the cavity 133, it is necessary to first etch the upper barrier layer 131 to obtain an etch window. The depth of the etch window is greater than the thickness of the upper barrier layer 131 to avoid An etchant is injected into the window to etch the sacrificial layer 132. Therefore, as shown in FIGS. 3A to 3C, one or more etching windows 134 may be formed on the upper barrier layer 132, and these etching windows 134 are located Both sides of the waveguide core layer 140 or the same side. It should be noted that the embodiment of the present application does not limit the size, shape, and number of the etching window 134, and the etching window 134 may specifically be a rectangle, a rounded rectangle, a circle, or a triangle.
其中,牺牲层132的材料可以为铟镓砷InGaAs、铟铝砷InAlAs或者依次由InP、InAlAs以及InP三层材料组成,当牺牲层132的材料为InGaAs或InAlAs时,上阻挡层131的材料可以为InP,当牺牲层132依次由InP、InAlAs以及InP三层材料组成时,上阻挡层131的材料可以为InGaAs、InAlAs或铟镓砷磷InGaAsP。The material of the sacrificial layer 132 may be InGaAs, InAlAs, InAlAs, or three layers of InP, InAlAs, and InP. When the material of the sacrificial layer 132 is InGaAs or InAlAs, the material of the upper barrier layer 131 may be When the sacrificial layer 132 is composed of three layers of InP, InAlAs, and InP, the material of the upper barrier layer 131 may be InGaAs, InAlAs or InGaAsP InGaAsP.
通常情况下,波导芯层140的折射率大于波导芯层140周围的材料(如第二掺杂层130)的折射率,形成一定的折射率差,以将光信号限制在波导芯层140中传输,减少光信号的泄漏。因此,在上阻挡层131的折射率与波导芯层140的折射率较接近(例如当下包层)的场景下,第二掺杂层130还可以包括下包层135,下包层135位于波导芯层140与上阻挡层131之间,相对于下包层135,上阻挡层131较薄,此时,波导结构100的立体示意图图4A所示,波导结构100在AA’方向上的剖面图如图4B所示,波导结构100在BB’方向上的剖面图如图4C所示。其中,下包层135的材料可以为InP。Generally, the refractive index of the waveguide core layer 140 is greater than the refractive index of the material around the waveguide core layer 140 (for example, the second doped layer 130), forming a certain refractive index difference to confine the optical signal in the waveguide core layer 140 Transmission, reducing the leakage of optical signals. Therefore, in a scenario where the refractive index of the upper barrier layer 131 is close to the refractive index of the waveguide core layer 140 (for example, the current lower cladding layer), the second doped layer 130 may also include a lower cladding layer 135, which is located in the waveguide. Between the core layer 140 and the upper barrier layer 131, compared to the lower cladding layer 135, the upper barrier layer 131 is thinner. At this time, a three-dimensional schematic diagram of the waveguide structure 100 is shown in FIG. 4A, a cross-sectional view of the waveguide structure 100 in the AA' direction As shown in FIG. 4B, the cross-sectional view of the waveguide structure 100 in the BB' direction is as shown in FIG. 4C. Wherein, the material of the under-cladding layer 135 may be InP.
进一步地,第一掺杂层120可以包括缓冲层121和下阻挡层122,缓冲层121位于下阻挡层1221和衬底110上之间,此时,波导结构100的立体示意图图5A所示,波导结构100在AA’方向上的剖面图如图5B所示,波导结构10在BB’方向上的剖面图如图5C所 示。由图5B可知,在第一掺杂层120包括缓冲层121和下阻挡层122的场景下,空腔133的底壁为下阻挡层122的上表面的部分区域。其中,缓冲层121用于以对衬底110进行晶格匹配,以提高衬底110上生长的材料的质量。缓冲层121与下阻挡层122的掺杂类型性均相同,当第一掺杂层120为P型掺杂层时,缓冲层121和下阻挡层122的掺杂类型性也为P型掺杂,当第一掺杂层130为N型掺杂层时,缓冲层121和下阻挡层122的掺杂类型性也为N型掺杂。Further, the first doped layer 120 may include a buffer layer 121 and a lower barrier layer 122. The buffer layer 121 is located between the lower barrier layer 1221 and the substrate 110. At this time, a three-dimensional schematic diagram of the waveguide structure 100 is shown in FIG. 5A. The cross-sectional view of the waveguide structure 100 in the AA' direction is shown in FIG. 5B, and the cross-sectional view of the waveguide structure 10 in the BB' direction is shown in FIG. 5C. It can be seen from FIG. 5B that in the scenario where the first doped layer 120 includes the buffer layer 121 and the lower barrier layer 122, the bottom wall of the cavity 133 is a partial area of the upper surface of the lower barrier layer 122. Wherein, the buffer layer 121 is used to perform lattice matching on the substrate 110 to improve the quality of the material grown on the substrate 110. The doping types of the buffer layer 121 and the lower barrier layer 122 are the same. When the first doped layer 120 is a P-type doped layer, the doping types of the buffer layer 121 and the lower barrier layer 122 are also P-type doping. When the first doping layer 130 is an N-type doping layer, the doping types of the buffer layer 121 and the lower barrier layer 122 are also N-type doping.
缓冲层121的材料通常为InP,下阻挡层122的材料通常与上阻挡层131的材料相同,可以为InP、InGaAs或InAlAs等。因此,上阻挡层131、牺牲层132以及下阻挡层122所采用的材料的组合包括但不限于以下几种中的任意一种:(1)上阻挡层131为InP,牺牲层132为InGaAs,下阻挡层122为InP;(2)上阻挡层131为InP,牺牲层132为InAlAs,下阻挡层122为InP;(3)上阻挡层131为InGaAs,牺牲层132为依次由InP、InAlAs以及InP三层材料组成的,下阻挡层122为InGaAs;(4)上阻挡层131为InAlAs,牺牲层132为依次由InP、InAlAs以及InP三层材料组成的,下阻挡层122为InAlAs。其中,当下阻挡层122为InP时,缓冲层121与下阻挡层122可以视为同一层材料。The material of the buffer layer 121 is usually InP, and the material of the lower barrier layer 122 is usually the same as the material of the upper barrier layer 131, and may be InP, InGaAs, InAlAs, or the like. Therefore, the combination of materials used in the upper barrier layer 131, the sacrificial layer 132, and the lower barrier layer 122 includes but is not limited to any of the following: (1) the upper barrier layer 131 is InP, and the sacrificial layer 132 is InGaAs, The lower barrier layer 122 is InP; (2) the upper barrier layer 131 is InP, the sacrificial layer 132 is InAlAs, and the lower barrier layer 122 is InP; (3) the upper barrier layer 131 is InGaAs, and the sacrificial layer 132 is composed of InP, InAlAs, and It is composed of three layers of InP, the lower barrier layer 122 is InGaAs; (4) the upper barrier layer 131 is InAlAs, the sacrificial layer 132 is composed of InP, InAlAs and InP in sequence, and the lower barrier layer 122 is InAlAs. Wherein, when the lower barrier layer 122 is InP, the buffer layer 121 and the lower barrier layer 122 can be regarded as the same layer of material.
进一步地,如图6所示,波导结构100还可以包括在波导芯层140上形成的第三掺杂层150,当第二掺杂层130为N型掺杂层时,第三掺杂层150为P型掺杂层,当第二掺杂层130为P型掺杂层时,第三掺杂层150为N型掺杂层,即第二掺杂层130与第三掺杂层150的掺杂类型相反。其中,第三掺杂层150的材料可以为InP。Further, as shown in FIG. 6, the waveguide structure 100 may further include a third doped layer 150 formed on the waveguide core layer 140. When the second doped layer 130 is an N-type doped layer, the third doped layer 150 is a P-type doped layer. When the second doped layer 130 is a P-type doped layer, the third doped layer 150 is an N-type doped layer, that is, the second doped layer 130 and the third doped layer 150 The doping type is opposite. The material of the third doped layer 150 may be InP.
通过上述方案,由于波导结构100的第二掺杂层130中具有至少一个空腔133,且位于空腔133的正上方的上阻挡层131的厚度可以根据实际需求控制到较小值,进而可以增大位于空腔133的正上方的上阻挡层131的阻抗,减小位于空腔133的正上方的上阻挡层131在沿波导芯层140延伸的方向上传输的电流。另外,第一掺杂层120与第二掺杂层130的掺杂类型相反,使得在波导结构100中在空腔133相对两侧形成的,共用波导结构100的衬底110、第一掺杂层120以及第二掺杂层130的有源光器件之间形成PNP结构或NPN结构,在上述有源光器件工作时该PNP结构或者NPN结构反向截止,进一步抑制第二掺杂层130在沿波导芯层延伸的方向上传输的电流。因此,本申请实施例提供的波导结构100能够有效抑制第二掺杂层130在沿波导芯层延伸的方向上传输的电流,进而可以实现集成光芯片中通过波导结构100空腔133相对两侧形成的有源光器件之间的电学隔离。Through the above solution, since the second doped layer 130 of the waveguide structure 100 has at least one cavity 133, and the thickness of the upper barrier layer 131 directly above the cavity 133 can be controlled to a smaller value according to actual requirements, The impedance of the upper barrier layer 131 directly above the cavity 133 is increased, and the current transmitted by the upper barrier layer 131 directly above the cavity 133 in the direction along which the waveguide core layer 140 extends is reduced. In addition, the first doped layer 120 and the second doped layer 130 have opposite doping types, so that the waveguide structure 100 is formed on opposite sides of the cavity 133 and shares the substrate 110 and the first doped layer of the waveguide structure 100. A PNP structure or an NPN structure is formed between the active optical device of the layer 120 and the second doped layer 130. When the active optical device is working, the PNP structure or the NPN structure is reversely cut off, further suppressing the second doping layer 130 A current that travels in the direction in which the core of the waveguide extends. Therefore, the waveguide structure 100 provided by the embodiments of the present application can effectively suppress the current transmitted by the second doped layer 130 in the extending direction of the waveguide core layer, and then can realize the integrated optical chip through the waveguide structure 100 on opposite sides of the cavity 133. The electrical isolation between the formed active optical devices.
基于以上实施例,本申请还提供了一种集成光芯片200,俯视图如图7A所示,集成光芯片200包括上述任意一种可能的实施方式所述的波导结构100、第一有源组件210和第二有源组件220。如图7B所示,第一有源组件210和第二有源组件设置220在波导结构100的上阻挡层的上表面,第一有源组件210和第二有源组件220分别位于空腔133的相对的两侧,第一有源组件的正下方为牺牲层132的一部分,第二有源组件132的正下方为牺牲层132的另一部分,第一有源组件210正下方的牺牲层132与第二有源组件220正下方的牺牲层132,被空腔133隔离开来,即牺牲层132被空腔133划分为至少两个部分。Based on the above embodiments, the present application also provides an integrated optical chip 200. A top view is shown in FIG. 7A. The integrated optical chip 200 includes the waveguide structure 100 and the first active component 210 described in any one of the above possible embodiments. And second active component 220. As shown in FIG. 7B, the first active component 210 and the second active component 220 are disposed on the upper surface of the upper barrier layer of the waveguide structure 100, and the first active component 210 and the second active component 220 are respectively located in the cavity 133 On the two opposite sides of the first active device, just below the first active component is a part of the sacrificial layer 132, directly below the second active component 132 is another part of the sacrificial layer 132, and the sacrificial layer 132 directly below the first active component 210 The sacrificial layer 132 directly below the second active component 220 is separated by the cavity 133, that is, the sacrificial layer 132 is divided into at least two parts by the cavity 133.
其中,第一有源组件210包括从下到上依次层叠的第二波导芯层211和第四掺杂层212第二有源组件220包括从下到上依次层叠的第三波导芯层221和第五掺杂层222,第二波导芯层211和第三波导芯层221分别与第一波导芯层140相连接。Wherein, the first active component 210 includes a second waveguide core layer 211 and a fourth doped layer 212 stacked sequentially from bottom to top. The second active component 220 includes a third waveguide core layer 221 and a fourth doped layer stacked sequentially from bottom to top. The fifth doped layer 222, the second waveguide core layer 211 and the third waveguide core layer 221 are respectively connected to the first waveguide core layer 140.
第二掺杂层130为N型掺杂层,第四掺杂层212以及第五掺杂层222均为P型掺杂层;或者,第二掺杂层130为P型掺杂层,第四掺杂层212以及第五掺杂层222均为N型掺杂 层。The second doped layer 130 is an N-type doped layer, and the fourth doped layer 212 and the fifth doped layer 222 are both P-type doped layers; or, the second doped layer 130 is a P-type doped layer, The fourth doped layer 212 and the fifth doped layer 222 are both N-type doped layers.
具体地,第一有源组件210和波导结构100中位于第一有源组件210正下方的部分(包括第一有源组件210正下方的第二掺杂层130、第一掺杂层120和衬底110)形成第一有源光器件230,第二有源组件220以及波导结构100中位于第二有源组件220正下方的部分(包括第二有源组件220正下方的第二掺杂层130、第一掺杂层120和衬底110)形成第二有源光器件,也就是说,第一有源光器件230和第二有源光器件240共用衬底110、第一掺杂层120以及第二掺杂层130。Specifically, the first active component 210 and the part of the waveguide structure 100 directly below the first active component 210 (including the second doped layer 130 directly below the first active component 210, the first doped layer 120 and The substrate 110) forms the first active optical device 230, the second active component 220, and the portion of the waveguide structure 100 directly below the second active component 220 (including the second doping directly below the second active component 220). The layer 130, the first doped layer 120 and the substrate 110) form a second active optical device, that is, the first active optical device 230 and the second active optical device 240 share the substrate 110, the first doped The layer 120 and the second doped layer 130.
进一步地,由于集成光芯片200工作时,并不是集成光芯片200中所有的有源光器件的第二掺杂层130之间均存在电压差,因此,为了节约集成光芯片200的成本,以及降低集成光芯片200的加工复杂度,可以只将工作时第二掺杂层130之间存在电压差的有源光器件设置在空腔133相对的两侧接。也就是说,集成光芯片200工作时,第一有源器件230的电压,与第二有源器件240的电压不同,尤其是,第一有源器件230中的第二掺杂层130上的电压与第二有源器件240中的第二掺杂层130上的电压不同。Furthermore, because when the integrated optical chip 200 is working, not all the active optical devices in the integrated optical chip 200 have a voltage difference between the second doped layers 130. Therefore, in order to save the cost of the integrated optical chip 200, and To reduce the processing complexity of the integrated optical chip 200, only active optical devices with a voltage difference between the second doped layers 130 during operation can be arranged on opposite sides of the cavity 133 and connected. That is to say, when the integrated optical chip 200 is working, the voltage of the first active device 230 is different from the voltage of the second active device 240, in particular, the voltage on the second doped layer 130 in the first active device 230 The voltage is different from the voltage on the second doped layer 130 in the second active device 240.
进一步地,第一有源光器件230可以为调制器,第二有源光器件240可以为激光器、光放大器或光探测器。例如,当第一有源器件230为调制器时,如图8所示,调制器依次包括衬底110、第一掺杂层120、第二掺杂层130、第二波导芯层211以及第四掺杂层212。第二掺杂层130上设置有第一电极213,第四掺杂层212上设置有第二电极214,第一掺杂层120可以为基于InP的P型掺杂层,第二掺杂层130可以为基于InP的N型掺杂层,第四掺杂层212可以为基于InP的P型掺杂层。调制器工作时第一电极213上的电压高于第二电极214上的电压,第二波导芯层211基于量子限制斯塔克效应(quantum confined stark effect,QCSE)或其他光电效应进行电光调制。Further, the first active optical device 230 may be a modulator, and the second active optical device 240 may be a laser, an optical amplifier, or an optical detector. For example, when the first active device 230 is a modulator, as shown in FIG. 8, the modulator sequentially includes a substrate 110, a first doped layer 120, a second doped layer 130, a second waveguide core layer 211, and a first doped layer. Four doped layers 212. The second doped layer 130 is provided with a first electrode 213, and the fourth doped layer 212 is provided with a second electrode 214. The first doped layer 120 may be a P-type doped layer based on InP, and the second doped layer 130 may be an InP-based N-type doped layer, and the fourth doped layer 212 may be an InP-based P-type doped layer. When the modulator works, the voltage on the first electrode 213 is higher than the voltage on the second electrode 214, and the second waveguide core layer 211 performs electro-optic modulation based on the quantum confined stark effect (QCSE) or other photoelectric effects.
进一步地,为了实现第一有源光器件230以及第二有源光器件240在除第一波导芯层140延伸方向外其他方向上的电学隔离,在波导结构100的两侧的分别具有第一凹槽250和第二凹槽260,第一凹槽250以及第二凹槽260均贯穿第二掺杂层130,使得电流无法通过有源器件之间除第一波导芯层140延伸方向外其他方向上的第二掺杂层130传输,此时,集成光芯片200的俯视图如图9A所示,集成光芯片200在AA’方向上的剖面图如图9B所示。Further, in order to realize the electrical isolation of the first active optical device 230 and the second active optical device 240 in directions other than the extending direction of the first waveguide core layer 140, the first waveguide structure 100 has first The groove 250 and the second groove 260, the first groove 250 and the second groove 260 both penetrate the second doped layer 130, so that current cannot pass between the active devices except for the extending direction of the first waveguide core layer 140. The second doped layer 130 in the direction is transmitted. At this time, the top view of the integrated optical chip 200 is shown in FIG. 9A, and the cross-sectional view of the integrated optical chip 200 in the AA′ direction is shown in FIG. 9B.
其中,第一有源光器件230、第二有源光器件240和隔离器件270均位于第一凹槽250和第二凹槽260之间,隔离器件270包括第一波导芯层140、第二掺杂层130、第一掺杂层120中位于第二掺杂层130正下方的部分,以及衬底110位于第二掺杂层130正下方的部分,如图9B所示。在波导结构100包括第三掺杂层150的场景下,隔离器件270还包括第一波导芯层140上方的第三掺杂层150,即隔离器件270包括第一波导芯层140上方的第三掺杂层150、第一波导芯层140、第二掺杂层130、第一掺杂层120中位于第二掺杂层130正下方的部分,以及衬底110位于第二掺杂层130正下方的部分。上述波导结构100可以为隔离器件270。Wherein, the first active optical device 230, the second active optical device 240, and the isolation device 270 are all located between the first groove 250 and the second groove 260. The isolation device 270 includes a first waveguide core layer 140, a second The doped layer 130, the portion of the first doped layer 120 directly below the second doped layer 130, and the portion of the substrate 110 directly below the second doped layer 130, as shown in FIG. 9B. In the scenario where the waveguide structure 100 includes the third doped layer 150, the isolation device 270 further includes the third doped layer 150 above the first waveguide core layer 140, that is, the isolation device 270 includes the third doped layer 150 above the first waveguide core layer 140. The doped layer 150, the first waveguide core layer 140, the second doped layer 130, the portion of the first doped layer 120 directly below the second doped layer 130, and the substrate 110 is located directly on the second doped layer 130 The lower part. The aforementioned waveguide structure 100 may be an isolation device 270.
在具体实施中,第一凹槽250以及第二凹槽260还可以贯穿位于衬底110上的第一掺杂层120。In a specific implementation, the first groove 250 and the second groove 260 may also penetrate the first doped layer 120 on the substrate 110.
需要说明的是,本申请实施例并不对第一有源器件的个数以及第二有源器件的个数进行限定。由于集成光芯片200中多个第一有源光器件230或多个第二有源光器件240之间不存在电压差,因此多个第一有源光器件230或多个第二有源光器件240可以位于空腔133 的同一侧,即多个第一有源光器件230之间或多个第二有源光器件240之间可以不用通过空腔133进行电学隔离。例如,如图10A所示,集成光芯片200中包括的调制器、激光器和光放大器,调制器与激光器分别位于第一空腔133的相对两侧,调制器与光放大器位于第二空腔133的相对两侧;如图10B所示,集成光芯片200中包括的调制器、激光器和光放大器,调制器与光放大器分别位于空腔133的相对两侧,激光器与光放大器位于同一侧,由集成光芯片200工作时,激光器与光放大器之间没有电压差,因此激光器与光放大器之间可以不用通过空腔133进行电学隔离;如图10C所示,集成光芯片200中调制器、激光器、光放大器和光探测器,调制器与光放大器分别位于空腔133的相对两侧,激光器、光探测器与光放大器位于同一侧,由集成光芯片200工作时,激光器、光探测器与光放大器之间没有电压差,因此激光器、光探测器与光放大器之间可以不用通过空腔133进行电学隔离。It should be noted that the embodiments of the present application do not limit the number of first active devices and the number of second active devices. Since there is no voltage difference between the plurality of first active optical devices 230 or the plurality of second active optical devices 240 in the integrated optical chip 200, the plurality of first active optical devices 230 or the plurality of second active optical devices The devices 240 may be located on the same side of the cavity 133, that is, between the plurality of first active optical devices 230 or between the plurality of second active optical devices 240 may not be electrically isolated by the cavity 133. For example, as shown in FIG. 10A, the modulator, laser, and optical amplifier included in the integrated optical chip 200 are located on opposite sides of the first cavity 133, and the modulator and the optical amplifier are located in the second cavity 133. On opposite sides; as shown in FIG. 10B, the modulator, laser, and optical amplifier included in the integrated optical chip 200, the modulator and the optical amplifier are respectively located on opposite sides of the cavity 133, the laser and the optical amplifier are located on the same side, by the integrated optical When the chip 200 is working, there is no voltage difference between the laser and the optical amplifier, so the laser and the optical amplifier do not need to be electrically isolated by the cavity 133; as shown in Figure 10C, the modulator, laser, and optical amplifier in the integrated optical chip 200 And the optical detector, the modulator and the optical amplifier are located on opposite sides of the cavity 133, and the laser, the optical detector and the optical amplifier are on the same side. When the integrated optical chip 200 works, there is no space between the laser, the optical detector and the optical amplifier. Because of the voltage difference, the laser, the photodetector and the optical amplifier can be electrically isolated without the cavity 133.
应当理解的是,本申请实施例提供的集成光芯片200为一个完整的集成光芯片,也具备已知的集成光芯片具有的结构(如有源光器件的驱动电路),在此仅对集成光芯片中涉及实现集成光芯片中有源器件的共用掺杂层的电学隔离的相关结构进行说明,对于其他结构不予赘述。It should be understood that the integrated optical chip 200 provided by the embodiment of the present application is a complete integrated optical chip, and also has the structure of a known integrated optical chip (such as a driving circuit of an active optical device). The related structure of the optical chip involved in realizing the electrical isolation of the common doped layer of the active device in the integrated optical chip will be described, and other structures will not be repeated.
基于以上实施例,本申请还提供了一种实现集成光芯片中有源光器件之间的电学隔离的方法,也即制备波导结构100的方法。如图11所示,该方法主要包括以下步骤:Based on the above embodiments, this application also provides a method for realizing electrical isolation between active optical devices in an integrated optical chip, that is, a method for preparing the waveguide structure 100. As shown in Figure 11, the method mainly includes the following steps:
S1101:在衬底110上依次生长第一掺杂层120、第二掺杂层130以及第一波导芯层140。S1101: The first doped layer 120, the second doped layer 130, and the first waveguide core layer 140 are sequentially grown on the substrate 110.
其中,第一波导芯层140覆盖第二掺杂层130的上表面的部分区域,第二掺杂层130包括上阻挡层131和牺牲层132,牺牲层132位于第一掺杂层120与上阻挡层131之间;第一掺杂层120可以为N型掺杂层或P型掺杂层,当第一掺杂层120为N型掺杂层时,第二掺杂层130为P型掺杂层,当第一掺杂层120为P型掺杂层时,第二掺杂层130为N型掺杂层,即第一掺杂层120与第二掺杂层130的掺杂类型相反。Wherein, the first waveguide core layer 140 covers a part of the upper surface of the second doped layer 130. The second doped layer 130 includes an upper barrier layer 131 and a sacrificial layer 132. The sacrificial layer 132 is located on the first doped layer 120 and above. Between the barrier layers 131; the first doped layer 120 may be an N-type doped layer or a P-type doped layer, when the first doped layer 120 is an N-type doped layer, the second doped layer 130 is a P-type Doped layer. When the first doped layer 120 is a P-type doped layer, the second doped layer 130 is an N-type doped layer, that is, the doping type of the first doped layer 120 and the second doped layer 130 in contrast.
S1102:对第一波导芯层140进行刻蚀,形成波导沟槽(waveguide trench)。其中,波导沟槽的深度大于第一波导芯层140的厚度,以露出第一波导心层140下的第二掺杂层130。S1102: Etching the first waveguide core layer 140 to form a waveguide trench. The depth of the waveguide groove is greater than the thickness of the first waveguide core layer 140 to expose the second doped layer 130 under the first waveguide core layer 140.
S1103:对波导沟槽中露出的第二掺杂层130进行刻蚀,在第二掺杂层130中形成至少一个空腔133。S1103: The second doped layer 130 exposed in the waveguide trench is etched, and at least one cavity 133 is formed in the second doped layer 130.
其中,刻蚀后剩余的牺牲层132用于支撑上阻挡层131,空腔133沿空腔133的延伸方向贯穿第二掺杂层130,第一波导芯层140位于空腔133的正上方,且空腔133的延伸方向与第一波导芯层140的延伸方向相互垂直。The sacrificial layer 132 remaining after etching is used to support the upper barrier layer 131, the cavity 133 penetrates the second doped layer 130 along the extending direction of the cavity 133, and the first waveguide core layer 140 is located directly above the cavity 133. The extension direction of the cavity 133 and the extension direction of the first waveguide core layer 140 are perpendicular to each other.
进一步地,步骤S1103中对波导沟槽中露出的第二掺杂层130进行刻蚀,在第二掺杂层130中形成至少一个空腔133,包括以下步骤:i、对波导沟槽中露出的上阻挡层131进行刻蚀,形成至少一个刻蚀窗口134;其中,刻蚀窗口134的深度大于上阻挡层131的厚度,以使刻蚀剂能够与牺牲层132接触,进而对牺牲层132进行刻蚀形成空腔133;ii、将腐蚀剂加入至少一个刻蚀窗口中,对牺牲层132进行腐蚀,形成至少一个空腔133。具体地,在对波导沟槽中露出的第二掺杂层130进行刻蚀时,通过掩膜保护除刻蚀窗口以外的区域。Further, in step S1103, etching the second doped layer 130 exposed in the waveguide trench to form at least one cavity 133 in the second doped layer 130 includes the following steps: i. Exposing the waveguide trench The upper barrier layer 131 is etched to form at least one etch window 134; wherein the depth of the etch window 134 is greater than the thickness of the upper barrier layer 131, so that the etchant can contact the sacrificial layer 132, and then to Etching is performed to form a cavity 133; ii, an etchant is added to at least one etching window to etch the sacrificial layer 132 to form at least one cavity 133. Specifically, when the second doped layer 130 exposed in the waveguide trench is etched, the area except for the etching window is protected by a mask.
执行步骤S1103之后,该方法还包括:向位于空腔133正上方的部分上阻挡层131中注入目标离子。其中,目标离子用于增加位于空腔133正上方的部分上阻挡层131的阻抗。After step S1103 is performed, the method further includes: implanting target ions into the upper barrier layer 131 directly above the cavity 133. Among them, the target ions are used to increase the impedance of the blocking layer 131 on the portion directly above the cavity 133.
具体实施中,为了使得位于空腔133正上方,第一波导芯层140正下方的部分上阻挡层131中也能够注入目标离子,通常从与波导结构100的厚度方向呈一定角度的方向(离子注入角度)进行离子注入,并根据注入深度与离子注入能量和剂量的匹配结果,选择合适的离子注入能量和剂量,向位于空腔133正上方的部分上阻挡层131中注入目标离子。In specific implementation, in order to make the portion of the upper barrier layer 131 directly above the cavity 133 directly below the first waveguide core layer 140 also be able to implant target ions, usually from a direction (ion The implantation angle) performs ion implantation, and selects appropriate ion implantation energy and dose according to the matching result of the implantation depth, ion implantation energy and dose, and implants target ions into the upper barrier layer 131 directly above the cavity 133.
示例性地,如图12所示,当目标离子以角度α注入到第一波导芯层140正下方的上阻挡层131与波导芯层140的在厚度方向上的中心线的交点O处时,角度α与波导芯层140的宽度w以及离子注入深度d满足以下公式:Exemplarily, as shown in FIG. 12, when target ions are injected at the intersection point O of the upper barrier layer 131 directly below the first waveguide core layer 140 and the center line of the waveguide core layer 140 in the thickness direction at an angle α, The angle α, the width w of the waveguide core layer 140 and the ion implantation depth d satisfy the following formula:
Figure PCTCN2019099441-appb-000001
Figure PCTCN2019099441-appb-000001
在实施中离子注入的深度可以大于或等于
Figure PCTCN2019099441-appb-000002
以使位于空腔133正上方,第一波导芯层140正下方的部分上阻挡层131中均注入有目标离子。
The depth of ion implantation can be greater than or equal to
Figure PCTCN2019099441-appb-000002
So that the upper barrier layer 131 located directly above the cavity 133 and directly below the first waveguide core layer 140 is implanted with target ions.
综上,本申请实施例提供一种波导结构、集成光芯片以及电学隔离方法,采用本申请实施例提供的方案,可以实现集成光芯片中有源光器件之间的电学隔离,进而可以减小所述集成光芯片的功耗以及发热,保证所述集成光芯片正常工作。In summary, the embodiments of the present application provide a waveguide structure, an integrated optical chip, and an electrical isolation method. Using the solutions provided in the embodiments of the present application, electrical isolation between active optical devices in the integrated optical chip can be achieved, thereby reducing The power consumption and heat generation of the integrated optical chip ensure the normal operation of the integrated optical chip.
显然,本领域的技术人员可以对本申请进行各种改动和变型而不脱离本申请的精神和范围。这样,倘若本申请的这些修改和变型属于本申请权利要求及其等同技术的范围之内,则本申请也意图包含这些改动和变型在内。Obviously, those skilled in the art can make various changes and modifications to the application without departing from the spirit and scope of the application. In this way, if these modifications and variations of this application fall within the scope of the claims of this application and their equivalent technologies, this application also intends to include these modifications and variations.

Claims (14)

  1. 一种波导结构,其特征在于,应用于集成光芯片,所述波导结构包括从下到上依次层叠设置的衬底、第一掺杂层、第二掺杂层以及第一波导芯层,所述第一波导芯层覆盖所述第二掺杂层的上表面的部分区域;A waveguide structure, which is characterized in that it is applied to an integrated optical chip. The waveguide structure includes a substrate, a first doped layer, a second doped layer, and a first waveguide core layer stacked in sequence from bottom to top. The first waveguide core layer covers a partial area of the upper surface of the second doped layer;
    其中,所述第二掺杂层包括上阻挡层和牺牲层,所述牺牲层位于所述上阻挡层和所述第一掺杂层之间且用于支撑所述上阻挡层;所述第二掺杂层具有至少一个空腔,所述空腔沿所述空腔的延伸方向贯穿所述第二掺杂层,所述第一波导芯层位于所述空腔的正上方,且所述空腔的延伸方向与所述第一波导芯层的延伸方向相互垂直;Wherein, the second doped layer includes an upper barrier layer and a sacrificial layer, the sacrificial layer is located between the upper barrier layer and the first doped layer and is used to support the upper barrier layer; The second doped layer has at least one cavity, the cavity penetrates the second doped layer along the extending direction of the cavity, the first waveguide core layer is located directly above the cavity, and the The extending direction of the cavity and the extending direction of the first waveguide core layer are perpendicular to each other;
    所述第一掺杂层为N型掺杂层,所述第二掺杂层为P型掺杂层;或者,所述第一掺杂层为P型掺杂层,所述第二掺杂层为N型掺杂层。The first doped layer is an N-type doped layer, and the second doped layer is a P-type doped layer; or, the first doped layer is a P-type doped layer, and the second doped layer is The layer is an N-type doped layer.
  2. 如权利要求1所述的波导结构,其特征在于,所述第一波导芯层在所述空腔的底壁所在平面上的投影位于所述空腔的底壁内,其中,所述空腔的底壁是所述第一掺杂层的上表面的部分区域。The waveguide structure according to claim 1, wherein the projection of the first waveguide core layer on the plane of the bottom wall of the cavity is located in the bottom wall of the cavity, wherein the cavity The bottom wall of is a partial area of the upper surface of the first doped layer.
  3. 如权利要求1或2所述的波导结构,其特征在于,位于所述空腔正上方的部分上阻挡层中被注入有目标离子,所述目标离子用于增加所述部分上阻挡层的阻抗。The waveguide structure according to claim 1 or 2, wherein a part of the upper barrier layer directly above the cavity is implanted with target ions, and the target ions are used to increase the impedance of the upper barrier layer .
  4. 如权利要求3所述的波导结构,其特征在于,所述上阻挡层的厚度小于或等于设定值,所述设定值为所述目标离子能够注入到所述上阻挡层中的最大深度。The waveguide structure of claim 3, wherein the thickness of the upper barrier layer is less than or equal to a set value, and the set value is the maximum depth at which the target ion can be implanted into the upper barrier layer .
  5. 如权利要求1-4任意一项所述的波导结构,其特征在于,还包括:第三掺杂层,所述第三掺杂层位于所述第一波导芯层的上方,其中,所述第二掺杂层为N型掺杂层,所述第三掺杂层为P型掺杂层;或者,所述第二掺杂层为P型掺杂层,所述第三掺杂层为N型掺杂层。The waveguide structure according to any one of claims 1 to 4, further comprising: a third doped layer, the third doped layer is located above the first waveguide core layer, wherein the The second doped layer is an N-type doped layer, and the third doped layer is a P-type doped layer; or, the second doped layer is a P-type doped layer, and the third doped layer is N-type doped layer.
  6. 如权利要求1-5任意一项所述的波导结构,其特征在于,所述第一掺杂层包括缓冲层和下阻挡层,所述缓冲层位于所述下阻挡层与所述衬底之间;The waveguide structure according to any one of claims 1-5, wherein the first doped layer comprises a buffer layer and a lower barrier layer, and the buffer layer is located between the lower barrier layer and the substrate. between;
    所述空腔的底壁为所述下阻挡层的上表面的部分区域。The bottom wall of the cavity is a partial area of the upper surface of the lower barrier layer.
  7. 一种集成光芯片,其特征在于,包括如权利要求1-6任意一项所述的波导结构、第一有源组件和第二有源组件;其中,所述上阻挡层的上表面设置有相互隔离的所述第一有源组件和所述第二有源组件,所述第一有源组件和所述第二有源组件分别位于所述空腔的相对的两侧,所述第一有源组件的正下方为所述牺牲层的一部分,所述第二有源组件的正下方为所述牺牲层的另一部分;An integrated optical chip, characterized by comprising the waveguide structure according to any one of claims 1-6, a first active component and a second active component; wherein the upper surface of the upper barrier layer is provided with The first active component and the second active component are isolated from each other, the first active component and the second active component are respectively located on opposite sides of the cavity, and the first Immediately below the active component is a part of the sacrificial layer, and directly below the second active component is another part of the sacrificial layer;
    所述第一有源组件包括从下到上依次层叠的第二波导芯层和第四掺杂层,所述第二有源组件包括从下到上依次层叠的第三波导芯层和第五掺杂层,其中,所述第二波导芯层和所述第三波导芯层分别与所述第一波导芯层相连接;The first active component includes a second waveguide core layer and a fourth doped layer that are sequentially stacked from bottom to top, and the second active component includes a third waveguide core layer and a fifth waveguide core layer that are stacked sequentially from bottom to top. A doped layer, wherein the second waveguide core layer and the third waveguide core layer are respectively connected to the first waveguide core layer;
    所述第二掺杂层为N型掺杂层,所述第四掺杂层以及所述第五掺杂层均为P型掺杂层;或者,所述第二掺杂层为P型掺杂层,所述第四掺杂层以及所述第五掺杂层均为N型掺杂层。The second doped layer is an N-type doped layer, and the fourth doped layer and the fifth doped layer are both P-type doped layers; or, the second doped layer is a P-type doped layer. The doped layer, the fourth doped layer and the fifth doped layer are both N-type doped layers.
  8. 如权利要求7所述的集成光芯片,其特征在于,所述第一有源组件和所述波导结构中位于所述第一有源组件正下方的部分形成第一有源光器件;8. The integrated optical chip of claim 7, wherein the first active component and the part of the waveguide structure directly below the first active component form a first active optical device;
    所述第二有源组件以及所述波导结构中位于所述第二有源组件正下方的部分形成第二有源光器件。The second active component and the portion of the waveguide structure directly below the second active component form a second active optical device.
  9. 如权利要求8所述的集成光芯片,其特征在于,在所述波导结构延伸方向上的两侧分别具有第一凹槽和第二凹槽,所述第一凹槽以及所述第二凹槽均贯穿所述第二掺杂层,其中,所述第一有源光器件、所述第二有源光器件和隔离器件均位于所述第一凹槽和所述第二凹槽之间,所述隔离器件包括所述第二掺杂层、所述第一波导芯层、所述第一掺杂层中位于所述第二掺杂层正下方的部分,以及所述衬底位于所述第二掺杂层正下方的部分。The integrated optical chip according to claim 8, wherein a first groove and a second groove are respectively provided on both sides in the extending direction of the waveguide structure, the first groove and the second groove The grooves all penetrate the second doped layer, wherein the first active optical device, the second active optical device, and the isolation device are all located between the first groove and the second groove , The isolation device includes the second doped layer, the first waveguide core layer, a portion of the first doped layer directly below the second doped layer, and the substrate is located The part directly below the second doped layer.
  10. 如权利要求8或9所述的集成光芯片,其特征在于,所述集成光芯片工作时,所述第一有源器件的电压,与所述第二有源器件的电压不同。9. The integrated optical chip according to claim 8 or 9, wherein when the integrated optical chip works, the voltage of the first active device is different from the voltage of the second active device.
  11. 如权利要求8-10任意一项所述的集成光芯片,其特征在于,所述第一有源光器为调制器,所述第二有源光器为激光器、光放大器或光探测器。The integrated optical chip according to any one of claims 8-10, wherein the first active optical device is a modulator, and the second active optical device is a laser, an optical amplifier, or an optical detector.
  12. 一种实现电学隔离的方法,其特征在于,应用于集成光芯片,所述方法包括:A method for realizing electrical isolation, characterized in that it is applied to an integrated optical chip, and the method includes:
    在衬底上依次生长第一掺杂层、第二掺杂层以及第一波导芯层;其中,所述第一波导芯层覆盖所述第二掺杂层的上表面的部分区域,所述第二掺杂层包括上阻挡层和牺牲层,所述牺牲层位于所述第一掺杂层与所述上阻挡层之间,所述第一掺杂层为N型掺杂层,所述第二掺杂层为P型掺杂层;或者,所述第一掺杂层为P型掺杂层,所述第二掺杂层为N型掺杂层;A first doped layer, a second doped layer, and a first waveguide core layer are sequentially grown on a substrate; wherein the first waveguide core layer covers a partial area of the upper surface of the second doped layer, and The second doped layer includes an upper barrier layer and a sacrificial layer, the sacrificial layer is located between the first doped layer and the upper barrier layer, the first doped layer is an N-type doped layer, and the The second doped layer is a P-type doped layer; or, the first doped layer is a P-type doped layer, and the second doped layer is an N-type doped layer;
    对所述第一波导芯层进行刻蚀,形成波导沟槽,其中,所述波导沟槽的深度大于所述第一波导芯层的厚度;Etching the first waveguide core layer to form a waveguide trench, wherein the depth of the waveguide trench is greater than the thickness of the first waveguide core layer;
    对所述波导沟槽中露出的所述第二掺杂层进行刻蚀,在所述第二掺杂层中形成至少一个空腔;其中,刻蚀后剩余的所述牺牲层用于支撑所述上阻挡层,所述空腔沿所述空腔的延伸方向贯穿所述第二掺杂层,所述第一波导芯层位于所述空腔的正上方,且所述空腔的延伸方向与所述第一波导芯层的延伸方向相互垂直。The second doped layer exposed in the waveguide trench is etched to form at least one cavity in the second doped layer; wherein the sacrificial layer remaining after etching is used to support the The above barrier layer, the cavity penetrates the second doped layer along the extending direction of the cavity, the first waveguide core layer is located directly above the cavity, and the extending direction of the cavity The extension direction of the first waveguide core layer is perpendicular to each other.
  13. 如权利要求12所述的方法,其特征在于,对所述波导沟槽中露出的所述第二掺杂层进行刻蚀,在所述第二掺杂层中形至少一个空腔,包括:11. The method of claim 12, wherein etching the second doped layer exposed in the waveguide trench to form at least one cavity in the second doped layer comprises:
    对所述波导沟槽中露出的所述上阻挡层进行刻蚀,形成至少一个刻蚀窗口;其中,所述刻蚀窗口的深度大于所述上阻挡层的厚度;Etching the upper barrier layer exposed in the waveguide trench to form at least one etching window; wherein the depth of the etching window is greater than the thickness of the upper barrier layer;
    将腐蚀剂加入所述至少一个刻蚀窗口中,对所述牺牲层进行腐蚀,形成所述至少一个空腔。An etchant is added to the at least one etching window to etch the sacrificial layer to form the at least one cavity.
  14. 如权利要求12或13所述的方法,其特征在于,对所述波导沟槽中露出的所述第二掺杂层进行刻蚀,在所述第二掺杂层中形成至少一个空腔之后,还包括:The method of claim 12 or 13, wherein the second doped layer exposed in the waveguide trench is etched, and after at least one cavity is formed in the second doped layer ,Also includes:
    向位于所述空腔正上方的部分上阻挡层中注入目标离子;其中,所述目标离子用于增加位于所述空腔正上方的部分上阻挡层的阻抗。Implanting target ions into the upper barrier layer located directly above the cavity; wherein the target ions are used to increase the impedance of the upper barrier layer located directly above the cavity.
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