Abstract:
A vertical cavity surface emitting laser (VCSEL) ( 100 ) has a substrate ( 104 ), on which are disposed first and second distributed Bragg reflectors (DBRs) ( 106, 112 ), each DBR comprising a stack of layers of alternating refractive index, an active layer ( 108 ) disposed between the DBRs, and an aperture layer ( 110 ) disposed either between the DBRs or within one of the DBRs. The aperture layer ( 110 ) has a border ( 116 ) having an internal boundary with a plurality of indented portions defining one or more apertures. Such a VCSEL is easily manufacturable and provides a narrow bandwidth output, as well as mitigating at least some of the problems of prior art VCSELs. Mesa ( 102 ) may be etched to be non-circular and subsequent selective oxidation of aperture layer ( 110 ) results in a non-circular current confinement aperture ( 114 ) promoting higher-order lateral modes (LP 21 ).

Description:
FIELD OF THE INVENTION 
       [0001]    This invention relates to a vertical cavity surface emitting semiconductor laser, in particular such a laser in which the lasing of different transverse optical cavity modes is at least partially controlled, and a method for fabrication of such a laser. 
       BACKGROUND OF THE INVENTION 
       [0002]    The vertical cavity surface emitting laser (VCSEL) has become an important light source within many technological fields, such as optical telecommunications and sensing. VCSELs are attractive since they can have low threshold currents, low power consumption and high quality far field patterns. Further, VCSELs can have a low manufacturing and testing cost due to their small wafer footprint and the ability to perform quality assessment at wafer scale. 
         [0003]    The optical cavity of a VCSEL is typically short, and so it is inherently only capable of lasing on a single longitudinal mode of the laser&#39;s optical cavity. However, the transverse dimensions of the optical cavity are typically considerably larger than the length of the optical cavity. Consequently the emitted output beam may comprise a plurality of transverse modes, including a fundamental mode and higher order modes. 
         [0004]    Different transverse modes of a VCSEL have different lateral extensions. Consequently, different transverse modes typically experience different round-trip cavity losses. Further the current density within the active layer is typically lower within the centre of the VCSEL than away from the centre. This can be particularly pronounced in VCSELs having both a top electrode with an emission window and a current injection aperture within the laser cavity that is narrower than the emission window. Consequently the optical gain within the active layer will be inhomogeneous, and different transverse modes will experience different levels of optical gain. 
         [0005]    The round trip cavity losses and gains for different transverse modes determine which transverse mode or modes preferentially lase. The losses and gains vary with the current injection and ambient conditions of the VCSEL, and consequently which transverse modes lase can vary. The problem can be exacerbated by two further factors as laser drive current increases. Firstly, due to spatial hole burning the exitation of existing lasing modes will typically not increase in amplitude as quickly as other modes. Secondly, as new modes commence lasing and grow in excitation they may cannibalise existing lasing modes. 
         [0006]    Different transverse modes lase at slightly different wavelengths, and consequently in uncontrolled or variable multimode operation the optical bandwidth of the VCSEL output is broader than in single mode operation. However, many VCSEL applications require a narrow optical bandwidth output. In particular the transmission of high data rate telecommunications signals requires narrow optical bandwidths in order to minimize the mode dispersion that occurs during transmission along lengthy optical fibres, which degrades the shape of the optical data signals carried by the light. 
         [0007]    Furthermore when the VCSEL is able to lase in different transverse modes the operation can be unstable, with different transverse modes dominating the output under different operating conditions. This instability can introduce intensity noise into transmitted signals carried by the VCSEL. Consequently, there is a need to control the lasing behaviour of VCSEL modes. 
         [0008]    The fundamental transverse cavity mode of a typical VCSEL has a circular cross-section and an intensity profile with a single central peak. By contrast the higher order transverse modes typically comprise an even number of peaks arranged around a ring in a pattern having n-fold rotational symmetry. These higher order transverse modes have a broader lateral extension than the fundamental mode. Consequently an approach to stabilising the output of a VCSEL and reducing its bandwidth is to introduce lateral attenuation elements into the laser cavity, which preferentially suppress the higher order modes with respect to the fundamental mode, to cause single fundamental transverse mode operation of the laser. Examples of such approaches include the designs disclosed in EP1276188 and EP1496583. 
         [0009]    The lateral width of the fundamental transverse mode is narrow, which limits the optical output power that a single fundamental mode VCSEL is capable of producing. Consequently to achieve higher optical output powers it would be desirable to drive one or more higher order transverse modes of the VCSEL, whilst at least partially limiting the range of driven modes, thereby narrowing the output optical bandwidth compared with an unlimited design and reducing instability. 
         [0010]    EP1835577 discloses a design of VCSEL comprising a pit that is etched into the centre of the upper reflector of the laser cavity. The pit modifies the reflectivity of the upper reflector of the laser cavity so as to preferentially suppress modes that optically overlap the pit, in particular the fundamental mode, thereby narrowing the bandwidth of the optical output. 
         [0011]    However, the production of the etch pit of EP1835577 requires several additional lithographic processing steps within the VCSEL manufacturing process, such as photoresist deposition, photolithographic exposure, photoresist development, etching and resist removal. Such extra steps increase the complexity of the manufacturing process, and inaccuracies reduce the reliability and attendant yield of that manufacturing process. 
         [0012]    U.S. Pat. No. 6,990,128 discloses an alternative design in which a surface of the laser cavity is selectively etched with a pattern of holes or grooves. The patterns of holes or grooves modify the reflectivity of the upper reflector of the laser cavity. The patterned reflectivity of the upper reflector suppresses transverse modes that optically overlap with the etched pattern, thereby preferentially enhancing a lasing mode in which the intensity profile corresponds with the gaps between the etched regions. Such a design seeks to enable a VCSEL to be driven on substantially a single higher order transverse mode. 
         [0013]    However, the production of the etch pattern of U.S. Pat. No. 6,990,128 requires several additional lithographic processing steps within the VCSEL manufacturing process. Such extra steps increase the complexity of the manufacturing process, and inaccuracies reduce the reliability and attendant yield of that manufacturing process. 
         [0014]    In particular variations in the dimensions and alignment of the etch pattern will affect the performance of the manufactured VCSELs. 
         [0015]    Thus, there remains in the industry a need for an easily manufacturable VCSEL that provides a narrow bandwidth output, and which seeks to mitigate at least some of the problems of prior art VCSELs. 
       SUMMARY OF THE INVENTION 
       [0016]    It is an object of the present invention to provide a vertical cavity surface emitting laser that seeks to overcome at least some of the disadvantages described above, and a method of making such a laser. 
         [0017]    In accordance with a first aspect of the present invention, there is provided a vertical cavity surface emitting laser (VCSEL) comprising a substrate, on which are disposed first and second distributed Bragg reflectors (DBRs), each DBR comprising a stack of layers of alternating refractive index, an active layer disposed between the DBRs, and an aperture layer disposed either between the DBRs or within one of the DBRs, wherein the aperture layer has a border having an internal boundary with a plurality of indented portions defining one or more apertures. 
         [0018]    In accordance with a second aspect of the present invention, there is provided a vertical cavity surface emitting laser (VCSEL) comprising a substrate, on which are disposed first and second distributed Bragg reflectors (DBRs), each DBR comprising a stack of layers of alternating refractive index, an active layer disposed between the DBRs, and an aperture layer disposed either between the DBRs or within one of the DBRs, wherein the aperture layer has a border having an internal boundary defining a plurality of apertures. 
         [0019]    In accordance with a third aspect of the present invention, there is provided a method of manufacturing a VCSEL on a substrate, wherein the VCSEL comprises first and second DBRs, each DBR comprising a stack of layers of alternating refractive index, an active layer disposed between the DBRs, and an aperture layer disposed either between the DBRs or within one of the DBRs, wherein the aperture layer has an aperture provided within a border having an internal boundary with a plurality of indented portions, the method comprising partially oxidising the aperture layer to form the aperture therein. 
         [0020]    In accordance with a fourth aspect of the present invention, there is provided a method of manufacturing a VCSEL on a substrate, wherein the VCSEL comprises first and second DBRs, each DBR comprising a stack of layers of alternating refractive index, an active layer disposed between the DBRs, and an aperture layer disposed either between the DBRs or within one of the DBRs, wherein the aperture layer has a aperture provided within a border having an internal boundary, the method comprising partially oxidising the aperture layer to form a plurality of apertures therein. 
         [0021]    The cross-section of the internal boundary may be generally circular, or have a shape like leaflets of a clover-leaf, or may be shaped like a star with rounded corners. 
         [0022]    The aperture may have n-fold mirror symmetry with respect to mirror planes passing through a centre and/or n-fold rotational symmetry about the centre, where n is an even number of 4 or more. 
         [0023]    The VCSEL may comprise a mesa, the aperture layer may be disposed within the mesa and the border may have an external boundary coincident with an edge of the mesa. The external boundary may have n-fold mirror symmetry with respect to mirror planes passing through a centre and/or n-fold rotational symmetry about the centre, where n is an even number of 4 or more. The cross-section of the external boundary may be generally circular, or have a shape like leaflets of a clover-leaf, or may be shaped like a star with rounded corners. 
         [0024]    The external boundary may have a plurality of indented portions. The indented portions of the internal boundary may correspond with grooves in a side wall of the mesa. The indented portions of the external boundary may correspond with grooves in a side wall of the mesa. 
         [0025]    The gap between the internal and external boundaries may be of substantially uniform width. 
         [0026]    The VCSEL may comprise a plurality of etch pits distributed around the aperture. 
         [0027]    The aperture may be a current aperture and/or an optical aperture. 
         [0028]    The aperture layer may comprise an oxidation layer, the aperture may comprise an unoxidised region of the aperture layer, and the border may comprise an oxidised region of the aperture layer. Alternatively the aperture and the border may comprise regions of the aperture layer having different tunnel junction properties. 
         [0029]    The VCSEL may have an emission window within which an etched pattern may be provided. The etched pattern may have n-fold mirror symmetry with respect to mirror planes passing through a centre and/or n-fold rotational symmetry about the centre, where n may be an even number of 4 or more, and the mirror symmetry lines of the etched pattern may be aligned with mirror symmetry lines of the internal boundary. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0030]    For a better understanding of the present invention and to show more clearly how it may be carried into effect, reference will now be made, by way of example only, to the accompanying drawings, in which: 
           [0031]      FIG. 1  is a schematic three-dimensional view of a first VCSEL according to the present invention 
           [0032]      FIG. 2  illustrates a schematic cross-section through the VCSEL of  FIG. 1 , perpendicular to the substrate 
           [0033]      FIG. 3  illustrates a schematic plan view of the mesa of the VCSEL of  FIG. 1   
           [0034]      FIG. 4  illustrates a schematic plan view of a mesa of a second VCSEL according to the present invention provided with a etched pattern 
           [0035]      FIG. 5  illustrates a schematic plan view of a third VCSEL according to the present invention 
           [0036]      FIG. 6  illustrates a schematic plan view of a fourth VCSEL according to the present invention 
           [0037]      FIG. 7  illustrates a schematic plan view of a fifth VCSEL according to the present invention 
       
    
    
     DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS 
       [0038]    Referring to  FIG. 1  of the accompanying drawings, a vertical cavity surface emitting laser (VCSEL)  100  according to an embodiment of the present invention is illustrated. The VCSEL  100  comprises a mesa  102  etched from a series of semiconductor layers deposited on a substrate  104 . The mesa  102  is shown with sides that are perpendicular to the plane of the substrate, however, it is also known for the mesa to be tapered with inclined sides. 
         [0039]    The semiconductor structure of the VCSEL  100  comprises the substrate  104 , a first distributed Bragg reflector (DBR)  106 , an active region  108 , aperture layer  110  and a second DBR  112 . The VCSEL is further provided with a top electrode  118  having an emission window  120  through which the output of the VCSEL is emitted, and a back electrode  122  on the opposite side of the substrate from the mesa  102 . The electrodes  118  and  122  enable electrical connection to opposite sides of the active region  108 , and comprise metallisations, as are known within the industry, such as Ti—Pt—Au. The emission window  120  may conveniently be circular, or may be shaped in correspondence with the mesa shape. 
         [0040]    The VCSEL structure is grown on the substrate by one of the known epitaxial growth techniques, including, but not limited to, MBE and MOVPE. A brief description of the structure and manufacture of the VCSEL is given below. Further details concerning the epitaxial structure and growth of VCSELs with aperture layers can be found within the literature, including for example EP1276188 and EP1496583. 
         [0041]    In this example the substrate  104  is a GaAs substrate, and the structure described corresponds with the GaAs based material system. However, the use of other substrates and corresponding material systems are also know within the industry, such as the InP, GaP, GaSb and GaN material systems. The first and second DBRs  106  and  112  comprise a plurality of pairs of doped layers of alternating high and low refractive indices. The thickness of each pair of doped layers is equivalent to an optical path length of substantially a half the lasing wavelength of the VCSEL  100 . The plurality of doped layers of the DBRs  106  and  112  are shown schematically in  FIG. 2 , which illustrates a cross-section through the VCSEL of  FIG. 1 . The DBRs  106  and  112  in this example are formed from AlGaAs layers with alternating chemical compositions. The laser active region  108  comprises a plurality of layers, and in this example comprises either a p-i-n or n-i-p structure, with corresponding doping of the DBR adjacent to the p- and n-doped sides of the active regions  108 . The laser active region  108  will typically comprise a heterostructure and include quantum wells, although it will be appreciated that other restricted quantum effect structures may be used. 
         [0042]    In the manufactured VCSEL  100 , the aperture layer  110  comprises an aperture  114  that is substantially electrically conductive and a border  116  that is substantially electrically insulating. Consequently the aperture  114  constricts electrical current flow through the VCSEL. The border  116  has an internal boundary  116 A and external boundary  116 B. 
         [0043]    The aperture  114  is substantially optically transparent having a first refractive index and a first optical path length. However, the border  116  has a different, second refractive index and a different, second optical path length. Consequently, light transmitted through the border  116  is out of phase with parallel light transmitted through the aperture  114 . This results in light transmitted through the border  116  experiencing a lower reflectivity from a DBR  106  or  112  than for light transmitted through the aperture  114 . Thus the border  116  provides an optical spatial filter, since transverse modes that optically overlap with the border experience preferentially increased optical losses. 
         [0044]    At time of epitaxial growth the aperture layer  110  is not laterally patterned, and the border  116  is formed subsequently. At the time of epitaxial growth of the VCSEL of the present example, the aperture layer  110  comprises a semiconductor material having an increased proportion of aluminium relative to the remainder of the layers within the mesa, providing a high oxidation rate during a subsequent step in which the border is formed, as will be discussed below. In this example the oxidation layer is AlAs. 
         [0045]    Following epitaxial growth of the semiconductor layers upon the substrate  104 , an etch mask is created on the upper layer for use in selectively etching the layers to produce the mesa  102 . The shape of the etch mask used will correspond with the desired cross-sectional shape of the mesa  102 . The mesa  102  has a generally circular cross-sectional shape  124 , being either generally cylindrical or generally conic. The mesa  102  is further provided with mesa indentations  126  running up the sides of the mesa. The mesa indentations  126  are more clearly apparent in cross-section, as illustrated in  FIG. 3 , which shows a plan view of the top of the mesa  102 . The mesa indentations  126  may be shallow, or may be concave as illustrated. Consequently the periphery of the mesa  102  is non-circular, having a maximum mesa radius R M  with respect to the centre C (corresponding with a central axis of the mesa), and portions of the periphery with a reduced mesa radius R R  corresponding with the indentations  126 . To produce a mesa  102  with mesa indentations  126 , the shape of the corresponding mask feature should also be provided with indentations. Following deposition and patterning of the masking material, the semiconductor layers will be etched to the desired depth to form the mesa  102 , which will include etching through the aperture layer  110  to expose its edge within the mesa. Suitable anisotropic etching processes are known in the industry. 
         [0046]    Subsequent to the mesa etch step the aperture layer  110  within the mesa  102  is laterally patterned. In the present example a selective wet oxidation process is performed, in which a thickness of the aperture layer  110  adjacent to the surface of the mesa  102  is oxidised, such that the aluminium within the layer is converted to aluminium oxide. The size and shape of the aperture  114  formed is subject to the oxidation rate of the aperture layer, which is dependant upon the oxidation chemistry, the aluminium concentration, the oxidation time and the mesa shape. Due to the way in which the oxidation front progresses during oxidation, the aperture  114  will acquire a shape in correspondence with the cross-sectional shape of the periphery of the aperture layer  110  within the mesa  102 . Accordingly, in the present example, the aperture  112  will also be provided with aperture indentations  128  in correspondence with the mesa indentations  126  in the side of the mesa  102 . Consequently the aperture  112  will be non-circular, having a maximum aperture radius r M  and portions of the aperture with a reduced aperture radius r R . 
         [0047]    In the present example the mesa has a maximum mesa radius of 14 um, a reduced mesa radius of 12 um within the indentations, and the aperture layer is oxidised to produce a border 8 um wide. Consequently the aperture has a maximum aperture radius of 6 um and indentations with a reduced aperture radius of 4 um. 
         [0048]    In operation, a bias is applied between the top and back electrodes  118  and  122 , producing a bias across the active region  108 . The active region  108  is the gain region within the laser cavity of the VCSEL defined between the two DBRs  106  and  112 . The emission window  120  has a window radius W. The aperture  114  is generally smaller than the emission window  120 . 
         [0049]    The shape of the aperture (or apertures) of the present invention patterns the current density within the active region  108  relative to a VCSEL having a complete rotational symmetry. In particular the current density is patterned in correspondence with the shape of the aperture  114 . However, it is known that gain and refractive index are linked by the Kramers-Kronig relations. Accordingly, the refractive index within the mesa is modified in correspondence with the patterning of the current density. This leads to preferential gain guiding of corresponding transverse modes. The VCSEL may preferably be substantially gain guided. 
         [0050]    The mesa  102  and corresponding aperture  114  of the VCSEL  100  of  FIG. 1  have four-fold rotational and mirror symmetries, and the inhomogeneous current injection will also have such symmetries. Such a current injection will preferentially enhance the driving of a higher order transverse mode that also has such symmetries, for example the LP 21  mode. Further this preferential enhancement of certain modes can enable more stable driving of particular modes, reducing cannibalisation of one mode by another as drive current and ambient conditions change, thereby serving to stabilise the relative intensities of those particular modes of the laser. In particular, the indentations may serve to provide patterning of the current density within the active layer and/or the resistance experienced by current flowing through the active layer. This patterning is in correspondence with the optical intensities of selected optical modes. In particular the patterning can correspond with an optical mode that has a more centrally concentrated intensity, such as the fundamental mode. This can reduce the susceptibility of the selected mode or modes to cannibalisation by other modes. 
         [0051]    Many modes of the laser may be excited, but to a lesser extent than the preferred modes. In particular preferential driving of a higher order mode and optical spatial filtering by the aperture will suppress other higher order modes, thereby reducing the bandwidth of the emitted signal with respect to a similar VCSEL with a circular aperture, and mode competition noise in the VCSEL output. 
         [0052]    Further spatial filtering of the transverse cavity modes can be provided by means of an etch pattern  130  etched into the top surface of the mesa with the emission window  120 , as is illustrated in  FIG. 4 . The etch pattern can comprise a multi-legged star, as per the four-legged star shown. Alternatively another pattern having such rotational and mirror symmetries may be used, such as a pattern of etched dots. The legs  132  of the etch pattern  130  are aligned coplanar with those planes of mirror symmetry MS of the mesa  102  and aperture  112  that pass through the mesa indentations  126  and aperture indentations  128 . 
         [0053]    The etched regions of the etch pattern  130  provide a reduced reflectivity compared with the unetched regions, and consequently serve as a spatial filter that preferentially attenuates modes which do not have the same symmetry pattern as the etch pattern. Consequently the etch pattern  130  of  FIG. 4  preferentially attenuates all modes except for a mode  134  with four-fold mirror symmetry, which is preferentially driven. In particular the centre of the etch pattern  130  corresponds with the centre of the fundamental mode, providing particularly acute attenuation of that mode. 
         [0054]      FIGS. 5 and 6  illustrate plan views of mesas  102  of further VCSELs  100  according to the present invention, with more substantial mesa indentations  126  than in  FIG. 1 , resulting in mesas with a substantially cross-like or clover-leaf-like cross-sectional shape. Correspondingly, the aperture  112  of  FIG. 5  has a more pronounced cross-like or clover-leaf-like shape than the aperture of  FIG. 1 . In the case of the  FIG. 6 , the mesa indentations  126  and border  116  are configured such that the aperture  112 ′ comprises a plurality of separate apertures. 
         [0055]      FIG. 7  illustrates a further type of VCSEL  100 ″ in which, rather than etching a mesa, a series of etch pits  134  are formed exposing an edge of the aperture layer, such that following an oxidation step an oxidised region forms in the aperture layer around each etch pit, and adjacent oxidised regions coalesce to produce a composite oxidised region. The composite oxidised regions provide a border within which an aperture  114 ″ is defined, which has aperture indentations  128 ″. 
         [0056]    The accompanying figures illustrate only VCSELs having four-fold rotational and mirror symmetries that correspondingly, preferentially excite a higher order mode with corresponding symmetries, e.g. LP 21 . However, it will be appreciated that the present invention may also be applied to devices having other orders of symmetry. 
         [0057]    For example the device may have only two-fold or six-fold rotational symmetry and respectively preferentially excite the LP 11  or LP 31  transverse mode, which have a peak intensity with corresponding two-fold or six-fold rotational symmetry. 
         [0058]    Advantageously the symmetries of the aperture may be aligned with major crystallographic planes of the substrate. 
         [0059]    Advantageously the VCSEL may also comprise a further aperture layer having a further aperture between the DBRs or within one of the DBRs. The further aperture would advantageously also be non-circular, being provided within a further border having a further internal boundary with a plurality of indented portions. 
         [0060]    It will be appreciated that the present invention is also applicable to VCSELs that emit through the substrate and back of the device. Such VCSELs may be provided with an emission window within the back electrode, aligned with the VCSEL. It will also be appreciated that VCSELs according to the present invention may be provided with an electrode on the top surface of the wafer, surrounding the mesa, in place of the back electrode.