1. Field of the Invention
The present invention relates to an array type light-receiving device and a hyperspectral spectrometer including the array type light-receiving device.
2. Description of the Related Art
Patent Literature 1 (Japanese Unexamined Patent Application Publication No. 2013-93385) discloses light-receiving devices and related techniques. The light-receiving device described in Patent Literature 1 has a plurality of pixels disposed on a semiconductor substrate. Each of the pixels of the light-receiving device includes a light-receiving layer for receiving light, a p-n junction disposed in the light-receiving layer, and a mesa structure defined by grooves. The plurality of pixels is spaced apart from each other by the grooves disposed around the mesa structures. An impurity wall layer is disposed on a wall surface of the mesa structure so as to prevent the p-n junction from being exposed at the wall surface of the mesa structure. Patent Literature 2 (Japanese Unexamined Patent Application Publication No. 2013-201219) discloses light-receiving devices and related techniques. The light-receiving device described in Patent Literature 2 has a plurality of pixels disposed on a semiconductor substrate. Each of the pixels includes a mesa structure defined by a groove. The mesa structure includes a light-receiving layer disposed in a stacked semiconductor layer, and a p-n junction located at an interface between the light-receiving layer and a p-type semiconductor layer disposed on the light-receiving layer. The plurality of pixels is separated from each other by the grooves disposed between the mesa structures. The groove is extended from a surface of the stacked semiconductor layer toward the semiconductor substrate through the p-n junction. The sidewall of the mesa structure is tapered such that the sectional area of the light-receiving layer is decreased toward the p-n junction. The semiconductor layer disposed on the light-receiving layer has an overhang portion that surrounds the p-n junction. The overhang portion of the semiconductor layer is overhung toward the grooves defining the mesa structure. Non-Patent Literature 1 (“MOVPE grown InGaAs/GaAsSb Type II Quantum Well Photodiode for SWIR Focal Plane Array”, H. Inada, H. Mori, Y. Nagai, Y. Iguchi, T. Saitoh, K. Fujii, T. Ishizuka, K. Akita, Proceeding of SPIE, vol. 8012 801220 (2011)) discloses a technique related to photodiodes having a type-II InGaAs/GaAsSb quantum well structure. Non-Patent Literature 1 describes a pixel size with a pixel pitch of 30 μm and a diameter of 15 μm.
A hyperspectral camera includes a two-dimensional array sensor that includes a plurality of pixels arranged in a lateral direction and a longitudinal direction. From the pixels arranged in the lateral direction, spatial information (image information) is obtained. In addition, from the pixels arranged in the longitudinal direction, wavelength information is obtained. By using the hyperspectral camera, the optical spectrum for each of the pixels arranged in the lateral direction for obtaining the spatial information (image information) is simultaneously obtained. For example, in the two-dimensional array sensor having 320×256 pixels, the 320 pixels arranged in the lateral direction provide spatial information. The 256 pixels arranged in the longitudinal direction provide wavelength information. In order to obtain the wavelength information, light that has been reflected from or passed through an object to be measured is spectrally diffracted by a spectroscope such as a prism. The light components diffracted spectrally are then incident on the 256 pixels of the array sensor arranged in the longitudinal direction so as to be converted into electrical signals (photocurrent). Where necessary, the object to be measured is irradiated with light by using a halogen lamp as a light source, especially in infrared hyperspectral systems. The electrical signals output from the array sensor are accumulated in capacitors in a read-out IC for a predetermined time (for example, 1 msec) and are thereafter read out to the outside. Usually, the array sensor has a responsivity having a wavelength dependence related to the semiconductor material constituting a light-receiving layer included in the pixels. When the light-receiving layer in the pixels is made of InGaAs, for example, the array sensor has a peak of responsivity at a wavelength of 1620 nm. Therefore, the photocurrent output from the pixel received a light component having a wavelength of 1620 nm is larger than the photocurrents output from the pixels received light components having wavelengths other than the wavelength of 1620 nm even when the light components have the same optical intensity. Capacitors in a read-out IC can store a limited amount of charges. The conditions (incident light intensity and accumulation time) to fully charge capacitors in a read-out IC are different in each of the capacitors according to the pixels connected to the capacitors. Specifically, when the light-receiving layer in the pixels is made of InGaAs, the capacitor connected to the pixel that receives light with a wavelength near 1620 nm is fully charged with a smaller optical intensity of the incident light and/or in a smaller accumulation time as compared with the capacitor connected to a pixel that receives light having a wavelength (a wavelength of below 1000 nm or above 1620 nm). When the conditions of the incident light intensity and the accumulation time of the capacitor are adjusted so that the capacitor connected to a pixel receiving a light having a wavelength at which the pixel has a smaller responsivity has an optimum amount of charges, the capacitor connected to a pixel receiving a light having a wavelength near 1620 nm at which the pixel has a larger responsivity is oversaturated. In the reverse case, the capacitor connected to a pixel receiving a light having a wavelength at which the pixel has a smaller responsivity is charged insufficiently and consequently the S/N ratio (the signal to noise ratio) of the pixel is decreased as compared with the capacitor connected to a pixel receiving a light having a wavelength near 1620 nm at which the pixel has a larger responsivity. In order to improve the S/N ratio of the pixel in the array sensor, it is desirable that conditions allow charges to be accumulated until immediately before the capacitors are saturated. However, the wavelength dependency of the responsivity of the pixel in the array sensor causes significant variations in the amounts of charges accumulated in the capacitors depending on wavelengths. Consequently, the S/N ratios are variable depending on wavelengths.
An array type light-receiving device according to an aspect of the present invention includes a plurality of pixels two-dimensionally arranged in a first direction and a second direction perpendicular to the first direction, each of the pixels including a light-receiving layer having a responsivity to a wavelength of light. The pixels arranged in the second direction constitute a plurality of pixel lines extending in the second direction, the plurality of pixel lines being arranged in the first direction to form an array. The pixels in each of the pixel lines have different pixel areas from each other. In addition, the pixel area of each of the pixels included in at least one of the pixel lines is determined in accordance with the responsivity to a wavelength of light received by each of the pixels.
First, embodiments of the present invention will be listed and described. An array type light-receiving device according to an aspect of the present invention includes a plurality of pixels two-dimensionally arranged in a first direction and a second direction perpendicular to the first direction, each of the pixels including a light-receiving layer having a responsivity to a wavelength of light. The pixels arranged in the second direction constitute a plurality of pixel lines extending in the second direction, the plurality of pixel lines being arranged in the first direction to form an array. The pixels in each of the pixel lines have different pixel areas from each other. In addition, the pixel area of each of the pixels included in at least one of the pixel lines is determined in accordance with the responsivity to a wavelength of light received by each of the pixels.
In the array type light-receiving device according to one aspect of the invention, preferably, the pixels included in each of the pixel lines include a first pixel configured to receive light with a wavelength at which the pixel has a lowest responsivity in the responsivities to the wavelengths of incident light, and a second pixel other than the first pixel. The first pixel has the largest pixel area of the pixels included in the pixel line. The second pixel has a pixel area determined by the relational expression:
Aβ=E/Rβ,
where Aβ represents the pixel area of the second pixel, E represents product of the responsivity of the first pixel at the wavelength of light received by the first pixel multiplied by the pixel area of the first pixel, and Rβ represents the responsivity of the second pixel at the wavelength of light received by the second pixel.
In the array type light-receiving device, the pixel area of each of the pixels included in at least one of the pixel lines is determined in accordance with the responsivity to the wavelength of light received by each of the pixels. Specifically, the pixel areas of the pixels are determined so that the product of the responsivity to the wavelength of light received by each of the pixels multiplied by the pixel area is constant. As a result, the amounts of light received by the pixels are controlled by changing the pixel areas of the pixels in accordance with the responsivities to wavelengths of light received by the pixels. Accordingly, photocurrents (charges) output from the pixels are uniform in receiving light components with the same intensity even when light components received by the pixels have different wavelengths. The difference in photocurrents (charges) output from the pixels due to the spectral sensitivity characteristics depending on the wavelengths of light is reduced. Accordingly, the S/N ratios of the pixels in the array type light-receiving device are improved.
In the array type light-receiving device according to one aspect of the invention, preferably, the plurality of pixels included in each of the pixel lines are arranged so as to receive corresponding light components having different wavelengths, the light components being separated along the second direction depending on the wavelengths. In the array type light-receiving device, the pixels included in each of the pixel lines receive corresponding light components having predetermined wavelengths. The pixel areas of the pixels are determined in accordance with the responsivities to the predetermined wavelengths of light components.
In the array type light-receiving device according to one aspect of the invention, the pixels arranged in the first direction may constitute a plurality of pixel rows extending in the first direction. The pixel areas of the pixels in each of the pixel rows may be approximately equal to each other.
Preferably, the array type light-receiving device according to one aspect of the invention further includes a plurality of mesas corresponding to the pixels, each of the mesas including the light-receiving layer, a passivation film disposed on a top surface and a side surface of the mesa, the passivation film including an opening on the top surface of the mesa, and an electrode disposed in the opening in contact with the top surface of the mesa.
Preferably, the array type light-receiving device according to one aspect of the invention further includes a plurality of impurity diffusion regions corresponding to the pixels, each of the impurity diffusion regions extending from a top surface of the pixel toward the light-receiving layer, a mask disposed on the top surface of the pixel, the mask having an opening on the impurity diffusion region, and an electrode disposed in the opening in contact with a top surface of the impurity diffusion region.
In the array type light-receiving device according to one aspect of the invention, the light-receiving layer may include an InGaAs layer. In addition, the light-receiving layer may have a multi quantum well structure including InGaAs layers and GaAsSb layers stacked alternately.
A hyperspectral spectrometer according to another aspect of the present invention includes an array type light-receiving device and a spectroscope configured to disperse an incident light spectrally into a plurality of light components having different wavelengths, the spectroscope outputting a dispersed light to the array type light-receiving device. The array type light-receiving device includes a plurality of pixels two-dimensionally arranged in a first direction and a second direction perpendicular to the first direction, each of the pixels including a light-receiving layer having a responsivity to a wavelength of light. The pixels arranged in the second direction constitute a plurality of pixel lines extending in the second direction, the plurality of pixel lines being arranged in the first direction to form an array. The light components of the dispersed light are separated along the second direction depending on the wavelengths. Each of the pixels in the pixel line is configured to receive at least one of the light components. In addition, the pixels in each of the pixel line have different pixel areas, each of which is determined in accordance with the responsivity to the wavelength of the light component received by each of the pixels.
Specific examples of the array type light-receiving devices according to embodiments of the present invention will be described below with reference to the drawings. However, the scope of the invention is defined by the appended claims and is not limited to such examples. It is intended that the scope of the invention covers all modifications that are within the spirit and scope equivalent to the claims.
The arrangement of N1×N2 pixels Kα×β that constitute a pixel array KA of the array type light-receiving device 22 will be described with reference to
N1 and N2 are both integers of 2 or greater. For example, N1 is 320 and N2 is 256. The N1×N2 pixels Kα×β are two-dimensionally arranged along the direction D1 and direction D2 on the surface S2 of the array type light-receiving device 22. The positions of the pixels Kα×β in the direction D1 correspond to the positions on a line of the object Ob1 at which light P1 is reflected from or passed through the object Ob1. The positions of the pixels Kα×β in the direction D2 correspond to the wavelengths of the light P2 dispersed by the spectroscopic device 3.
N1 indicates the number of pixels Kα×β in the direction D1. N2 indicates the number of pixels Kα×β in the direction D2. The character α indicates the position of the pixel in the array of the pixels Kα×β in the direction D1, specifically, is any of the integers of 1 to N1. The character β indicates the position of the pixel in the array of the pixels Kα×β in the direction D2, specifically, is any of the integers of 1 to N2. The N1 pixels Kα×β arranged in the direction D1 have constant pitches L1. The N2 pixels Kα×β arranged in the direction D2 have constant pitches L2.
The number of the plurality of pixels Kα×β arranged in the direction D1 (the line of pixels having a constant β) is N1. Specifically, the pixels Kα×β include a pixel K1×β, a pixel K2×β, . . . and a pixel KN1×β (β is constant) arranged sequentially in the direction D1. The pixels Kα×β (β is constant) arranged in the direction D1 constitute a plurality of pixel rows extending in the direction D1. The pixel K1×β, the pixel K2×β, . . . and the pixel KN1×β (β is constant) have identical shapes such as squares or circles as seen in the direction D3 that is perpendicular to the direction D1 and the direction D2, and also have approximately equal pixel areas as seen in the direction D3. Of the light P2 entering the array type light-receiving device 22, a light component having a predetermined wavelength is incident on the pixel K1×β, the pixel K2×β, . . . and the pixel KN1×β (β is constant).
On the other hand, the number of the plurality of pixels Kα×β arranged in the direction D2 (the line of pixels having a constant α) is N2. Specifically, the pixels Kα×β include a pixel Kα×1, a pixel Kα×2, . . . and a pixel Kα×N2 (α is constant) arranged sequentially in the direction D2. The pixels Kα×β (α is constant) arranged in the direction D2 constitute a plurality of pixel lines extending in the direction D2. The pixel Kα×1, the pixel Kα×2, . . . and the pixel Kα×N2 (α is constant) have identical shapes such as squares or circles as seen in the direction D3. The pixel Kα×1, the pixel Kα×2, . . . and the pixel Kα×N2 (α is constant) have different pixel areas from each other. The respective pixel areas (areas as seen in the direction D3) of the pixel Kα×1, the pixel Kα×2, . . . and the pixel Kα×N2 (α is constant) are determined in accordance with the wavelengths of light incident on the respective pixels.
The method for determining the respective pixel areas of a pixel Kα×1, a pixel Kα×2, . . . and a pixel Kα×N2 (α is constant) will be described below. It is provided that the pixel Kα×1, the pixel Kα×2, . . . and the pixel Kα×N2 (α is constant) each have a responsivity Rβ (β is an integer of 1 to N2) and a pixel area Aβ (β is an integer of 1 to N2) as seen in the direction D3 in accordance with the wavelengths of light incident on the respective pixels. Specifically, the light P2 dispersed by the spectroscopic device 3 includes a plurality of light components having a wavelength λ1, a wavelength λ2, . . . and a wavelength λN2. In the line of the pixel Kα×1, the pixel Kα×2, . . . and the pixel Kα×N2 (α is constant), a light component having a wavelength λβ is incident on the pixel Kα×β (α is constant and β is an integer of 1 to N2). The magnitudes of the values of the wavelength λ1, the wavelength λ2, . . . and the wavelength λN2 are λ1<λ2< . . . <λN2. Provided that the pixels Kα×β (α is constant and β is an integer of 1 to N2) show the lowest responsivity at a certain wavelength λi among the wavelength λ1 the wavelength λ2, . . . and the wavelength λN2, this lowest responsivity Ri of the responsivities Rβ is exhibited by a pixel in which β is i, namely, a pixel Kα×i. In other words, the pixel Kα×i is least responsive to the wavelength of light incident thereon among the pixels in the same pixel line, namely, the pixel Kα×1, the pixel Kα×2, . . . and the pixel Kα×N2 (α is constant). The pixel area Ai of this pixel Kα×i is made to be largest of the pixel areas Aβ. In other words, the pixel Kα=i is given the largest pixel area Ai of all the pixels included in the line of the pixel Kα×1, the pixel Kα×2, . . . and the pixel Kα×N2 (α is constant). The pixel area Ai is multiplied by the responsivity Ri to give a product E, and the pixel areas Aβ are determined using Aβ=E/Rβ. That is, specifically, the pixel areas Aβ of the pixels Kα×β (β is not i) in the line of the pixel Kα×1 the pixel Kα×2, . . . and the pixel Kα×N2 except the pixel Kα×i (α is constant) are the quotients of the product E divided by the responsivities Rβ of the pixels Kα×β (β is not i). Here, the product E is defined as the product of the responsivity Ri and the pixel area Ai of the pixel Kα×i. The responsivities Rβ of the pixels Kα×β (β is not i) correspond to the wavelengths of light incident on the respective pixels Kα×β (β is not i).
As described above, the pixel areas Aβ of the pixels Kα×β are determined such that the product of the responsivity Rβ multiplied by the pixel area Aβ is constant (the product E). Consequently, the pixels Kα×β are allowed to output uniform charges (or photocurrents) even when each of the pixels Kα×β receives one of light components of the light P2 having different wavelengths from each other. That is, an amount of light received by each of the pixels Kα×β is adjusted by controlling the pixel area Aβ according to the responsivity Rβ of the pixels Kα×β. As a result, the difference in charges (or photocurrents) output from the pixels Kα×β is reduced. Accordingly, the signals of the wavelength information having uniform and large S/N ratios are obtained for the pixels Kα×β (α is constant and β is an integer of 1 to N2) in the array type light-receiving device 22.
As mentioned above,
The arrangement of pixels Kα×β illustrated in
Referring to the spectral sensitivity characteristics illustrated in
Configurations of the photodetectors 2 will be described with reference to
The plurality of mesas M corresponds to the plurality of pixels Kα×β. The pixel areas of the plurality of pixels Kα×β are defined by the mesas M. Specifically, the pixel areas of the plurality of pixels Kα×β correspond to areas of the mesas M as seen in the direction D3 that is the direction perpendicular to the principal surface of the substrate 22a. The buffer layer 22b is disposed on the principal surface of the substrate 22a. The light-receiving layer 22c is disposed on the buffer layer 22b. The capping layer 22d is disposed on the light-receiving layer 22c. The mesas M are disposed on the substrate 22a. The mesa M includes the buffer layer 22b, the light-receiving layer 22c and the capping layer 22d. A region E1 shown in
The buffer layer 22b, the light-receiving layer 22c and the capping layer 22d are semiconductor layers sequentially disposed on the substrate 22a. For example, the substrate 22a is made of Fe-doped InP. The buffer layer 22b is made of n-type InGaAs doped with Si. The thickness of the buffer layer 22b is about 0.5 μm. The light-receiving layer 22c is made of non-doped InGaAs. The thickness of the light-receiving layer 22c is about 3 μm. The capping layer 22d is made of p-type InGaAs doped with Zn. The thickness of the capping layer 22d is about 1 μm. The p-side electrode 22f includes Ti/Pt/Au. The n-side electrode 22g includes Au/Ge/Ni. The passivation film 22e is made of a dielectric material such as SiO2 or SiN.
A process for manufacturing the photodetectors 2 will be schematically described with reference to
Next, the stacked semiconductor layer including the semiconductor layer 22b_1, the semiconductor layer 22c_1 and the semiconductor layer 22d_1 is etched by using a dry etching method. This etching results in the formation of mesas M corresponding to the pixels. A p-n junction is formed at an interface between the semiconductor layer 22c_1 (light-receiving layer 22c) and the semiconductor layer 22d_1 (capping layer 22d) in each of the mesas M. Further, a passivation film of SiO2 (corresponding to the passivation film 22e) is formed on the surface of the mesas M. The passivation film covers the p-n junction exposed at a side surface of the mesa M to reduce a leak current. Next, openings are formed in the passivation film to reach the surface of the semiconductor layer 22d_1, and p-side electrodes 22f are formed in the openings of the passivation film. Further, n-side electrodes 22g are formed on the surface of the semiconductor layer 22b_1 at locations corresponding to outer peripheries of array type light-receiving devices 22. Through these steps, a wafer is formed which includes array type light-receiving devices 22 illustrated in
Another configuration of the mesas M illustrated in
A process for manufacturing the photodetectors 2 of Modified Example 1 will be schematically described with reference to
Next, the stacked semiconductor layer including the semiconductor layer 22b_1, the semiconductor layer 22i_1, the semiconductor layer 22j_1 and the semiconductor layer 22k_1 is etched by using a dry etching method to form mesas M corresponding to the pixels. A p-n junction is formed at an interface between the semiconductor layer 22i_1 (light-receiving layer 22i) and the semiconductor layer 22j_1 (semiconductor layer 22j) in each of the mesas M. Further, a passivation film of SiO2 (corresponding to the passivation film 22e) is formed on the surface of the mesas M. The passivation film covers the p-n junction exposed at a side surface of the mesa M to reduce a leak current. Next, openings are formed in the passivation film to reach the surface of the semiconductor layer 22k_1, and p-side electrodes 22f are formed in the openings of the passivation film. Further, n-side electrodes 22g are formed on the surface of the semiconductor layer 22b_1 at locations corresponding to outer peripheries of array type light-receiving devices 22 of Modified Example 1. Through these steps, a wafer is formed which includes array type light-receiving devices 22 of Modified Example 1. Thereafter, the wafer is divided into a plurality of chips corresponding to the array type light-receiving devices 22 of Modified Example 1. On each of the chips, a plurality of bumps 23 is formed. This chip and a read-out circuit board 21 are bonded to each other through the plurality of bumps 23 by flip chip bonding. Through these steps, the photodetectors 2 of Modified Example 1 are produced.
Configurations of photodetectors 2_1 will be described with reference to
The plurality of impurity diffusion regions 22r corresponds to the plurality of pixels Kα×β. The pixel areas of the plurality of pixels Kα×β, are defined by the impurity diffusion regions 22r. Specifically, the pixel areas of the plurality of pixels Kα×β correspond to areas of the impurity diffusion regions 22r as seen in the direction D3 that is the direction perpendicular to the principal surface of the substrate 22m. The buffer layer 22n is disposed on the principal surface of the substrate 22m. The light-receiving layer 22p is disposed on the buffer layer 22n. The capping layer 22q is disposed on the light-receiving layer 22p. The impurity diffusion regions 22r are disposed on the surface (the surface S2) of the capping layer 22q. The impurity diffusion regions 22r extend from the surface of the capping layer 22q toward the light-receiving layer 22p. A region E2 shown in
The buffer layer 22n, the light-receiving layer 22p and the capping layer 22q are semiconductor layers sequentially disposed on the substrate 22m. For example, the substrate 22m is made of Si-doped InP. The buffer layer 22n is made of n-type InGaAs doped with Si. The thickness of the buffer layer 22n is about 0.5 m. The light-receiving layer 22p is made of non-doped InGaAs. The thickness of the light-receiving layer 22p is about 3 μm. The capping layer 22q is made of non-doped InP. The thickness of the capping layer 22q is about 1.5 μm. The p-side electrode 22t includes Au/Zn. The n-side electrode 22u includes Au/Ge/Ni. The mask 22s is made of a SiN film, for example.
A process for manufacturing the photodetectors 2_1 will be schematically described with reference to
Next, a mask composed of a SiN film (corresponding to the mask 22s) is provided on the surface of the semiconductor layer 22q_1. The mask has a pattern having openings through which p-type impurity such as zinc (Zn) is selectively diffused. Through the mask, zinc (Zn) is diffused from the surface of the semiconductor layer 22q_1 (capping layer 22q) toward the semiconductor layer 22p_1 (light-receiving layer 22p). This diffusion results in the formation of impurity diffusion regions 22r corresponding to the pixels. A p-n junction is formed at a diffusion front of Zn in the impurity diffusion regions 22r. For example, the p-n junction is formed at an interface between the semiconductor layer 22q_1 and the semiconductor layer 22p_1 in each of the pixels. The p-n junction may be formed at an upper portion of the semiconductor layer 22p_1. Next, p-side electrodes 22t are formed in the openings of the mask in contact with the top surface of the impurity diffusion regions 22r. In the embodiment, the mask on the surface of the semiconductor layer 22q_1 that is used for diffusing zinc (Zn) is not removed and becomes the mask 22s. Further, n-side electrodes 22u are formed on the surface of the semiconductor layer 22n_1 at locations corresponding to outer peripheries of array type light-receiving devices 22_1. Through these steps, a wafer is formed which includes array type light-receiving devices 22_1 illustrated in
Next, another configuration illustrated in
A process for manufacturing the photodetectors 2_1 of Modified Example 2 will be schematically described with reference to
Next, a mask composed of a SiN film is formed on the surface of the semiconductor layer 22y_1. The mask has a pattern having openings through which p-type impurity such as zinc (Zn) is selectively diffused. Through the mask, zinc (Zn) is selectively diffused from the surface of the semiconductor layer 22y_1 (capping layer 22y) toward the semiconductor layer 22w_1 (light-receiving layer 22w) through the semiconductor layer 22x_1 (semiconductor layer 22x). This selective diffusion results in the formation of impurity diffusion regions 22z corresponding to the pixels. A p-n junction is formed at a diffusion front of Zn in the impurity diffusion regions 22z. The concentration and diffusion depth of Zn impurity in the semiconductor layer 22w_1 (light-receiving layer 22w) is controlled by adjusting the thickness of the semiconductor layer 22x_1. For example, the p-n junction is formed in the semiconductor layer 22x_1 or at an interface between the semiconductor layer 22x_1 and the semiconductor layer 22w_1. The p-n junction may be formed at an upper portion of the semiconductor layer 22w_1. Next, p-side electrodes 22t are formed in the openings of the mask on the surface of the impurity diffusion regions 22z while remaining the mask on the surface of the semiconductor layer 22y_1. The p-side electrodes 22t are in contact with the top surface of the impurity diffusion regions 22z. Further, n-side electrodes 22u are formed on the surface of the semiconductor layer 22n_1 at locations corresponding to outer peripheries of array type light-receiving devices 22_1 of Modified Example 2. Through these steps, a wafer is formed which includes array type light-receiving devices 22_1 of Modified Example 2. Thereafter, the wafer is divided into a plurality of chips corresponding to the array type light-receiving devices 22_1 of Modified Example 2. On each of the chips, a plurality of bumps 23 is formed. This chip and a read-out circuit board 21 are bonded to each other through the plurality of bumps 23 by flip chip bonding. Through these steps, the photodetectors 2_1 of Modified Example 2 are produced.
While preferred embodiments have been discussed above while illustrating the principle of the present invention, those skilled in the art will appreciate that various modifications may be made to the configurations and the details discussed above without departing from the principle of the invention. The scope of the invention is not limited to any specific configurations disclosed in the embodiments. Therefore, the features defined in the appended claims and all modifications and alterations which are within the spirit of the invention are claimed.
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2014-115879 | Jun 2014 | JP | national |
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20150355026 A1 | Dec 2015 | US |