US20020005524A1 - Semiconductor photoreceiving device - Google Patents
Semiconductor photoreceiving device Download PDFInfo
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- US20020005524A1 US20020005524A1 US09/732,728 US73272800A US2002005524A1 US 20020005524 A1 US20020005524 A1 US 20020005524A1 US 73272800 A US73272800 A US 73272800A US 2002005524 A1 US2002005524 A1 US 2002005524A1
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/30—Coatings
- H10F77/306—Coatings for devices having potential barriers
- H10F77/331—Coatings for devices having potential barriers for filtering or shielding light, e.g. multicolour filters for photodetectors
- H10F77/337—Coatings for devices having potential barriers for filtering or shielding light, e.g. multicolour filters for photodetectors using interference filters, e.g. multilayer dielectric filters
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F30/00—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors
- H10F30/20—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors
- H10F30/21—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation
- H10F30/22—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes
- H10F30/221—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes the potential barrier being a PN homojunction
- H10F30/2215—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes the potential barrier being a PN homojunction the devices comprising active layers made of only Group III-V materials
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F30/00—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors
- H10F30/20—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors
- H10F30/21—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation
- H10F30/22—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes
- H10F30/222—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes the potential barrier being a PN heterojunction
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F30/00—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors
- H10F30/20—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors
- H10F30/21—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation
- H10F30/22—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes
- H10F30/223—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes the potential barrier being a PIN barrier
Definitions
- the present invention relates to a semiconductor photoreceiving device that is suitable for use in optical communications and performs opto-electric conversion of light at high speeds, and more particularly to a semiconductor photoreceiving device that can selectively extract a signal of long wavelength light in multiplexed optical communications (especially with two wavelengths).
- the photoreceiving device be an element that can selectively receive both 1.3 ⁇ m optical signals and 1.55 ⁇ m optical signals.
- the photoreceiving devices that selectively receive optical signals with wavelengths of 1.3 ⁇ m (hereinafter referred to as short wavelength) are provided with a light-absorbing layer composed of InGaAsP with a band gap wavelength of about 1.4 ⁇ m.
- the light-absorbing layer generally has the property of absorbing light with wavelengths shorter than the band gap wavelength of the light-absorbing layer. Accordingly, it is very difficult to form a light-absorbing layer that can receive only an optical signal of 1.55 ⁇ m (hereinafter referred to as long wavelength) in a single layer.
- the method of interposing an optical filter between the multiplexed light entering the photoreceiving device and the photoreceiving surface of the photoreceiving device has been used for the selective reception of long wavelength optical signals, as disclosed in the Reference 1 (Ishigami et al., “Automatic Machine For Bonding Fiber Block To Planar Lightwave Circuit”, 1998 Institute of Electronics, Information and Communication Engineers, Electronics Society Conference C-3-87), Reference 2 (Hashimoto et al., “1.3/1.55 ⁇ m WDM optical module for full duplex operation using PLC platform”, 1998 Institute of Electronics, Information and Communication Engineers, Electronics Society Conference C-3-110), and Reference 3 (Maeda et al., “WDM by multilayered dielectric filter on silica based waveguide (3)”, 1998 Institute of Electronics, Information and Communication Engineers, Electronics Society Conference C-3-150).
- the semiconductor photoreceiving device in Reference 4 comprises a first light-absorbing layer and a second light-absorbing layer in that order within an optical path for multiplexed light; wherein this first light-absorbing layer is composed of a material with a band gap wavelength longer than 1.3 ⁇ m and shorter than 1.55 ⁇ m (for example, InGaAsP), and the second light-absorbing layer is composed of a material having a band gap wavelength longer than 1.55 ⁇ m (for example, InGaAs). Shorter wavelength light is thereby absorbed by the first light-absorbing layer and long wavelength light that passes through this first light-absorbing layer is absorbed by the second light-absorbing layer.
- the first light-absorbing layer In a photoreceiving device comprising a first light-absorbing layer and a second light-absorbing layer, the first light-absorbing layer must be thick so that the selection ratio of short wavelength light to long wavelength light is the desirable selection ratio for the photoreceiving device. As a result, there is high stress between the first light-absorbing layer and the layers formed on top of the first light-absorbing layer, and there is a risk of strain occurring in each layer formed on top of the first light-absorbing layer. Also, the first light-absorbing layer is formed by epitaxial growth; the cost of the photoreceiving device increases in proportion to the thickness of the epitaxial layer.
- the present invention is to provide a semiconductor photoreceiving device having the following constitution for selectively receiving long wavelength light from multiplexed light including long wavelength light and short wavelength light.
- this semiconductor photoreceiving device comprises a multilayered film of alternately stacked layers of materials having mutually different indexes of refraction. The thickness of each layer and the number of layers in the multilayered film are designed such that long wavelength light is transmitted and short wavelength light is reflected by the multilayered film.
- the photoreceiving device further comprises a first light-absorbing layer that is composed of a material having a band gap wavelength longer than the long wavelength light. Also, the photoreceiving device has a structure such that multiplexed light enters the first light-absorbing layer through the multilayered film.
- This type of semiconductor photoreceiving device preferably comprises a substrate having a first main surface and a second main surface; the first light-absorbing layer may be established on the first main surface side of the substrate and the multilayered film may be established on the second main surface side of the substrate.
- the semiconductor photoreceiving device having this type of constitution is referred to as a back surface incidence (or entry) type photoreceiving device.
- the semiconductor photoreceiving device may also be constituted such that the substrate has a first main surface and the multilayered film is established on the first main surface side of the substrate with the first light-absorbing layer interposed therebetween.
- a photoreceiving device with such a constitution is referred to as a top surface incidence (or entry) type photoreceiving device in contrast to the abovementioned back surface incidence type photoreceiving device.
- multiplexed light including long wavelength light and short wavelength light first enters the multilayered film and then the short wavelength light is reflected by this multilayered film. After that, the long wavelength light passes through the multilayered film, passes through the substrate, reaches the first light-absorbing layer, and is absorbed (received) by this first light-absorbing layer.
- top surface incidence type and back surface incidence type photoreceiving devices are suitable for use in the case of incident light spread over a broad range, such as in monitor photodiodes (MPD), for example, because the photoreceiving surface can be made as large as the chip size.
- MPD monitor photodiodes
- the constitution of the semiconductor photoreceiving device is preferably provided a substrate having a first main surface and a side surface.
- the first light-absorbing layer may be established on the first main surface side of the substrate and the multilayered film may be established on the side surface of the substrate.
- a mesa surface is preferably established on the substrate so that light passing through the multilayered film is reflected towards the first light-absorbing layer.
- a photoreceiving device with such a constitution is called the end surface incidence (or entry) type.
- the end surface incidence type device is able to operate at higher speeds than the top surface or back surface incidence type devices. Because a mesa surface is established on the substrate, light passing through the multilayered film and entering (or impinging on or arriving at) the substrate is reflected by the mesa surface and this reflected light enters the second light-absorbing layer from the first main surface of the substrate. The short wavelength light in the multiplexed light is thereby reflected by the multilayered film. After this, only the long wavelength light is absorbed by the first light-absorbing layer.
- the semiconductor photoreceiving devices according to the present invention may also be provided with a substrate having a first main surface, and may be constituted so that the first light-absorbing layer is established on this first main surface side and the multilayered film is disposed so that the light passing through the multilayered film is refracted and is incident on or enters the first light-absorbing layer.
- This type of constitution can be given as a variation of the end surface incidence type discussed above.
- a V-shaped groove is formed in the second main surface of the substrate by wet etching and an end surface comprising the mesa surface of the V-shaped groove is formed by cleavage or the like (for example, scribing, dicing, etching) near the peak of this V-shaped groove.
- This end surface becomes the photoreceiving surface and the multilayered film is established thereon.
- the short wavelength light in the multiplexed light entering the multilayered film is thereby reflected by the multilayered film.
- the light passing through the multilayered film is refracted by the end surface and passes through the substrate to reach the first light-absorbing layer. After this, the long wavelength light is absorbed by the first light-absorbing layer.
- a semiconductor photoreceiving device having the constitution discussed above preferably further comprises a second light-absorbing layer for selectively absorbing short wavelength light from the multiplexed light.
- This second light-absorbing layer may be established at a position such that the light passing through the multilayered film enters the first light-absorbing layer through the second light-absorbing layer.
- the second light-absorbing layer is preferably composed of a material having a band gap wavelength longer than the short wavelength light and shorter than the long wavelength light.
- a multilayered film therefore should be formed into a thickness such that there is no such risk of its properties deteriorating and a second light-absorbing layer is established in the light path through which the light passing through the multilayered film reaches the first light-absorbing layer.
- This second light-absorbing layer has a band gap wavelength longer than the short wavelength light and shorter than the long wavelength light, and therefore the short wavelength light that is not reflected by the multilayered film can be absorbed by this layer. Meanwhile, the long wavelength light passes through this second light-absorbing layer and reaches the first light-absorbing layer.
- Such a photoreceiving device can be caused to selectively intercept long wavelength light at the preferred intensity selection ratio by the actions of both the multilayered film and the second light-absorbing film that selectively absorbs short wavelength light. Accordingly, it is not necessary for either the multilayered film or the second light-absorbing layer to be thick. The risk of the strain of each layer is thereby eliminated and cost reductions for the photoreceiving device can be achieved.
- FIG. 1 is a cross sectional view showing the schematic constitution of the semiconductor photoreceiving device according to the first embodiment
- FIG. 2 is a cross sectional view showing the schematic constitution of the semiconductor photoreceiving device according to the second embodiment
- FIG. 3 is a cross sectional view showing the constitution of a first variation of the second embodiment
- FIG. 4 is a cross sectional view showing the constitution of a second variation of the second embodiment
- FIG. 5 is a cross sectional view showing the constitution of a third variation of the second embodiment
- FIG. 6 is a schematic view showing the constitution of the multilayered film designed for the embodiments of the present invention.
- FIG. 7 shows the transmittance of the multilayered film according to the embodiments.
- FIG. 1 is a cross sectional view showing the schematic constitution of the semiconductor photoreceiving device.
- the semiconductor photoreceiving device 10 is used in multiplexed optical communications including the long wavelength light A and short wavelength light B. This semiconductor photoreceiving device 10 selectively intercepts the long wavelength light A from the multiplexed light incident on (or entering or impinging on or arriving at) the photoreceiving surface 10 a.
- This photoreceiving device 10 comprises, at least, a substrate 12 and a first light-absorbing layer 14 established on the first main surface 12 a side of the substrate 12 and composed of a material having a band gap wavelength longer than the long wavelength light A.
- multiplexed light comprises long wavelength light A with a wavelength of 1.55 ⁇ m and short wavelength light B with a wavelength of 1.3 ⁇ m.
- the photoreceiving device 10 comprises an n-type InP substrate 12 and an InGaAs layer, as the first light-absorbing layer 14 , established on the upper surface, or first main surface 12 a, of this n-type InP substrate 12 .
- the InGaAs layer 14 has a band gap wavelength of 1.7 ⁇ m, and therefore absorbs both the 1.55 ⁇ m wavelength light A and the 1.3 ⁇ m wavelength light B.
- a p-type InP layer 16 is established as a contact layer on the upper surface of the InGaAs layer 14 .
- a p-type electrode 18 is established on the upper surface of this p-type InP layer 16 .
- an n-type electrode 20 is established in a region separate from the region where the InGaAs layer 14 is established on the first main surface 12 a of the n-type InP substrate 12 .
- the optical signal absorbed by the first light-absorbing layer (InGaAs layer) 14 undergoes opto-electric conversion and is extracted as an electrical signal from the p-type electrode 18 and n-type electrode 20 (FIG. 1).
- the photoreceiving device is a back surface incident type element.
- the photoreceiving surface 10 a of the photoreceiving device 10 is the second main surface 12 b (back surface) side of the substrate 12 .
- a multilayered film 22 formed of stacked layers of materials with mutually different indexes of refraction laminated together, is established on the photoreceiving surface 10 a.
- This multilayered film 22 is a multilayered film 22 wherein the thickness of each layer and the number of layers are designed so that the long wavelength light A is transmitted and short wavelength light B is refracted (FIG. 1).
- the thickness of each layer and the number of layers in the multilayered film 22 are determined on the basis of the conventional optical computation method for the multilayered film used in optical coatings, with consideration of the intensity selection ratio of the short wavelength light B to the long wavelength light A.
- the reflectance of the multilayered film is as disclosed in the Reference 5 (Yoshida, “Applied Physics and Optics Selection 3, Thin Films”, Baifukan, 1997, pp. 173-174). Based on a method using the effective Fresnel coefficient in this Reference 5, a program is prepared to determine the thickness of each layer and the number of layers according to the desired reflectance.
- the necessary settings and conditions, such as the desired reflectance, the index of refraction of the materials constituting the layers, and the wavelengths used are added to this program and the thickness of each layer and the number of layers in the multilayered film are determined by calculations using a computer. Moreover, the abovementioned selection ratio in the multilayered film 22 is optimally within a range of ⁇ 27 to ⁇ 33 dB.
- the 1.55 ⁇ m wavelength light A can be transmitted and the 1.3 ⁇ m wavelength light B can be reflected.
- the photoreceiving device 10 When multiplexed light composed of the 1.55 ⁇ m wavelength light A and the 1.3 ⁇ m wavelength light B enters the photoreceiving device 10 according to the present embodiment, the 1.3 ⁇ m wavelength light B is reflected and the 1.55 ⁇ m wavelength light A is transmitted by the multilayered film 22 . Afterwards, the 1.55 ⁇ m wavelength light A that has passed through the n-type InP substrate 12 enters the InGaAs layer 14 . The 1.55 ⁇ m wavelength light A is absorbed by this InGaAs layer 14 , and undergoes opto-electric conversion and is extracted as an electrical signal from the p-type electrode 18 and the n-type electrode 20 (FIG. 1).
- the semiconductor photoreceiving device allows the reception of only the long wavelength light A without cutting away the PLC waveguide and establishing an optical filter between the photoreceiving device and the incoming light.
- FIG. 2 is a cross sectional view of the constitution of the semiconductor photoreceiving device according to the second embodiment.
- the semiconductor photoreceiving device 30 relating to the present embodiment is a photoreceiving device 30 used in multiplexed optical communications, using multiplexed light comprising 1.55 ⁇ m wavelength light as the long wavelength light A and 1.3 ⁇ m wavelength light as the short wavelength light B, and selectively intercepts the long wavelength light A.
- the photoreceiving device comprises at least a substrate 32 and a first light-absorbing layer 14 established on the first main surface side 32 a of the substrate 32 .
- This first light-absorbing layer 14 is composed of a material having a band gap wavelength longer than the long wavelength light A.
- the photoreceiving surface 30 a of this photoreceiving device 30 is the second main surface 32 b of the substrate 32 ; the same type of multilayered film 22 as in the first embodiment is formed on that surface.
- a second light-absorbing layer 34 for selectively absorbing the short wavelength light B is established in the light path from the multilayered film 22 to the first light-absorbing layer 14 .
- the photoreceiving device 30 in this example comprises an InP substrate 32 and further comprises an an InGaAsP layer as the second light-absorbing layer 34 , an n-type InP layer 36 as a buffer layer, an InGaAs layer as the first light-absorbing layer 14 , and a p-type InP layer 16 as the contact layer, which are established this order on the first main surface 32 a of the InP substrate 32 .
- the photoreceiving device 30 in this example is a back surface incidence type element.
- a p-type electrode 18 is established on the upper surface of the p-type InP layer 16 and an n-type electrode 20 is established on the upper surface of the n-type InP layer 36 in a separate region from where the InGaAs layer 14 is established (FIG. 2).
- the band gap wavelength of the InGaAsP layer 34 is 1.4 ⁇ m.
- the 1.55 ⁇ m wavelength light A is transmitted and the 1.3 ⁇ m wavelength light B is absorbed by this layer 34 .
- the 1.3 ⁇ m wavelength light B is reflected to a certain extent by the multilayered film 22 and then the 1.3 ⁇ m wavelength light b that is transmitted without being reflected is absorbed by the second light-absorbing layer 34 , that has the property of transmitting the 1.55 ⁇ m wavelength light A while absorbing the 1.3 ⁇ m wavelength light B. Accordingly, after the 1.3 ⁇ m wavelength light B and b are removed by the multilayered film 22 and the second light-absorbing layer 34 , only the 1.55 ⁇ m wavelength light A is absorbed by the first light-absorbing layer 14 .
- the photoreceiving device 30 is designed to have a property that the intensity selection ratio of the 1.3 ⁇ m wavelength light B to the 1.55 ⁇ m wavelength light A becomes ⁇ 27 to ⁇ 33 dB, for example.
- the thickness of each layer and the number of layers constituting the multilayered film 22 are determined so that the abovementioned selection ratio becomes ⁇ 20 dB in the multilayered film 22 .
- the method for determining the thickness of each layer and the number of layers is the same as that explained in the first embodiment.
- the light A and the light b that have passed through the multilayered film pass through the InP substrate 32 and reach the InGaAsP layer 34 .
- the residual light b is absorbed by this InGaAsP layer 34 while only the 1.55 ⁇ m wavelength light A is transmitted.
- the 1.55 ⁇ m wavelength light A that has reached the InGaAs layer 14 is absorbed by this layer 14 , undergoes opto-electric conversion, and is extracted as an electrical signal from the p-type electrode 18 and the n-type electrode 20 .
- the 1.55 ⁇ m wavelength light A can be selected at the preferred selection ratio and received by the actions of both the multilayered film 22 and the second light-absorbing layer 34 .
- the thickness of these films (layers) must be as thick as strain is produced in the films or the properties are deteriorated. In this embodiment, however, this is not necessary. Consequently, a photoreceiving device that is inexpensive and has good properties can be obtained.
- FIGS. 3 through 5 show alternative examples of the constitution of the photoreceiving device according to the second embodiment.
- FIG. 3 is an example of the constitution of the present invention applied to a top surface incidence type photoreceiving device 40 .
- FIGS. 4 and 5 are examples of the constitution of the present invention applied to end surface incidence type photoreceiving devices 50 and 60 . These figures all show cross sectional views of the constitution of the photoreceiving devices.
- the photoreceiving device shown in FIG. 3 has the following layers established in this order on the first main surface 42 a of the n-type InP substrate 42 : an InGaAs layer that is the first light-absorbing layer 14 , a p-type InP layer 16 , an InGaAsP layer that is the second light-absorbing layer 34 , and the multilayered film 22 .
- An n-type electrode 20 is established on the second main surface 42 b of the n-type InP substrate 42 and a p-type electrode 18 is established on the p-type InP layer 16 in a region separate from where the InGaAsP layer 34 is established (FIG. 3).
- the photoreceiving surface 40 a of this photoreceiving device 40 is the surface 34 a that is opposite to the surface 34 b on the substrate side of the InGaAsP layer 34 .
- the photoreceiving device 50 shown in FIG. 4 has the following layers established in this order on the first main surface 32 a of the InP substrate 32 : an InGaAsP layer that is the second light-absorbing layer 34 , an n-type InP layer 36 , an InGaAs layer that is the first light-absorbing layer 14 , and a p-type InP layer 16 .
- a p-type electrode 18 is established on the p-type InP layer 16 and an n-type electrode 20 is established on the n-type InP layer 36 in a region separate from where the InGaAs layer 14 is established.
- a multilayered film 22 is established on one end 52 a of the laminated body 52 composed of the InP substrate 32 , InGaAsP layer 34 , and an n-type InP layer 36 . Furthermore, a V-shaped groove 54 is formed in the second main surface 32 b side of the InP substrate 32 .
- This V-shaped groove 54 is designed such that the passage of light is directed to the second light-absorbing layer 34 , by reflecting light with the mesa surface 56 of the groove 54 when light incident from the end surface 52 a passes through the substrate 32 . It is preferable that this V-shaped groove 54 be established so as to be parallel to the end surface 52 a. This V-shaped groove is formed by etching the second main surface 32 b side of the InP substrate 32 .
- the photoreceiving device 60 in FIG. 5 is also an end surface incidence type element.
- the constitution of the first main surface 32 a of the InP substrate 32 is the same as the device 50 in FIG. 4. Specifically, the following are established in this order on the first main surface 32 a of the InP substrate 32 : an InGaAsP layer that is the second light-absorbing layer 34 , an n-type InP layer 36 , an InGaAs layer that is the first light-absorbing layer 14 , and a p-type InP layer 16 .
- a p-type electrode 18 is established on the p-type InP layer 16 and an n-type electrode 20 is established on the n-type InP layer 36 in a region separate from where the InGaAs layer 14 is established (FIG. 5).
- part of the corner including the angle at which the second main surface 32 b and end surface 32 x of the InP substrate 32 intersect, is formed obliquely.
- This mesa surface 32 y is an inclined surface with respect to the second main surface 32 b and the end surface 32 x, and the angle of this mesa surface 32 y to the incoming light is determined such that the light incident on or entering the mesa surface 32 y is refracted by this mesa surface 32 y and the refracted light enters the second light-absorbing layer 34 without being entirely reflected.
- this mesa surface 32 y is formed by cleavage, scribing, dicing, or etching near the peak of this V-shaped groove. Part of the surface of this V-shaped groove attained by cleavage or the like becomes the mesa surface 32 y.
- FIG. 2 shows the constitution of the semiconductor photoreceiving device
- FIG. 6 shows the constitution of the multilayered film designed for this embodiment
- FIG. 7 shows the transmittance properties of the multilayered film in FIG. 6 in the 1.20 ⁇ m to 1.60 ⁇ m wavelength band.
- the multilayered film 22 used in this photoreceiving device 30 comprises Si layers 24 and SiO layers 26 which are stacked alternately (see FIG. 2).
- the thickness of the layers and the number of layers are determined on the basis of the method explained above so that the selection ratio of the 1.3 ⁇ m wavelength light B to the 1.55 ⁇ m wavelength light A becomes about ⁇ 20 dB.
- the multilayered film 22 that was designed comprises 10 layers in the following order from the second main surface 32 b side of the InP substrate 32 : a first Si layer 24 a with a thickness of 290.68 nm, a first SiO layer 26 a with a thickness of 475.92 nm, a second Si layer 24 b with a thickness of 82.64 nm, a second SiO layer 26 b with a thickness of 521.98 nm, a third Si layer 24 c with a thickness of 286.07 nm, a third SiO layer 26 c with a thickness of 535.77 nm, a fourth Si layer 24 d with a thickness of 280.45 nm, a fourth SiO layer 26 d with a thickness of 174.58 nm, a fifth Si layer 24 e with a thickness of 262.76 nm, and a fifth SiO layer 26 e with a thickness of 323.50 nm (FI
- FIG. 7 shows the spectral properties of the light passing through this multilayered film 22 .
- the transmittance of the multilayered film 22 for the 1.3 ⁇ m wavelength light B was 0.898% while the transmittance for the 1.55 ⁇ m wavelength light A was 99.990% (FIG. 7).
- the photoreceiving device 30 have the property that the selection ratio of the 1.3 ⁇ m wavelength light B to the 1.55 ⁇ m wavelength light A, when absorbed by the first light-absorbing layer 14 , becomes ⁇ 30 dB. For this reason, a second light-absorbing layer 34 of InGaAsP with a band gap wavelength of 1.4 ⁇ m is established (FIG. 2). Because the selection ratio of ⁇ 20 dB is obtained in the multilayered film 22 , the thickness of the InGaAsP layer 34 may be 2.6 ⁇ m in order that the selection ratio in the second light-absorbing layer 34 becomes ⁇ 30 dB.
- the thickness of the multilayered film 22 is 3.2 ⁇ m in all and the thickness of the InGaAsP layer 34 is 2.6 ⁇ m.
- the multilayered film or the second light-absorbing layer must be much thicker than the abovementioned thicknesses (3.2 ⁇ m or 2.6 ⁇ m). In this example, however, because the ⁇ 30 dB selection ratio may be attained with the multilayered film 22 and the second light-absorbing layer 34 together, the thicknesses may be thinner than in the conventional case.
- the InGaAsP layer 34 formed by epitaxial growth, may also be thin. Accordingly, a photoreceiving device that is inexpensive but has stable properties can be obtained.
- the InGaAsP layer must have a thickness of 8.5 ⁇ m in order to achieve a ⁇ 30 dB selection ratio of the 1.3 ⁇ m wavelength light to the 1.55 ⁇ m wavelength light.
- This 8.5 ⁇ m thickness will be a factor to increase the cost of the photoreceiving device and is also be a factor to cause film separation and deterioration of the properties because of the high film stress.
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Abstract
Description
- This application is a counterpart application of Japanese application Serial Number 212945/2000, filed Jul. 13, 2000, the subject matter of which is incorporated herein by reference.
- 1. Field of the Invention
- The present invention relates to a semiconductor photoreceiving device that is suitable for use in optical communications and performs opto-electric conversion of light at high speeds, and more particularly to a semiconductor photoreceiving device that can selectively extract a signal of long wavelength light in multiplexed optical communications (especially with two wavelengths).
- 2. Description of Related Art
- In general, light of wavelengths 1.3 μm and 1.55 μm is used as the optical signal in optical communications, especially flat mounted optical modules. In optical integrated circuits, this 1.3 μm and 1.55 μm optical signal is present as multiplexed light. Accordingly, it is necessary that the photoreceiving device be an element that can selectively receive both 1.3 μm optical signals and 1.55 μm optical signals.
- Conventionally, the photoreceiving devices that selectively receive optical signals with wavelengths of 1.3 μm (hereinafter referred to as short wavelength) are provided with a light-absorbing layer composed of InGaAsP with a band gap wavelength of about 1.4 μm. However, the light-absorbing layer generally has the property of absorbing light with wavelengths shorter than the band gap wavelength of the light-absorbing layer. Accordingly, it is very difficult to form a light-absorbing layer that can receive only an optical signal of 1.55 μm (hereinafter referred to as long wavelength) in a single layer.
- Consequently, the method of interposing an optical filter between the multiplexed light entering the photoreceiving device and the photoreceiving surface of the photoreceiving device has been used for the selective reception of long wavelength optical signals, as disclosed in the Reference 1 (Ishigami et al., “Automatic Machine For Bonding Fiber Block To Planar Lightwave Circuit”, 1998 Institute of Electronics, Information and Communication Engineers, Electronics Society Conference C-3-87), Reference 2 (Hashimoto et al., “1.3/1.55 μm WDM optical module for full duplex operation using PLC platform”, 1998 Institute of Electronics, Information and Communication Engineers, Electronics Society Conference C-3-110), and Reference 3 (Maeda et al., “WDM by multilayered dielectric filter on silica based waveguide (3)”, 1998 Institute of Electronics, Information and Communication Engineers, Electronics Society Conference C-3-150).
- As another method for the selective reception of long wavelength optical signals, the inventors of the present invention previously proposed a semiconductor photoreceiving device disclosed in Reference 4 (Japanese Unexamined Patent Publication No. 2000-77702). The semiconductor photoreceiving device in Reference 4 comprises a first light-absorbing layer and a second light-absorbing layer in that order within an optical path for multiplexed light; wherein this first light-absorbing layer is composed of a material with a band gap wavelength longer than 1.3 μm and shorter than 1.55 μm (for example, InGaAsP), and the second light-absorbing layer is composed of a material having a band gap wavelength longer than 1.55 μm (for example, InGaAs). Shorter wavelength light is thereby absorbed by the first light-absorbing layer and long wavelength light that passes through this first light-absorbing layer is absorbed by the second light-absorbing layer.
- However, in the case of using an optical filter with the object of selectively receiving long wavelength light, it becomes necessary to perform a process of making a recess on the waveguide of the optical integrated circuit (PLC: planar lightwave circuit) in order to insert the optical filter. This results in a high insertion loss for the optical waveguide, increases PLC processing costs, and results in relatively high part costs for the optical filter.
- In a photoreceiving device comprising a first light-absorbing layer and a second light-absorbing layer, the first light-absorbing layer must be thick so that the selection ratio of short wavelength light to long wavelength light is the desirable selection ratio for the photoreceiving device. As a result, there is high stress between the first light-absorbing layer and the layers formed on top of the first light-absorbing layer, and there is a risk of strain occurring in each layer formed on top of the first light-absorbing layer. Also, the first light-absorbing layer is formed by epitaxial growth; the cost of the photoreceiving device increases in proportion to the thickness of the epitaxial layer.
- It is an object of the present invention to provide a photoreceiving device used in multiplexed optical communications including short wavelength light and long wavelength light for selectively receiving long wavelength light, that is inexpensive and has good properties, without cutting away the PLC waveguide and inserting an optical filter.
- In order to achieve this object, the present invention is to provide a semiconductor photoreceiving device having the following constitution for selectively receiving long wavelength light from multiplexed light including long wavelength light and short wavelength light. Specifically, this semiconductor photoreceiving device comprises a multilayered film of alternately stacked layers of materials having mutually different indexes of refraction. The thickness of each layer and the number of layers in the multilayered film are designed such that long wavelength light is transmitted and short wavelength light is reflected by the multilayered film. The photoreceiving device further comprises a first light-absorbing layer that is composed of a material having a band gap wavelength longer than the long wavelength light. Also, the photoreceiving device has a structure such that multiplexed light enters the first light-absorbing layer through the multilayered film.
- When multiplexed light comprising long wavelength light and short wavelength light enters this multilayered film, the short wavelength light is reflected by the multilayered film and the long wavelength light passes through the multilayered film and reaches the light-absorbing layer. The long wavelength light can thereby be selectively absorbed, or received, by the light-absorbing layer. Therefore, it is unnecessary to insert a conventional optical filter requiring a cutting operation, between the photoreceiving device and the incoming multiplexed light. Consequently, problems arising from establishing the optical filter (PLC processing costs, optical filter costs, optical waveguide insertion loss) are avoided.
- This type of semiconductor photoreceiving device preferably comprises a substrate having a first main surface and a second main surface; the first light-absorbing layer may be established on the first main surface side of the substrate and the multilayered film may be established on the second main surface side of the substrate.
- When the photoreceiving surface for the multiplexed light is assumed to be the second main surface side of the substrate, and the first main surface of the substrate is referred to as the top surface, while the second main surface is referred to as the back surface, the semiconductor photoreceiving device having this type of constitution is referred to as a back surface incidence (or entry) type photoreceiving device.
- The semiconductor photoreceiving device may also be constituted such that the substrate has a first main surface and the multilayered film is established on the first main surface side of the substrate with the first light-absorbing layer interposed therebetween.
- A photoreceiving device with such a constitution is referred to as a top surface incidence (or entry) type photoreceiving device in contrast to the abovementioned back surface incidence type photoreceiving device.
- In these back surface incidence type and top surface incidence type photoreceiving devices, multiplexed light including long wavelength light and short wavelength light first enters the multilayered film and then the short wavelength light is reflected by this multilayered film. After that, the long wavelength light passes through the multilayered film, passes through the substrate, reaches the first light-absorbing layer, and is absorbed (received) by this first light-absorbing layer.
- The top surface incidence type and back surface incidence type photoreceiving devices are suitable for use in the case of incident light spread over a broad range, such as in monitor photodiodes (MPD), for example, because the photoreceiving surface can be made as large as the chip size.
- The constitution of the semiconductor photoreceiving device is preferably provided a substrate having a first main surface and a side surface. The first light-absorbing layer may be established on the first main surface side of the substrate and the multilayered film may be established on the side surface of the substrate. Furthermore, a mesa surface is preferably established on the substrate so that light passing through the multilayered film is reflected towards the first light-absorbing layer.
- A photoreceiving device with such a constitution is called the end surface incidence (or entry) type. The end surface incidence type device is able to operate at higher speeds than the top surface or back surface incidence type devices. Because a mesa surface is established on the substrate, light passing through the multilayered film and entering (or impinging on or arriving at) the substrate is reflected by the mesa surface and this reflected light enters the second light-absorbing layer from the first main surface of the substrate. The short wavelength light in the multiplexed light is thereby reflected by the multilayered film. After this, only the long wavelength light is absorbed by the first light-absorbing layer.
- The semiconductor photoreceiving devices according to the present invention may also be provided with a substrate having a first main surface, and may be constituted so that the first light-absorbing layer is established on this first main surface side and the multilayered film is disposed so that the light passing through the multilayered film is refracted and is incident on or enters the first light-absorbing layer. This type of constitution can be given as a variation of the end surface incidence type discussed above. A V-shaped groove is formed in the second main surface of the substrate by wet etching and an end surface comprising the mesa surface of the V-shaped groove is formed by cleavage or the like (for example, scribing, dicing, etching) near the peak of this V-shaped groove. This end surface becomes the photoreceiving surface and the multilayered film is established thereon. The short wavelength light in the multiplexed light entering the multilayered film is thereby reflected by the multilayered film. The light passing through the multilayered film is refracted by the end surface and passes through the substrate to reach the first light-absorbing layer. After this, the long wavelength light is absorbed by the first light-absorbing layer.
- A semiconductor photoreceiving device having the constitution discussed above preferably further comprises a second light-absorbing layer for selectively absorbing short wavelength light from the multiplexed light. This second light-absorbing layer may be established at a position such that the light passing through the multilayered film enters the first light-absorbing layer through the second light-absorbing layer.
- The second light-absorbing layer is preferably composed of a material having a band gap wavelength longer than the short wavelength light and shorter than the long wavelength light.
- It is necessary to increase the thickness of the multilayered film in order to have a selection ratio of short wavelength light to long wavelength light of about −30 dB, for example, in order to further improve the properties of the photoreceiving device. However, when the multilayered film becomes too thick, strain occurs due to the stress on the film. As a result, there is a risk of the film separating or its properties deteriorating, causing increased current leakage or a reduced transmission rate. A multilayered film therefore should be formed into a thickness such that there is no such risk of its properties deteriorating and a second light-absorbing layer is established in the light path through which the light passing through the multilayered film reaches the first light-absorbing layer. This second light-absorbing layer has a band gap wavelength longer than the short wavelength light and shorter than the long wavelength light, and therefore the short wavelength light that is not reflected by the multilayered film can be absorbed by this layer. Meanwhile, the long wavelength light passes through this second light-absorbing layer and reaches the first light-absorbing layer.
- Such a photoreceiving device can be caused to selectively intercept long wavelength light at the preferred intensity selection ratio by the actions of both the multilayered film and the second light-absorbing film that selectively absorbs short wavelength light. Accordingly, it is not necessary for either the multilayered film or the second light-absorbing layer to be thick. The risk of the strain of each layer is thereby eliminated and cost reductions for the photoreceiving device can be achieved.
- The foregoing and other objects, features and advantages of the present invention will be better understood from the following description taken in connection with the accompanying drawings, in which:
- FIG. 1 is a cross sectional view showing the schematic constitution of the semiconductor photoreceiving device according to the first embodiment;
- FIG. 2 is a cross sectional view showing the schematic constitution of the semiconductor photoreceiving device according to the second embodiment;
- FIG. 3 is a cross sectional view showing the constitution of a first variation of the second embodiment;
- FIG. 4 is a cross sectional view showing the constitution of a second variation of the second embodiment;
- FIG. 5 is a cross sectional view showing the constitution of a third variation of the second embodiment;
- FIG. 6 is a schematic view showing the constitution of the multilayered film designed for the embodiments of the present invention; and
- FIG. 7 shows the transmittance of the multilayered film according to the embodiments.
- The embodiments of the present invention will be explained below with reference to the drawings. These drawings merely have the purpose of showing the forms, sizes, and positional relationships of various components in order that the invention be understood. Consequently, the present invention is in no way limited by these drawings.
- The constitution of the semiconductor photoreceiving device according to the first embodiment of the present invention will be explained below with reference to FIG. 1. FIG. 1 is a cross sectional view showing the schematic constitution of the semiconductor photoreceiving device.
- The
semiconductor photoreceiving device 10 is used in multiplexed optical communications including the long wavelength light A and short wavelength light B. Thissemiconductor photoreceiving device 10 selectively intercepts the long wavelength light A from the multiplexed light incident on (or entering or impinging on or arriving at) thephotoreceiving surface 10 a. Thisphotoreceiving device 10 comprises, at least, asubstrate 12 and a first light-absorbinglayer 14 established on the firstmain surface 12 a side of thesubstrate 12 and composed of a material having a band gap wavelength longer than the long wavelength light A. - In this example, multiplexed light comprises long wavelength light A with a wavelength of 1.55 μm and short wavelength light B with a wavelength of 1.3 μm. The
photoreceiving device 10 comprises an n-type InP substrate 12 and an InGaAs layer, as the first light-absorbinglayer 14, established on the upper surface, or firstmain surface 12 a, of this n-type InP substrate 12. TheInGaAs layer 14 has a band gap wavelength of 1.7 μm, and therefore absorbs both the 1.55 μm wavelength light A and the 1.3 μm wavelength light B. In thisphotoreceiving device 10, a p-type InP layer 16 is established as a contact layer on the upper surface of theInGaAs layer 14. A p-type electrode 18 is established on the upper surface of this p-type InP layer 16. Furthermore, an n-type electrode 20 is established in a region separate from the region where theInGaAs layer 14 is established on the firstmain surface 12 a of the n-type InP substrate 12. The optical signal absorbed by the first light-absorbing layer (InGaAs layer) 14 undergoes opto-electric conversion and is extracted as an electrical signal from the p-type electrode 18 and n-type electrode 20 (FIG. 1). - In the example shown in FIG. 1, the photoreceiving device is a back surface incident type element. In other words, the
photoreceiving surface 10 a of thephotoreceiving device 10 is the secondmain surface 12 b (back surface) side of thesubstrate 12. Amultilayered film 22, formed of stacked layers of materials with mutually different indexes of refraction laminated together, is established on thephotoreceiving surface 10 a. Thismultilayered film 22 is amultilayered film 22 wherein the thickness of each layer and the number of layers are designed so that the long wavelength light A is transmitted and short wavelength light B is refracted (FIG. 1). - In this example, the
multilayered film 22 is a film comprising Si layers 24 with a high index of refraction (n=3.5) and SiO layers 26 with a low index of refraction (n=1.7 to 2.0), which are stacked alternately. Otherwise, the combination of materials comprising themultilayered film 22 may be selected from among combinations of cryolite (fluoride of Na and Al: Na3AlF6 (n=1.35)) and ZnS (n=2.3), SiO2 (n=1.46) and TiO2 (n=2.3), Al2O3 (n=1.7) and Si (n=3.5), SiO2 and Al2O3, and SiO2 and Si. - The thickness of each layer and the number of layers in the
multilayered film 22 are determined on the basis of the conventional optical computation method for the multilayered film used in optical coatings, with consideration of the intensity selection ratio of the short wavelength light B to the long wavelength light A. The reflectance of the multilayered film is as disclosed in the Reference 5 (Yoshida, “Applied Physics and Optics Selection 3, Thin Films”, Baifukan, 1997, pp. 173-174). Based on a method using the effective Fresnel coefficient in this Reference 5, a program is prepared to determine the thickness of each layer and the number of layers according to the desired reflectance. The necessary settings and conditions, such as the desired reflectance, the index of refraction of the materials constituting the layers, and the wavelengths used are added to this program and the thickness of each layer and the number of layers in the multilayered film are determined by calculations using a computer. Moreover, the abovementioned selection ratio in themultilayered film 22 is optimally within a range of −27 to −33 dB. - Due to the use of such a
multilayered film 22, the 1.55 μm wavelength light A can be transmitted and the 1.3 μm wavelength light B can be reflected. - When multiplexed light composed of the 1.55 μm wavelength light A and the 1.3 μm wavelength light B enters the
photoreceiving device 10 according to the present embodiment, the 1.3 μm wavelength light B is reflected and the 1.55 μm wavelength light A is transmitted by themultilayered film 22. Afterwards, the 1.55 μm wavelength light A that has passed through the n-type InP substrate 12 enters theInGaAs layer 14. The 1.55 μm wavelength light A is absorbed by thisInGaAs layer 14, and undergoes opto-electric conversion and is extracted as an electrical signal from the p-type electrode 18 and the n-type electrode 20 (FIG. 1). - In this way, the semiconductor photoreceiving device according to the present invention allows the reception of only the long wavelength light A without cutting away the PLC waveguide and establishing an optical filter between the photoreceiving device and the incoming light.
- The constitution of the semiconductor photoreceiving device according to the second embodiment of the present invention will be explained next with reference to FIG. 2. FIG. 2 is a cross sectional view of the constitution of the semiconductor photoreceiving device according to the second embodiment.
- Like the first embodiment, the
semiconductor photoreceiving device 30 relating to the present embodiment is aphotoreceiving device 30 used in multiplexed optical communications, using multiplexed light comprising 1.55 μm wavelength light as the long wavelength light A and 1.3 μm wavelength light as the short wavelength light B, and selectively intercepts the long wavelength light A. Like the first embodiment, the photoreceiving device comprises at least asubstrate 32 and a first light-absorbinglayer 14 established on the firstmain surface side 32 a of thesubstrate 32. This first light-absorbinglayer 14 is composed of a material having a band gap wavelength longer than the long wavelength light A. Thephotoreceiving surface 30 a of thisphotoreceiving device 30 is the secondmain surface 32 b of thesubstrate 32; the same type ofmultilayered film 22 as in the first embodiment is formed on that surface. In the present embodiment, in particular, a second light-absorbinglayer 34 for selectively absorbing the short wavelength light B is established in the light path from themultilayered film 22 to the first light-absorbinglayer 14. - For this reason, the
photoreceiving device 30 in this example comprises anInP substrate 32 and further comprises an an InGaAsP layer as the second light-absorbinglayer 34, an n-type InP layer 36 as a buffer layer, an InGaAs layer as the first light-absorbinglayer 14, and a p-type InP layer 16 as the contact layer, which are established this order on the firstmain surface 32 a of theInP substrate 32. As already explained, because the same type ofmultilayered film 22 as in the first embodiment is established on the secondmain surface 32 b side of theInP substrate 32, thephotoreceiving device 30 in this example is a back surface incidence type element. Also, a p-type electrode 18 is established on the upper surface of the p-type InP layer 16 and an n-type electrode 20 is established on the upper surface of the n-type InP layer 36 in a separate region from where theInGaAs layer 14 is established (FIG. 2). - In the
photoreceiving device 30 with this type of constitution, the band gap wavelength of theInGaAsP layer 34 is 1.4 μm. As a result, the 1.55 μm wavelength light A is transmitted and the 1.3 μm wavelength light B is absorbed by thislayer 34. - In the
photoreceiving device 30 according to the present embodiment, the 1.3 μm wavelength light B is reflected to a certain extent by themultilayered film 22 and then the 1.3 μm wavelength light b that is transmitted without being reflected is absorbed by the second light-absorbinglayer 34, that has the property of transmitting the 1.55 μm wavelength light A while absorbing the 1.3 μm wavelength light B. Accordingly, after the 1.3 μm wavelength light B and b are removed by themultilayered film 22 and the second light-absorbinglayer 34, only the 1.55 μm wavelength light A is absorbed by the first light-absorbinglayer 14. - In the present embodiment, the
photoreceiving device 30 is designed to have a property that the intensity selection ratio of the 1.3 μm wavelength light B to the 1.55 μm wavelength light A becomes −27 to −33 dB, for example. In this example, the thickness of each layer and the number of layers constituting themultilayered film 22 are determined so that the abovementioned selection ratio becomes −20 dB in themultilayered film 22. The method for determining the thickness of each layer and the number of layers is the same as that explained in the first embodiment. - When multiplexed light composed of 1.55 μm wavelength light A and 1.3 μm wavelength light B enters this type of
photoreceiving device 30, the 1.3 μm wavelength light B is reflected and the 1.55 μm wavelength light A is transmitted by thismultilayered film 22. In thismultilayered film 22, the selection ratio of the 1.55 μm wavelength light A to the 1.3 μm wavelength light B is about −20 dB, and therefore a small amount of 1.3 μm wavelength light b passes through themultilayered film 22. This 1.3 μm wavelength light b is called the residual light b. The light A and the light b that have passed through the multilayered film pass through theInP substrate 32 and reach theInGaAsP layer 34. The residual light b is absorbed by thisInGaAsP layer 34 while only the 1.55 μm wavelength light A is transmitted. Afterwards, the 1.55 μm wavelength light A that has reached theInGaAs layer 14 is absorbed by thislayer 14, undergoes opto-electric conversion, and is extracted as an electrical signal from the p-type electrode 18 and the n-type electrode 20. - As a result, in the present embodiment, the 1.55 μm wavelength light A can be selected at the preferred selection ratio and received by the actions of both the
multilayered film 22 and the second light-absorbinglayer 34. For this reason, in order to obtain a photoreceiving device having a selection ratio of about −30 dB, if only the multilayered film or only the second light-absorbing layer is established in the photoreceiving device, the thickness of these films (layers) must be as thick as strain is produced in the films or the properties are deteriorated. In this embodiment, however, this is not necessary. Consequently, a photoreceiving device that is inexpensive and has good properties can be obtained. - FIGS. 3 through 5 show alternative examples of the constitution of the photoreceiving device according to the second embodiment.
- FIG. 3 is an example of the constitution of the present invention applied to a top surface incidence
type photoreceiving device 40. FIGS. 4 and 5 are examples of the constitution of the present invention applied to end surface incidence 50 and 60. These figures all show cross sectional views of the constitution of the photoreceiving devices.type photoreceiving devices - The photoreceiving device shown in FIG. 3 has the following layers established in this order on the first
main surface 42 a of the n-type InP substrate 42: an InGaAs layer that is the first light-absorbinglayer 14, a p-type InP layer 16, an InGaAsP layer that is the second light-absorbinglayer 34, and themultilayered film 22. An n-type electrode 20 is established on the secondmain surface 42 b of the n-type InP substrate 42 and a p-type electrode 18 is established on the p-type InP layer 16 in a region separate from where theInGaAsP layer 34 is established (FIG. 3). - The
photoreceiving surface 40 a of thisphotoreceiving device 40 is thesurface 34 a that is opposite to thesurface 34 b on the substrate side of theInGaAsP layer 34. - The
photoreceiving device 50 shown in FIG. 4 has the following layers established in this order on the firstmain surface 32 a of the InP substrate 32: an InGaAsP layer that is the second light-absorbinglayer 34, an n-type InP layer 36, an InGaAs layer that is the first light-absorbinglayer 14, and a p-type InP layer 16. A p-type electrode 18 is established on the p-type InP layer 16 and an n-type electrode 20 is established on the n-type InP layer 36 in a region separate from where theInGaAs layer 14 is established. Amultilayered film 22 is established on oneend 52 a of thelaminated body 52 composed of theInP substrate 32,InGaAsP layer 34, and an n-type InP layer 36. Furthermore, a V-shapedgroove 54 is formed in the secondmain surface 32 b side of theInP substrate 32. This V-shapedgroove 54 is designed such that the passage of light is directed to the second light-absorbinglayer 34, by reflecting light with themesa surface 56 of thegroove 54 when light incident from theend surface 52 a passes through thesubstrate 32. It is preferable that this V-shapedgroove 54 be established so as to be parallel to theend surface 52 a. This V-shaped groove is formed by etching the secondmain surface 32 b side of theInP substrate 32. - The
photoreceiving device 60 in FIG. 5 is also an end surface incidence type element. The constitution of the firstmain surface 32 a of theInP substrate 32 is the same as thedevice 50 in FIG. 4. Specifically, the following are established in this order on the firstmain surface 32 a of the InP substrate 32: an InGaAsP layer that is the second light-absorbinglayer 34, an n-type InP layer 36, an InGaAs layer that is the first light-absorbinglayer 14, and a p-type InP layer 16. A p-type electrode 18 is established on the p-type InP layer 16 and an n-type electrode 20 is established on the n-type InP layer 36 in a region separate from where theInGaAs layer 14 is established (FIG. 5). In this constitution, part of the corner, including the angle at which the secondmain surface 32 b and endsurface 32 x of theInP substrate 32 intersect, is formed obliquely. This mesa surface 32 y is an inclined surface with respect to the secondmain surface 32 b and theend surface 32 x, and the angle of thismesa surface 32 y to the incoming light is determined such that the light incident on or entering themesa surface 32 y is refracted by thismesa surface 32 y and the refracted light enters the second light-absorbinglayer 34 without being entirely reflected. After the formation of the V-shaped groove by wet etching the secondmain surface 32 b of theInP substrate 32, thismesa surface 32 y is formed by cleavage, scribing, dicing, or etching near the peak of this V-shaped groove. Part of the surface of this V-shaped groove attained by cleavage or the like becomes themesa surface 32 y. - The semiconductor photoreceiving devices explained with the second embodiment and with reference to FIGS. 2, 6, and 7 are explained below with a more specific example. FIG. 2 shows the constitution of the semiconductor photoreceiving device, FIG. 6 shows the constitution of the multilayered film designed for this embodiment, and FIG. 7 shows the transmittance properties of the multilayered film in FIG. 6 in the 1.20 μm to 1.60 μm wavelength band.
- The
multilayered film 22 used in thisphotoreceiving device 30 comprises Si layers 24 and SiO layers 26 which are stacked alternately (see FIG. 2). The thickness of the layers and the number of layers are determined on the basis of the method explained above so that the selection ratio of the 1.3 μm wavelength light B to the 1.55 μm wavelength light A becomes about −20 dB. - As a result, the
multilayered film 22 that was designed comprises 10 layers in the following order from the secondmain surface 32 b side of the InP substrate 32: afirst Si layer 24 a with a thickness of 290.68 nm, afirst SiO layer 26 a with a thickness of 475.92 nm, asecond Si layer 24 b with a thickness of 82.64 nm, a second SiO layer 26 b with a thickness of 521.98 nm, athird Si layer 24 c with a thickness of 286.07 nm, athird SiO layer 26 c with a thickness of 535.77 nm, afourth Si layer 24 d with a thickness of 280.45 nm, afourth SiO layer 26 d with a thickness of 174.58 nm, afifth Si layer 24 e with a thickness of 262.76 nm, and afifth SiO layer 26 e with a thickness of 323.50 nm (FIG. 6). The total thickness of thismultilayered film 22 was 3.2 μm. Accordingly, the selection ratio of the 1.3 μm light B to the 1.55 μm light A became −20.47 dB. - FIG. 7 shows the spectral properties of the light passing through this
multilayered film 22. According to FIG. 7, the transmittance of themultilayered film 22 for the 1.3 μm wavelength light B was 0.898% while the transmittance for the 1.55 μm wavelength light A was 99.990% (FIG. 7). - It is also desirable that the
photoreceiving device 30 have the property that the selection ratio of the 1.3 μm wavelength light B to the 1.55 μm wavelength light A, when absorbed by the first light-absorbinglayer 14, becomes −30 dB. For this reason, a second light-absorbinglayer 34 of InGaAsP with a band gap wavelength of 1.4 μm is established (FIG. 2). Because the selection ratio of −20 dB is obtained in themultilayered film 22, the thickness of theInGaAsP layer 34 may be 2.6 μm in order that the selection ratio in the second light-absorbinglayer 34 becomes −30 dB. - Consequently, in this example of the
photoreceiving device 30, the thickness of themultilayered film 22 is 3.2 μm in all and the thickness of theInGaAsP layer 34 is 2.6 μm. In the case of attaining the −30 dB selection ratio with only themultilayered film 22 or only the second light-absorbinglayer 34, the multilayered film or the second light-absorbing layer must be much thicker than the abovementioned thicknesses (3.2 μm or 2.6 μm). In this example, however, because the −30 dB selection ratio may be attained with themultilayered film 22 and the second light-absorbinglayer 34 together, the thicknesses may be thinner than in the conventional case. With such thicknesses, there is no risk of creating strain due to film stress or of the properties deteriorating. Cost reductions are achieved because theInGaAsP layer 34, formed by epitaxial growth, may also be thin. Accordingly, a photoreceiving device that is inexpensive but has stable properties can be obtained. - In the case of using only the InGaAsP layer without the multilayered film in this example, the InGaAsP layer must have a thickness of 8.5 μm in order to achieve a −30 dB selection ratio of the 1.3 μm wavelength light to the 1.55 μm wavelength light. This 8.5 μm thickness will be a factor to increase the cost of the photoreceiving device and is also be a factor to cause film separation and deterioration of the properties because of the high film stress.
- Also, 1.55 μm wavelength light was used as the long wavelength light and 1.3 μm wavelength light was used as the short wavelength light in the embodiments and example discussed above, but the light used in a semiconductor photoreceiving device according to the present invention is not limited to light of these wavelengths.
Claims (20)
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2000212945A JP2002033503A (en) | 2000-07-13 | 2000-07-13 | Semiconductor light receiving element |
| JP212945/2000 | 2000-07-13 | ||
| JP2000-212945 | 2000-07-13 |
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| US20020005524A1 true US20020005524A1 (en) | 2002-01-17 |
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| US09/732,728 Expired - Lifetime US6399968B2 (en) | 2000-07-13 | 2000-12-11 | Semiconductor photoreceiving device |
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Cited By (8)
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| WO2003103060A3 (en) * | 2002-06-04 | 2004-08-19 | Finisar Corp | Wavelength selective detector |
| US20050057671A1 (en) * | 2003-09-17 | 2005-03-17 | Cole Bryan G. | Method to filter EM radiation of certain energies using poly silicon |
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| US20070116333A1 (en) * | 2005-11-18 | 2007-05-24 | Dempski Kelly L | Detection of multiple targets on a plane of interest |
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| US5017986A (en) | 1989-08-28 | 1991-05-21 | At&T Bell Laboratories | Optical device mounting apparatus |
| JP3244205B2 (en) | 1993-06-17 | 2002-01-07 | 信越半導体株式会社 | Semiconductor device |
| JP3449516B2 (en) * | 1996-08-30 | 2003-09-22 | 株式会社リコー | Semiconductor multilayer mirror, semiconductor multilayer antireflection film, surface emitting semiconductor laser, and light receiving element |
| JP2000022276A (en) * | 1998-06-29 | 2000-01-21 | Sony Corp | Semiconductor device, semiconductor light emitting device and semiconductor light receiving device |
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2000
- 2000-07-13 JP JP2000212945A patent/JP2002033503A/en active Pending
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| WO2003103060A3 (en) * | 2002-06-04 | 2004-08-19 | Finisar Corp | Wavelength selective detector |
| US20050057671A1 (en) * | 2003-09-17 | 2005-03-17 | Cole Bryan G. | Method to filter EM radiation of certain energies using poly silicon |
| US20060202297A1 (en) * | 2005-03-14 | 2006-09-14 | Mitsubishi Denki Kabushiki Kaisha | Semiconductor photodetector device |
| US20080191241A1 (en) * | 2005-03-14 | 2008-08-14 | Mitsubishi Denki Kabushiki Kaisha | Semiconductor photodetector device |
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| US20070116333A1 (en) * | 2005-11-18 | 2007-05-24 | Dempski Kelly L | Detection of multiple targets on a plane of interest |
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| CN115036378A (en) * | 2022-04-28 | 2022-09-09 | 南昌大学 | AlInGaN-based single pn junction multicolor detector and signal detection method |
Also Published As
| Publication number | Publication date |
|---|---|
| US6399968B2 (en) | 2002-06-04 |
| JP2002033503A (en) | 2002-01-31 |
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