Abstract:
A photodiode that is used in an optical communication system using two different wavelengths, λ1 and λ2 (λ1&lt;λ2), and that enables a reduction in the optical crosstalk caused by outgoing light having a longer wavelengths, λ2. A photodiode that receives light having a shorter wavelengths, λ1, is provided with an absorption layer made of a mate having a bandgap wavelength, λg. (λ1&lt;λg&lt;λ2), to detect the light having λ1. A filter layer that absorbs unwanted light having λ2 is provided over the absorption layer so that the light having λ2 cannot return to the absorption layer after passing through it once.

Description:
BACKGROUND OF THE INVENTION  
         [0001]    1. Field of the Invention  
           [0002]    The present invention relates to the structure of a photodiode used in an optical transceiver module for an optical communication system in which one optical fiber is used for carrying out transmission and reception of signals by using two different wavelengths, λ1 and λ2 (λ1&lt;λ2). The photodiode can detect light having a shorter wavelength, λ1, by dexterously eliminating the influence of outgoing light having a longer wavelength, λ2. It should be noted that the photodiode is for detecting light having a shorter wavelength, not for detecting light having a longer wavelength. To be blocked is the light having a longer wavelength, not the light having a shorter wavelength.  
           [0003]    2. Description of Related Arts  
           [0004]    When one optical fiber is used for both transmission and reception of signals, a laser diode (LD), which emits outgoing light, and a photodiode (PD), which receives incoming light, are placed usually in the same housing or on the same platform. Similarly, when one optical fiber is used for transmitting signals uni-directionally by using two or more different wavelengths, two or more PDs are placed usually on the same platform. A PD is a device having high sensitivity. An LD emits intense outgoing light to transfer signals to a distant place. Although the PD and LD act at different wavelengths, the PD has sensitivity to the outgoing light and detects it. When an LD and a PD are placed on the same terminal, if the PD detects the outgoing light emitted by the LD, this phenomenon is called optical crosstalk. The outgoing light acts as noise for the PD. When the PD detects the outgoing light, incoming light cannot be detected accurately. Therefore, it is necessary to minimize the crosstalk between the PD and LD. Undoubtedly, there can be electrical crosstalk between a transmitter and a receiver caused by the magnetic coupling between their electric circuits. However, to be solved here is the problem of optical crosstalk.  
           [0005]    Researchers and engineers have devised various types of transceivers that carry out transmission and reception of signals over one optical fiber. Those transceivers employ different methods for separating the outgoing light and incoming light. The most popular method uses an optical wavelength demultiplexer to branch the path for the outgoing light and the path for the incoming light. Such a method in which the two paths are separated spatially can solve the problem of optical crosstalk relatively easily. There is a rather special transceiver module in which a PD and an LD are arranged in a straight line. Such a method in which almost the same path is used for both transmission and reception makes it difficult to solve the problem of optical crosstalk.  
           [0006]    [0006]FIG. 1 shows a system of simultaneous bidirectional optical communication in which one optical fiber connects a central office and a subscriber for carrying out bidirectional signal transmission by using two different wavelengths, λ1 and λ2. This is a system of wavelength division multiplexing (WDM) bidirectional communication. A central office generates a signal using LD1 and sends it to PD2 at a subscriber via an optical fiber  1 , an optical wavelength demultiplexer  2 , an optical fiber  3 , an optical wavelength demultiplexer  4 , and an optical fiber  5 . The subscriber generates another signal using LD2 and sends it to PD1 at the central office via an optical fiber  6 , the optical wavelength demultiplexer  4 , the optical fiber  3 , the optical wavelength demultiplexer  2 , and an optical fiber  7 . Thus, signals can be transmitted in opposite directions at the same time over one optical fiber.  
           [0007]    At the central office, the optical wavelength demultiplexer  2  is connected to the optical fibers  7  and  1  to separate an upstream signal and a downstream signal according to their wavelengths. The outgoing light carrying downstream signals has the wavelength λ2 and the incoming light carrying upstream signals has the wavelength λ1. The downstream and upstream signals travel over the one optical fiber  3  at the same time.  
           [0008]    At the subscriber, the optical wavelength demultiplexer  4  is connected to the optical fibers  5  and  6  to separate incoming light and outgoing light. The photodiode PD2 receives incoming light having the wavelength λ2, and LD2 generates outgoing light having the wavelength λ1. Although not shown, there are individual electric circuits beyond PD2 and LD2.  
           [0009]    The present invention addresses problems related to a transceiver at a central office. Problems at a central office are different from those at a subscriber because the aspect related to wavelength is reversed In the example shown in FIG. 1, the optical wavelength demultiplexers  2  and  4  spatially separate the optical paths of the outgoing light and the incoming light. Therefore, the problem of optical crosstalk can be solved by the improvement of the performance of the optical wavelength demultiplexer, for example. The problem to be solved by the present invention is the optical crosstalk between the PD and LD at a central office.  
           [0010]    [0010]FIG. 2 shows another system in which two signals are transmitted unidirectionally from a central office to a subscriber by using different wavelengths, λ1 and λ2. This is a system of WDM unidirectional communication. A central office generates two signals by using two different LDs. They are combined at an optical wavelength multiplexer  8  and transmitted from the central office to a subscriber over one optical fiber. At the subscriber, the two signals are separated according to their wavelengths by an optical wavelength demultiplexer  4 . The photodiodes PD1 and PD2 selectively receive the signals. Here, crosstalk between PD1 and PD2 also poses a problem.  
           [0011]    [0011]FIG. 3 shows a typical example of a conventional PD module used as a receiver in an optical communication system in which the optical paths are separated as shown in FIGS. 1 and 2. This type of PD module is still mainly used. Lead pins  9  are provided at a circular metal stem  10 , at the center of which a submount  11  supports a PD chip  12 . A lens  13  is attached to a cylindrical cap  14  welded to the stem  10  in alignment. A cylindrical sleeve  15  is placed on the cap. A ferrule  16  is inserted into the mandrel hole of the sleeve  15 . The ferrule  16  supports the end of an optical fiber  17 . The tip of the ferrule  16  is polished on the skew. The sleeve  15  is covered with a bend limiter  18  to protect the optical fiber  17 . This explains the structure of a PD module currently in use. The systems shown in FIGS. 1 and 2 also include LD modules. In an LD module, only the PD shown in FIG. 3 is replaced by an LD. Therefore, an LD module has a structure similar to that of a PD module, and no explanation about it is provided here. PD modules and LD modules now in use employ a metal case, so that optical fibers are arranged stereoscopically (three-dimensionally). Although high in performance, those modules require centering work at the time of assembly. The centering is a time-consuming job and increases the manufacturing cost. Because of the high price, those modules are not suitable in achieving widespread application.  
           [0012]    Researchers and engineers have been energetically studying surface-mounted types for use as less costly PD modules, LD modules, or PD-LD modules. FIG. 4 shows an example of a conventional surface-mounted-type module that uses a back-illuminated-type PD. A rectangular silicon platform  19  is provided with a longitudinal, V-shaped groove  20  at the center. The groove is formed by etching. A slanted mirror face  21  is provided at the end of the V-shaped groove  20 . The etching work simultaneously forms the mirror face  21  also. A PD chip  23  is fixed directly above the end portion of the V-shaped groove  20 . The PD chip  23 , a back-illuminated-type PD, is provided with a photo-sensitive area  24  at the upper zone. The light emerging from an optical fiber  22  propagates in the V-shaped groove  20  in parallel with the surface of the silicon platform, is reflected upward by the mirror face  21 , enters the PD  23  at the back side, and reaches the photo-sensitive area  24 . A surface-mounted-type module has no centering portion. Elimination of centering work accomplishes easy manufacturing.  
           [0013]    Both the PD modules shown in FIGS. 3 and 4 can be used for detecting the incoming light separated by the optical wavelength demultiplexers shown in FIGS. 1 and 2. An optical wavelength demultiplexer can be produced, for example, by forming a wavelength-selective branching waveguide on a silicon platform. There is also a prism-type optical wavelength demultiplexer as shown in FIG. 5. A dielectric multilayer film  27  is deposited on the oblique face of transparent triangular-column glass blocks  25  and  26  for wavelength selectivity. For example, when light emerges from an optical fiber  28 , the light having a specific wavelength is reflected and the other light having a different wavelength is transmitted In FIG. 5, however, the wavelength selectivity is used for distinguishing the outgoing light from the incoming light. More specifically, the incoming light (wavelength: λ2) emerging from the optical fiber  28  is reflected by the multilayer film  27  and introduced into a PD  30 . The outgoing light (wavelength: λ1) emitted from an LD  29  passes through the multilayer film  27  and enters the optical fiber  28 .  
           [0014]    However, the present invention whose intention is to minimize the optical crosstalk can be most suitably applied to a transceiver module in which the optical paths are not separated by an optical wavelength demultiplexer. Such a module is called an optical path non-separated type in the present invention in order to distinguish from the foregoing optical path-separated type. In the optical path non-separated type, a PD is placed at the side of the optical fiber and an LD is placed in line with the optical fiber. This type requires no optical wavelength demultiplexer. This is advantageous because the size becomes smaller and the structure becomes simpler. On the other hand, this type has a common optical axis for outgoing light and incoming light. As a result, the problem of optical crosstalk becomes more serious.  
           [0015]    [0015]FIG. 6 shows an example of an optical path non-separated type for a module at a subscriber. The wavelengths of the outgoing light and incoming light are opposite to those at a central office. Although not shown, there is a silicon platform in a housing  31 . An optical fiber  32  is housed longitudinally. An LD  33  is mounted opposite to the end of the optical fiber  32 . A WDM filter  35  is provided at some point in the optical fiber  32  near its end to carry out wavelength distinction. A PD  34  is placed directly above the WDM filter  35 . The outgoing light (wavelength: λ1) emitted by the LD  33  is as powerful as 1 mW, for example. The outgoing light propagates to the outside through the optical fiber  32 . The incoming light (wavelength: λ2) having propagated through the optical fiber  32  from the outside is reflected by the WDM filter  35 , enters the PD  34  at the back side, and is detected by a photo-sensitive area  36 . Whereas the out-going light is intense, the incoming light is weak. The outgoing light propagates to the WDM filter  35  through the same optical fiber  32  in the direction opposite to the incoming light. When passing through the WDM filter, part of the outgoing light may enter the PD. This intruding light causes the optical crosstalk. Notwithstanding the small percentage, the intruding light becomes an un-ignorable noise in comparison with the intensity of the incoming light, because the outgoing light is intense and the incoming light is weak.  
           [0016]    [0016]FIG. 7 shows a conventional PD that has a wide range of sensitivity. When this type of PD is used, the problem of optical crosstalk becomes more serious. The structure of the InP-based PD shown in FIG. 7 is based on an epitaxial wafer in which an n-InP buffer layer  38 , an n-InGaAs absorption layer  39 , and an n-InP cap layer  40  are laminated on an n-InP substrate  37 . At the upper zone of the PD, a p-type region  41  and a p electrode passivation layer  44  are formed. On the bottom surface, a ring-shaped n electrode  45  and an anti-reflection layer  46  are provided. When such a PD is used as a photodetector, the level of the noise caused by the outgoing light becomes higher than the signal level of the incoming light. In other words, the signal/noise ratio (S/N ratio) becomes smaller than one. When an ordinary PD, which has sensitivity to both λ2 and λ1, is used, the foregoing undesirable phenomenon occurs.  
           [0017]    [0017]FIG. 8 is a graph showing the sensitivity characteristics of the PD shown in FIG. 7. The P portion in the shorter wavelength region, in which the sensitivity decreases with decreasing wavelength, corresponds to the bandgap of the InP substrate. The light having a shorter wavelength than that corresponding to the bandgap is not detected because it is absorbed by the InP substrate. The R portion in the longer wavelength region, in which the sensitivity decreases with increasing wavelength, corresponds to the bandgap of the InGaAs absorption layer. The Light having a longer wavelength than that corresponding to the bandgap is not detected because its energy is lower than the bandgap of the absorption layer. In other words, the PD has sensitivity in a wide range of Q from the bandgap wavelength P of the InP substrate to the bandgap wavelength R of the InGaAs absorption layer. Therefore, the PD has sufficient sensitivity not only at the 1.3-μm band but also at the 1.55-μm band.  
           [0018]    As described above, the PD having a conventional structure as shown in FIG. 7 has sensitivity in a wide range of 1.0 to 1.65 μm as shown in FIG. 8. It is advantageous to have sensitivity in a wide range as above because the same PD can be used for both the 1.3-μm band and 1.55-μm band. Therefore, the PD having a structure as shown in FIG. 7 is most widely used for the long-wavelength light employed in optical communications. However, when the PD is used for a transceiver module, the PD also detects the outgoing light in addition to the incoming light, which means that the outgoing light acts as noise. Consequently, the PD is disadvantageous in that optical crosstalk occurs between the outgoing light and incoming light.  
           [0019]    In the transceiver module shown in FIG. 6, not all the intense outgoing light (wavelength: λ1) emitted from the LD placed on the silicon platform (silicon bench) enters the optical fiber. The light emitted from the LD spreads out at a considerably wide angle. Some of the light strikes the silicon platform and plastics to be scattered. The silicon platform is transparent to the outgoing light. The outgoing light having entered the space made by the silicon platform and transparent plastics passes through the silicon, is reflected, and is scattered Various complicated scattered rays of light are produced according to the distribution of the plastics, the shape of the silicon platform, and the arrangement of the other devices. When looked from the PD, the entire silicon platform shines brightly due to the scattering of the outgoing light. Such components of the outgoing light that enter the PD through various paths other than the designed path are called “scattered light” or “stray light.” 
           [0020]    Some components of the outgoing light enter the PD from various directions and at various heights. They enter the PD at the back side, at the front side, and at the side face. Such components of the outgoing light that enter the PD without entering the optical fiber cause the crosstalk. Such crosstalk caused by the scattered light (stray light) that does not pass through the WDM filter cannot be suppressed by the improvement of the performance of the WDM filter. When the output power of the LD is increased, the outgoing light propagating through the optical fiber increases the amount of the leakage at the WDM filter. The component of the outgoing light emitted from the LD that enters the PD after being refracted and reflected at the WDM filter is called “leakage light.” 
           [0021]    The unexamined Japanese patent publication (Tokukaihei) No.4-213876 entitled “Photodetector” proposes a photodetector that is a PD comprising two stages of absorption layers. A layer structure that absorbs 1.55-μm light is provided on an InP substrate and a p electrode is provided on the layer structure. On part of the layer structure, another layer structure that absorbs 1.3-μm light is provided and another p electrode is provided on this layer structure. A common n electrode is provided on the bottom surface of the InP substrate. Consequently, the photodetector has a two-stage structure in which PD1 for absorbing the light having λ1 (1.3 μm) is placed at the top and PD2 for absorbing the light having λ2 (1.55 μm) is placed at the bottom.  
           [0022]    The light having λ2 and the light having λ1 enter the photodetector at the front side. Since the light having λ2 has a longer wavelength, it passes through the upper layer structure and reaches the lower layer structure to generate optical current there. In other words, PD2 absorbs the light having λ2 at the bottom. The light having λ1, which is shorter, is absorbed by PD1 in the upper structure to generate optical current there. In other words, PD1 can detect the light having λ1 at the top. In order to prevent the penetration of the light having λ1 into the lower structure, a layer having a thickness of d=mλ 1/(2n), where m is a plus integer and n is a refractive index, is provided between PD1 and PD2. The object of this layer is to reflect the light having λ1 upward so that the light having λ1 cannot enter PD2. Hence, this layer is called a “selective reflection layer.” If the light having λ1 enters PD2, the light causes PD2 to generate optical current, so that crosstalk occurs. The selective reflection layer is provided to prevent this type of crosstalk.  
           [0023]    However, this patent application provides no preventive measure against crosstalk in the opposite case. Such a case is out of its expectations. There is no measure against the phenomenon that the light having λ2 is reflected by the n electrode at the bottom, returns to PD1, and adversely affects its performance. Since the selective reflection layer provided between PD1 and PD2 reflects the light having λ1 but transmits the light having λ2, the light having λ2 reflected at the bottom face can pass through the layer upward.  
           [0024]    Another unexamined Japanese patent publication, (Tokukaihei) No.9-166717, entitled “Optical receiver module and optical transceiver module” proposes a photodetector for a system in which two signals having different wavelengths, λ1=1.3 μm and λ2=1.55 μm, are transmitted through one optical fiber. A first photodiode, PD1, absorbs the light having λ1 and transmits the light having λ2. A second photodiode, PD2, placed behind PD1, absorbs the light having λ2. Two independent PDs are combined in tandem. They are not such composite devices as described above. The photodiode PD1 has an absorption layer that has an intermediate bandgap wavelength as expressed in λ1&lt;λg&lt;λ2, where λg represents the bandgap wavelength of the absorption layer. Since λg is longer than λ1, the absorption layer absorbs and detects the light having λ1. The light having λ2 passes through PD1 and is detected by PD2. FIG. 9 shows the structure of the PD for absorbing the light having λ1 proposed by Tokukaihei No.9-166717. The PD is placed in an intermediate place to transmit the light having the longer wavelength. For this purpose, the PD has another opening at the side opposite to the light-entering face to allow the light having the longer wavelength to leave the PD. The PD can be called a dual opening type, because it has openings at both sides for transmitting light.  
           [0025]    An n-InP buffer layer  51 , an n-InGaAsP absorption layer  52  (λg=1.42 μm), and an n-InGaAsP window layer  53  are grown epitaxially on an n-IP substrate  50 . At the center portion, Zn is diffused to provide a p-type region  54 . The center portion of the p-type region  54  is covered by an anti-reflection layer  56 . Around the anti-reflection layer  56 , a ring-shaped p electrode  55  is provided At the outside of the p electrode  55 , a passivation layer  57  is formed to protect the edge portion of the pn junction. A ring-shaped n electrode  58  is formed on the bottom surface of the InP substrate  50 . The inside of the n electrode  58  forms an opening and is covered by an anti-reflection layer  59 . Both the front and back sides have openings for transmitting light. The ring-shaped electrodes are provided without overlapping with these openings. The anti-reflection layers are provided at the openings to prevent incident light from attenuating due to reflection.  
           [0026]    [0026]FIG. 10 shows a transmittance spectrum of the InGaAsP absorption layer  52  (λg=1.42 μm). The mixing ratio of its quaternary mixed crystal is decided for the bandgap wavelength to take an intermediate value between 1.3 μm and 1.55 μm. The measured restart proves the design concept. The light having a wavelength shorter than 1.4 μm is absorbed almost completely, which means that the light practically does not pass through the layer. A wavelength of 1.42 μm forms the boundary condition. Almost one hundred percent of the light having a wavelength longer than 1.5 μm passes through the absorption layer. The transmittance varies with the thickness. The absorption layer has an enough thickness so that the light having a shorter wavelength can be absorbed completely.  
           [0027]    The present invention intends to prevent a PD that detects the light having a shorter wavelength from suffering the crosstalk caused by the light having a longer wavelength. In the explanation below, the shorter wavelength, λ1, is supposed to be 1.3 μm and the longer wavelength, λ2, to be 1.55 μm in order to specifically show the relation between the two wavelengths. In the present invention, however, λ1 is in the range of 1.2 to 1.38 μm, and λ2 is in the range of 1.45 to 1.65 μm. At a central office, if a PD as shown in FIG. 7, which usually has sensitivity in a wide range, is used as a photodetector, it also detects the scattered light and leakage light of the outgoing light. At a central office, the incoming light has a wavelength of 1.3 μm, and the outgoing light, 1.55 μm. This combination of wavelengths is advantageous in eliminating the effect of the outgoing light. Dexterous exploitation of the basic properties of the semiconductor enables the production of a PD for a central office that detects the incoming light (λ1=1.3 μm ) but does not detect the outgoing light (λ2=1.55 μm). This can be accomplished by selecting the bandgap wavelength λg of the absorption layer of the PD to satisfy the following formula:  
           λ1(incoming light)&lt;λg&lt;λ2(outgoing light).  
           [0028]    This is possible because the two wavelengths at a central office have such an advantageous relationship. If the bandgap wavelength λg of the absorption layer is decided to be 1.35 to 1.45 μm, for example, then the absorption layer should have a desirable quality that it detects the incoming light but does not detect the outgoing light. A bandgap wavelength can be adjusted to 1.35 to 1.45 μm by using a quaternary mixed crystal of InGaAsP. In the present invention, however, λg is in the range of 1.3 to 1.5 μm.  
           [0029]    [0029]FIG. 10 shows a light transmittance of an InGaAsP quaternary mixed-crystal layer having a bandgap wavelength of 1.42 μm. The absorption layer of the PD shown in FIG. 9 is made of such a mixed-crystal. Its transmittance is zero for 1.3-μm light (incoming light). In other words, it absorbs and detects 1.3-μm light completely. On the other hand, its transmittance is almost one hundred percent for 1.55-μm light (outgoing light). In other words, it transmits 1.55-μm light almost completely, which means it does not detect 1.55-μm light. Therefore, a PD as shown in FIG. 9, which has wavelength selectivity, can be used singly as a photodetector at a central office. The PD shown in FIG. 9 has an opening both at the front and back sides, because behind the PD another PD for detecting 1.55-μm light is to be placed. However, when a PD is used at a central office, only one opening is required because the PD has only to absorb 1.3-μm light. If the PD is a back-illuminated type, the front side is covered by the p electrode. If the PD is a front-illuminated type, the back side is covered entirely by the n electrode. Such a PD can be used as a photodetector at a central office without modification.  
           [0030]    [0030]FIG. 11 shows a back-illuminated type PD conceived on the basis of the above-described consideration for the use in a central office. Although the PD is almost the same as that shown in FIG. 9, it has a slightly different structure in the vicinity of the p electrode. An n-InP buffer layer  61 , an n-InGaAsP absorption layer  62  (λg=1.42 μm), and an n-InP cap layer  63  are grown epitaxially on an n-InP substrate  60 . At the center portion of the chip, Zn is diffused to provide a p-type region  64 . A p electrode  65  having no opening is provided to cover almost the entire p-type region  64 . Since the front side is not required to admit light, no opening is provided there. At the outside of the p electrode  65 , a passivation layer  67  is formed to protect the edge of the pn junction. Since light enters the PD at the back side, the back-side structure is the same as in FIG. 9. A ring-shaped n electrode  68  is formed on the bottom surface of the InP substrate  60 . The inside of the n electrode  68  forms an opening for admitting light and is covered by an anti-reflection layer  69 . The ring-shaped electrode is provided without overlapping with the opening.  
           [0031]    It should be possible to use a PD having such a structure as a photodetector at a central office. Nevertheless, the present inventors found that when such a PD is used as a photodetector at a central office, crosstalk occurs due to the influence of 1.55-μm light (outgoing light at the central office). It was out of the present inventors&#39; expectations. The InGaAsP absorption layer  62  has a bandgap wavelength of 1.42 μm. Since it is shorter than 1.55 μm, the present inventors expected the absorption layer to be insensitive to 1.55-μm light as an ideal case. However, the result showed differently. The present inventors found that when the absorption layer  62  has a thickness of 5 μm, it detects about 0.2% of 1.55-μm light. The absorption layer absorbs 100% of 1.3-μm light. The fact that the absorption layer detects 1.55-μm light even in small magnitudes poses a problem. Although 1.55-μm light has an energy lower than the bandgap energy, there are some impurity levels in the bandgap, and these levels effect the slight sensitivity to 1.55-μm light. At a central office, there is imbalance in intensity of light. Whereas the 1.55-μm outgoing light generated in the office is intense, the 1.3-μm incoming light having propagated over an optical fiber is weak. The 1.55-μm outgoing light is more intense than the 1.3-μm incoming light by orders of magnitude. Therefore, even the 0.2% sensitivity can produce an un-ignorable magnitude in noise level because the multiplier has a considerable magnitude.  
         SUMMARY OF THE INVENTION  
         [0032]    An object of the present invention is to offer a photodiode in which crosstalk caused by the intrusion of intense 1.55-μm outgoing light into the 1.3-μm-light detection portion at a central office can be reduced. This reduction in crosstalk can be accomplished by devising the configuration of the photodiode.  
           [0033]    The present invention intends to reduce the crosstalk caused by 1.55-μm light by preventing or impeding the return of the outgoing light (λ2=1.55 μm) to the absorption layer after passing through the absorption layer once. In order to achieve this purpose, a layer for absorbing 1.55-μm light is additionally provided at the inside or at the outside of a PD. In the present invention, this additionally provided absorption layer is called a “filter layer.” Since these filter layers absorb unwanted 1.55-μm light, the light does not return to the absorption layer for 1.3-μm light, or its intensity is notably reduced even if it returns. This measure can effectively reduce the crosstalk to the 1.3-μm light by the 1.55-μm light predominant at a central office. The methods for providing filter layer for absorbing the 1.55-μm light include the following four types:  
           [0034]    Type 1: To replace the InP cap layer by a thick InGaAs cap layer;  
           [0035]    Type 2: To provide an InGaAs filter layer by epitaxial growth and remove its peripheral region;  
           [0036]    Type 3: To laminate an InGaAs filter layer on the p-type region by the selective growing method; and  
           [0037]    Type 4: To laminate a filter layer made of a plastic resin or another material on the entire top surface of a chip.  
           [0038]    When a material that absorbs 1.55-μm light is provided on the p-type region as mentioned above, the 1.55-μm light (outgoing light) that has once passed through the p-type region does not return to the absorption layer, or it loses its intensity notably even if it returns. The methods are not limited to the above-mentioned four types providing that a newly conceived method can achieve a similar effect. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0039]    In the drawings:  
         [0040]    [0040]FIG. 1 is a schematic diagram showing a system of simultaneous bidirectional optical communication in which one optical fiber connects a central office and a subscriber for carrying out bidirectional signal transmission by using two different wavelength, λ1 and λ2;  
         [0041]    [0041]FIG. 2 is a schematic diagram showing a system of simultaneous unidirectional optical communication in which one optical fiber connects a central office and a subscriber for carrying out unidirectional signal transmission by using two different wavelength, λ1 and λ2;  
         [0042]    [0042]FIG. 3 is a partial cutaway and partial cross-sectional view of a conventional PD that is housed in a metal housing and that has a three-dimensional structure;  
         [0043]    [0043]FIG. 4 is a cross-sectional view of a conventional surface-mounted-type PD module;  
         [0044]    [0044]FIG. 5 is a schematic diagram showing the constitution of a prism-type optical wavelength demultiplexer comprising glass blocks provided with a dielectric multilayer film;  
         [0045]    [0045]FIG. 6 is a schematic diagram showing the constitution of a conventional optical transceiver module at a subscriber that has an LD for generating outgoing going light (wavelength: λ1) and a PD for receiving incoming light (wavelength: λ2) (λ1&lt;λ2);  
         [0046]    [0046]FIG. 7 is a cross-sectional view of a conventional PD having an InGaAs absorption layer having sensitivity in a wide range including λ1 and λ2;  
         [0047]    [0047]FIG. 8 is a graph showing the sensitivity-wavelength characteristic of a conventional PD, in which the axis of abscissa represents wavelength (μm) and the axis of ordinate represents sensitivity (A/W);  
         [0048]    [0048]FIG. 9 is a cross-sectional view of the 1.3-μm-light-detecting PD in the combination of a 1.3-μm-light-detecting PD and a 1.55-μm-light-detecting PD that is disclosed in the published Japanese patent application Tokukaihei 9-166717;  
         [0049]    [0049]FIG. 10 is a graph showing the light transmittance-wavelength characteristic of the InGaAsP layer of the PD shown in FIG. 9, in which the axis of abscissa represents wavelength (μm) and the axis of ordinate represents transmittance (%);  
         [0050]    [0050]FIG. 11 is a cross-sectional view of a 1.3-μm-light-detecting PD produced by dosing the front-side opening of the 1.3-μm-light-detecting PD shown in FIG. 9 by the p electrode;  
         [0051]    [0051]FIG. 12 is a cross-sectional view of a PD for detecting light having λ1 (λ1 &lt;λ2) of Type 1 of the present invention, in which an InGaAs cap layer that can absorb light having λ2 is provided on the entire absorption layer;  
         [0052]    [0052]FIG. 13 is a cross-sectional view of a PD for detecting light having λ1 (λ1 &lt;λ2) of Type 2 of the present invention, in which an InGaAs filter layer that can absorb light having λ2 is provided only on the center portion of the cap layer;  
         [0053]    [0053]FIG. 14 is a cross-sectional view of a PD for detecting light having λ1 (λ1 &lt;λ2) of Type 3 of the present invention, in which an InGaAs filter layer that can absorb light having λ2 is selectively grown at the inside of the p electrode.  
         [0054]    [0054]FIG. 15 is a cross-sectional view of a PD for detecting light having λ1 (λ1 &lt;λ2) of Type 4 of the present invention, in which a plastic resin that can absorb light having λ2 is applied to the entire top surface of the chip.  
         [0055]    [0055]FIG. 16 is a cross-sectional view of an example in which the Type 4 PD of the present invention is used for a surface-mounted-type PD module at a central office.  
         [0056]    [0056]FIG. 17 is a cross-sectional view of an example in which the Type 4 PD of the present invention is used for a surface-mounted-type transceiver module at a central office. 
     
    
     DETAILED DESCRIPTION OF THE INVENTION  
       [0057]    The present invention features a back-illuminated-type PD that has on the p-type region a layer made of a material that absorbs light having λ2 for preventing the return of the light after reflection so that the light cannot pass through the absorption layer twice. Although this PD does not prevent the first passage of light having λ2 through the absorption layer, it can prevent the second passage. This concept is realized through the process described below.  
         [0058]    The PD for 1.3-μm light shown in FIG. 9 detects 0.1% of 1.55-μm light. However, the PD for 1.3-μm light produced for central-office use shown in FIG. 11 has a higher sensitivity to 1.55-μm light; it detects 0.2% of 1.55-μm light. Although the two PDs have the same absorption-layer thickness, 5 μm, the effects differ by a factor of two. The study on the difference revealed that the sensitivity increase is caused by the phenomenon that the 1.55-μm light is reflected by the p electrode  65 , which covers the entire p-type region, and passes through the absorption layer once more. In FIG. 11, the thicker arrow represents the light (λ1=1.3 μm) to be detected. This light is absorbed by the InGaAsP absorption layer  62 , generates an optical current in proportion to its intensity, and disappears. This function is in accordance with the design concept and poses no problem. At a central office, however, when the intense outgoing going 1.55-μm light enters at the back side, it passes through the InGaAsP absorption layer  62  upward from under, generating a slight optical current. This does not terminate the action of the light. It is reflected by the under side of the p electrode  65  and passes through the absorption layer  62  once more in the opposite direction, generating optical current again. As a result, crosstalk occurs twice. This is the reason why the PD shown in FIG. 9 has a sensitivity of 0.1% to 1.55-μm light and the PD shown in FIG. 11 has a sensitivity two times as much, 0.2%.  
         [0059]    The present invention intends to reduce the crosstalk caused by 1.55-μm light by preventing or impeding the return of the 1.55-μm light to the absorption layer after passing through the absorption layer once. In order to achieve this purpose, a layer (filter layer) for absorbing 1.55-μm light is additionally provided at the inside or outside of the PD structure. Since these filter layers absorb unwanted 1.55-μm light, the light does not return to the absorption layer for 1.3-μm light, or its strength is notably reduced even if it returns. This measure can effectively reduce the crosstalk to the 1.3-μm light by the 1.55-μm light predominant at a central office. The present invention provides a material that absorbs light having λ2 on the p-type region. The providing methods are classified into four groups, which are explained below, according to their differences.  
         [0060]    Type 1: Thick Cap Layer (FIG. 12)  
         [0061]    [0061]FIG. 12 shows an embodiment of the present invention in which a thick InGaAs cap layer (filter layer) is provided on the absorption layer. An n-InP buffer layer  61 , an n-InGaAsP absorption layer  62  (λg=1.42 μm), and an n-InGaAs cap layer (filter layer)  78  are grown epitaxially on an n-InP substrate  60 . At the center portion of the chip, Zn is diffused to provide a p-type region  64 . Another p-type region is formed at the periphery of the chip at the same time. This additional p-type region is referred to as a Zn-diffused shield layer  71 . A ring-shaped p electrode  65  is provided on the p-type region  64 . Directly under the ring-shaped p electrode  65 , there lies a portion in which the n-InGaAs cap layer  78  is converted into the p-type region. Since the p electrode has an opening at its inside, it is called a ring-shaped electrode. The p electrode  65  can have any inside and outside shapes, such as a circle, oval, square, pentagon, or hexagon (this is to be applied also to Types 2 to 4).  
         [0062]    An InP layer is used usually as the cap layer on the absorption layer. However, InP cannot absorb light having λ2 because it has a wide bandgap. Consequently, Type 1 employs InGaAs in place of InP as the cap layer so that the layer itself can absorb light having λ2. Because InGaAs has a narrow bandgap, it can absorb light having λ2. Therefore, the cap layer can also be called a filter layer.  
         [0063]    An anti-reflection layer  72  is formed on the p-type region  64  at the inside of the p electrode  65 . Since the PD is a back-illuminated type, the anti-reflection layer  72  is not for admitting light, but for allowing the unwanted light having λ2 to leave the PD without being reflected. At the outside of the p electrode  65 , a passivation layer  67  is formed to protect the edge of a pn junction  66 . Since light enters the PD at the back side, the back-side structure is the same as in FIG. 9. A ring-shaped n electrode  68  is formed on the bottom surface of the InP substrate  60 . The inside of the n electrode  68  forms an opening and is covered by an anti-reflection layer  69 . As with the p electrode  65 , the n electrode  68  can have any inside and outside shapes, such as a circle, oval, square, or octagon (this is to be applied also to Types 2 to 4). Table I shows the thickness and carrier concentration of the epitaxial layers.  
                                     TABLE I                               Carrier           Layer&#39;s thickness   concentration       Layer&#39;s name   (μm)   (cm −3 )                                InGaAs cap layer (filter layer) (78)   5   p = 10 18         InGaAsP absorption layer (62)   5   n = 10 15         InP buffer layer (61)   4   n = 10 15         InP substrate (60)   200   n = 10 18                    
 
         [0064]    The p-InGaAs cap layer is produced by converting the n-InGaAs cap layer  78  into a p type by the diffusion of Zn. The layer is as thick as 5 μm in order to absorb and attenuate light having λ2. The unwanted light having λ2 passes through the absorption layer upward from under. It is absorbed by the cap layer  78 , and the remaining light leaves the PD. Dissimilar to the PD in FIG. 11, the light having λ2 is not reflected by the p electrode, so that it does not return to the absorption layer. The anti-reflection layer  72  provided at the top surface is for preventing the reflection of the light having λ2=1.55 μm when it leaves the PD, not for preventing the reflection of light incident from outside. When stray light having λ2 enters the PD from above, the InGaAs cap layer can prevent the influence of the light. Because the layer has high hole concentration, the hole-electron pairs produced by the absorption of the light having λ2 recombine without generating optical current. In short, Type 1 replaces the InP window layer in the internal structure of a conventional PD by a thick InGaAs cap layer for the purpose of absorbing light having λ2 so that it cannot return to the absorption layer.  
         [0065]    Type 2: Local and Thick Filter Layer (FIG. 13)  
         [0066]    [0066]FIG. 13 shows another embodiment of the present invention in which a thick InGaAs filter layer is provided only at the center portion of a chip. Whereas Type 1 shown in FIG. 12 has a uniformly thick InGaAsP cap layer, Type 2 is designed with the concept that the light having λ2 passing through the center portion of the chip can be handled with a thick filter layer provided only at the center portion. Consequently, the cap layer is made of InP.  
         [0067]    An n-InP buffer layer  61 , an n-InGaAsP absorption layer  62  (λg=1.42 μm), an n-InP cap layer  63 , and an InGaAs filter layer  74  are grown epitaxially on an n-InP substrate  60 . At the center portion of the chip, Zn is diffused to provide a p-type region  64 . Another p-type region is formed at the periphery of the chip at the same time. This additional p-type region is a Zn-diffused shield layer. The peripheral portion of the InGaAs filter layer  74  is removed so that the center portion, which is converted into a p-type region, can be remained. A ring-shaped p electrode  70  is provided on the protruding portion at the center. An anti-reflection layer  72  is formed on the InGaAs filter layer  74  at the inside of the p electrode  70 . Since the PD is a back-illuminated type, the anti-reflection layer  72  is not for admitting light, but for allowing the unwanted light having λ2 to leave the PD without being reflected.  
         [0068]    Directly under the ring-shaped p electrode  70 , there lies the p-InGaAs filter layer  74 , followed by the p-InP cap layer and the p-InGaAsP absorption layer Usually, an InP cap layer is placed on the absorption layer. However, InP has a wide bandgap and cannot absorb light having λ2. Consequently, Type 2 further laminates an InGaAs layer, which can absorb light having λ2, on the InP cap layer. Dissimilar to Type 1, this type absorbs light having λ2 by the thick InGaAs filter layer provided only at the center portion.  
         [0069]    At the outside of the InGaAs filter layer  74 , a passivation layer  67  is provided to protect the edge of the pn junction. Since light enters the PD at the back side, the back-side structure is the same as in FIG. 12. A ring-shaped n electrode  68  is formed on the bottom surface of the n-InP substrate  60 . The inside of the n electrode  68  forms an opening and is covered by an anti-reflection layer  69 . The p-InGaAs filter layer  74  has a thickness of 5 μm and a carrier concentration of p =10 18 cm −3 . The layer is as thick as 5 μm in order to absorb and attenuate light having λ2. The unwanted light having λ2 passes through the absorption layer upward from under. It is absorbed by the filter layer, and the remaining light leaves the PD. Dissimilar to the PD in FIG. 11, the light having λ2 is not reflected by the p electrode, so that it does not return to the absorption layer.  
         [0070]    The anti-reflection layer  72  provided at the top surface is for preventing the reflection of the light having λ2=1.55 μm when it leaves the PD, not for preventing the reflection of light incident from outside. When stray light having λ2 enters the PD from above, the InGaAs filter layer  74  can prevent the influence of the light. Because the layer has high hole concentration, the hole-electron pairs produced by the absorption of the light having λ2 recombine without generating optical current. In short, Type 2 additionally provides a thick InGaAs filter layer for absorbing light having λ2 so that it cannot return to the absorption layer.  
         [0071]    Type 3: Selectively Grown Thick Filter Layer (FIG. 14)  
         [0072]    [0072]FIG. 14 shows yet another embodiment of the present invention in which a thick filter layer is provided at the center portion of a chip. In Type 2 shown in FIG. 13, the layers up to and including the filter layer are formed by the epitaxial growth method. Type 3, however, uses an ordinary epitaxial wafer in which the layers up to and including an n-InP cap layer are grown. An InGaAs filter layer at the center portion is selectively grown by utilizing the electrode structure after the formation of the pn junction.  
         [0073]    An n-InP buffer layer  61 , an n-InGaAsP absorption layer  62  (λg=1.42 μm), and an n-InP cap layer  63  are grown epitaxially on an n-InP substrate  60 . At the center portion of the chip, Zn is diffused to provide a p-type region  64 . Another p-type region is formed at the periphery of the chip at the same time. This additional p-type region is a Zn-diffused shield layer. A ring-shaped p electrode  70  is provided on the p-type region  64 . At the outside of the ring-shaped p electrode  70 , a passivation layer  67  is provided to protect the pn junction.  
         [0074]    An InGaAs filter layer  75  that absorbs light having λ2 is selectively grown on the center portion of the chip&#39;s top surface that is surrounded by the ring-shaped p electrode  70 . The filter layer can be epitaxially grown by a method such as molecular-beam epitaxy (MBE), metalorganic chemical vapor deposition (MOCVD), etc. Because InGaAs cannot grow on the passivation layer and the metal electrode, it selectively grows only on the InP cap layer. Since the p electrode lies outside the periphery of the InGaAs filter layer  75 , no electric field exists in the InGaAs.  
         [0075]    A ring-shaped n electrode  68  and an anti-reflection layer  69  are formed on the bottom surface. Incoming light (λ1=1.3 μm) and outgoing light (λ2=1.55 μm) enter at the back side. The light having λ1 is absorbed by the absorption layer  62  and detected by generating optical current. The light having λ2 passes through the absorption layer upward after being absorbed slightly by the absorption layer. The light having λ2 is absorbed mainly by the InGaAs filter layer  75 . Even if a slight amount of the light having λ2 leaves the PD, the amount of the light reflected somewhere at the outside further decreases. Virtually no light having λ2 returns to the absorption layer  62 . The light having λ2 passes through the absorption layer only once. Therefore, the crosstalk caused by the returning light having λ2 can be prevented effectively.  
         [0076]    Type 4: Chip Whose Entire Top Surface is Covered by Plastic (FIG. 15)  
         [0077]    Types 1 to 3 absorb light having λ2 by the semiconductor material InGaAs. However, the light can be absorbed also by plastic. FIG. 15 shows such an embodiment. An n-InP buffer layer  61 , an n-InGaAsP absorption layer  62  (λg=1.42 μm), and an n-InP cap layer  63  are grown epitaxially on an n-InP substrate  60 . Table II shows the thickness and carrier concentration of the epitaxial layers.  
                                     TABLE II                               Carrier           Layer&#39;s thickness   concentration       Layer&#39;s name   (μm)   (cm −3 )                                InP cap layer (63)   3   n = 5 × 10 15         InGaAsP absorption layer (62)   5   n = 10 15         InP buffer layer (61)   4   n = 10 15         InP substrate (60)   200   n = 10 18                    
 
         [0078]    At the center portion of the chip, Zn is diffused to provide a p-type region  64 . Another p-type region is formed at the periphery of the chip at the same time. This additional p-type region is a Zn-diffused shield layer A ring-shaped p-electrode  70  is provided on the p-type region  64 . At the outside of the ring-shaped p electrode  70 , a passivation layer  67  is provided to protect the pn junction. No anti-reflection layer is provided at the inside of the p electrode  70 . A ring-shaped n electrode  68  and an anti-reflection layer  69  are formed on the bottom surface. They are produced through the wafer process. After a chip is cut out from the wafer and mounted on a package, the p electrode  70  is connected to a lead pin with a lead wire  77 . Then, a plastic resin  76  that absorbs light having λ2 is applied to the entire top surface of the chip. The plastic resin is required to absorb light having λ2; it is not required to absorb the light exclusively. Therefore, the plastic resin can be black.  
         [0079]    Incoming light (λ1=1.3 μm) and outgoing light (λ2=1.55 μm) enter at the back side. The light having λ1 is absorbed by the absorption layer and detected by generating optical current. The light having λ2 passes through the absorption layer upward after being absorbed slightly by the absorption layer. Then, the light leaves the cap layer and is absorbed by the plastic resin  76 . Only a slight amount of the light having λ2 leaves the PD. Even if the light is reflected at the case and parts, it does not return to the absorption layer. As with Types 1 to 3, the light having λ2 passes through the absorption layer only once. Therefore, the crosstalk caused by the returning light having λ2 can be prevented effectively. Type 4 requires no extra epitaxial growth. Type 4 accomplishes its purpose by applying the plastic resin after the chip is mounted on a package. As a result, Type 4 can be employed easily in practical application.  
       EXAMPLES  
       [0080]    [0080]FIG. 16 shows a surface-mounted-type PD module on which a Type 4 PD is mounted. A V-shaped groove  81  is provided longitudinally on the surface of an Si platform  80 . A mirror face is provided at the end of the V-shaped groove. An optical fiber  82  is inserted into the V-shaped groove  81  and fixed there. A back-illuminated-type PD  83  of the present invention is fixed on the V-shaped groove  81 . Although it is a back-illuminated type, the PD has an opening at the top surface through which light can pass. The top surface is covered by a plastic resin  85  that absorbs light having λ2.  
         [0081]    At a central office, the incoming light having λ1 emerges from the optical fiber  82 , enters the V-shaped groove  81 , is reflected at the mirror face, and enters the PD  83  at the back side. The light reaches an absorption layer  84 , generates optical current, and is detected by the PD. When the stray light and scattered light produced by the intense outgoing light having λ2 enter the PD from the V-shaped groove, the absorption layer scarcely detects them. After passing through the absorption layer upward, they do not return to the absorption layer. There also exists stray light having λ2 above the PD. However, since it is absorbed by a plastic resin  85 , it does not enter the absorption layer of the PD. Consequently, light having λ2 passes through the absorption layer only once. Therefore, crosstalk caused by the light having λ2 can be suppressed to 0.1% or less. The plastic resin can be applied to the PD at the stage of the chip mounting, without increasing the wafer process.  
         [0082]    [0082]FIG. 17 shows a schematic- cross-sectional view of a surface-mounted-type optical transceiver module that uses a Type 4 PD. The transceiver module is constructed on an Si platform, which is not shown in FIG. 17, in a housing  86 . An optical fiber  87  is attached to the Si platform. An LD  89  for generating outgoing going light having λ2 at a central office is mounted opposite to the end of the optical fiber. A WDM filter  88  is provided on the skew at some point in the optical fiber near its end Aback-illuminated-type PD  90  of the present invention is placed obliquely above the WDM filter. The PD  90  is a Type 4 PD, which has on the top surface a plastic resin  92  that can absorb light having λ2.  
         [0083]    A signal carried by the outgoing light (λ2=1.55 μm) emitted from the LD  89  enters the optical fiber  87  to be transmitted to a subscriber The incoming light (λ1=1.3 μm) carrying a signal from the subscriber propagates through the optical fiber  87 , is reflected by the WDM filter  88 , enters the PD  90  at the back side, and is absorbed by an absorption layer  91 , generating optical current. The intense outgoing light having λ2 generated by the LD  89  produces stray light and scattered light, which surround the PD. The light having λ2 which enters the PD at the back side passes through the absorption layer once, generating optical current sightly. However, the light having λ2 which enters the plastic resin  92  at the top surface is absorbed by the plastic resin, without penetrating into the PD. Therefore, the module can minimize the influence of the outgoing light at a central office.  
         [0084]    Industrial Applicability  
         [0085]    A central office receives light having a shorter wavelength (λ1=1.3 μm) and transmits light having a longer wavelength (λ2=1.55 μm). When the bandgap wavelength of a semiconductor is represented by λg, the light having λ2, which is longer than λg, was thought to pass through the semiconductor without causing any influence. Therefore, the phenomenon that the light having λ2 causes crosstalk to the light having λ1 was not known to a person skilled in the art. There was no concept that light having a longer wavelength causes crosstalk, to a PD for a shorter wavelength. In other words, the present inventors first found the necessity of reducing the above-mentioned crosstalk.  
         [0086]    The present inventors first found that contrary to the conventional knowledge, the absorption layer of a PD for a shorter wavelength, λ1, slightly detects a longer wavelength, λ2. The present invention admits that in a back-illuminated-type PD for λ1, light having λ2 passes through the absorption layer once. The present invention, however, prevents the light from passing through the layer again after being reflected The first passage generates a crosstalk of 0.1%; the second passage increases it to 0.2%. The present invention prevents this increase and thereby enables the reduction of the crosstalk hitherto unknown to a person skilled in the art.