Phase locked laser arrays with single lobe output beam

Abstract: A semiconductor laser array includes a set of low-loss waveguides (32) for transmitting generated light waves from amplification waveguides (30) to an external facet. The width of the output waveguides (32) is less than a critical width required for complete confinement of the transmitted light so that the spot width of the light transmitted by each waveguide is increased to greater than 75% of the spacing between the output waveguides to produce a single-lobed beam. In one embodiment (Fig. 5), scanning contacts (50,52) induce a bias on the set of low-loss output waveguides to scan an output beam.

Description: The invention relates to a phased-array semiconductor laser. Phased-array lasers include a set of directly coupled waveguide amplifiers which generate in-phase light waves. Each waveguide has a terminal aperture at a laser facet that radiates the light waves generated in the waveguide amplifier. Typically, a radiated output beam from the phased-array laser includes a high-intensity central lobe and several low intensity sidelobes. These sidelobes increase the width of the beam and divert energy from the central beam. Many laser applications require a highly resolved output beam. Accordingly, much effort has been expended to develop a phased-array laser that produces an output beam having only a single lobe. It is well-known that for an array of radiators having aperture size S and spacing distance D the ratio of S to D must be greater than 75% to obtain a single-lobed output beam. In existing systems, the output waveguides are forward biased to amplify the light waves propagating therethrough. Thus, if the distance, D, between waveguides is reduced to obtain a single-lobed output beam then evanescent coupling between the output waveguides will occur. Conversely, if the output waveguides are flared to increase the size of the output apertures then higher order transverse modes may be supported. Either evanescent coupling or higher order modes may destabilize the laser output beam. In US-A-4,718,069, Streifer et al. teach variable spacing of the output waveguides to achieve a single-lobed output beam. Y-shaped couplers are used to assure coupling between widely spaced output waveguides and the output waveguides are forward-biased to achieve light amplification. Additionally, many systems, such as a facet scanning system or optical fiber array input scanning, require an output beam which may be scanned in a controllable manner. Typically, an output structure utilizing scanning electrodes is used to vary the index of refraction according to some function across the array. Generally, the bias induced by the scanning electrode is impressed on an amplifying portion of the laser and interferes with the bias applied to cause amplification. Such interference can affect the stability of the laser output beam. An object of the present invention is the provision of a laser array for forming a single-lobed output beam that enables problems of the prior art to be avoided. According to one aspect of the present invention, an output structure for a laser includes a set of output waveguides which are transparent to the light generated by the laser. The output structure does not amplify the light waves generated in the laser and thus does not affect the output stability of the laser. According to a further aspect of the invention, the width of the output waveguides is less than the critical width required to completely confine the guided light waves within the waveguide so that the spot size of light radiated from the output waveguides is increased to greater than about 75% of the spacing between the waveguides to produce a single-lobed output beam. According to another aspect of the invention, a scanning contact electrode pair is used to bias an array of transparent output waveguides to scan a laser output beam. The output stability of the laser is not adversely affected because the scanning bias is not applied to gain regions of the laser. More specifically, the present invention provides a semiconductor laser array comprising a semiconductor structure with first and second parts and having an active layer for light amplification and propagation under lasing conditions; means, electrically coupled only to said first part, for applying an electrical bias to said first part to generate light waves in said active layer; a plurality of index-guided amplification waveguides disposed in said first part for propagating only an in-phase array mode; a plurality of parallel, spaced apart, low-loss, two-dimensional index-guided passive output waveguides disposed in said second part, each output waveguide oriented co-axially to a corresponding amplification waveguide and co-extensively coupled thereto at a first boundary, with each output waveguide being of width S and separated from an adjacent output waveguide by a distance D, said output waveguide for guiding said amplified light waves generated in said corresponding coupled amplification waveguide, wherein the width S and refractive index of each output waveguide are such that the width, W, of the optical field of said generated light guided by said waveguide is greater than S and greater than 75% of D. The present invention further provides a semiconductor laser array comprising a semiconductor structure, with first and second parts, having a plurality of semiconductor heterostructure layers disposed over a substrate, at least one of said layers being an active layer for light amplification and propagation under lasing conditions; means, electrically coupled only to said first part, for applying an electrical forward bias to said layers in said first part to generate light waves in said active layer; a plurality of index-guided amplification waveguides disposed in said first part for propagating only an in-phase array mode and terminating at a boundary; a plurality of parallel, spaced apart, low-loss, two-dimensional index-guided passive output waveguides disposed in said second part, each output waveguide oriented co-axially to a corresponding amplification waveguide and co-extensively coupled thereto at said boundary, with each output waveguide being of width S and separated from an adjacent waveguide by a distance D, for guiding said amplified light waves generated in said corresponding coupled amplification waveguide; wherein the width S and refractive index of each output waveguide are such that the width, W, of the optical field of said generated light guided by said waveguide is greater than S and greater than 75% of D; and means, electrically coupled to only said second part, for applying a voltage bias to a voltage region part, disposed under said means, of each of said plurality of output waveguides, with the length of the voltage region part varying according to a predetermined contact function across said plurality of output waveguides to deflect said output beam by a predetermined angle. The output waveguides may be disposed on a III-V semiconductor. In an embodiment of the invention, the output waveguides are disposed in lithium niobate. The plurality of amplification waveguides may be in the form of a y-coupled array. Likewise, the plurality of output waveguides may be in the form of a y-coupled array. The present invention also provides a semiconductor laser array comprising a monolithic semiconductor structure, divided into first, second, and third parts with the first and second parts separated by a first boundary and the second and third parts separated by a second boundary, each part having a plurality of semiconductor heterostructure layers disposed over a substrate, at least one of said layers of each part being an active layer for light amplification and propagation under lasing conditions; means, electrically coupled only to said second part, for applying an electrical forward bias to said layers in said second part; a first plurality of parallel, spaced apart, low-loss, two-dimensional index-guided passive output waveguides, disposed in the active region of said first part, oriented parallel to an axis in said active layer, with each of said low-loss waveguides having a predetermined width, and having a first end terminating at said first boundary; a second plurality, equal to one more than said first plurality, of parallel, spaced apart, two-dimensional, low-loss, index-guided passive output waveguides, disposed in the active region of said third part, oriented parallel to said axis in said active layer, with each of said low-loss waveguides having a predetermined width, and having a first end terminating at said second boundary; a first plurality of parallel, spaced apart, two-dimensional index-guided amplification waveguides disposed in the active region of said second part, each amplification waveguide oriented co-axially to a corresponding passive waveguide in said first part and coextensively coupled thereto at said first boundary, with each amplification waveguide for generating and amplifying lightwaves at a given wavelength in response to said electrical forward bias; a second plurality of parallel, spaced apart, two-dimensional index-guided amplification waveguides disposed in the active region of said second part, each amplification waveguide oriented co-axially to a corresponding passive waveguide in said third part and co-extensively coupled thereto at said second boundary, with each amplification waveguide for generating and amplifying lightwaves at a given wavelength in response to said electrical forward bias; and a plurality of, two-dimensional index-guided y-shaped coupling amplification waveguides, disposed in the active region of said second part, for interconnecting each amplification waveguide in said first plurality with two adjacent amplification waveguides in said second plurality to radiate out-of-phase modes so that the laser operates in the in-phase mode; wherein the width S and the refractive index of each output waveguide are such that the width W of the optical field of the laser light guided by the output waveguides is greater than the width S and greater than 75% of the distance D between adjacent output waveguides. The present invention further provides a semiconductor laser array comprising a monolithic structure, divided into first, second and third parts with the first and second parts separated by a first boundary and the second and third parts separated by a second boundary, and each part having an active layer; means for electrically forward biasing only said second part; a first plurality of parallel, low-loss, passive output waveguides disposed in said first part and terminating at said first boundary; a second plurality of parallel, low-loss, passive output waveguides disposed in said third part oriented parallel to said first plurality of output waveguides, and terminating at said second boundary; and a plurality of index-guided amplification waveguides disposed in the second part for propagating only an in-phase array mode and oriented co-axially and coupled with the passive waveguides at said first and second boundaries; wherein the width S and the refractive index of each output waveguide are such that the width W of the optical field of the laser light guided by the output waveguides is greater than the width S and greater than 75% of the distance D between adjacent output waveguides. By way of example only, embodiments of the invention will now be described with reference to the accompanying drawings, in which: Fig 1 is a cross-sectional view of a typical layer structure in a semiconductor laser; Fig. 2A is a top view of a layer of a semiconductor laser array in accordance with the present invention; Fig. 2B is a perspective view of a hybrid structure including a separate laser and coupler; Fig. 2C is view similar to Fig 2A of a laser array having two output structures; Fig. 2D is part of a view similar to Fig. 2A of a laser array having a y- coupled passive output structure; Fig. 3 is a graph of the light wave intensity for an index-guided waveguide; Figs. 4A-4E are graphs depicting output beam intensities against angular position ϑ across a laser array; and Fig. 5 illustrates a semiconductor laser array incorporating a scanning system. Referring now to FIGS. 1 and 2A, there is illustrated an enlarged view of a semiconductor structure 10 comprising a plurality of epitaxially deposited layers 22-28 on substrate 20. As an example, semiconductor structure 10 may be a semiconductor heterostructure comprising (see Fig. 2A) a central section 11, which may be an active medium, and a passive waveguide section 13 separated from the central section 11 by a boundary 15. Substrate 20 may comprise n-GaAs and epitaxial layers 22-28 may be consecutively deposited in an MO-CVD reactor as is known in the art. These epitaxially deposited layers may be, for example, as follows: Cladding layer 22 of n-Ga1-yAlyAs wherein, for example, y = 0.40; active region 24 comprising a layer of GaAs or Ga1-xAlxAs where y>x, or a single quantum well layer of GaAs or a multiple quantum well of alternating layers of GaAs and Ga1-xAlxAs or alternating layers of Ga1-xAlxAs and Ga1-zAlzAs where y>z>x; cladding layer 26 of p-Ga1-yAlyAs and a cap layer 28 of p + GaAs. In the particular example here, active region 24 comprises multiple quantum wells. This multiple well structure is comprised of four 12 nm quantum wells of Ga1-xAlxAs, wherein x = 0.05. separated by three 6 nm barriers of Ga1-zAlzAs, wherein z = 0.20. Therefore, the layer structure has a width, Lz, of approximately 66 nm. In Fig. 2A, a set of index-guided stripes 30, disposed in the active layer 24 of the central section 11, are joined in a Y-coupled configuration. The central section is forward-biased so that light of a given wavelength is generated and amplified under lasing conditions. The Y-couplers cause excited out-of-phase modes to radiate from the straight sections and cause the light waves generated in the stripes 30 to be phase locked. Y-guides are used as an example of any configuration that leads to phase locked operation in the fundamental mode. A set of index-guided output waveguides 32, disposed in the active layer 24 of the output section 13, are oriented co-axially to the stripes 30 and joined thereto at the boundary 15. These output waveguides 32 are narrower than the stripes 30 and are transparent to the light waves generated in the stripes 30. This set of waveguides serves as an output coupler for the phase-locked array. A method for forming the index-guided stripes 30 and transparent index-guided waveguides 32 using impurity induced disordering techniques is fully disclosed in U.S. Patent number 4,802,182 to Thornton et al. Alternatively, laser patterned desorption (LPD) waveguides may be utilized. This process is disclosed in EP-A-0 364 259. The index-guided stripes and waveguides 30 and 32 in active layer 24 have a greater index of refraction than the neighboring areas of active layer 24 and of cladding layers 22 and 26. Thus, the light generated in the stripes and waveguides 30 and 32 is confined by the well-known phenomena of total internal reflection. Figs. 2C and 2D depict alternative embodiments. In Fig. 2C the semiconductor structure has a third section in which another set of output waveguides is disposed and which is also separated from the central section 11 by a boundary whereby, in this embodiment, output couplers 13a and b are attached to each end of the amplification part 11 of the array. In Fig. 2D the output coupler 13 is a passive y-coupled array that phase-locks the light generated in the amplification section 11. Fig. 3 is a planar top view schematically depicting the amplitude of the light waves in an index- guided stripe or waveguide 30 or 32 formed in the active region 24. As stated above, the index of refraction of the stripe or waveguide 30 or 32 is greater than the index for the exterior part 24e of the active region 24. The line 39 indicates the strength of the light wave field. In the exterior region 24e the strength of the field decays proportionally to exp[-S/2(abs(x))] so that the spreading of the light becomes greater when the width of the waveguide becomes smaller. The characteristics of the output beam emitted from the output waveguides 32 will now be described with reference to Figs. 4A-4E. The near-field emission pattern is depicted in Fig. 4A where W is the spot width of the light radiated by each output waveguide 32 and D is the spacing between the centers of the output waveguides 32. The far-field single waveguide emission pattern 40 of each waveguide is depicted in Fig. 4B and the point array pattern 42 of an array of point emitters separated by D is depicted in Fig. 4C. The single waveguide pattern 40 has a very small magnitude for values of ϑ greater than a cut-off point equal to about λ/W, where ϑ is the angle of light wave radiation relative to the normal from the output mirror of the array and λ is the wavelength of the emitted light. The actual far field emission pattern for the array depicted in Fig. 4A is the product of the emission patterns of Figs. 4B and 4C and is depicted in Fig. 4D. Note that in Fig. 4D the constant heights of the peaks of the point array pattern 42 are modulated by the single waveguide pattern 40. As depicted in Fig. 4D, for a spot width greater than Ws only the first peak will be located before the cut-off point of the single waveguide pattern 40 so that the array pattern 44 will be single- lobed as depicted in Fig. 4E. As is well-known in the art, a single lobed output beam is obtained when W is equal to about .75D. Typically, waveguides have been designed to obtain nearly complete confinement of the guided light waves so the W, the spot width, is equal to S, the width of the waveguide. Attempts to increase S lead to the problems of extra modes and evanescent coupling described above. In the present system, the width of the waveguides is decreased below a critical width necessary to obtain complete confinement so that the optical field begins to spread as described above with reference to Fig. 3. Typically, for GaAs lasers this critical width is about 1 micron. Since the output waveguides 32 are narrowed they do not physically interfere as in prior art structures. Additionally, the output waveguides are transparent so that no biasing is required to reduce absorption. Accordingly, the output structure is not affected by changes in bias voltages or current densities in the active medium 24. Fig. 5 depicts a system for scanning the far- field angle of the output beam of the laser array. In Fig. 5 a pair of triangular shaped scanning contact pairs 50 and 52 are disposed on the top surface of the second part 13 of the substrate 10. Each contact pair 50 or 52 has a first edge oriented parallel to the boundary 15 and a second edge oriented at 45° to the boundary. A scanning voltage is applied to the scanning contacts 50 or 52 to reverse-bias the activated length of each output waveguide 32 disposed between the scanning contacts to provide a phase shift in the beam radiated from each output waveguide 32 via the electro-optic effect. The magnitude of the phase shift, P, induced in a given output waveguide 32 is proportional to the length of the output waveguide 32 which is reverse-biased and is equal to: P = 4πLn/λ where n is the index of refraction and n is the wavelength of the generated light waves. The induced phase shift, P, can be varied by varying the magnitude of the scanning voltage applied to the scanning contacts 50 or 52. In the embodiment depicted in Fig. 5, for the triangular first contact pair 50 the magnitude of the activated length of each output waveguide 30 varies linearly across the array of output waveguides. This linear variation results in a scanning angle β defined by the relationship: sinβ = Pλ2πD. Applying a scanning voltage to the first contact 50 increases the phase shift from the bottom to the top of the output waveguide array and therefore scans the beam in a first direction. Biasing the second contact pair 52 increases the phase shift from the top to the bottom of the array and therefore scans the beam in an opposite direction. The scanning contact pairs 50 and 52 may be forward-biased to obtain a phase-shift due to the variation of the index of refraction caused by the free carrier effect. Further, the shape of the contacts may be changed to vary the magnitude of the activated length across the output waveguide array according to a predetermined function. The edge of the contact 52 can have other geometric shapes. For example, if the edge were shaped as a parabola the width of the central lobe could be increased. The bias induced by the scanning electrode pairs 50 or 52 is applied to the second part 13 of the structure where the output waveguides do not function to amplify the light waves generated in the stripes 30. Accordingly, this scanning bias does not interfere with the forward bias used to achieve amplification in the stripes 30 so that the laser output is stable. It is not required to amplify the light waves propagating in the output waveguides 32 because these waveguides 32 are transparent to the light waves generated in the stripes 30. Substitutions and modifications may be made in the embodiments of the invention described above. For example, as depicted in Fig. 28 the coupled 13 and laser 11 may be separate hybrid structures joined at boundary 15. In that case the output waveguides 32 could be formed using an active region of lithium niobate. In the embodiments of the invention described above, problems of evanescent coupling and support of extra modes are obviated because there is no gain in the transparent output waveguides 32 which support only one mode.

Claims: A semiconductor laser array comprising: a semiconductor structure (10) with first and second parts (11, 13) and having an active layer (24) for light amplification and propagation under lasing conditions; means (12, 14), electrically coupled only to said first part (11), for applying an electrical bias to said first part to generate light waves in said active layer; a plurality of index-guided amplification waveguides (30) disposed in said first part for propagating only an in-phase array mode; a plurality of parallel, spaced apart, low-loss, two-dimensional index-guided passive output waveguides (32) disposed in said second part (13), each output waveguide oriented co-axially to a corresponding amplification waveguide and co-extensively coupled thereto at a first boundary (15), with each output waveguide being of width S and separated from an adjacent output waveguide by a distance D, said output waveguide for guiding said amplified light waves generated in said corresponding coupled amplification waveguide, wherein the width S and refractive index of each output waveguide are such that the width, W, of the optical field of said generated light guided by said waveguide is greater than S and greater than 75% of D. A laser array as claimed in claim 1, further comprising: means (50, 52), electrically coupled to only said second part, for applying a voltage bias to a voltage region part, disposed under said means, of each of said plurality of output waveguides, with the length of the voltage region part varying according to a predetermined contact function across said plurality of output waveguides to deflect said output beam by a predetermined angle. A semiconductor laser array comprising: a semiconductor structure (10), with first and second parts (11, 13), having a plurality of semiconductor heterostructure layers (22, 24, 26, 28) disposed over a substrate (20), at least one (24) of said layers being an active layer for light amplification and propagation under lasing conditions; means, electrically coupled only to said first part (11), for applying an electrical forward bias to said layers in said first part to generate light waves in said active layer; a plurality of index-guided amplification waveguides (30) disposed in said first part for propagating only an in-phase array mode and terminating at a boundary (15); a plurality of parallel, spaced apart, low-loss, two-dimensional index-guided passive output waveguides (32) disposed in said second part (13), each output waveguide oriented co-axially to a corresponding amplification waveguide and co-extensively coupled thereto at said boundary, with each output waveguide being of width S and separated from an adjacent waveguide by a distance D, for guiding said amplified light waves generated in said corresponding coupled amplification waveguide; wherein the width S and refractive index of each output waveguide are such that the width, W, of the optical field of said generated light guided by said waveguide is greater than S and greater than 75% of D; and means (50, 52), electrically coupled to only said second part, for applying a voltage bias to a voltage region part, disposed under said means, ot each of said plurality of output waveguides, with the length of the voltage region part varying according to a predetermined contact function across said plurality of output waveguides to deflect said output beam by a predetermined angle. A laser array as claimed in claim 2 or claim 3, wherein said means for applying a voltage bias comprises: an electrode pair, disposed over a surface of the second part of said structure, having a first edge oriented parallel to said boundary and having a second edge oriented at an angle to said boundary. A laser array as claimed in claim 4, wherein the shape of said second edge is a selected geometric shape. A laser array as claimed in any one of claims 2 to 5 wherein: said predetermined contact function is a linear function. A laser array as claimed in any one of the preceding claims, in which the semiconductor structure further comprises a third part (13b) and a second plurality of substantially parallel, spaced apart, low-loss, two-dimensional index-guided output waveguides disposed in said third part, each output waveguide in said third part being oriented co-axially to a corresponding amplification waveguide and co-extensively coupled thereto at a second boundary, and being of width S and separated from an adjacent output waveguide by said distance D, said output waveguides in the third part being provided for guiding said amplified light waves generated in said corresponding coupled amplification waveguide, and providing less confinement of guided light waves than said amplification waveguides. A laser array as claimed in any one of the preceding claims, wherein said ouput waveguides and/or said amplification waveguides are in the form of a y-coupled waveguide array. A laser array as claimed in any one of the preceding claims, wherein said output waveguides and/or said amplification waveguides are structures formed utilizing a layer disordering technique. A laser array as claimed in any one of the preceding claims, wherein the first and second parts of the semiconductor structure comprise respective monolithic structures and said first boundary ( 15) is the boundary between those monolithic structures. (Fig. 2B). A semiconductor laser array comprising: a monolithic semiconductor structure, divided into first, second, and third parts (13a, 11, 13b) with the first and second parts (13a, 11) separated by a first boundary and the second and third parts (11, 13b) separated by a second boundary, each part having a plurality of semiconductor heterostructure layers disposed over a substrate, at least one of said layers of each part being an active layer for light amplification and propagation under lasing conditions; means, electrically coupled only to said second part, for applying an electrical forward bias to said layers in said second part; a first plurality of substantially parallel, spaced apart, low-loss, two-dimensional index-guided passive waveguides, disposed in the active region of said first part, oriented parallel to an axis in said active layer, with each of said low-loss waveguides having a predetermined width, and having a first end terminating at said first boundary; a second plurality, equal to one more than said first plurality, of substantially parallel, spaced apart, two-dimensional, low-loss, index-guided passive waveguides, disposed in the active region of said third part, oriented parallel to said axis in said active layer, with each of said low-loss waveguides having a predetermined width, and having a first end terminating at said second boundary; a first plurality of substantially parallel, spaced apart, two-dimensional index-guided amplification waveguides disposed in the active region of said second part, each amplification waveguide oriented co-axially to a corresponding passive waveguide in said first part and coextensively coupled thereto at said first boundary, with each amplification waveguide for generating and amplifying lightwaves at a given wavelength in response to said electrical forward bias; a second plurality of parallel, spaced apart, two-dimensional index-guided amplification waveguides disposed in the active region of said second part, each amplification waveguide oriented co-axially to a corresponding passive waveguide in said third part and co-extensively coupled thereto at said second boundary, with each amplification waveguide for generating and amplifying lightwaves at a given wavelength in response to said electrical forward bias; and a plurality of, two-dimensional index-guided y-shaped coupling amplification waveguides, disposed in the active region of said second part, for interconnecting each amplification waveguide in said first plurality with two adjacent amplification waveguides in said second plurality to radiate out-of-phase modes so that the laser operates in the in-phase mode; wherein the width S and the refractive index of each output waveguide are such that the width W of the optical field of the laser light guided by the output waveguides is greater than the width S and greater than 75% of the distance D between adjacent output waveguides. (Fig.2C). A semiconductor laser array comprising: a monolithic structure, divided into first, second and third parts (13a, 11, 13b) with the first and second parts (13a, 11) separated by a first boundary and the second and third parts (11, 13b) separated by a second boundary, and each part having an active layer; means for electrically forward biasing only said second part; a first plurality of parallel, low-loss, passive output waveguides disposed only in said first part and terminating at said first boundary; a second plurality of parallel, low-loss, passive output waveguides disposed only in said third part oriented parallel to said first plurality of output waveguides and terminating at said second boundary; and a plurality of index-guided amplification waveguides disposed in the second part for propagating only an in-phase array mode and oriented co-axially and coupled with the passive waveguides at said first and second boundaries; wherein the width S and the refractive index of each output waveguide are such that the width W of the optical field of the laser light guided by the output waveguides is greater than the width S and greater than 75% of the distance D between adjacent output waveguides (Fig. 2C). A laser array as claimed in claim 12, wherein said plurality of amplification waveguides in said second part is in the form of a y-coupled waveguide array. A laser array as claimed in any one of claims 11 to 13, wherein at least one of said first, second, and third parts is formed utilizing a layer disordering technique. A laser array as claimed in any one of claims 11 to 14, wherein at least one of said first, second, and third parts is formed by utilizing impurity induced layer disordering.

Inventors: PAOLI THOMAS L, PAOLI, THOMAS L.
Applicants: XEROX CORP, XEROX CORPORATION
Application year: 1991
Main classification: H01S3
IPC codes: H01S5