Patent Document

BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     This invention relates to an integrated semiconductor device comprising a light modulator of an electro-absorption type semiconductor and an optical device, such as a semiconductor laser, useful for an optical communication and/or optical data processing. 
     2. Description of the Related Art 
     An integrated EA-DFB device comprising an electro-absorption type (hereinafter “EA”) modulator and a distributed feed back type (hereinafter “DFB”) laser converts high-speed electrical signals to optical signals. 
     Continuous wave (hereinafter “CW”) light which is generated when electric current is applied to the DFB laser is input to the EA modulator through a butt joint section where the DFB laser and the EA modulator are joined. The butt joint section is an interface between an active layer of the DFB laser for oscillating a laser beam and a light absorption layer of the EA modulator. The EA modulator has an electro-absorption effect, wherein the amount of absorbed light is changed due to the change of the semiconductor band structure when a voltage is applied to the EA modulator. Accordingly, when a reverse bias voltage is applied to the EA modulator, the amount of absorbed light is increased so that light does not permeate through the light absorption layer of the EA modulator. When a voltage is not applied to the EA modulator, light permeates the EA modulator (ON condition) and, when a reverse voltage is applied, light is cut off (OFF condition), thereby to modulate light. The EA modulator converts electrical signals to optical signals by changing the light absorption rate by applying a voltage to the light absorption layer from outside. 
       FIGS. 4 and 5  show a conventional EA-DFB device. A DFB laser (hereinafter “LD”)  41  and an EA modulator  42  are formed on a substrate. A separation region  43  is provided between an upper electrode  46  of the LD  41  and an upper electrode  48  of the EA modulator  42 . In the LD  41 , a lower clad layer  53 , an active layer  54 , an upper clad layer (not shown), and an ohmic contact layer (not shown) to be brought into contact with the electrode are formed in this order on a substrate  52 . Tn the EA modulator  42 , the lower clad layer  53 , a light absorption layer  56 , the upper clad layer, and the ohmic contact layer are formed in this order on the substrate  52 . Tn the separation region  43 , the lower clad layer  53 , a wave guide layer  55 , the upper clad layer, and the ohmic contact layer are formed in this order on the substrate  52 . An etched channel  49  is provided on sides of the LD  41  and the EA modulator  42  so as to form a ridge structure. 
     A forward bias voltage is applied between the upper electrode  46  and a lower electrode  47  of the LD  41  so as to generate CW light from the active layer  54 . A reverse bias voltage is applied between the upper electrode  48  and the lower electrode  47  of the EA modulator  42  so as to change the amount of light absorbed by the absorption layer  56  for performing modulation. The contact layer under a pad of the upper electrode  48  is etched so as to prevent deterioration of the frequency characteristics caused by the increased electric capacity of the pad electrode. 
     However, in this conventional EA-DFB device, when input light is intense, the vicinity of the incident area of the EA modulator  42 , where the amount of absorbed light is the largest, is adversely affected by the heat generation by the absorption of light. Accordingly, there has been a problem that intense light cannot be input. 
       FIG. 6  shows an EA-DFB device proposed by Japanese Patent Application Kokai Number 2001-117058 to solve the above-mentioned problem. In the same manner as the conventional art shown in  FIG. 5 , an LD  61  and an EA modulator  62  are formed on a substrate, and a separation region  63  is provided between a upper electrode  66  of the LD  61  and an upper electrode  68  of the EA modulator  62 . In the LD  61 , a lower clad layer  73 , an active layer  74 , an upper clad layer (not shown), and an ohmic contact layer (not shown) to be brought into contact with the electrode are formed in this order on a substrate  72 . In the EA modulator  62 , the lower clad layer  73 , a light absorption layer  76 , the upper clad layer, and the ohmic contact layer are formed in this order on the substrate  52 . In the separation region  63 , the lower clad layer  73 , a wave guide layer  75 , the upper clad layer, and ohmic contact layer are formed in this order on the substrate  72 . An etched channel  79  is provided on sides of the LD  61  and the EA modulator  62 . 
     The EA-DFB device shown in  FIG. 6 , however, is provided with a region  64 , where the upper clad layer is extended such that the channel  79  in the vicinity of the incident area of the EA modulator  62  is made narrower (the separation  63  region is made wider) . This structure improves the heat-radiation property in the vicinity of the incident area where the rise of temperature is highest, thus enabling the input of more intense light. 
     However, the above EA-DFB device has a problem that the EA modulator and the LD are not completely separated electrically so that when a forward bias of +1.2 V is applied to the LD and a reverse bias of −3 V is applied to the EA modulator, the separation region between the EA modulator and the LD has a strong electric field. Consequently, the absorption of light is not performed in the EA modulator but in the separation region so that the heat generated in the separation region by photo-current is not radiated efficiently in the region  64  in the vicinity of incident area of the EA. 
       FIG. 7  shows the principle of heat generation in the above EA-DFB device. A forward bias of +1.2 V is applied between the upper and lower electrodes  66  and  67  of the LD  61  to emit CW light from the active layer  64  and a reverse bias of −3 V is applied between the upper and lower electrodes  68  and  67  of the EA modulator  62  to change the amount of light absorbed in the absorption layer  65 . Under this condition, a high voltage is applied between the upper electrodes  66  and  68  so that a light absorption  69  is performed in the separation region  63  resulting in the increased heat generation in the separation region  63 . 
       FIG. 8  shows the result of simulation for relationship between the positions of the LD, the separation region, and the EA modulator, and photo-current generated by the light absorption. The simulation shows that the photocurrent in the separation region is highest, which means that the heat-generation in the separation region is highest. 
     Also, a slab under the pad electrode of the EA modulator increases the electric capacity of the entire pad electrode, which adversely affects the frequency characteristics. 
     BRIEF SUMMARY OF THE INVENTION 
     Accordingly, it is an object of the present invention to provide a new or improved optical semiconductor device capable of efficiently radiating the heat generated by photo-current in the separation region so as to enable the input of intense light and controlling the electric capacity of the entire pad electrode so as to prevent deterioration of the frequency characteristics. 
     According to one aspect of the invention, an optical semiconductor device comprises a substrate, a semiconductor laser including a lower clad layer, an active layer, and an upper layer formed in this order on the substrate, an electroabsorptive modulator including the lower clad, a light absorption layer, and the upper clad layer formed in this order on the substrate, and a separation region provided between the semiconductor laser and the electroabsorptive modulator and including the lower clad layer, a wave guide layer, and the upper clad layer formed in this order on the substrate, wherein the upper clad layer extends from the semiconductor laser through the separation region to the electroabsorptive modulator, the semiconductor laser, separation region, and electroabsorptive modulator each have a side provided in parallel with each other, and the upper clad layer extends up to the side of the separation region. Also, a contact layer is provided on the upper clad layer, and a first and a second upper electrodes are provided on the contact layer in the semiconductor laser and the electroabsorptive modulator, respectively. A lower electrode is provided on an under-side of the substrate. In addition, a channel from which the upper clad layer is removed, is provided such that the channel surrounds the upper clad layer. The upper clad layer, which extends up to the side of the separation region, is called a slab and capable of efficiently radiating heat caused by the absorption of light. 
     Since the slab is not provided in the vicinity of the incident area of the EA modulator but in the separation region such that the slab extends up to the side of the separation region, the heat-radiation property of the EA-DFB device is improved, thus enabling the input of intense light. The channel extends up to the side of the separation region, the upper clad layer along the slab is removed, and no clad layer exists under the upper electrodes so that the increase of the electrical capacity of the pad electrodes is prevented, thus improving the frequency characteristics. 
     According to another aspect of the invention, the upper clad layer extends from the semiconductor laser through the separation region to the light modulator via each side thereof. That is, the slab joins with the upper clad layer outside the channel so that the heat-radiation property is further improved, enabling the input of more intensive light. 
     According to still another aspect of the invention, the contact layer in the separation region is removed and/or has a high resistance by ion-implantation so that the increase of the electrical capacity of the pad electrodes is prevented, improving the frequency characteristics and broadening the modulated band. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1(   a ) is a perspective view of an EA-DFB device according to the first embodiment of the present invention. 
         FIG. 1(   b ) is an enlarged top view of the RA-DFB device of  FIG. 1(   a ). 
         FIG. 2  is a top view of a separation region of an EA-DFB device according to the second embodiment of the present invention. 
         FIG. 3  is a top view of the vicinity of the separation region according to the third and fourth embodiments of the present invention. 
         FIG. 4  is a schematic diagram of an electrical arrangement of an EA-DFB device according to the prior art. 
         FIG. 5  is a perspective view of the EA-DFB device according to the prior art. 
         FIG. 6  is a perspective view of the EA-DFB device according to the Japanese Application Kokai Number 2001-117058. 
         FIG. 7  is schematic diagram of the EA-DFB device of  FIG. 6  showing the principle of heat generation. 
         FIG. 8  is a graph showing a simulation result of photocurrent caused by light absorption of the EA-DFB device. 
     
    
    
     DESCRIPTION OF THE PREFERRED EMBODIMENT 
     The same reference numerals will be used for elements having a substantially identical function, and the description thereof will be omitted. 
     (First Embodiment) 
     In  FIG. 1 , a DFB laser (LD)  11  and an EA modulator  12  are formed on a substrate  2  and a separation region  13  is provided between an upper electrode  16  of the LD  11  and an upper electrode  18  of the EA modulator  12 . In the LD  11 , a lower clad layer  3 , an active layer  4 , an upper clad layer  7 , and an ohmic contact layer  8  to be brought into contact with the electrode are formed in this order on a substrate  2 . In the EA modulator  12 , the lower clad layer  3 , a light absorption layer  6 , the upper clad layer  7 , and the ohmic contact layer  8  are formed in this order on the substrate  2 . In the separation region  13 , the lower clad layer  3 , a wave guide layer  5 , the upper clad layer  7 , and the ohmic contact layer  8  are formed in this order on the substrate  2 . 
     N-type indium phosphorus (InP) is used for the lower clad layer  3 , indium gallium arsenic phosphorus (InGaAsP) for the active layer  4  of the LD  11  and the light absorption layer  6  of the EA  12 , and p-type indium phosphorus (InP) for the upper clad layer. A channel  10 , which is not provided with the clad layer  7 , is provided in the LD  11  and the EA modulator  12 . A slab  14  includes the upper clad layer  7  which extends up to sides or edges of the EA DFB device in the separation region  13 . 
     The slab  14  is not provided in the vicinity of the incident area in the EA modulator. It is provided in the separation region  13  where the heat generation is highest and extends up to the sides of the device so as to create a flow  19  of heat, thus increasing the heat-radiation property. The upper clad layer  7  is removed along the slab  14  to reduce the electrical capacity of the upper electrode  18 , thus preventing the frequency characteristics from being deteriorated. 
     The operation principle is substantially same as that of the conventional art. That is, a forward bias is applied between the upper and lower electrodes  16  and  17  to generate electric current in the LD to emit CW light and a reverse bias is applied between the upper and lower electrodes  18  and  17  to change the amount of light absorbed to perform modulation. 
     As stated above, the slab  14  is provided in the separation region  13  to enable the input of intense light by improving the heat-radiation property. Also, since the slab is not provided under the pad electrode and the upper clad layer along the slab is removed up to the sides of the device, the electrical capacity of the pad electrode is reduced so that the frequency characteristics are not affected adversely. 
     (Second Embodiment) 
     In  FIG. 2 , a separation region  23  is provided between an LD  21  and an EA modulator  22 . In the same way as in the first embodiment, a slab  24  is provided in the separation region  23 . The slab  24 , however, joins with the upper clad layer  27  provided outside a channel  25  to further increase the heat radiation efficiency by improving a flow  29  of heat. 
     The operation principle is substantially same as that of the conventional art. That is, a forward bias is applied between the upper and lower electrodes to generate electric current in the LD to emit CW light and a reverse bias is applied between the upper and lower electrodes  18  and  17  to change the amount of light absorbed, making modulation. 
     According to the second embodiment, although the frequency characteristics are worse than those of the first embodiment because of the increase of the electrical capacity of the pad electrode, the heat radiation property is better than that of the first embodiment because the slab joins with the regions outside the channel, thereby to enable the input of intense light. 
     (Third Embodiment) 
     In  FIG. 3 , a separation region  33  is provided between an LD  31  and an EA modulator  32 . In the same way as in the first embodiment, a slab  34  is provided in the separation region  33 . However, according to the third embodiment, a contact layer provided on the upper clad layer on the separation region  33  and the slab  34 , which is hatched with diagonal lines, is removed to reduce the electrical capacity of the pad electrode. 
     The operation principle is substantially same as that of the conventional art. That is, a forward bias is applied between the upper and lower electrodes to generate electric current in the LD to emit CW light and a reverse bias is applied between the upper and lower electrodes  18  and  17  to change the amount of light absorbed, thereby providing modulation. 
     According to the third embodiment, in addition to the effect in the first embodiment, the frequency characteristics are improved and the modulated band is broaden because of the reduced electrical capacity of the pad electrode. 
     (Fourth Embodiment) 
     In the third embodiment, the contact layer in the hatched area in  FIG. 3  is removed. In the fourth embodiment, however, the hatched area is made such that it has large resistance to reduce the electrical capacity of the pad electrode. For example, proton (H + ) is ion-implanted to the contact layer made of zinc(Zn)-doped type indium phosphorus (InP). 
     The operation principle is same as that of the conventional art. That is, a forward bias is applied between the upper and lower electrodes to generate electric current in the LD to emit CW light and a reverse bias is applied between the upper and lower electrodes  18  and  17  to change the amount of light absorbed, providing optical modulation. 
     According to the fourth embodiment, in the same manner as the third embodiment, the frequency characteristics are improved and the modulated band is broaden because of the reduced electrical capacity of the pad electrode. 
     Although preferred embodiments have been described above with reference to the accompanying drawings, the present invention is not limited to those embodiments. A number of variations and modifications are possible within the technical concept of the claimed invention and, therefore, such variations and modifications should belong to the scope of the present invention. 
     As fully described above, according to the present invention, a slab is provided in a separation region instead of in the vicinity of the incident area of EA modulator to enable the input of light having a high power by increasing the heat radiation property of the EA-DFB device. In addition, the slab is provided outside the pad electrode to reduce the electrical capacity of the pad electrode, thus improving the frequency characteristics and broadening the modulated band.

Technology Category: 4