Optical semiconductor device and method for manufacturing an optical semiconductor device
By incorporating a protective film with an intermediate layer and dielectric multilayer film, the optical semiconductor element maintains low dark current levels under harsh conditions, addressing the issue of increased dark current due to electrode-filter contact.
Patent Information
- Authority / Receiving Office
- JP · JP
- Patent Type
- Applications
- Current Assignee / Owner
- DOWA ELECTRONICS MATERIALS CO LTD
- Filing Date
- 2024-12-18
- Publication Date
- 2026-06-30
AI Technical Summary
Optical semiconductor elements experience a significant increase in dark current under high temperature and high humidity conditions due to the contact between the electrode and optical filter, which is not effectively addressed by existing technologies.
The formation of a protective film containing SiO2 or Si3N4 on the uppermost layer of the optical filter, with an intermediate layer between the uppermost layer and the protective film, and the use of a dielectric multilayer film to cover the entire surface of the optical semiconductor element, including an opening that exposes a part of the electrode.
This configuration significantly reduces the increase in dark current, maintaining low dark current levels even under high temperature and high humidity conditions, with a dark current of 0.185nA or less and a change rate of 3.5 times or less after 24 hours of high-speed accelerated life testing.
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Figure 2026108480000001_ABST
Abstract
Description
Technical Field
[0001] The present invention relates to an optical semiconductor device and a method for manufacturing the optical semiconductor device.
Background Art
[0002] Conventionally, optical semiconductor devices have been used in various applications such as communication applications and sensing applications. In order to select a reception wavelength, multilayer film technology has been developed so far.
[0003] For example, Patent Document 1 discloses a light receiving element for optical communication. In Patent Document 1, in order to selectively receive light in each of the 1,300 nm band and the 1,550 nm band, a technique of forming a filter (multilayer film such as SiO2 / SiN / Al2O3) on the upper surface of a chip is disclosed. The document also proposes electrically separating a semiconductor laminated portion at a boundary portion between adjacent filters by etching or the like.
[0004] In addition, Patent Document 2 describes a technique related to a light receiving element in which an ultraviolet region is cut by a multilayer film filter. In the document, on the incident surface of a semiconductor chip, an optical filter of a dielectric multilayer film is formed entirely across a p-n junction on its upper surface. Further, Patent Document 3 proposes a light receiving element in which a region other than a specific wavelength region is reflected by a multilayer film of Si and SiO2. In addition, Patent Document 4 proposes a specific optical filter that reduces only a part of harmful light in a light emission spectrum emitted by a light emitting element.
Prior Art Documents
Patent Documents
[0005]
Patent Document 1
Patent Document 2
Patent Document 3
Patent Document 4
[0006] In recent years, sensors using light-emitting elements and light-receiving elements that emit light at specific wavelengths have been widely developed as sensing technologies for acquiring information about objects such as people. For such sensor applications, there has been a growing demand for optical semiconductor elements that include light-receiving elements with optical filters to block information other than the specific wavelength, and light-emitting elements that emit only the specific wavelength.
[0007] To maximize the blocking effect of wavelengths other than specific wavelengths, it is necessary to provide an optical filter without gaps on the main surface side that receives or emits light. However, it has been found that when the optical filter is in contact with the electrode, the leakage current (i.e., dark current) of the optical semiconductor element tends to increase significantly when used or stored under high temperature and high humidity conditions. Therefore, the present invention aims to provide an optical semiconductor element in which the electrode and optical filter are in contact, and a method for manufacturing the same, which exhibits a small increase in dark current even under high temperature and high humidity conditions. [Means for solving the problem]
[0008] The inventors of the present invention have diligently studied ways to solve the above problems. As described above, when an optical filter is in contact with an electrode, the dark current of the optical semiconductor element tends to increase significantly when used or stored under high temperature and high humidity conditions. It was necessary to create an optical semiconductor element with an optical filter that could cover the entire upper surface of the optical semiconductor element, which is the surface that receives light or the surface that extracts light, or cover the entire light-receiving area of the optical semiconductor element by spanning the sides of the layer having the light-receiving part or the light-emitting part, while solving such reliability problems. The inventors of the present invention have found that forming a protective film on the uppermost layer of the optical filter and forming an intermediate layer between the uppermost layer of the optical filter and the protective film leads to the suppression of the increase in dark current. In other words, the gist of the present invention is as follows.
[0009] (1) Electrodes and, An optical filter in which at least a portion of the electrode is in contact, An optical semiconductor element comprising, The optical filter includes a dielectric multilayer film. The optical filter has a protective film containing SiO2 or Si3N4 on the uppermost layer, The uppermost layer and the protective film are characterized by having an intermediate layer between them that is observed to be darker than the uppermost layer and the protective film in a cross-sectional TEM image. Optical semiconductor device.
[0010] (2) The optical filter is a laminate containing a Si layer and an SiO2 layer, and the uppermost layer is the SiO2 layer. The optical semiconductor device described in (1) above.
[0011] (3) The intermediate layer contains SiO2 or SiON with oxygen defects, The optical semiconductor device described in (1) above.
[0012] (4) The thickness of the protective film is an integer multiple of the value obtained by dividing the light-receiving wavelength or emission wavelength of the optical semiconductor element by twice the refractive index of the protective film. The optical semiconductor device described in (1) above.
[0013] (5) The optical filter has an opening that exposes a part of the electrode, and the side surface of the opening is covered by the protective film. The optical semiconductor device described in (1) or (2) above.
[0014] (6) An electrode formation step in which electrodes are formed on an optical semiconductor device, An optical filter forming step in which an optical filter including a dielectric multilayer film is formed so as to be in contact with the electrode, A protective film forming step of forming a protective film containing SiO2 or Si3N4 on the uppermost layer of the optical filter, It has, The optical filter formation process uses the sputtering method. The aforementioned protective film formation process uses plasma CVD. A method for manufacturing an optical semiconductor device, characterized in that, in the protective film formation step, an intermediate layer is formed between the uppermost layer and the protective film, which is observed to be darker than the uppermost layer and the protective film in a cross-sectional TEM image.
[0015] (7) The optical filter comprises a laminate of a Si layer and an SiO2 layer, the uppermost layer being an SiO2 layer. A method for manufacturing an optical semiconductor device as described in (6) above.
[0016] (8) The intermediate layer contains SiO2 or SiON with oxygen defects, A method for manufacturing an optical semiconductor device as described in (6) above.
[0017] (9) The thickness of the protective film is an integer multiple of the value obtained by dividing the light-receiving wavelength or emission wavelength of the optical semiconductor element by twice the refractive index of the protective film. A method for manufacturing an optical semiconductor device as described in (6) above.
[0018] (10) The optical filter forming step includes the step of forming an opening that exposes a part of the electrode, and the third step includes covering the side surface of the opening with the protective film. A method for manufacturing an optical semiconductor device as described in (6) above.
[0019] (11) The optical semiconductor device is a photodetector having a photodetector layer made of an InGaAs layer, The dark current when a reverse bias voltage of 5V is applied to the aforementioned optical semiconductor device immediately after fabrication is 0.185nA or less. It is characterized by having a dark current change rate of 3.5 times or less after 24 hours of high-speed accelerated life testing. (1) The optoelectronic semiconductor device described above.
[0020] (12) Electrodes and, An optical filter in which at least a portion of the electrode is in contact, An optical semiconductor element comprising, The optical filter includes a dielectric multilayer film. The optical filter has a protective film containing SiO2 or Si3N4 on the uppermost layer, The optical filter includes a laminate of a Si layer and an SiO2 layer, The average D concentration in the SiO2 layer after 24 hours of high-speed accelerated life testing was 1.5 × 10⁻¹⁶ 21 atom / cm 3 The following are optical semiconductor devices.
[0021] (13) An electrode formation step in which electrodes are formed on an optical semiconductor device, An optical filter forming step in which an optical filter including a dielectric multilayer film of a Si layer and an SiO2 layer is formed so as to be in contact with the electrode, A protective film forming step of forming a protective film containing SiO2 or Si3N4 on the uppermost layer of the optical filter, It has, The optical filter formation process uses the sputtering method. The aforementioned protective film formation process uses plasma CVD. The average D concentration in the SiO2 layer after 24 hours of high-speed accelerated life testing was 1.5 × 10⁻¹⁶ 21 atom / cm 3 A method for manufacturing an optical semiconductor device, characterized by the following: [Effects of the Invention]
[0022] According to the present invention, it is possible to provide an optical semiconductor element in which an electrode and an optical filter are in contact, and a method for manufacturing the optical semiconductor element, in which the dark current does not increase even under high temperature and high humidity conditions. [Brief explanation of the drawing]
[0023] [Figure 1] This is a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention. [Figure 2A] This is a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 1. [Figure 2B] This is a top view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 1. Here, the cross-sectional view in Figure 2A is a schematic cross-sectional view when the semiconductor photodetector Figure 2B is cut along the dotted line. [Figure 3A] This is a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 2A. [Figure 3B] Figure 3A is a top view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 2B. Here, the cross-sectional view in Figure 3A is a schematic cross-sectional view when the semiconductor photodetector Figure 3B is cut along the dotted line. [Figure 4A] This is a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 3A. [Figure 4B] Figure 3B is a top view illustrating part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention. Here, the cross-sectional view in Figure 4A is a schematic cross-sectional view when the semiconductor photodetector in Figure 4B is cut along the dotted line. [Figure 5A] This is a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 4A. [Figure 5B] Figure 4B is a top view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention. Here, the cross-sectional view in Figure 5A is a schematic cross-sectional view when the semiconductor photodetector Figure 5B is cut along the dotted line. [Figure 6A] This is a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 5A. [Figure 6B] Figure 5B is a top view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention. Here, the cross-sectional view in Figure 6A is a schematic cross-sectional view when the semiconductor photodetector Figure 6B is cut along the dotted line. [Figure 7A] This is a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 6A. [Figure 7B] Figure 6B is a top view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention. Here, the cross-sectional view in Figure 7A is a schematic cross-sectional view when the semiconductor photodetector in Figure 7B is cut along the dotted line. [Figure 8A]This is a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention, following Figure 7A. [Figure 8B] Figure 7B is a top view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention. Here, the cross-sectional view in Figure 8A is a schematic cross-sectional view when the semiconductor photodetector Figure 8B is cut along the dotted line. [Figure 9] Figures 8A and 8B follow, illustrating a schematic cross-sectional view illustrating a part of the manufacturing process of a semiconductor photodetector according to one embodiment of the present invention. [Figure 10A] This is a STEM image of Example 1, including the boundary between the 22nd and 23rd layers of the optical filter, and the boundary between the 23rd layer of the optical filter and the protective film. [Figure 10B] This is a magnified TEM image of section A in Figure 10A (the boundary between the 23rd optical filter layer and the protective film). [Figure 11A] This is a STEM image of Example 3, including the boundary between the 22nd and 23rd layers of the optical filter, and the boundary between the 23rd layer of the optical filter and the protective film. [Figure 11B] This is a magnified TEM image of section A in Figure 11A (the boundary between the 23rd optical filter layer and the protective film). [Figure 12A] This is a STEM image of Comparative Example 2, including the boundary between the 22nd and 23rd layers of the optical filter, and the boundary between the 23rd layer of the optical filter and the protective film (continuation of the optical filter). [Figure 12B] This is a magnified TEM image of section A in Figure 12A (the boundary between the 23rd optical filter layer and the protective film (continuation of the optical filter)). [Figure 13A] This is a STEM image of Comparative Example 3, including the boundary between the 22nd and 23rd layers of the optical filter, and the boundary between the 23rd layer of the optical filter and the protective film. [Figure 13B] This is a magnified TEM image of section A in Figure 13A (the boundary between the 23rd optical filter layer and the protective film). [Figure 14] This is a top view of the measurement jig used for measuring the resistivity of the fabricated semiconductor photodetector. [Figure 15]It is a side view of a measurement jig for measuring the resistivity of the fabricated semiconductor light-receiving element.
Embodiments for Carrying Out the Invention
[0024] Prior to the situation of the embodiments according to the present invention, the following points will be explained in advance.
[0025] In this specification, when simply denoted as "InGaAs" without specifying the elemental composition ratio, the composition ratio of the total of group III elements In (indium) and Ga (gallium) and group V element As (arsenic) is 1:1, and the ratio of In and Ga as group III elements means an arbitrary compound, and when represented by In x Ga (1-x) GaAs, it is preferably 0 < x < 1. However, "InGaAs" may contain Al of 5% or less (molar concentration, the same hereinafter) with respect to the total of In and Ga. It may contain P (phosphorus) and Sb (antimony) within 5% with respect to As. Also, in the case of simply denoted as "InP", the composition ratio of group III elements and group V elements can be measured by photoluminescence measurement, X-ray diffraction measurement, etc.
[0026] In this specification, the resistivity of an optical filter after protective film formation is measured using a two-terminal method. The measurement method used in this specification will be described in detail below. Figure 14 shows a top view of the measurement method using the two-terminal method, and Figure 15 shows a side view thereof. First, an optical filter 90 and a protective film 91 are formed on an insulating quartz glass substrate (made of synthetic quartz, 400 μm thick, not shown) in the same manner as the method of lamination on a semiconductor laminate described later. Then, the quartz glass substrate is scribed and cut together with the optical filter 90, which has the protective film 91 in a strip shape with a width L. After that, an Au wire 5 (diameter 20 μm) is brought into contact with the sides of the quartz glass substrate at both ends of the width L, and Ag paste 6 is applied to the entire surface including the sides of the quartz glass substrate and the sides of the optical filter 90 and protective film 91 so as to enclose the Au wire 5. The paste is then heat-treated at 70°C for 2 hours to cure, and a resistivity measurement sample with two electrodes spaced apart by a width L is obtained. Here, the cross-sectional area S of the optical filter 90 and protective film 91 in contact with the electrode (Ag paste 6) is calculated from the length of the strip of the optical filter 90 (e.g., 1000 μm) and the thickness of the optical filter 90 and protective film 91. Then, as shown in Figure 14, an insulating glass plate 3 and an external connection terminal 7 are placed on the glass epoxy substrate 2, and the Au wire 5 is bonded to the glass plate 3 using an insulating adhesive 4, thereby suspending a strip-shaped resistivity measurement sample in the air using the Au wire 5, as shown in Figure 15. The Au wire 5 is connected to the external connection terminal 7, and a Source Measure Unit (SMU) is connected to the external connection terminal 7 to pass current and measure the VI curve. The resistance R of the optical filter 90 is calculated from its slope, and the resistance R (Ω), width L (μm), and cross-sectional area S (μm) are obtained. 2 The resistivity ρ = R × S / L (Ω·μm) is calculated from the value of ). The width L can be, for example, 200 μm. The method for measuring the resistivity of only the optical filter 90 without a protective film is the same.
[0028] In this specification, the light-receiving wavelength of a semiconductor photodetector is determined by spectral sensitivity spectroscopy. In the embodiments described later, a spectral sensitivity spectroscopy device (model: CARY7000) manufactured by Agilent Technologies was used.
[0029] In this specification, the conditions for the high-speed accelerated stress test (HAST) on the chip are 130°C, 85% RH humidity, and 2 atmospheres for 24 hours. The bias voltage is 0V. Furthermore, a special HAST test was performed to determine the extent to which water ingress was prevented, and the presence or absence of H2O ingress was quantitatively confirmed by SIMS (secondary ion mass spectrometry) analysis.
[0030] First, instead of ultrapure water (H2O), heavy water (D2O) is used as the water supplied to the HAST tank. Next, SIMS depth analysis is performed on the optical filter after HAST to quantify (average calculation) the concentration of element D (deuterium) and compare it between each sample. If the total film thickness of the optical filter is 4 μm or less, the entire filter is analyzed; if it exceeds 4 μm, the SIMS depth analysis is performed on the range from the outermost surface of the optical filter to 4 μm, and the average value is calculated. Similarly, the concentration of element H is also evaluated, and the D / H ratio is compared. The H element is thought to be due to the H element (e.g., hydrogen or water) originally present in the optical filter, while the D element is thought to be an element that entered from the outside due to HAST. Since D is a stable isotope, it is assumed that there is no exchange between D and H. Therefore, a large D / H value after HAST indicates that a large amount of D2O entered due to the HAST test.
[0031] In this specification, the presence or absence of an intermediate layer is determined by acquiring STEM (scanning transmission electron microscope) and TEM (transmission electron microscope) images and visually confirming the existence of a layer region that appears darker than the surrounding area using cross-sectional TEM. For example, a Hitachi HD2700 can be used with an acceleration voltage of 200kV, and the STEM image can be a ZC (Z-contrast image). If an intermediate layer is present, its width can also be measured by acquiring a TEM image. The magnification of the STEM image can be set to, for example, 130,000x, and the TEM image can be acquired at a magnification greater than or equal to the magnification of the STEM image. In TEM images, the scattering of transmitted electrons increases as the electron density of the sample increases, in other words, as the atomic number increases, resulting in a darker image. Furthermore, the scattering is weaker and the image brighter as the sample is composed of lighter elements. Therefore, an intermediate layer composed of SiO2 or Si3N4 that appears darker than the surrounding area is expected to be in a state closer to Si than its surroundings. For example, SiO2 with oxygen vacancies that are closer to Si than SiO2 is expected to appear darker. Similarly, silicon with oxygen vacancies closer to silicon than silicon is likely to be observed as darker.
[0032] The embodiments of the invention will be described below with reference to the drawings. In each drawing, for the sake of clarity, the aspect ratios of the substrate and each layer are exaggerated from the actual ratios. Also, the correspondence between each schematic cross-sectional view and the top view does not always coincide due to dimensional constraints, and the ratios are changed in cases where it becomes difficult to distinguish.
[0033] (First Embodiment) In the first embodiment, we will first describe the optical semiconductor element as a semiconductor photodetector 1.
[0034] —Manufacturing method for semiconductor photodetectors— A method for manufacturing a semiconductor photodetector according to the present invention includes at least an electrode formation step, an optical filter formation step, and a protective film formation step. Referring to Figures 1 to 9, a method for manufacturing a semiconductor photodetector 1 according to an embodiment of the present invention, including optional steps, includes a first step (semiconductor laminate formation step), a second step (contact region formation step), a third step (diffusion prevention layer formation step), a fourth step (Zn diffusion step), a fifth step (dielectric layer formation step), a sixth step (electrode formation step), a seventh step (optical filter formation step), an eighth step (protective film formation step), and a ninth step (backside electrode formation step), and a piece formation step (not shown). In Figures 1 to 9, Figures 2A, 2B, etc., indicate that Figure 2B is a top view of the semiconductor photodetector 1 under fabrication, and Figure 2A is a cross-sectional view taken at a cross-section perpendicular to the dotted line in Figure 2B. Hereafter, when simply referred to as Figure 2, etc., it refers to both Figure 2A and Figure 2B. Details of each step will be described below. Note that steps 1 through 9 are processes performed on a substrate where numerous elements, not individualized into separate pieces, are arranged; however, Figures 1 through 9 represent a typical element area on the substrate.
[0035] In the first step, a plurality of compound semiconductor layers, each containing at least a light-receiving layer 20, are stacked on a substrate 10 to form a semiconductor laminate 11. The semiconductor laminate 11 may also include a window layer 30 and a contact layer 40 (Figure 1). In the second step, a predetermined pattern is formed on the contact layer 40 (Figure 2). In the third step, a diffusion prevention layer 50 is formed to create an opening pattern for the Zn diffusion region, which will be described later (Figure 3). In the fourth step, the diffusion prevention layer 50 is used as a mask to diffuse p-type impurities from the surface side of the window layer 30 and the contact layer 40 (Figure 4). The contact layer 40 becomes a p-type contact layer 61, and the interface between the region where the p-type impurities of the semiconductor layer have diffused (p-type region 62) and the p-type impurity non-diffusing region in the light-receiving layer 20 becomes the light-receiving portion 63 (Figure 4A). In the fifth step, a dielectric layer 70 is formed over the entire surface, and a pattern is formed to expose the p-type contact layer 61 (Figure 5A). In the sixth step (electrode formation step), a frame-shaped electrode 81 is formed on the p-type contact layer 61 so as to surround the light-receiving section 63 fabricated above and to be spaced apart from the outer periphery of the semiconductor laminate 11, and a pad electrode 82 is formed to connect to a part of the frame-shaped electrode 81. The frame-shaped electrode 81 and the pad electrode 82 together are referred to as the upper electrode 80 (Figure 6). In the seventh step (optical filter formation step), an optical filter 90 is formed so as to be in contact with at least a part of the upper electrode 80 formed in the sixth step. The optical filter 90 includes a dielectric multilayer film. The optical filter 90 may cover the entire surface of the semiconductor laminate 11 and the frame-shaped electrode 81, except for the upper surface of the pad electrode 82 (Figure 7). In the eighth step (protective film formation step), a protective film 91 containing SiO2 or Si3N4 is formed on the uppermost layer of the optical filter 90 formed in the seventh step. The protective film 91 may be formed on the side surface of the optical filter 90 (Figure 8). The ninth step involves grinding the back surface of the substrate 10 to form back electrodes 100 on the back surface of the substrate 10 for electrical conductivity (Figure 9). The tenth step, although not shown, is a piece-forming step.
[0036] <1st process> As described above, the first step is to stack a plurality of compound semiconductor layers including at least a light-receiving layer 20 on a substrate 10 to form a semiconductor laminate 11 (Fig. 1). As the substrate 10, a growth substrate such as GaAs, InP, or InAs can be used, and an InP growth substrate is preferred. When using a growth substrate, an n-type substrate is preferred. Hereinafter, for the sake of convenience of explanation, an embodiment using an n-type InP growth substrate 10 as the substrate 10 will be described. An n-type InP growth substrate 10 that is generally available can be used, and the thickness only needs to be able to physically support the semiconductor laminate 11 and the optical filter 90 described later.
[0037] In the first step, the light-receiving layer 20, the window layer 30, and the contact layer 40 may be formed on the n-type InP growth substrate 10 in this order. The light-receiving layer 20 is preferably an InGaAs layer. The light-receiving layer 20 may be undoped or n-type, but it is preferably doped so that the average n-type impurity concentration determined by SIMS analysis is 2.5×10 14 / cm 3 or more and 1.0×10 15 / cm 3 or less. Preferably, it is doped to be 3.0×10 14 / cm 3 or more and 9.5×10 14 / cm 3It is more preferable to dope the material as follows: At least one n-type impurity is selected from Si, Ge, Sn, Pb, S, Se, and Te, with Si or Ge being preferred. The thickness of the light-receiving layer 20 is preferably 1.0 μm or more and 5.0 μm or less, and more preferably 2.0 μm or more and 4.0 μm or less. The window layer 30 can be an n-type InP layer, and the contact layer 40 can be an undoped InGaAs layer. The thickness of the window layer 30 is preferably 500 nm or more and 2.0 μm or less. The thickness of the contact layer 40 is preferably 50 nm or more and 200 nm or less, and more preferably 70 nm or more and 150 nm or less. A buffer layer may be provided between the n-type InP growth substrate 10 and the light-receiving layer 20 to eliminate lattice mismatch. The light-receiving layer 20, the window layer 30, the contact layer 40, and any other optional layers together are referred to as a semiconductor laminate 11. The total film thickness of the substrate 10 and the semiconductor laminate 11 is preferably 500 μm or less, and more preferably 400 μm or less. In addition to the layers mentioned above, a first buffer layer, a second buffer layer, or a first contact layer may be formed.
[0038] Here, each layer of the semiconductor described above can be formed by epitaxial growth, for example, by known thin-film growth methods such as metal-organic chemical vapor deposition (MOCVD), molecular beam epitaxy (MBE), or sputtering. For example, by using trimethylindium (TMIn) as the In source, trimethylgallium (TMGa) as the Ga source, and arsine (AsH3) as the As source in a predetermined mixing ratio, and growing these raw material gases in the vapor phase with a carrier gas, each layer can be formed to a desired thickness depending on the growth time. If each layer is to be dopanted into a p-type or n-type, a dopant source gas may be used as desired.
[0039] <Second process> The second step, as described above, is the step of forming a predetermined pattern on the contact layer 40 (Figure 2). By forming a resist pattern on the surface of the contact layer 40, etching the openings, and peeling off the resist, a predetermined pattern can be formed on the contact layer 40. When the contact layer 40 is an InGaAs layer, although not limited to this, for example, H2SO4:H2O2:H2O=1:1:7 can be used as the etching solution. Figure 2B is a top view of Figure 2, but the contact layer 40 does not necessarily have to be closed as a frame, and although it is rectangular except for the openings in Figure 2B, it may be circular or the like. The width of the contact layer 40 is preferably 5 nm to 20 nm, and more preferably 8 nm to 15 nm (see reference numeral 40 in Figure 2B). If it is narrower than this range, sufficient current will not flow to the light-receiving part described later, and if it is wider than this range, the amount of light reaching the light-receiving part will be small. In addition, the size of the inner circumference of the contact layer 40 can be set as appropriate depending on the application. For each application, it is preferable to design it so that sufficient current flows to the light-receiving part described later.
[0040] <3rd process> The third step, as described above, is the step of forming the diffusion prevention layer 50. That is, the step of depositing the diffusion prevention layer 50 on a part of the surface of the window layer 30, which includes the contact layer 40 on the upper surface of Figure 2A (Figure 3). The diffusion prevention layer 50 may be SiO2, SiON, etc., but it is preferably Si3N4. The thickness of the diffusion prevention layer 50 is preferably the same as the thickness of the contact layer 40. The thickness of the diffusion prevention layer 50 is preferably 50 nm to 200 nm, and more preferably 70 nm to 150 nm. The diffusion prevention layer 50 can be deposited by, for example, plasma CVD (Chemical Vapor Deposition). After that, a resist pattern can be formed on the diffusion prevention layer 50, the openings can be etched, and the resist can be peeled off to form a diffusion prevention layer 50 with a predetermined pattern. The etching solution for Si3N4 is BHF (ultra-high purity buffered hydrofluoric acid). It is preferable to form the diffusion prevention layer 50 on the outside of the contact layer 40. The formed diffusion-preventing layer 50 can be used as a mask during the diffusion of p-type impurities in the fourth step.
[0041] <4th process> The fourth step, as described above, is a step in which p-type impurities are diffused from the contact layer 40 and window layer 30 to the light-receiving layer 20, using the mask opening not covered by the diffusion prevention layer 50 as the entry point for diffusion. For example, Zn can be used as the p-type impurity. Since Zn is not easily diffused into the diffusion prevention layer 50 formed in the third step described above, it can be diffused using the MOCVD method from the mask opening not covered by the diffusion prevention layer 50 (window layer 30 and contact layer 40 in Figure 3B). In terms of the diffusion distance in the depth direction, it is preferable to adjust the conditions so that Zn diffuses to a depth of 0.1 μm to 0.5 μm from the interface between the window layer 30 and the light-receiving layer 20 towards the light-receiving layer 20. By diffusing Zn, the contact layer 40 becomes a p-type contact layer 61, and a part of the window layer 30 and the light-receiving layer 20 is p-type. The interface between the region where the p-type impurities have diffused in the semiconductor layer (p-type region 62) and the p-type impurity non-diffusing region in the light-receiving layer 20 is made into a light-receiving section 63 (Figure 4A). This allows for the formation of a semiconductor laminate 11 having a light-receiving portion 63 on an n-type InP growth substrate 10. The p-type contact layer 61, the p-type region 62, and the light-receiving portion 63 together form a Zn diffusion region 60. Here, the size of the inner circumference of the Zn diffusion region, excluding the pad electrode portion 82 described later, can be set appropriately according to the application. Lateral diffusion of Zn after entering through the opening is possible, but for the sake of explanation, when viewed from above (Figure 4B), the p-type region 62 (light-receiving portion 63) will be described as being approximately the same region as the mask opening of the diffusion prevention layer 50 used as a mask during p-type impurity diffusion.
[0042] <5th process> The fifth step, as described above, is the step of forming the dielectric layer 70. That is, the dielectric layer 70 is deposited on the surface including the diffusion prevention layer 50, p-type region 62, and p-type contact layer 61 formed in the fourth step (Figure 5). The dielectric layer 70 is preferably the same Si3N4 as the diffusion prevention layer 50, but it may also be SiO2 or SiON, etc. The thickness of the dielectric layer 70 may be the same as the thickness of the diffusion prevention layer 50, but it is preferable that it be thicker than the diffusion prevention layer 50. The dielectric layer 70 can be deposited, for example, by the plasma CVD (Chemical Vapor Deposition) method. After that, a resist pattern is formed on the dielectric layer 70, the openings are etched, and the resist is peeled off to form a dielectric layer 70 with a predetermined pattern. The etching solution for Si3N4 is BHF. When a dielectric layer 70 with a predetermined pattern is formed and the p-type contact layer 61 is exposed, the width of the opening of the p-type contact layer 61 is preferably 3 μm or more and 10 μm or less, and more preferably 5 μm or more and 8 μm or less (see reference numeral 61 in Figure 5). Furthermore, it is preferable that the p-type contact layer 61 is located in the center of the width of the contact layer 40 formed in the second step. It is also preferable that the Si3N4 on the outer periphery extends to the edge of the semiconductor layer, leaving the diffusion prevention layer 50 in place (Figure 5). In this embodiment, the dielectric layer 70 is formed with the diffusion prevention layer 50 in place, but the diffusion prevention layer 50 may be removed after the fourth step before forming the dielectric layer 70.
[0043] <6th process> The sixth step, as described above, is an electrode formation step in which the upper electrode 80 (frame electrode 81 and pad electrode 82) is formed (Figure 6). In the example shown in Figure 6, since there is a p-type region 63 on the main surface side that receives light, the frame electrode 81 is formed on the p-type contact layer 61, and the pad electrode 82 is formed on a part of the dielectric layer 70 so as to be electrically connected to the frame electrode 81 with a size that allows bonding with the outside. Here, when the light-receiving element 1 is viewed from above from the optical filter side, the frame electrode 81 may cast a shadow and reduce the amount of light reaching the light-receiving part 63, so it is preferable to place it near the outer circumference of the light-receiving part 63. Also, in order to prevent leakage current from traveling along the end face of the element, it is preferable to form the frame electrode 81 so as to be spaced away from the outer circumference of the semiconductor laminate 11. The distance of the frame electrode 81 from the outer circumference of the semiconductor laminate 11 is preferably 25 μm or more and 100 μm or less, and more preferably 30 μm or more and 70 μm or less. Furthermore, similar to the frame electrode 81, it is preferable that the pad electrode 82 be positioned inward so as to be spaced apart from the outer circumference of the semiconductor laminate 11. The shape of the frame electrode 81 depends on the shape of the contact layer 40 formed earlier, and the outer and inner shapes can be any shape, such as rectangular or circular. The pad electrode 82 is formed so as to be connected to a part of the frame electrode 81 (Figure 6B). The frame electrode 81 and the pad electrode 82 may be formed by vapor deposition or sputtering, but it is preferable to form them using EB metal vapor deposition. A predetermined resist pattern (electrode pattern) is formed on the dielectric layer 70 and the p-type contact layer 61, and the dielectric layer 70 at the opening is etched. A metal layer for conductivity is deposited by vapor deposition, and the resist is swollen to remove metal other than the electrode pattern, thereby forming the frame electrode 81 and the pad electrode 82. The frame electrode 81 and the pad electrode 82 can be formed from, for example, Ti, Pt, Au, etc. It is preferable that the frame electrode 81 and the pad electrode 82 are of the same height. The film thickness (or total film thickness) of the frame electrode 81 and the pad electrode 82 is not particularly limited. In the top view of Figure 6, the width of the frame electrode 81 and the diameter of the pad electrode 82 can be adjusted as appropriate depending on the application. The first to sixth steps described above are an example of a manufacturing method for obtaining a photodetector having electrodes on its top surface, and can be modified as appropriate within the range of a manufacturing method that can obtain a photodetector having electrodes on its top surface.
[0044] <7th process> As described above, the seventh step is an optical filter formation step in which an optical filter 90 is formed that is in contact with at least a portion of the upper electrode 80 formed in the sixth step (Figure 7). In this embodiment, the optical filter 90 is formed on the entire surface of the frame electrode 81 and the dielectric layer 70 (on the semiconductor laminate 11), excluding the external connection surface of the pad electrode 82. As shown in Figure 7A, the optical filter 90 is in contact with the upper electrode 80 (frame electrode 81 and pad electrode 82). The optical filter 90 includes a dielectric multilayer film and is formed using the sputtering method. Before forming the optical filter 90, a resist pattern is placed in advance, and a lift-off method is used to remove the resist along with a portion of the optical filter on the resist after film formation to form a predetermined opening in the optical filter 90. Alternatively, after forming the optical filter 90, a resist pattern is formed on the optical filter 90, the pad electrode 82 portion is etched, and the resist is peeled off to form an optical filter 90 having a predetermined opening. These are examples of steps in the optical filter formation step to form an opening that exposes a portion of the upper electrode 80. Since a portion of the surface of the pad electrode 82 is not covered by the optical filter 90 and is required to be exposed to allow for electrical wiring to the outside, the surface of the pad electrode 82 exposed by the opening of the optical filter 90 is called the external connection surface of the pad electrode 82. The reason why the above step is included in the optical filter formation process is to form an external connection surface of the pad electrode 82 that allows for electrical wiring to the outside of the semiconductor photodetector 1.
[0045] The optical filter 90 preferably includes a laminate of a Si layer and an SiO2 layer as a dielectric multilayer film, and the uppermost layer of the optical filter 90 is preferably an SiO2 layer. It is more preferable that the oxygen flow rate during SiO2 layer formation is 100 sccm or more and 500 sccm or less, and even more preferable that it is 100 sccm or more and 300 sccm or less. A dielectric multilayer film may also be formed from laminates of high refractive index, medium refractive index, and low refractive index using layers of materials other than the Si layer and SiO2 layer. When forming the optical filter 90 including the laminate of the Si layer and SiO2 layer, the resistivity of the optical filter 90 is 3.0 × 10⁻⁶. 12 It is preferable to form it to be Ωμm or larger, 3.8 × 10 12 It is more preferable that the thickness be Ωμm or greater. The film thickness of the optical filter 90 is preferably 2500nm to 3500nm, and more preferably 2800nm to 3300nm.
[0046] By changing the deposition rate, which depends on the power supplied to the sputtering target, and the gas flow rate (Ar, O2, H, etc.) used in the sputtering method, it is possible to adjust the resistivity range within a desired range. If adjustment is possible to obtain the desired resistivity, a deposition method such as ion beam-assisted deposition may also be used. Subsequently, a resist pattern is formed on the optical filter 90, the pad electrode 82 portion is etched, and the resist is removed to form an optical filter 90 with a predetermined pattern. The aperture diameter of the optical filter 90 is arbitrary as it depends on the method of connection to the outside of the pad electrode 82, but it is preferably 120 μm or less (Figure 7B).
[0047] <8th process> As described above, the eighth step is a protective film formation step in which a protective film 91 containing SiO2 or Si3N4 is formed on the uppermost layer of the optical filter 90 formed in the seventh step (Figure 8). The protective film 91 is formed using plasma CVD. Here, when forming the protective film 91, it is preferable to form it in a plasma CVD apparatus different from the apparatus used to form the optical filter 90. For example, after forming the optical filter 90 by sputtering, it may be removed from the deposition apparatus and then placed in a plasma CVD deposition apparatus to form the protective film 91 using plasma CVD. It is also preferable to cover the sides of the openings of the optical filter 90 formed in the seventh step with the protective film 91 (Figure 8A). In the protective film formation step of the eighth step, conditions such as plasma generation conditions and raw material gas flow rate are adjusted so that an intermediate layer is formed between the uppermost layer of the optical filter 90 and the protective film 91, which appears darker in the cross-sectional TEM image than the uppermost layer of the optical filter 90 and the protective film 91. The intermediate layer formed here is presumed to contain oxygen-depleted SiO2 or oxygen-depleted SiON. The thickness of the intermediate layer is preferably 5 nm to 30 nm, and more preferably 5 nm to 20 nm.
[0048] For optimal output improvement, the thickness of the protective film 91 is preferably an integer multiple (within 5% error) of the value obtained by dividing the light-receiving wavelength of the semiconductor photodetector 1 by twice the refractive index of the protective film 91. For example, if the light-receiving wavelength of the semiconductor photodetector 1 is λ1 and the refractive index of the protective film 91 is n1, the thickness of the protective film 91 can be expressed as k × (λ1 / 2n1) (where k is an integer of 1 or more). The material of the protective film 91 is preferably SiO2 or Si3N4, but other materials may also be used. The thickness of the protective film 91 is not particularly limited as long as the received light reaches the light-receiving part 63.
[0049] <9th process> The ninth step, as described above, is the step of forming a back electrode on the back surface of the substrate 10 for electrical conduction (Figure 9). The back surface of the substrate 10 may be ground before forming the back electrode, and the thickness of the substrate 10 after grinding is preferably 80 μm or more and 300 μm or less, and more preferably 200 μm or less. In addition, the overall thickness of the device including the substrate 10 and the semiconductor laminate 11 is preferably 100 μm or more and 350 μm or less, and more preferably 150 μm or more and 280 μm or less. After grinding the substrate 10, the back surface of the substrate 10 is cleaned, and the back electrode 100 can be formed by metal deposition or sputtering. For example, the back electrode 100 can be an alloy containing Au. The film thickness (total film thickness) of the back electrode 100 is not limited, but is preferably, for example, 500 nm or more and 1000 nm or less.
[0050] <10th process> The tenth step, as mentioned above, is the individualization step, although it is not shown in the diagram. The semiconductor photodetector 1 fabricated in Figure 9 is individualized into chips using a laser dicer. Individualization can be done by cutting from the optical filter to the substrate as shown in Figure 9, or by cutting partway and then using scribing or breaking in combination. Furthermore, if a mesa formation step is added between steps 5 and 9, and the semiconductor layer including the photodetector layer is partially removed along the planned cutting line in the individualization step by dry etching or the like, then in the individualization step, only the remaining part including the substrate needs to be cut.
[0051] In the first embodiment described above, an intermediate layer is formed between the uppermost layer of the optical filter 90 and the protective film 91 by performing a protective film formation step after the optical filter formation step. This makes it possible to manufacture a semiconductor photodetector 1 in which the upper electrode 80 and the optical filter 90 are in contact, yet the dark current does not increase even under high temperature and high humidity conditions. The embodiments of the manufacturing method according to the present invention are not limited to the above embodiment, and for example, the following modifications may be applied, or these may be combined.
[0052] (Variation 1) As a modification 1 of the first embodiment described above, a different type of light-receiving section is given. In the first embodiment described above, the light-receiving section 63 is a PIN junction or PN junction by Zn diffusion, but the light-receiving section 63 may be formed by doping during epitaxial growth instead of by the Zn diffusion method. Alternatively, the amount of doping may be adjusted to form an APD (avalanche photodiode) type. Furthermore, although the first embodiment describes an InGaAs-based light-receiving element using an n-type InP growth substrate 10 as an example, the dark current that can be suppressed by the presence of the intermediate layer in the present invention is considered to be the current in the path from the top electrode 80 through the optical filter 90 along the side of the element to the back electrode 100. In other words, since it is not due to the current flowing inside the element, the effects of the invention may be achieved regardless of the type of substrate 10 and semiconductor laminate 11. Depending on the type of substrate 10 and the light-receiving center wavelength, each layer constituting the semiconductor laminate 11 may be appropriately selected from a III-V semiconductor layer consisting of one or more elements selected from the group III elements Al, Ga, and In, and one or more elements selected from the group V elements N, As, P, and Sb.
[0053] (Modification 2) As a second modification of the first embodiment described above, a diffusion prevention layer 50 and a dielectric layer 70 with different ranges are provided. In the first embodiment described above, the diffusion prevention layer 50 and the dielectric layer 70 are formed up to the edge of the semiconductor photodetector 1, but these layers do not necessarily have to be formed up to the edge of the semiconductor photodetector 1. The diffusion prevention layer 50 and the dielectric layer 70 may not be formed at the edge of the semiconductor photodetector 1, and instead an optical filter 90 or a protective film 91 may be formed there.
[0054] (Variation 3) As described in our Japanese Patent Application No. 2024-073142, the present invention may also include a step of forming a bonding layer on the p-type electrode and the dielectric layer after forming the dielectric layer 70, and bonding the support substrate via the bonding layer. Examples of the support substrate include a Si substrate, a Ge substrate, a compound semiconductor substrate, a metal substrate (Cu-Mo, Mo, etc.), or a ceramic substrate (AlN sintered body, etc.). In this case, since the InP growth substrate is etched off, the frame electrode, pad electrode, optical filter, and protective film are formed on the side from which the InP growth substrate was removed.
[0055] —Semiconductor photodetector— Next, the semiconductor photodetector 1 described in the first embodiment, obtained through at least the electrode formation step, optical filter formation step, and protective film formation step described above, will be explained. As shown in Figure 9, this semiconductor photodetector 1 comprises an upper electrode 80 (frame-shaped electrode 81 and pad electrode 82) and an optical filter 90 that is in contact with at least a portion of the upper electrode 80. The optical filter 90 has an opening that exposes a portion of the upper electrode 80 in order to enable electrical wiring to the outside. It is preferable that the side surface of the opening is covered with a protective film 91. The optical filter 90 includes a dielectric multilayer film. It is preferable that the dielectric multilayer film included in the optical filter 90 includes a laminate of a Si layer and an SiO2 layer, and it is preferable that the uppermost layer of the optical filter 90 is an SiO2 layer. It is also possible to include laminates of high refractive index, medium refractive index, and low refractive index using layers of different materials from the Si layer and SiO2 layer. When forming the optical filter 90 including the laminate of the Si layer and SiO2 layer, the initial resistivity of the optical filter 90 after the formation of the protective film 91 is 3.0 × 10⁻⁶. 12 Preferably, the size is Ωμm or larger, and 3.8 × 10 12 It is more preferable that the resistivity be greater than Ωμm. Furthermore, the resistivity after a 24-hour HAST test at 130°C, 85%RH humidity, and 2 atmospheres is 9.0 × 10⁻⁶. 11 It is preferable that the resistivity is Ωμm or greater. Furthermore, the ratio (percentage change) of the difference between the resistivity after the HAST test and the initial resistivity of the optical filter 90 is preferably 90% or less, and more preferably 50% or less.
[0056] The semiconductor photodetector 1 has a protective film 91 containing SiO2 or Si3N4 placed on top of the uppermost layer of the optical filter 90. The thickness of the protective film 91 is preferably an integer multiple (within 5% error) of the value obtained by dividing the light-receiving wavelength of the semiconductor photodetector 1 by twice the refractive index of the protective film 91. For example, if the light-receiving wavelength of the semiconductor photodetector 1 is λ1 and the refractive index of the protective film 91 is n1, the thickness of the protective film 91 can be expressed as k × (λ1 / 2n1) (where k is an integer of 1 or more).
[0057] The semiconductor photodetector 1 has an intermediate layer between the uppermost layer of the optical filter 90 and the protective film 91, which is observed to be darker than the uppermost layer of the optical filter 90 and the protective film 91 in a cross-sectional TEM image. The intermediate layer formed here is presumed to contain SiO2 or SiON with oxygen vacancies. While HAST testing shows a tendency for the resistivity of the optical filter 90 to decrease and the dark current (reverse current) to increase, if the protective film 91 is formed on the optical filter 90 while the intermediate layer of the present invention is observed, the decrease in the resistivity of the optical filter 90 after the formation of the protective film 91 can be suppressed, as can the increase in the dark current. Furthermore, when the concentrations of hydrogen (H) and deuterium (D) in the SiO2 layer and Si layer of the optical filter 90 are measured using SIMS analysis, if the protective film is formed while the intermediate layer of the present invention is observed, the increase in deuterium (D) entering from the outside is suppressed in HAST testing, suggesting that the intermediate layer has a significant effect in preventing water intrusion.
[0058] When the semiconductor photodetector 1 is a photodetector having a photodetector layer made of an InGaAs layer as exemplified in the first embodiment, the dark current when a reverse bias voltage of 5V is applied is 0.185nA or less, preferably 0.184nA or less, and more preferably 0.183nA or less. Furthermore, the rate of change of the dark current after 24 hours of high-speed accelerated life testing is 3.5 times or less, and preferably 3.4 times or less.
[0059] The semiconductor photodetector 1 preferably has a photodetector peak wavelength (the wavelength at which the intensity in the photosensitivity spectrum is maximum) of 800 nm to 2500 nm, more preferably 850 nm to 2000 nm, and even more preferably 900 nm to 1700 nm. The photodetector layer 20 is preferably an InGaAs layer. The full width at half maximum of the peak in the photosensitivity spectrum is preferably, for example, 50 nm to 200 nm.
[0060] As detailed in the examples, it was experimentally confirmed that the semiconductor photodetector 1 provided with the intermediate layer described above does not experience an increase in dark current under high temperature and high humidity conditions, even when the electrodes and optical filter are in contact.
[0061] (Second Embodiment) In the second embodiment, in the seventh step of the semiconductor photodetector manufacturing method for forming the optical filter 90, the optical filter 90 includes a dielectric layer film consisting of a Si layer and an SiO2 layer. Furthermore, it is preferable that the uppermost layer of the optical filter 90 is an SiO2 layer. In addition, after forming the protective film 91 in the eighth step, the average D concentration in the SiO2 layer of the optical filter 90 after 24 hours of high-speed accelerated lifetime testing is 1.5 × 10⁻¹⁶. 21 atom / cm 3 The following applies. Except as stated above, the method for manufacturing the semiconductor photodetector is the same as in the first embodiment. The semiconductor photodetector 1 manufactured according to the second embodiment will be described. The optical filter 90 includes a laminate of a Si layer and an SiO2 layer. The uppermost layer is preferably an SiO2 layer. Furthermore, the average D concentration in the SiO2 layer of the optical filter 90 after 24 hours of high-speed accelerated lifetime testing is 1.5 × 10⁻¹⁰. 21 atom / cm 3 Except as described below, the semiconductor photodetector is identical to that in the first embodiment. The second embodiment also provides the same effects as the first embodiment. The average D concentration in the SiO2 layer of the optical filter 90 after 24 hours of high-speed accelerated life testing is 9.9 × 10⁻⁶. 20 atom / cm 3 It is more preferable that the following conditions apply: 4.0 × 10 20 atom / cm 3It is even more preferable that the following conditions are met: There is no particular lower limit, but the minimum resolution in SIMS is 2.0 × 10⁻¹⁶. 18 atom / cm 3 Therefore, for example, 2.0 × 10 18 atom / cm 3 That concludes the report. Furthermore, the average D concentration in the Si layer of optical filter 90 after 24 hours of high-speed accelerated life testing was 1.0 × 10⁻⁶. 20 atom / cm 3 Preferably, it is 5.0 × 10 19 atom / cm 3 The following is more preferable:
[0062] (Third embodiment) This disclosure is also applicable to semiconductor light-emitting elements, which are optical semiconductor devices, and it is possible to make the semiconductor light-emitting element 1 such that the optical filter 90 has the function of transmitting or reflecting a specific wavelength range. A semiconductor light-emitting element according to a third embodiment of the present invention will be described. For example, by replacing the light-receiving layer 20 in the first embodiment with an active layer, the optical semiconductor device of the present invention can be used as a semiconductor light-emitting element, and a semiconductor light-emitting element with a small dark current (also called reverse current) even under high temperature and high humidity conditions can be realized. That is, the semiconductor light-emitting element according to the second embodiment is an optical semiconductor light-emitting element comprising an electrode and an optical filter in which at least a part is in contact with the electrode, wherein the optical filter includes a dielectric multilayer film, has a protective film containing SiO2 or Si3N4 on the uppermost layer of the optical filter, and has an intermediate layer between the uppermost layer and the protective film which is observed to be darker than the uppermost layer and the protective film in a cross-sectional TEM image. This semiconductor light-emitting element may have an n-type semiconductor layer, an active layer and a p-type semiconductor layer between the substrate and the optical filter in this order.
[0063] In the method for manufacturing a semiconductor light-emitting element, in the first step described above, a plurality of compound semiconductor layers, each containing at least an active layer, are stacked on a substrate 10 to form a semiconductor stack 11. If the semiconductor stack 11 in the first step has a p-type semiconductor layer and an n-type semiconductor layer, the p-type impurity diffusion in the fourth step described above may be omitted. [Examples]
[0064] The present invention will be described in more detail below using examples, but the present invention is not limited in any way to the following examples. Reference numerals are shown in Figures 1 to 9.
[0065] 3-inch n-type InP growth substrate 10 (thickness: 350 μm, S-doped, carrier density: 2 × 10) 8 / cm 3 ) Using the MOCVD method, an undoped InP buffer layer (film thickness 0.5 μm) and a tracely Si-doped InP layer were formed. 0.53 Ga 0.47 As photodetector layer 20 (film thickness: 3.0 μm, average Si concentration 9 × 10⁻¹⁶ by SIMS analysis) 14 / cm 3 (Carrier density too low to measure), n-type InP window layer 30 (film thickness: 1.0 μm, Si doped, carrier density: 8 × 10) 15 / cm 3 ), and undoped In 0.53 Ga 0.47 As contact layers 40 (film thickness: 0.1 μm) were sequentially deposited to form a semiconductor laminate 11. This process is shown in Figure 1.
[0066] A pattern as shown in Figure 2 was formed on the undoped InGaAs contact layer 40. For this pattern formation, a resist pattern was created, and the openings (etched areas) were etched. A solution of H2SO4:H2O2:H2O = 1:1:7 was used as the etching solution for the InGaAs. Next, it was allowed to stand for 30 seconds, washed with ultrapure water, and dried. Afterward, the resist was removed by washing. As shown in Figure 2B, the InGaAs contact layer 40 was not a complete frame shape when viewed from above, but rather an open frame shape for the pad electrode 82, which will be described later. The width of the InGaAs contact layer 40 was 11 μm. Furthermore, when the InGaAs contact 40 was considered a closed rectangle, the inner circumference size of the rectangle was 396 μm × 396 μm, and the outer circumference size was 418 μm × 418 μm.
[0067] Next, a diffusion-blocking layer 50 (thickness: 100 nm) made of Si3N4 was deposited on the n-type InP window layer 30, including the undoped InGaAs contact layer 40 on which the above pattern was formed, using plasma CVD. A resist pattern was formed on the deposited Si3N4 diffusion-blocking layer 50, and the openings were etched. BHF solution was used as the etching solution for the Si3N4 diffusion-blocking layer 50, and it was allowed to stand for 3 minutes and 30 seconds, washed with ultrapure water, and dried. After that, the resist was removed by washing. In this way, a diffusion-blocking layer 50 as shown in Figure 3 was formed.
[0068] By supplying a Zn source gas while heating using the MOCVD method, Zn was diffused in the depth direction of the n-type InP window layer 30 and the undoped InGaAs contact layer 40. Zn was diffused from the interface between the undoped InGaAs contact layer 40 and the n-type InP window layer 30 and the undoped InGaAs photodetector layer 20 to the undoped InGaAs photodetector layer 20, up to a region of 300 nm. DEZn (diethylzinc) was used as the Zn source. Since Zn diffusion can form a p-type region, the InGaAs contact layer 40 after Zn diffusion becomes a p-type InGaAs contact layer 61, the portion of the n-type InP window layer 30 and the undoped InGaAs photodetector layer 20 where Zn has diffused and become p-type is a p-type region 62, and the interface with the p-type region 62 within the undoped InGaAs photodetector layer 20 is the photodetector portion 63. The average Zn concentration in the thickness direction of the p-type region 62 in the n-type InP window layer 30 is 5.0 × 10⁻¹⁴. 18 / cm 3 Furthermore, the size of the Zn diffusion region 60, excluding the area near the pad electrode 82, was 422 μm × 422 μm.
[0069] A dielectric layer 70 (thickness: 177 nm) made of Si3N4 was deposited by plasma CVD. A resist pattern was formed on the deposited Si3N4 dielectric layer 70, and the openings were etched. BHF solution was used as the etching solution for the Si3N4 dielectric layer 70, and it was allowed to stand for 6 minutes, washed with ultrapure water, and dried. After that, the resist was removed by washing. In this way, a dielectric layer 70 as shown in Figure 5 was formed. The width of the p-type contact layer 61 was 7 nm. The p-type contact layer 61 was located in the center of the undoped contact layer 40 formed in Figure 2. In Figure 5, the Si3N4 dielectric layer 70 covers all areas except for the p-type contact layer 61 portion exposed on the surface (Figure 5B).
[0070] A frame-shaped electrode 81 and a pad electrode 82, as shown in Figure 6, were formed on the surface of Figure 5. For electrode pattern formation, a resist pattern was first formed, and the electrode formation area was etched. Ti (film thickness: 30 nm) / Pt (film thickness: 50 nm) / Au (film thickness: 1000 nm) were deposited by EB metal deposition. Next, excess metal and resist were removed by lift-off, forming the electrode pattern shown in Figure 6. The width of the frame-shaped electrode 81 was 20 μm, and the distance from the outer periphery of the semiconductor laminate 11 was 40 μm. The diameter of the pad electrode 82 was 105 μm. The inner circumference of the frame-shaped electrode 81, excluding the pad electrode 82, was 390 μm × 390 μm. Similarly, the outer circumference of the frame-shaped electrode 81, excluding the pad electrode 82, was 430 μm × 430 μm. The frame-shaped electrode 81 and the pad electrode 82 were combined to form the top electrode 80.
[0071] An optical filter 90 was formed to cover the entire surface of the Si3N4 dielectric layer 70 and the frame-shaped electrode 81, except for the opening for the pad electrode 82 to connect to the outside. For the optical filter 90, first, a resist pattern was formed on the region that would become the external connection surface on the pad electrode 82, and a dielectric multilayer film consisting of a Si layer (amorphous silicon layer) and an SiO2 layer was formed by sputtering. In the sputtering apparatus, Si was used as the target, the TS distance was set to 110 mm, Ar gas was flowed at a flow rate of 300 sccm to a pressure of 0.6 Pa, and the discharge power was set to 9 kW. In addition, oxygen was flowed at 200 sccm during the formation of the SiO2 layer. The specific structure and film formation conditions of the examples and comparative examples of the optical filter 90 will be described later. Next, the excess dielectric multilayer film and resist on the external connection surface of the pad electrode 82 were removed by lift-off, and an optical filter 90 having an opening as shown in Figure 7 was formed. The opening diameter was 85 μm. Except for the opening of the pad electrode 82, the optical filter 90 was in contact with the upper electrode 80 (frame-shaped electrode 81 and pad electrode 82).
[0072] As shown in Figure 8, a protective film 91 containing SiO2 or Si3N4 was formed on the top layer of the optical filter 90. First, the protective film 91 was formed on the entire surface of the optical filter 90, including the opening shown in Figure 8, using plasma CVD. At this time, the sides of the opening of the optical filter 90 were also covered with the protective film 91. The specific structure and deposition conditions of the examples and comparative examples of the protective film 91 will be described later. Subsequently, a resist pattern was formed on the deposited protective film 91, and the protective film 91 was etched to expose the bottom of the opening and the external connection surface of the pad electrode 82. BHF solution was used as the etching solution for the protective film 91. After that, it was washed with ultrapure water and dried. Finally, the resist was removed by washing. In this way, a protective film 91 as shown in Figure 8 was formed.
[0073] The deposition conditions were adjusted so that an intermediate layer, which appears darker than the optical filter and protective film 91 in cross-sectional TEM, is formed between the uppermost layer of the optical filter 90 and the protective film 91. The specific conditions for the examples and comparative examples will be described later.
[0074] The back surface of the growth substrate 10 was ground to achieve an overall thickness of 150 μm. Furthermore, as shown in Figure 9, a back surface electrode 100 containing Au was formed on the back surface of the growth substrate 10.
[0075] Finally, the fabricated semiconductor photodetector 1 was separated into individual chips using a laser dicer.
[0076] Table 1 shows the layer structure of the optical filters 90 in Examples 1-4 and Comparative Examples 1-3. The layer structure of the optical filters 90 is the same in Examples 1-4 and Comparative Examples 1-3. Table 2 shows the layer structure of the protective films 91 in Examples 1-4 and Comparative Examples 1-3, respectively. In Table 2, p-CVD represents plasma CVD. In Examples 1-4, after forming the 23rd layer of the optical filter 90, the element was removed from the deposition apparatus, the excess dielectric layer and resist were removed by lift-off to expose a portion of the pad electrode 82, and then the element was placed in the p-CVD deposition apparatus to form the protective film 91 by the plasma CVD method. The SiO2 film thickness of the protective film 91 in Examples 1, Comparative Example 2, and Comparative Example 3, 390 nm, was set from the value of k × (λ1 / 2n1) when the light receiving wavelength is λ1 = 1130 nm, the refractive index of the protective film 91 is n1 = 1.459, and k = 1.
[0077] [Table 1]
[0078] [Table 2] * In Comparative Example 2, after the 23rd layer of the optical filter 90 has been deposited, a 390 nm thick layer of SiO2 is added by extending the deposition time for the 23rd layer without removing the element from the deposition apparatus (without exposing it to the atmosphere). For convenience, this is referred to as the protective film 91, but it is essentially an extension of the optical filter 90. **In Comparative Example 3, after depositing the 23rd layer of the optical filter 90, the element was temporarily removed from the deposition apparatus (opened to the atmosphere), the excess dielectric layer and resist were removed by lift-off to expose the pad electrode 82, and then the element was put back into the deposition apparatus to form a protective film 91 by sputtering.
[0079] Figures 10A, 11A, 12A, and 13A each show SEM images including the boundary between the 22nd and 23rd layers of the optical filter 90, and the boundary between the 23rd layer of the optical filter 90 and the protective film 91, for each of Example 1, Example 3, Comparative Example 2, and Comparative Example 3. Figures 10B, 11B, 12B, and 13B each show magnified TEM images of section A (the boundary between the 23rd layer of the optical filter 90 and the protective film 91) for each of Figures 10A (Example 1), 11A (Example 3), 12A (Comparative Example 2), and 13A (Comparative Example 3). The thick arrows in Figures 10B, 11B, 12B, and 13B indicate the boundary between the 23rd layer of the optical filter 90 and the protective film 91.
[0080] Table 3 shows the presence or absence of an intermediate layer between the 23rd layer of the optical filter 90 and the protective film 91, and, if an intermediate layer exists, its approximate width, for each of Examples 1-4 and Comparative Examples 1-3. Here, TEM images were obtained for Examples 1 and 3 and Comparative Examples 2 and 3, so the presence or absence and width of the intermediate layer were directly confirmed. However, for Examples 2 and 4, TEM images were not obtained, so the presence or absence of an intermediate layer was not directly confirmed. Therefore, since Example 2 was manufactured under the same conditions as Example 1, and Example 4 was manufactured under the same conditions as Example 2, it is assumed that the results regarding the presence or absence of an intermediate layer are similar for each. In Comparative Example 1, since the protective film 91 was not formed in the first place, it is natural to assume that no intermediate layer was formed.
[0081] [Table 3]
[0082] From the conditions for the protective film 91 in Table 2 and the results in Table 3, it can be seen that when the protective film 91 is formed by plasma CVD after the optical filter 90 has been formed, an intermediate layer is formed. Furthermore, although the intermediate layer is formed regardless of whether the material of the protective film 91 is SiO2 or Si3N4, a comparison between Example 1 and Example 3 shows that the width of the intermediate layer is thicker when Si3N4 is used. In Comparative Example 3, SiO2 was used as the material for the protective film 91, and the system was opened to the atmosphere before the protective film 91 was formed, but no intermediate layer was formed. From this, it can be said that in order to form an intermediate layer, among the material of the protective film 91, the deposition method, and film thickness, it is important to use plasma CVD as the deposition method rather than sputtering.
[0083] Tables 4 and 5 show the degree of water penetration into the optical filter 90 when the protective film 91 was formed in Examples 1-4 and Comparative Examples 1-3, using SIMS analysis. SIMS analysis was performed in the depth direction from the protective film surface at the center of the chip when viewed from above. Table 4 shows the average H (hydrogen) element concentration and average D (deuterium) element concentration of all SiO2 layers of the optical filter 90, and Table 5 shows the average H (hydrogen) element concentration and average D (deuterium) element concentration of all Si layers of the optical filter 90. Here, the initial average H (or D) concentration refers to the average H (or D) concentration immediately after fabrication of the photodetector.
[0084] [Table 4] ( * The minimum resolution of element D concentration in this SIMS analysis is 2.0 × 10⁻⁶. 18 atom / cm 3 That is the case.
[0085] [Table 5] ( * The minimum resolution of element D concentration in this SIMS analysis is 2.0 × 10⁻⁶. 18 atom / cm 3 That is the case.
[0086] From the SiO2 layer in Table 4 and the Si layer in Table 5, the average D concentration in the SiO2 layer of the optical filter 90 after 24 hours of the fast accelerated lifetime test (HAST) in the example is 1.5 × 10⁻¹⁶. 21 atom / cm 3 The following is true, and the average D concentration in the Si layer is 1.0 × 10⁻⁶. 20 atom / cm 3 The results were as follows: The average D concentration increased from the initial average D concentration in Examples 1 to 4 compared with Comparative Examples 1 to 3. Also, the D / H ratio after 24 hours of HAST was significantly smaller in Examples 1 to 4 compared with Comparative Examples 1 to 3. Since the element "D" entered from the outside through HAST, it is thought that this resulted in the formation of an intermediate layer, which prevented water from diffusing into the optical filter 90. Furthermore, Examples 1 and 2 in Table 4 had higher average D concentrations and higher D / H ratios after 24 hours of HAST than Examples 3 and 4. Comparing Examples 1 and 2 in Tables 4 and 5, it can be seen that Example 1 had a smaller average D concentration and D / H ratio after 24 hours of HAST. This indicates that even with the same protective film 91, a thicker film thickness reduces water diffusion into the optical filter 90. The same can be said for the comparison between Examples 3 and 4. Furthermore, while the protective film 91 in Examples 1 and 2 is made of SiO2, the protective film 91 in Examples 3 and 4 is made of Si3N4. This is because Si3N4 has lower water penetration and reactivity with water compared to SiO2, so when Si3N4 is used, the protective film 91 itself functions as a layer that prevents water penetration, thereby increasing the effect of preventing the diffusion of water mentioned above. As a result, the average D concentration in the SiO2 layer of the optical filter 90 after 24 hours of fast accelerated life testing (HAST) was 1.5 × 10⁻¹⁶. 21 atom / cm 3 It can be seen that the effects of the present invention can be obtained by forming a protective film 91 on the optical filter 90 as follows.
[0087] Table 6 shows the dark current flowing through the chip (semiconductor light-emitting element 1) when 5V was applied to Examples 1-4 and Comparative Examples 1-3. Here, the initial Ir(0) in Table 6 represents the dark current immediately after chip fabrication. From Table 6, it can be seen that the initial Ir(0) for Examples 1-4 is all 0.185nA or less, and the dark current change rate is 3.5 times (350%) or less. It can be seen that if an intermediate layer is present as in the examples, the increase in dark current can be suppressed even under high temperature and high humidity conditions. Furthermore, even after a 24-hour HAST test, the average D concentration in the SiO2 layer was 1.5 × 10⁻⁶. 21 atom / cm 3 The following conditions demonstrate that the increase in dark current can be suppressed even under high temperature and high humidity conditions.
[0088] [Table 6]
[0089] Table 7 shows the results of resistivity measurement using the same optical filter 90 as in Comparative Example 1, and the same optical filter 90 and protective film 91 as in Examples 1-4 and Comparative Examples 2-3. The resistivity measurement method in Table 7 is as described above, using a synthetic quartz substrate (resistivity 1.4 × 10⁻⁶). 14An optical filter 90 and (except for Comparative Example 1) a protective film 91 were deposited on a Ωμm (400μm thickness) film, and the samples were cut into small pieces measuring L200μm × 1000μm in length. Electrodes were formed as described above to create samples for resistivity measurement, and volume resistivity was measured using the two-terminal method by connecting Au wires as shown in Figures 14 and 15. The measurement temperature was 25°C, and measurements were taken using a Keithley Source Measure Unit (SMU). After holding the samples for 24 hours under the same conditions as the HAST test described above (130°C, 85%RH humidity, 2 atm), the resistivity was measured again. The rate of change (ρ(24)-ρ(0)) / ρ(0) between the initial resistivity ρ(0) and the resistivity ρ(24) after the 24-hour HAST test was smaller for Examples 1-4 than for Comparative Examples 1-3. This indicates that the resistivity of the optical filter 90 of the semiconductor light-emitting element 1 in Examples 1-4 was maintained at a higher level even after the 24-hour HAST test compared to the elements in Comparative Examples 1-3. Based on these results, it can be considered that the change in dark current in the chip is influenced by the change in the resistivity of the optical filter 90 due to moisture.
[0090] [Table 7] ( * The upper limit of this resistivity measurement is 1.4 × 10⁻⁶. 14 The resistance is Ωμm. (Measurement is not possible for resistance values higher than the measured value of the base synthetic quartz substrate.)
[0091] From the above results, it was confirmed that the semiconductor photodetector fabricated with the intermediate layer of the present invention suppressed the increase in dark current even under high temperature and high humidity conditions compared to the comparative example. Furthermore, the average D concentration in the SiO2 layer after a 24-hour HAST test was 1.5 × 10⁻⁶. 21 atom / cm 3 Under the following conditions, it was confirmed that the increase in dark current was suppressed even under high temperature and high humidity compared to the comparative example. [Explanation of symbols]
[0092] 1. Semiconductor photodetector 2. Glass epoxy substrate 3 glass plate 4. Adhesive 5 Au wires 6 Ag Paste 7 External connection terminals 10 circuit boards 11. Semiconductor Stack 20 Light-receiving layer 30 window layers 40 Contact Layers 50 Diffusion prevention layer 60 Zn diffusion region 61 p-type contact layer 62 p-type diffusion region 63 Light receiving section 70 Dielectric layer 80 Top electrode 81 Frame electrode 82 Pad electrodes 90 Optical Filters 91 Protective film 100 Backside electrode
Claims
1. Electrodes and, An optical filter in which at least a portion of the electrode is in contact, An optical semiconductor element comprising, The optical filter includes a dielectric multilayer film. SiO 2 or Si 3 N 4 It has a protective film containing, The uppermost layer and the protective film are characterized by having an intermediate layer between them that is observed to be darker than the uppermost layer and the protective film in a cross-sectional TEM image. Optical semiconductor device.
2. The optical semiconductor device according to claim 1, wherein the optical filter comprises a Si layer and SiO 2 It is a laminate including layers, the uppermost layer being SiO 2 A layered, optical semiconductor device.
3. The optical semiconductor device according to claim 1, wherein the intermediate layer is SiO with oxygen vacancies 2 Or an optoelectronic semiconductor device containing SiON.
4. An optical semiconductor element according to claim 1, wherein the thickness of the protective film is an integer multiple of the value obtained by dividing the light-receiving wavelength or emission wavelength of the optical semiconductor element by twice the refractive index of the protective film.
5. An optical semiconductor element according to claim 1, wherein the optical filter has an opening that exposes a part of the electrode, and the side surface of the opening is covered by the protective film.
6. An electrode formation process in which electrodes are formed on a photo-semiconductor device, An optical filter forming step in which an optical filter including a dielectric multilayer film is formed so as to be in contact with the electrode, On the uppermost layer of the optical filter, SiO 2 or Si 3 N 4 A protective film forming step of forming a protective film containing the above, It has, The optical filter formation process uses the sputtering method. The aforementioned protective film formation step uses a plasma CVD method. A method for manufacturing an optical semiconductor device, characterized in that, in the protective film formation step, an intermediate layer is formed between the uppermost layer and the protective film, which is observed to be darker than the uppermost layer and the protective film in a cross-sectional TEM image.
7. A method for manufacturing an optical semiconductor device according to claim 6, wherein the optical filter comprises a Si layer and SiO 2 It includes a laminate of layers, the uppermost layer being SiO 2 A method for manufacturing a layered optical semiconductor device.
8. A method for manufacturing an optical semiconductor device according to claim 6, wherein the intermediate layer is SiO with oxygen vacancies 2 A method for manufacturing an optoelectronic semiconductor device, or a method for manufacturing an optoelectronic semiconductor device containing SiON.
9. A method for manufacturing an optical semiconductor element according to claim 6, wherein the thickness of the protective film is an integer multiple of the value obtained by dividing the light-receiving wavelength or emission wavelength of the optical semiconductor element by twice the refractive index of the protective film.
10. A method for manufacturing an optical semiconductor element according to claim 6, wherein the optical filter forming step includes a step of forming an opening that exposes a part of the electrode, and the protective film forming step covers the side surface of the opening with the protective film.
11. The aforementioned optical semiconductor device is a photodetector having a photodetector layer made of an InGaAs layer, The dark current when a reverse bias voltage of 5V is applied to the aforementioned optical semiconductor device immediately after fabrication is 0.185nA or less. It is characterized by having a dark current change rate of 3.5 times or less after 24 hours of high-speed accelerated life testing. The optical semiconductor device according to claim 1.
12. Electrodes and, An optical filter in which at least a portion of the electrode is in contact, An optical semiconductor element comprising, The optical filter includes a dielectric multilayer film. SiO 2 or Si 3 N 4 It has a protective film containing, The optical filter consists of a Si layer and SiO 2 Including a laminate of layers, The SiO after 24 hours of high-speed accelerated life test 2 The average D concentration within the layer is 1.5 × 10⁻⁶ 21 atom / cm 3 The following are optical semiconductor devices.
13. An electrode formation process in which electrodes are formed on a photo-semiconductor device, A Si layer and SiO are placed in contact with the electrode. 2 An optical filter formation process that forms an optical filter including a dielectric multilayer film of layers, SiO 2 or Si 3 N 4 A protective film forming step that forms a protective film including, It has, The optical filter formation process uses the sputtering method. The aforementioned protective film formation step uses a plasma CVD method. The SiO after 24 hours of high-speed accelerated life test 2 The average D concentration within the layer is 1.5 × 10⁻⁶ 21 atom / cm 3 A method for manufacturing an optical semiconductor device, characterized by the following: