Patent Publication Number: US-RE48577-E

Title: Vertical cavity surface emitting laser

Description:
CROSS REFERENCES TO RELATED APPLICATIONS 
     The present invention contains subject matter related to Japanese Patent Application JP 2008-002822 filed in the Japanese Patent Office on Jan. 10, 2008, and Japanese Patent Application JP 2008-305349 filed in the Japanese Patent Office on Nov. 28, 2008, the entire contents of which being incorporated herein by references.This application is a reissue of U.S. patent application Ser. No. 12/318,421, filed on Dec. 29, 2008, issued on Dec. 13, 2011, now U.S. Pat. No. 8,077,752, which claims priority to Japanese Patent Application No. 2008-002822, filed on Jan. 10, 2008 in the Japanese Patent Office, and claims priority to Japanese Patent Application No. 2008-305349, filed on Nov. 28, 2008 in the Japanese Patent Office, the entire contents of all of which are herein incorporated by reference.  
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention relates to a Vertical Cavity Surface Emitting Laser (VCSEL) that emits laser light from the top face, particularly to a VCSEL suitably applicable to purposes necessitating transverse mode control. 
     2. Description of the Related Art 
     A VCSEL emits light in the direction orthogonal to a substrate differently from the existing edge-emitting laser diodes. In the VCSEL, many devices are able to be arranged in a state of a two dimensional array on the same substrate. Therefore, the VCSEL has recently attracted attention as a light source for a digital copy machine or a printer. 
     In the past, in the foregoing type of VCSEL, a pair of multilayer film reflectors is formed over a semiconductor substrate, and an active layer as a light emitting region is provided between the pair of multilayer film reflectors. In one of the multilayer film reflectors, in order to improve efficiency of current injection into the active layer and lower the threshold value current, a current confinement layer having a structure in which a current injection region is confined is provided. Further, a lower electrode is provided on the bottom face side, and a p-side electrode is provided on the top face side. The p-side electrode is provided with a light emitting aperture to emit laser light. In the VCSEL, a current is confined by the current confinement layer, and then injected into the active layer where light is emitted. While the emitted light repeats reflection between the pair of multilayer film reflectors, the light is emitted as laser light from the light emitting aperture of the p-side electrode. 
     In general, in the foregoing VCSEL, high-order transverse mode oscillation is easily generated. Therefore, for example, in Japanese Unexamined Patent Application Publication No. 2004-119582, a reflectance adjustment layer is provided in the central part of a light emitting aperture of the top face of a mesa, a region where fundamental transverse mode is mainly shown is set to a region with high reflectance, and a region where high-order transverse mode is mainly shown is set to a region with low reflectance. Thereby, oscillation of the high-order transverse mode is prevented, and single transverse mode oscillation is realized. 
     SUMMARY OF THE INVENTION 
     However, the foregoing measure of Japanese Unexamined Patent Application Publication No. 2004-119582, in the region where the high-order transverse mode is mainly shown, oscillation of the fundamental transverse mode is prevented. Thus, there is a disadvantage that it is not easy to obtain high output of the fundamental transverse mode. 
     In view of the foregoing, in the invention, it is desirable to provide a VCSEL capable of obtaining high output of the fundamental transverse mode while preventing oscillation of the high-order transverse mode. 
     According to an embodiment of the present invention, there is provided a first Vertical Cavity Surface Emitting Laser including a semiconductor layer including an active layer and a current confinement layer; and a transverse mode adjustment section formed on the semiconductor layer. The current confinement layer has a current injection region and a current confinement region. The transverse mode adjustment section has a high reflectance area and a low reflectance area. The high reflectance area is formed in a region including a first opposed region opposing to a center point of the current injection region, and a center point of the high reflectance area is arranged in a region different from the first opposed region. On the other hand, the low reflectance area is formed in a region where the high reflectance area is not formed, in an opposed region opposing to the current injection region. 
     In the first VCSEL of the embodiment of the invention, in the transverse mode adjustment section on the semiconductor layer, the high reflectance area is formed in the region including a first opposed region opposing to a center point of the current injection region, and a center point of the high reflection region is arranged in a region different from the first opposed region. On the other hand, the low reflectance area is formed in a region where the high reflectance area is not formed, in an opposed region opposing to the current injection region. This enables to lower the reflectance of the specific region in an opposed region opposing to the region generating a high order transverse mode including four peaks of double rotation symmetry or quad rotation symmetry than the reflectance of the region including the first opposed region. In the case where the specific region is the region corresponding to two peaks facing each other with a region other than the first opposed region in between, gain of the high order transverse mode is able to be largely decreased while minimizing the lowering of gain of the fundamental transverse mode. 
     The double rotation symmetry means that the number of rotational positions symmetric to the position before rotation while a rotation object is rotated by 360 degree is two. The quad rotation symmetry means that the number of rotational positions symmetric to the position before rotation while a rotation object is rotated by 360 degree is four. 
     According to an embodiment of the present invention, there is provided a second A Vertical Cavity Surface Emitting Laser including a semiconductor layer including an active layer and a current confinement layer, and a transverse mode adjustment section formed on the semiconductor layer. The current confinement layer has a current injection region and a current confinement region. The transverse mode adjustment section has a high reflectance area and a low reflectance area. The high reflectance area is formed in a region including a first opposed region opposing to a center point of the current injection region, and has a shape of cross. On the other hand, the low reflectance area is formed in a region where the high reflectance area is not formed, in an opposed region opposing to the current injection region. 
     In the second VCSEL of the embodiment of the invention, in the transverse mode adjustment section on the semiconductor layer, the high reflectance area is formed in the region including a first opposed region opposing to a center point of the current injection region, and has a shape of cross. On the other hand, the low reflectance area is formed in a region where the high reflectance area is not formed, in an opposed region opposing to the current injection region. This enables to lower the reflectance of the specific region in an opposed region opposing to the region generating a high order transverse mode including four peaks of double rotation symmetry or quad rotation symmetry than the reflectance of the region including the first opposed region. In the case where the specific region is the region corresponding to the four peaks, gain of the high order transverse mode is able to be largely decreased while minimizing the lowering of gain of the fundamental transverse mode. 
     According to the first and the second VCSELs of the embodiment of the invention, the gain of the high-order transverse mode is largely lowered while minimizing the lowering of the gain of the fundamental transverse mode. Therefore, high output of the fundamental transverse mode is able to be obtained while oscillation of the high-order transverse mode is prevented. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  is a perspective view of a laser diode according to an embodiment of the invention; 
         FIG. 2  is a cross sectional view taken along arrows A-A of the laser diode of  FIG. 1 ; 
         FIGS. 3A to 3C  are plan structural views of the current confinement layer of  FIG. 2 ; 
         FIGS. 4A to 4C  are schematic views for explaining a relation between the transverse mode adjustment section of  FIG. 2  and high-order transverse mode; 
         FIG. 5  is a distribution view for explaining reflectance distribution of the transverse mode adjustment section of  FIG. 2 ; 
         FIGS. 6A and 6B  are cross sectional views for explaining manufacturing process of the laser diode illustrated in  FIG. 1 ; 
         FIGS. 7A and 7B  are cross sectional views for explaining steps following the steps of  FIGS. 6A and 6B ; 
         FIGS. 8A and 8B  are cross sectional views for explaining steps following the steps of  FIGS. 7A and 7B ; 
         FIGS. 9A and 9B  are schematic views for explaining a relation between a transverse mode adjustment section of a comparative example and high-order transverse mode; 
         FIG. 10  is a characteristics diagram for explaining a relation between a width of a current confinement layer and mirror loss/light output; 
         FIGS. 11A to 11C  are schematic views for explaining a modified example of the transverse mode adjustment section of  FIG. 2 ; 
         FIGS. 12A to 12C  are schematic views for explaining another modified example of the transverse mode adjustment section of  FIG. 2 ; 
         FIGS. 13A to 13C  are schematic views for explaining still another modified example of the transverse mode adjustment section of  FIG. 2 ; and 
         FIG. 14  is a characteristics diagram for explaining a relation between a width of the current confinement layer and mirror loss/light output in the case where the transverse mode adjustment sections of  FIGS. 11A to 11C  and  FIGS. 13A to 13C  are used. 
     
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT 
     Descriptions will be given of an embodiment of the invention in detail with reference to the drawings. 
       FIG. 1  illustrates a perspective view of a laser diode  1  of VCSEL according to an embodiment of the invention.  FIG. 2  illustrates a cross sectional structure taken along arrows A-A of the laser diode  1  of  FIG. 1 .  FIG. 3A  to  FIG. 3C  illustrate a cross sectional structure in the lamination in-plane direction of a current confinement layer  15  of  FIG. 2 .  FIG. 1  to  FIG. 3C  are schematic views, and thus the dimensions and the shapes thereof are different from the actual dimensions and the actual shapes. 
     The laser diode  1  includes a semiconductor layer  30  (resonator) in which a lower DBR layer  11 , a lower spacer layer  12 , an active layer  13 , an upper spacer layer  14 , the current confinement layer  15 , an upper DBR layer  16 , and a contact layer  17  are layered in this order on one face of a substrate  10 . The upper part of the semiconductor layer  30 , specifically, the upper part of the lower DBR layer  11 , the lower spacer layer  12 , the active layer  13 , the upper spacer layer  14 , the current confinement layer  15 , the upper DBR layer  16 , and the contact layer  17  structure a mesa  18 . In this embodiment, the lower DBR layer  11  corresponds to a specific example of “a first multilayer film reflector” of the invention and the current confinement layer  15  and the upper DBR layer  16  correspond to a specific example of “a second multilayer film reflector” of the invention. 
     The substrate  10  is formed from, for example, n-type GaAs. The lower DBR mirror layer  11  is formed by layering a plurality of sets of a low refractive index layer (not illustrated) and a high refractive index layer (not illustrated). The low refractive index layer is formed from n-type Al x1 Ga 1-x1 As (0&lt;x1&lt;1) being λ/4n a  thick (λ is an oscillation wavelength, and n a  is a refractive index), for example. The high refractive index layer is formed from n-type Al x2 Ga 1-x2 As (0&lt;x2&lt;x1) being λ/4n b  thick (n b  is a refractive index), for example. The lower spacer layer  12  is formed from, for example, Al x3 Ga 1-x3 As (0&lt;x3&lt;1). As an n-type impurity included in the substrate  10 , the lower DBR layer  11 , and the lower spacer layer  12 , for example, silicon (Si), selenium (Se) or the like is included. 
     The active layer  13  is made of, for example, a GaAs-based material. In the active layer  13 , the central part in the lamination in-plane direction (the region opposed to an after-mentioned current injection region  15 B) is a light emitting region  13 A. In the light emitting region  13 A, the central region corresponds to a region where fundamental transverse mode oscillation is mainly generated, and the region surrounding the central region is a region where high-order transverse mode oscillation is mainly generated. 
     The upper spacer layer  14  is formed from, for example, p-type Al x4 Ga 1-x4 As (0≤x4&lt;1). The upper DBR layer  16  is formed by layering a plurality of sets of the low refractive index layer (not illustrated) and the high refractive index layer (not illustrated). The uppermost layer of the upper DBR layer  16  is the high refractive index layer. The low refractive index layer is formed from p-type Al x5 Ga 1-x5 As (0&lt;x5&lt;1) being λ/4n c  thick (n c  is a refractive index), for example. The high refractive index layer is formed from p-type Al x6 Ga 1-x6 As (0&lt;x6&lt;x5) being λ/4n d  thick (n d  is a refractive index), for example. The contact layer  17  is made of, for example, p-type GaAs, and is provided with, for example, a circular aperture in a region opposed to the after-mentioned current injection region  15 B. As a p-type impurity included in the upper spacer layer  14 , the upper DBR layer  16 , and the contact layer  17 , zinc (Zn), magnesium (Mg), beryllium (Be) or the like is included. 
     The current confinement layer  15  has a current confinement region  15 A in a region with a certain depth from the side face of mesa  18 , and the other region thereof (central region of the mesa  18 ) is the current injection region  15 B. The current injection region  15 B is formed from, for example, p-type Al x7 Ga 1-x7 As (0&lt;x7≤1). The current confinement region  15 A contains, for example, Al 2 O 3  (aluminum oxide) and is obtained by oxidizing highly concentrated Al included in an oxidized layer  15 D from the side face as will be described later. Therefore, the current confinement layer  15  has a function to confine a current. 
     Further, for example, as illustrated in  FIG. 3A , the current injection region  15 B is in the shape of a quadrangle (regular tetragon) having diagonal lines in the directions of [011] and [01-1], and has in-plane anisotropy. This is because, for example, the oxidation rate of Al x7 Ga 1-x7 As in the directions of [011] and [01-1] is different from that in the directions of [001] and [010] at an angle of 45 degrees with the directions of [011] and [01-1]. The length of the diagonal lines of the quadrangle is, for example, in the range about from 3 μm to 10 μm, both inclusive. 
     The current injection region  15 B may be, for example, as illustrated in  FIG. 3B , circular. Otherwise, for example, as illustrated in  FIG. 3C , the current injection region  15 B may be in the shape of a quadrangle (rhombus) having diagonal lines in the directions of [011] and [01-1]. 
     The mesa  18  includes the current injection region  15 B of the current confinement layer  15 , and for example, is in the shape of a cylinder being about 20 μm to 30 μm in diameter, both inclusive. The diameter is appropriately adjusted according to oxidation rate, oxidation time and the like in the oxidation step so that a non-oxidized region (current injection region  15 B) having a certain size is left inside the mesa  18  in the after-mentioned oxidation step. 
     On the top face of the mesa  18  (top face of the contact layer  17 ), a circular upper electrode  19  having an aperture in a region opposed to the current injection region  15 B is formed. On the side face and the surrounding surface of the mesa  18 , a protective film  20  is formed. On the surface of the protective film  20 , an electrode pad  21  for bonding a wire (not illustrated) is provided. The electrode pad  21  is electrically connected to the upper electrode  19 . Further, on the rear face of the substrate  10 , a lower electrode  22  is provided. The upper electrode  19  and the electrode pad  21  are formed by layering, for example, titanium (Ti), platinum (Pt), and gold (Au) in this order, and are electrically connected to the contact layer  17  located in the upper part of the mesa  18 . The lower electrode  22  has a structure in which, for example, an alloy of gold (Au) and germanium (Ge), nickel (Ni), and gold (Au) are layered in this order from the substrate  10  side, and is electrically connected to the substrate  10 . 
     In this embodiment, in the aperture of the upper electrode  19 , that is, in the central region of the top face of the mesa  18 , a transverse mode adjustment section  23  is provided. The transverse mode adjustment layer  23  is provided being contacted with the uppermost layer of the upper DBR layer  16 , and includes a first adjustment layer  23 A, a second adjustment layer  23 B, and a third adjustment layer  23 C. 
     The first adjustment layer  23 A is made of a material in which the film thickness is (2a−1)λ/4n 1  (a is an integer number of 1 or more, and n 1  is a refractive index) and the refractive index n 1  is lower than the refractive index of the high refractive index layer provided on the surface of the upper DBR layer  16 , for example, a dielectric material such as SiO 2  (silicon oxide). The second adjustment layer  23 B is made of a material in which the film thickness is (2b−1)λ/4n 2  (b is an integer number of 1 or more, and n 2  is a refractive index) and the refractive index n 2  is higher than the refractive index n 1  of the first adjustment layer  23 A, for example, a dielectric material such as SiN (silicon nitride). Therefore, the laminated structure composed of the first adjustment layer  23 A and the second adjustment layer  23 B has a function to reflect light from the active layer  13  at high reflectance. 
     The third adjustment layer  23 C is made of a material in which the film thickness is (2c−1)λ/4n 3  (c is an integer number of 1 or more, and n 3  is a refractive index) and the refractive index n 3  is higher than the refractive index n 1  of the first adjustment layer  23 A, for example, a dielectric material such as SiN (silicon nitride). Therefore, the third adjustment layer  23 C has a function to reflect light from the active layer  13  at lower reflectance than that of the laminated structure composed of the first adjustment layer  23 A and the second adjustment layer  23 B. 
     The second adjustment layer  23 B and the third adjustment layer  23 C preferably have the same film thickness and are preferably made of the same material. Thereby, as will be described later, these layers are able to be formed collectively, and the manufacturing step is simplified. 
     In this embodiment, a laminated structure  23 D (high reflectance area) composed of the first adjustment layer  23 A and the second adjustment layer  23 B is circular, for example, as illustrated in  FIGS. 4A, 4B, and 4C . The laminated structure  23 D is formed in a region including an opposed region C 1  (first opposed region) opposing to the center point of the current injection region  15 B, and is arranged so that a center point C 2  of the laminated structure  23 D is located in a region different from the opposed region C 1 . 
     More specifically, the first adjustment layer  23 A and the second adjustment layer  23 B are arranged in a region to avoid a specific region  23 E (in a region other than the specific region  23 E) that corresponds to two peaks P opposed with a region other than the opposed region C 1  in between, in an opposed region opposing to a region where high-order transverse mode (primary mode) including four peaks P of double rotation symmetry or quad rotation symmetry. Meanwhile, the third adjustment layer  23 C (low reflectance area) is formed in a region where the first adjustment layer  23 A and the second adjustment layer  23 B are not formed in an opposed region opposing to the current injection region  15 B, that is, in a region including the foregoing specific region  23 E. 
     Therefore, as illustrated in  FIG. 5 , in the transverse mode adjustment section  23 , reflectance R 2  in the third adjustment layer  23 C (region including the specific region  23 E) is lower than reflectance R 1  in the laminated structure  23 D (the opposed region C 1 ) composed of the first adjustment layer  23 A and the second adjustment layer  23 B. 
     A width W 1  (diameter) of the laminated structure  23 D is preferably in the range satisfying the following Formula 1, where a length (or diameter) of the diagonal line (in the short axis direction) of the current injection region  15 B is W 2 . Further, a difference (shift length) S between the center of the first adjustment layer  23 A and the second adjustment layer  23 B and the center point of the current injection region  15 B is preferably in the range satisfying the following Formula 2.
 
W 1 ≥0.6×W 2    Formula 1
 
S≥0.1×W 2    Formula 2
 
     Further, where the reflectance in the case where the foregoing adjustment layers are not provided in the aperture of the upper electrode  19  is R 3 , each refractive index is preferably adjusted to satisfy the following Formula 3. Thereby, high-order transverse mode oscillation is able to be selectively prevented without decreasing the light output of the fundamental transverse mode.
 
R 1 ≥R 3 ≥R 2    Formula 3
 
     The laser diode  1  according to this embodiment may be manufactured, for example, as follows. 
       FIGS. 6A and 6B  to  FIGS. 8A and 8B  illustrate the manufacturing method in the order of steps.  FIGS. 6A and 6B  to  FIGS. 8A and 8B  respectively illustrate a structure of a cross section taken along the same direction as the direction of arrows A-A of  FIG. 1  of a device in process of manufacture. 
     Here, compound semiconductor layers made of GaAs over the substrate  10  are formed by MOCVD (Metal Organic Chemical Vapor Deposition) method, for example. As a raw material of Group III-V compound semiconductor, for example, trimethyl aluminum (TMA), trimethyl gallium (TMG), trimethyl indium (TMIn), and arsine (AsH 3 ) are used. As a raw material of a donor impurity, for example, H 2 Se is used. As a raw material of an acceptor impurity, for example, dimethyl zinc (DMZ) is used. 
     First, the lower DBR layer  11 , the lower spacer layer  12 , the active layer  13 , the upper spacer layer  14 , the oxidized layer  15 D, the upper DBR layer  16 , and the contact layer  17  are layered over the substrate  10  in this order. After that, a resist layer R 1  is formed on the contact layer  17  ( FIG. 6A ). 
     Next, the contact layer  17 , the upper DBR layer  16 , the oxidized layer  15 D, the upper spacer layer  14 , the active layer  13 , the lower spacer layer  12 , and the upper part of the lower DBR layer  11  are selectively etched by, for example, RIE (Reactive Ion Etching) method to form the mesa  18  ( FIG. 6B ). 
     Next, oxidation treatment is performed at high temperature in the water vapor atmosphere to selectively oxidize Al of the oxidized layer  15 D from the side face of the mesa  18 . Thereby, the peripheral region of the oxidized layer  15 D becomes an insulating layer (aluminum oxide). That is, the peripheral region becomes the current confinement region  15 A, and only the central region becomes the current injection region  15 B. Accordingly, the current confinement layer  15  is formed ( FIG. 7A ). After that, the resist layer R 1  is removed. 
     Next, a resist layer R 2  is formed on the top of the mesa  18 . After that, the central part of the contact layer  17  is selectively removed by, for example, wet etching to form an aperture ( FIG. 7B ). After that, the resist layer R 2  is removed. 
     Next, the foregoing dielectric material is deposited on the entire surface including the surface of the mesa  18  by, for example, CVD (Chemical Vapor Deposition) method. After that, the deposited dielectric material is selectively removed by etching so that the portion corresponding to the region other than the specific region  23 E is left in the top face of the mesa  18 . Thereby, the first adjustment layer  23 A is formed ( FIG. 8A ). 
     Next, by using the method similar to the foregoing method, the second adjustment layer  23 B is formed on the first adjustment layer  23 A. After that, the third adjustment layer  23 C is formed in the specific region  23 E of the top face of the mesa  18 . Further, the protective film  20  is formed on the side face of the mesa  18  and the surface on the periphery of the mesa  18  ( FIG. 8B ). The foregoing dielectric material has superior selectivity for semiconductors such as the upper DBR layer  16 . Further, the foregoing dielectric material does not need to be formed in a complicated shape. Therefore, the first adjustment layer  23 A is able to be easily formed by etching. 
     In the case where the second adjustment layer  23 B, the third adjustment layer  23 C, and the protective film  20  have the same film thickness and are made of the same material, these layers are preferably formed collectively in order to simplify the manufacturing process. 
     Next, the foregoing metal material is layered on the entire surface by, for example, vacuum evaporation method. After that, for example, by selective etching of the metal layer, the upper electrode  19  having an aperture in the central region of the top face of the mesa  18  is formed, and the electrode pad  21  is formed on the surface on the periphery of the mesa  18 . 
     Next, the rear face of the substrate  10  is polished as appropriate and the thickness thereof is adjusted. After that, the lower electrode  22  is formed on the rear face of the substrate  10 . Consequently, the laser diode  1  of this embodiment is manufactured. 
     Next, a description will be given of operation and effect of the laser diode  1 . 
     In the laser diode  1 , when a given voltage is applied between the upper electrode  19  and the lower electrode  22 , a current is injected into the active layer  13  through the current injection region  15 B of the current confinement layer  15 . Thereby, light is emitted due to electron-hole recombination. Such light is reflected by the pair of the lower DBR layer  11  and the upper DBR layer  16 . Laser oscillation is generated at a given wavelength λ. Then, the light is emitted as a laser beam outside. 
     In general, in the VCSEL, there is a tendency that light output of the fundamental transverse mode is largest in the central part of the light emitting aperture, and is decreased with distance from the opposed region opposing to the center point of the current injection region. Therefore, in the case where the VCSEL is used for high output purposes, it is preferable that the aperture (light emitting window) of the upper electrode is large enough to extract laser light of the fundamental transverse mode as much as possible. However, in general, there is a tendency that light output of the high-order transverse mode is largest in a region away from the center point of the current injection region at a certain distance, and is decreased with distance from such a region toward the center point of the current injection region Thus, in the case where the light emitting window is excessively large, the laser light of the high-order transverse mode may be also outputted on high output. 
     Therefore, in the VCSEL of related art, the laser light of the high-order transverse mode is prevented from being emitted by the following measures. That is, the size of the current injection region is decreased. Otherwise, a reflectance adjustment layer is provided in the central part of the light emitting window, and thereby a region where the fundamental transverse mode is mainly shown is set to a region with high reflectance, and a region where high-order transverse mode is mainly shown is set to a region with low reflectance. 
     For example, as illustrated in  FIGS. 9A and 9B , in the case where the laminated structure  23 D is arranged so that the center point C 2  of the laminated structure  23 D corresponds to the opposed region C 1  opposing to the center point of the current injection region  15 B, as illustrated in α 1  and β 1  of  FIG. 10 , the smaller the width (diameter) W 1  of the laminated structure  23 D is, the larger the difference between mirror loss of 0 order transverse mode and mirror loss of primary order transverse mode is. However, in the case where the width W 1  of the laminated structure  23 D is small (for example, 3.2 μm), the light output is lower than 90% of the light output in the case where the transverse mode adjustment section  23  is not provided on the upper DBR layer  16 . Meanwhile, however, in the case where the width W 1  of the laminated structure  23 D is large (for example, 4.5 μm), the light output exceeds 90% of the light output in the case where the transverse mode adjustment section  23  is not provided on the upper DBR layer  16 , but the difference between the mirror loss of the 0 order transverse mode and the mirror loss of the primary order transverse mode becomes extremely small, and it is difficult to obtain gain of the high-order transverse mode that is extremely smaller than gain of the fundamental transverse mode. As a result, high-order transverse mode oscillation is generated, and NFP (Near Field Pattern) is distorted. As described above, in the existing method, light output and NFP are in relation of trade-off. 
     Meanwhile, in this embodiment, the laminated structure  23 D is provided in the region other than the specific region  23 E in the top face of the mesa  18 , and the third adjustment layer  23 C is provided in the region including the specific region  23 E. Thereby, as illustrated in  FIG. 5B , the reflectance in the third adjustment layer  23 C (high reflectance area) is lower than the reflectance in the laminated structure  23 D (low reflectance area). Thus, in the foregoing primary mode including the four peaks P of double rotation symmetry or quad rotation symmetry, at least one gain out of a pair of peaks opposing with the opposed region C 1  in between is inhibited. The foregoing primary mode is a mode in which two sets of a pair of peaks opposing with the opposed region C 1  in between are overlapped. Therefore, by suppressing at least one gain out of the two peaks respectively included in each set, gains of each set are able to be suppressed. 
     For example, in the case where the laminated structure  23 D is arranged in the region other than the specific region  23 E, and the center point C 2  of the laminated structure  23 D is deviated from the opposed region C 1  by about 1 μm, as shown in α 2  and β 2  of  FIG. 10 , not only in the case where the width W 1  of the laminated structure  23 D is small (for example, 3.2 μm) but also in the case where the width W 1  of the laminated structure  23 D is large (for example, 4.5 μm), the difference between the mirror loss of the 0 order transverse mode and the mirror loss of the primary order transverse mode is able to be increased. That is, only by deviating the center point C 2  of the laminated structure  23 D from the opposed region C 1 , the difference between the mirror loss of the 0 order transverse mode and the mirror loss of the primary order transverse mode is able to be increased. Thereby, it is possible to obtain gain of the high-order transverse mode that is extremely smaller than gain of the fundamental transverse mode. Thus, high-order transverse mode oscillation is able to be prevented, and NFP is able to be in the shape of a top hat. The light output in the case where the width W 1  of the laminated structure  23 D is large (for example, 4.5 μm) exceeds 90% of the light output in the case where the transverse mode adjustment section  23  is not provided on the upper DBR layer  16 . Therefore, it is found that by setting the width W 1  of the laminated structure  23 D to an appropriate size, it is possible to obtain high output of the high-order transverse mode while suppressing the high-order transverse mode oscillation. That is, in this embodiment, both light output and NFP are able to be satisfied. 
     The foregoing mirror loss is defined individually and respectively for the fundamental transverse mode and the primary transverse mode. Specifically, where a volume in a portion where a high reflectance area of the transverse mode adjustment section  23  (laminated structure  23 D) and the fundamental transverse mode are overlapped is V o (high) , a volume in a portion where the high reflectance area of the transverse mode adjustment section  23  (laminated structure  23 D) and the primary mode are overlapped is V 1 (high) , a volume in a portion a high reflectance area of the transverse mode adjustment section  23  (laminated structure  23 D) and the fundamental transverse mode are not overlapped is V o (low) , and a volume in a portion where the high reflectance area of the transverse mode adjustment section  23  (laminated structure  23 D) and the primary mode are not overlapped is V 1 (low) , mirror loss  αM (high)  of the high reflectance area (laminated structure  23 D) and mirror loss  αM (low)  of a low reflectance area (portion other than the laminated structure  23 D of the transverse mode adjustment section  23 ) are derived from Febry-Perot model as shown in the following Mathematical formulas 1 and 2. V o (high)  and V 1 (low)  are normalized for every mode as shown in the following Formulas 4 and 5. 
     
       
         
           
             
               
                 
                   
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                   ⁢ 
                   
                       
                   
                   ⁢ 
                   1 
                 
               
             
             
               
                 
                   
                     α 
                     
                       M 
                       ⁡ 
                       
                         ( 
                         low 
                         ) 
                       
                     
                   
                   = 
                   
                     
                       1 
                       
                         2 
                         ⁢ 
                         L 
                       
                     
                     · 
                     
                       
                         L 
                         n 
                       
                       [ 
                       
                         1 
                         
                           
                             
                               R 
                               
                                 t 
                                 ⁡ 
                                 
                                   ( 
                                   low 
                                   ) 
                                 
                               
                             
                             · 
                             
                               R 
                               b 
                             
                           
                         
                       
                       ] 
                     
                   
                 
               
               
                 
                   Mathmatical 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   2 
                 
               
             
             
               
                 
                   
                     
                       V 
                       
                         0 
                         ⁢ 
                         
                           ( 
                           high 
                           ) 
                         
                       
                     
                     + 
                     
                       V 
                       
                         0 
                         ⁢ 
                         
                           ( 
                           low 
                           ) 
                         
                       
                     
                   
                   = 
                   1 
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   4 
                 
               
             
             
               
                 
                   
                     
                       V 
                       
                         1 
                         ⁢ 
                         
                           ( 
                           high 
                           ) 
                         
                       
                     
                     + 
                     
                       V 
                       
                         1 
                         ⁢ 
                         
                           ( 
                           low 
                           ) 
                         
                       
                     
                   
                   = 
                   1 
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   5 
                 
               
             
           
         
       
     
     Rb in Mathematical formulas 1 and 2 represents reflectance of the lower DBR layer  11 . R t (high)  represents reflectance of a high reflectance area of the upper DBR layer  16 . R t (low)  represents reflectance of a low reflectance area of the upper DBR layer  16 . It is needless to say that, due to reflectance relation,  αM (high)  is smaller than  αM (low) . 
     Accordingly, mirror loss  α   0   M  of the fundamental transverse mode and mirror loss  α   1   M  of the primary transverse mode are as shown in the following Mathematical formula 3. As understood from Mathematical formula 3, in the case where the high reflectance area becomes larger, V o (high)  and V 1 (high)  become larger and V 0 (low)  and V 1 (low)  become smaller. Therefore,  α   0   M  and  α   1   M  become smaller, and finally become equal to  αM (high) . 
     
       
         
           
             
               
                 
                   
                     1 
                     
                       α 
                       m 
                       M 
                     
                   
                   = 
                   
                     
                       
                         V 
                         
                           m 
                           ⁡ 
                           
                             ( 
                             high 
                             ) 
                           
                         
                       
                       
                         α 
                         
                           M 
                           ⁡ 
                           
                             ( 
                             high 
                             ) 
                           
                         
                       
                     
                     + 
                     
                       
                         V 
                         
                           m 
                           ⁡ 
                           
                             ( 
                             low 
                             ) 
                           
                         
                       
                       
                         α 
                         
                           M 
                           ⁡ 
                           
                             ( 
                             low 
                             ) 
                           
                         
                       
                     
                   
                 
               
               
                 
                   Mathmatical 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   3 
                 
               
             
             
               
                 
                   ( 
                   
                     
                       m 
                       = 
                       0 
                     
                     , 
                     1 
                   
                   ) 
                 
               
               
                 
                     
                 
               
             
           
         
       
     
     Further, in this embodiment, even in the case where the center point C 2  of the laminated structure  23 D is deviated from the opposed region C 1 , or in the case where the shape of the laminated structure  23 D is a shape other than a circle (for example, in the shape of a convex or a cross), the center position of NFP corresponds with the center point C 1  of the current injection region  15 B, and NFP becomes circular irrespective of the shape of the laminated structure  23 D. Therefore, there is no possibility that the general versatility of the laser diode  1  is lowered. 
     Further, in this embodiment, as described above, it is extremely easy to selectively etch the first adjustment layer  23 A, and it is not necessary to form the first adjustment layer  23 A, the second adjustment layer  23 B, and the third adjustment layer  23 C in a complicated shape. Therefore, the laser diode  1  is easily manufactured. 
     Further, in this embodiment, it is not necessary to use a special substrate, and it is not necessary to provide a component with a complicated shape and a complicated structure in the aperture of the upper electrode  19 . Thus, the laser diode  1  is able to be easily and inexpensively manufactured. Further, it is not necessary to decrease the size of the mesa  18 . Thus, it is possible to secure a large area of the current injection region  15 B and the aperture of the upper electrode  19 , and it is possible to obtain low resistance of the semiconductor layer  30  (resonator) and high output of the laser light. Therefore, a practical VCSEL is obtainable. 
     MODIFIED EXAMPLES 
     In the foregoing embodiment, the laminated structure  23 D is circular. However, for example, as illustrated in  FIGS. 11A  to  11 C, the laminated structure  23 D may be in the shape of a convex protruding toward a region sandwiched between the specific regions  23 E. Otherwise, for example, as illustrated in  FIGS. 12A to 12C , the laminated structure  23 D may be in the shape having double convexes protruding toward two regions sandwiched between the specific regions  23 E. Further, for example, as illustrated in  FIGS. 13A to 13C , the laminated structure  23 D may be in the shape of a cross in the region other than the region corresponding to each peak P of the opposed region opposing to the current injection region  15 B. 
     For example, if the laminated structure  23 D is circular, and the laminated structure  23 D is arranged so that the center point C 2  of the laminated structure  23 D corresponds to the opposed region C 1 , as illustrated in  FIG. 14 , output of a simple transverse mode is able to be largest in the case where the width W 1  of the laminated structure  23 D is about 3.65 μm. However, even in this case, the light output is about 90% of the light output in the case where the transverse mode adjustment section  23  is not provided on the upper DBR layer  16 . 
     Meanwhile, for example, as illustrated in  FIGS. 11A to 11C , in the case where the laminated structure  23 D is in the shape of a convex and the width W 1  of the laminated structure  23 D is about 3.0 μm, as illustrated in  FIG. 14 , the difference between the mirror loss of the 0 order transverse mode and the mirror loss of the primary transverse mode is able to be increased while the magnitude of mirror loss of the primary transverse mode is almost equal to that in the case where the laminated structure  23 D is circular. Thereby, the gain of the high-order transverse mode is able to be extremely smaller than the gain of the fundamental transverse mode. Thus, the high-order transverse mode oscillation is able to be prevented, and NFP is able to be in the shape of a top hat. Further, compared to the case that the laminated structure  23 D is circular, the light output is able to be increased up to about 96%. 
     Further, for example, as illustrated in  FIGS. 13A to 13C , in the case where the laminated structure  23 D is in the shape of a cross and the width W 1  of the laminated structure  23 D is about 3.5 μm, as illustrated in  FIG. 14 , the difference between the mirror loss of the 0 order transverse mode and the mirror loss of the primary transverse mode is able to be large while the magnitude of mirror loss of the primary transverse mode is almost equal to that in the case where the laminated structure  23 D is circular. Thereby, the gain of the high-order transverse mode is able to be extremely smaller than the gain of the fundamental transverse mode. Thus, the high-order transverse mode oscillation is able to be prevented, and NFP is able to be in the shape of a top hat. Further, compared to the case that the laminated structure  23 D is circular, the light output is able to be increased up to about 94%. 
     As described above, in the foregoing each modified example, the output of the fundamental transverse mode is able to be further increased, while oscillation of the high-order transverse mode is prevented. 
     In  FIGS. 11A to 11C ,  FIGS. 12A to 12C , and  FIGS. 13A to 13C , the width W 1  of the laminated structure  23 D is a value twice the distance between the portion closest to the center point C 1  of the current injection region  15 B in the outer rim of the laminated structure  23 D and the center point C 1  of the current injection region  15 B. 
     Descriptions have been hereinbefore given of the invention with reference to the embodiment and the modified examples. However, the invention is not limited to the foregoing embodiment and the like, and various modifications may be made. 
     For example, in the foregoing embodiment, the transverse mode adjustment section is composed of the first adjustment layer  23 A, the second adjustment layer  23 B, and the third adjustment layer  23 C. However, the transverse mode adjustment section may have other structure. In short, any structure may be adopted as long as in the foregoing primary mode including the four peaks P of double rotation symmetry or quad rotation symmetry, at least one gain of a pair of peaks opposing with the opposed region C 1  in between is prevented. 
     Further, in the foregoing embodiment and the like, the invention has been described with reference to the AlGaAs-based compound laser diode as an example. However, the invention is also applicable to other compound laser diodes such as a GaInP-based laser diode, an AlGaInP-based laser diode, an InGaAs-based laser diode, a GaInP-based laser diode, an InP-based laser diode, a GaN-based laser diode, a GaInN-based laser diode, and a GaInNAs-based laser diode. 
     It should be understood by those skilled in the art that various modifications, combinations, sub-combinations and alternations may occur depending on design requirements and other factors insofar as they are within the scope of the appended claims or the equivalents thereof.