SEMICONDUCTOR DIODE LASER, IN PARTICULAR A LASER AMPLIFIER, AND METHOD OF MANUFACTURING THIS LASER

Abstract: The invention relates to a III-V laser (amplifier) with an active region (4A) which encloses a small angle with the end faces (50, 51), is separated therefrom by a preferably current-blocking cladding layer (5) and has a tapering end (40) of which a first side face (42) coincides with a side face (42) of the remainder of the strip-shaped active region (4A), while a second side face (43) thereof encloses an acute angle with the perpendicular to the end faces (50, 51). Such a laser has an amplification ripple, which is undesirable. In a laser according to the invention, the second side face (43) of the tapering portion (40) encloses an angle with the perpendicular to the end face (50, 51) which lies between 0 and 30 DEG , preferably between 0 and 10 DEG , and which is preferably approximately 0 DEG . The laser according to the invention has a particularly low reflection, as a result of which said amplification ripple is absent or at least very small. No differences in growing processes against said side faces occur since both the first and the second side faces (42, 43) of the active region (4A) are mutually substantially parallel. Accordingly, the laser is preferably of the buried hetero type. In that case, the growth around the active region (4A) is very homogeneous, which benefits the yield and quality of the lasers. The laser is preferably constructed as an amplifier, for which purpose the end faces (50, 51) are provided with an anti-reflection layer. The invention, finally, also relates to a method by which the desired laser is obtained in a simple manner.

Description: Semiconductor diode laser, in particular a laser amplifier, and method of manufacturing this laser. The invention relates to a semiconductor diode laser, in particular a semiconductor diode laser amplifier referred to as laser for short hereinafter, with a semiconductor body of III-V semiconductor materials comprising a substrate and an overlaying semiconductor layer structure with at least a first cladding layer of a first conductivity type, a second cladding layer of a second conductivity type opposed to the first, said cladding layers being provided with current supply means, and between the first and second cladding layers an active layer and a pn junction which, given a sufficient current strength in the forward direction, is capable of amplifying or generating electromagnetic radiation in a strip-shaped active region which forms part of the active layer, which lies within a resonance cavity formed between two parallel end faces, the longitudinal axis of said resonance cavity enclosing a small angle with the peφendicular to the end faces, and which has at least one end which is situated adjacent an end face and is separated from said end face by a third cladding layer which is preferably current-blocking and which is provided with a tapering portion, as seen in projection, of which a first side face coincides with a side face of the strip-shaped active region outside the tapering portion and of which a second side face encloses an acute angle with the perpendicular to the end face. Such a laser finds its application as a source or amplifier in optical registration or glass fiber communication systems. The term " laser " in the present application accordingly also covers a laser amplifier. The wavelength at which the laser operates may vary between approximately 0.5 and, for example, 1.5 μ . The invention also relates to a method of manufacturing such a laser. Such a laser is known from the English abstract JP-A-5-175611 published under no. 62 E 1452 in Patent Abstracts of Japan, vol. 17, no. 583, 22 October 1993. This abstract relates to a laser amplifier. To reduce the reflection at an end face of the radiation amplified or to be amplified, the strip-shaped active region encloses a small angle with the end faces which are preferably provided with an anti-reflection layer, also with the purpose of reducing this reflection. The ends of the active region lie at a certain distance from the end faces for the same reason and are separated therefrom by a cladding layer. The angle enclosed by said radiation and the end faces should be approximately equal to 90° outside the active region in order to couple the radiation amplified or to be amplified readily into a glass fiber. For this purpose, the active region is provided with a tapering end, seen in projection, of which a side face coincides with a side face of the active region outside the tapering end, while another side face encloses an angle with the perpendicular to the end faces which will lie between approximately 90 and approximately 60°. The value required for this angle depends on the angle enclosed by the longitudinal direction of the active region and the peφendicular to the end faces, and on the difference in reflective index between the active region and the (third) cladding layer: if die latter angle is approximately 0°, the former angle should be 90°); if the latter angle is approximately 20° - which is a maximum value in practice -, the value required for the former angle is approximately 60°. A disadvantage of the known laser is that it has a too great amplification ripple, i.e. the amplification is not constant in the case of minor variations in the wavelength to be amplified. This is undesirable. The present invention has for its object inter alia to provide a laser which does not have the above disadvantage, or at least to a much lesser degree, i.e. which has substantially no amplification ripple. The invention also has for its object to provide a method by which such a laser may be readily manufactured. According to the invention, a laser of the kind mentioned in the opening paragraph is for this puφose characterized in that the second side face of said tapering portion encloses an angle with the peφendicular to the end face which lies between zero and 30°. The invention is based on the recognition first of all that said problem of a ripple occurring in the amplification is connected with a too high reflection. It is also based on the recognition that the reflection can be further reduced in that the reflection occurring between the active region and the third cladding layer is reduced. This is achieved in the laser according to the invention by giving the second side face an angle to the peφendicular to an end face which lies between 0 and 30°. This enlarges the region over which the active layer has a tapering shape. A result of this is that the difference in effective refractive index between the active region and the third cladding layer is reduced, so that the reflection therebetween is strongly reduced. Preferably, the angle last mentioned is chosen to lie between 0 and 10°, and in a preferred embodiment this angle is approximately 0°. Said reflection is particularly low in this case. The incoming or outgoing radiation is no longer peφendicular to an end face in the laser according to the invention, it is true, but this disadvantage may readily be eliminated in that, for example, a glass fiber used is positioned at an angle to an end face, for example an angle of approximately 35°. An amply sufficient coupling efficiency can thus be achieved in practice. An important additional advantage of a laser according to the invention is that both the first and the second side face of the tapering portion of the active region enclose only a (very) small angle with one another and with the peφendicular to the end face. This latter face corresponds to either the <01-1 > or the equivalent < 110> direction, or the <011 > or the equivalent <-110> direction in III-V materials. Growing of a III-V material against a surface extending in said directions progresses somewhat differently for the two (groups of) directions. In the laser according to the invention, nothing or substantially nothing is experienced of said differences because both the first and the second side face extend (substantially) in the same direction. The laser according to the invention is thus particularly suitable for embodiments of the so-called buried hetero type. A (current-blocking) cladding layer is present in this type not only between the active region and an end face but also on either side of the active region. In a major embodiment of a laser according to the invention, accordingly, the strip-shaped active region forms part of a strip-shaped mesa which also comprises the first and the second cladding layer, which coincides with the strip-shaped active region seen in projection, and which is surrounded by a further cladding layer which is current-blocking. Such a laser is of the so-called SIPBH (= Semi Insulating Planar Buried Hetero) type and is particularly suitable for use in a glass fiber communication system when constructed as a laser (amplifier). This modification of the laser may also be manufactured comparatively easily by MOVPE (= Metal Organic Vapor Phase Epitaxy), which is a very attractive technology. In a particularly favorable modification of the latter embodiment, the strip-shaped mesa is bounded on either side by a fourth cladding layer which is current- blocking and forms a further strip-shaped mesa therewith which has a side face coinciding with the second side face and which is surrounded by the third cladding layer. The manufacture of this modification does comprise more steps than a process in which the third cladding layer is entirely provided directly around the strip-shaped mesa, but this is counteracted by an important advantage. Underetching and rounding of the tapering portion of the strip-shaped active region is avoided or limited thanks to the presence of the fourth cladding layer on either side of the strip-shaped mesa (i.e. on either side of the strip-shaped active region) when the second side face is formed by etching. Indeed, said rounding will be restricted to portions of the fourth cladding layer. Problems may arise there during growing of the third cladding layer because in that location the mask used during etching, which also serves as a mask in the (selective) application of the third cladding layer, projects comparatively far. The irregularities arising therefrom, such as air-filled pockets in the III-V crystal of the third cladding layer, however, will not be present in the radiation path provided the further mesa is sufficiently wide. As a result, the radiation pattern of a laser according to the invention is an optimum because it is not disturbed. Reference is also made here to the discussion of a method according to the invention given below by way of further explanation. Preferably, the further strip-shaped mesa does not become wider than one to ten times the width of the strip-shaped mesa. In this case the area to be grown during the application of the third cladding layer is still comparatively large, i.e. substantially the entire laser surface area. This has the advantage that the growing process of the third cladding layer can take place in a very controlled manner, which promotes inter alia the crystal quality and planeness of the third cladding layer. In a laser according to the invention, preferably, the longitudinal axis of the strip-shaped active region encloses an angle with the end face which lies between 0 and 20° and which is preferably approximately 10°. On the one hand the reflection reduction at the end faces as a result of said angle is comparatively great with such angles, while on the other hand coupling of the radiation is still very well possible. A laser according to the invention is preferably constructed from a semiconductor body in the InP/InGaAsP material system, while the end faces are provided with an anti-reflection layer. The laser is particularly suitable then for use as an amplifier in an optical communication system within the wavelength window from 1 to 1.6 μm. A method of manufacturing a semiconductor diode laser according to the invention whereby a semiconductor layer structure is provided on a substrate with at least a first cladding layer of a first conductivity type, an active layer, and a second cladding layer of a second conductivity type opposed to the first, which cladding layers are provided with current supply means, while a strip-shaped active region is formed within the active layer so as to lie within two end faces such that the longitudinal axis of the strip-shaped active region encloses a small angle with the peφendicular to the end faces and at least one end of the strip-shaped active region is separated from an end face by a third cladding layer and is provided with a tapering portion, as seen in projection, such that a first side face thereof coincides with a side face of the portion of the strip-shaped active region which lies outside the tapering portion, and a second side face diereof encloses an acute angle with the peφendicular to the end face, is characterized according to the invention in that an angle is chosen for the acute angle which is at most 30°, preferably at most 10°, and preferably approximately 0°. A laser according to the invention is obtained thereby in a simple manner. In a preferred embodiment of a method according to the invention, a strip- shaped region is formed in die active layer in a first manufacturing step, after which in a further manufacturing step die strip-shaped region is provided widi the tapering portion constituting me strip-shaped active region by means of etching with the use of a mask. Preferably, the strip-shaped region is also formed by etching during the first step. Alternatively, however, it may be formed by, for example, selective deposition. The fact that the tapering portion is formed in a separate (etching) step achieves iat mis tapering portion of the strip-shaped active region has very plane side faces and a shaφ tip. Were me strip- shaped active region formed, for example, in a single etching step, me tapering portion mereof would have curved side faces owing to underetching and no shaφ tip, and the mask used would project comparatively far beyond me mesa in these locations. This is disadvantageous for a furϋ er growing process against die mesa, as was explained above. In an important modification of a me iod according to the invention, a strip-shaped mesa is formed in Lhe semiconductor layer structure, a fourth cladding layer which is current-blocking is provided on either side of die strip-shaped mesa, a further strip- shaped mesa is formed which encompasses the strip-shaped mesa and the adjoining fourth cladding layer, whereupon die further strip-shaped mesa is provided with a tapering end by means of etching with the use of a mask, a first side face of said end coinciding with a side face of die further strip-shaped mesa outside the tapering portion thereof and a second side face extending parallel to die peφendicular to an end face to be formed, and subsequently the mird cladding layer is provided around die further strip-shaped mesa. The formation of me further strip-shaped mesa limits the underetching effect mentioned above still further, so diat the second side face of die tapering portion of die strip-shaped active region is perfectly plane. Moreover, any underetching still present is shifted to outside the radiation path of the laser. This manufacture thus results in a substantially optimum laser. The invention will now be explained in more detail with reference to an embodiment and the accompanying drawing, in which Fig. 1 shows a semiconductor diode laser according to the invention diagrammatically and in perspective view; Fig. 2 shows the laser of Fig. 1 diagrammatically in a cross-section taken on me line II-II; Fig. 3 shows the laser of Fig. 1 diagrammatically in a cross-section taken Fig. 4 shows me laser of Fig. 1 diagrammatically in a cross-section taken Figs. 5 to 10 show the laser of Fig. 1 diagrammatically and in perspective view in consecutive stages of its manufacture by a method according to die invention. The Figures are diagrammatic and not drawn to scale, the dimensions in uie diickness direction being particularly exaggerated for greater clarity. Corresponding parts have been given die same reference numerals as much as possible in the various Figures. Fig. 1 shows a semiconductor diode laser according to the invention, here constructed as an amplifier, diagrammatically and in perspective view. Figs. 2, 3 and 4 show the laser of Fig. 1 diagrammatically and in cross-sections taken on the lines II-II, III-III, and IV-IV, respectively. The laser (see Fig. 2) comprises a semiconductor body 10 with a substrate 1 , in this example an n-type InP substrate with a thickness of approximately 100 μm and a doping concentration of 5 x 10" S at/cm 3 and a (001) orientation. A 1.5 μm thick portion 2 of the substrate 1 in this example acts as a first cladding layer 2 for an active layer 4 with a strip-shaped active region 4A of In 0 . 5 7Ga 0 . 3 As 9 ,P 0 .o (λ = 1.55 μm) of 0.1 μm thickness. A second cladding layer 3 of p-type InP with a doping of 5 x IO 17 Zn at/cm 3 and a thickness of approximately 1 μm is disposed diereon. Electromagnetic radiation can be generated or amplified widiin die strip-shaped active region 4A by means of the pn junction formed between me cladding layers 2, 3, given a sufficient current strength in the forward direction. The cladding layers 2, 3 are for this puφose provided widi current supply means 11, 12 in the form of metal layers 11, 12 usual for InP/InGaAsP. The strip-shaped active region 4A lies within a resonance cavity which is formed (see Fig. 4) between two parallel end faces 50, 51, has a longitudinal axis which encloses a small angle with me peφendicular to the end faces 50, 51, and is separated from the end faces 50, 51 by a third, current- blocking cladding layer 5 which is made of SI (= Semi Insulating) InP and is approximately 2.2 μm thick. The strip-shaped active region 4A furd er comprises a portion 40 which has a tapering shape seen in projection, of which a first side face coincides wid a side face 42 of die strip-shaped active region 4A outside die tapering portion 40 thereof, and of which a second side face 43 encloses an acute angle widi the peφendicular to me end faces 50, 51. According to me invention, die second side face 43 of the tapering portion 40 of the strip-shaped active region 4A encloses an angle widi die peφendicular to the end faces which lies between 0 and 30°, preferably between 0 and 10°, and preferably is, as in this example, approximately 0°. The result is that die strips-shaped active region 4A tapers strongly over a comparatively great distance. This implies mat the step in the effective refractive index between die active region 4A and the third cladding layer 5, and dius die reflection therebetween, is substantially reduced. Given an angle of approximately 0°, said reflection, and dius die amplification ripple, is substantially an optimum. The radiation entering or leaving the laser then encloses an angle of, for example, 35° widi die end faces 50, 51 but can still be satisfactorily coupled into a glass fiber (not shown). This renders the laser of this example particularly suitable for use in an optical communication system. Moreover, growing against said side faces 42, 43 is very uniform because both the first side face 42 and die second side face 43 of the strip-shaped active region 4A and of the tapering portion 40 thereof are sufficiently parallel to die <01-1 > direction here. This strongly benefits die yield and quality of die laser if the latter is, for example, of the buried hetero type, as in the present case. The strip-shaped active region 4A (see Fig. 2) of the laser in this example, which is of the SIPBH type mentioned earlier, forms part of a strip-shaped mesa 20 which further comprises me two cladding layers 2, 3, which coincides with the strip-shaped active region 4A seen in projection, and which is surrounded by a further cladding layer, here a fourth cladding layer 6 of Sl-InP widi a thickness of more than 2 μ with which the mesa 20 forms a further strip-shaped mesa 21 which has a side face 43 which coincides with the second side face 43 and which is surrounded by die third cladding layer 5. In this example, the third and fourth cladding layers 5, 6 comprise respective thin portions 5 A, 6A of n-type InP, approximately 0.3 μm thick in this case. A fifth cladding layer 7 of p-type InP and 0.5 μm thickness is present thereon, extending over the entire laser. A contact layer 8 of p-type Iii o j 7 Ga 043 As 0 . ,P 0.o o with a doping of 1 x IO 19 Zn at/cm 3 and 0.5 μm thick is present on d e fifdi cladding layer. The lengdi of the mesas 20 and 21 is 820 μm, and die respective widdis of die mesas 20 and 21 are 2 to 3 μm and 10 μm. The dimensions of the semiconductor body 10 are 850 x 300 x 100 μm 3 . The angle enclosed by the longitudinal axis of die strip-shaped active region 4A and the peφendicular to the end faces 50, 51 lies between 0 and 20° and is preferably approximately 10°, as in die present example. The above implies that the length of die second side face 43 of me tapering portion 40 of die active layer 4A is between 11.5 and 17.5 μm, depending on the widdi of the mesa 20. The end faces 50, 51 in this example are provided widi a l/4λ anti-reflection layer (not shown) made from a silicon oxynitride widi a refractive index of 1.78. Figs. 5 to 10 show die laser of Fig. 1 diagrammatically and in perspective view in consecutive stages of its manufacture by a method according to die invention. Manufacture starts (see Fig. 5) with die formation of a semiconductor body 10 comprising an approximately 350 μm diick (001) substrate 1 and having two cladding layers 2, 3 between which an active layer 4 is present. The first cladding layer 2 is formed here by an upper portion 2 of the substrate 1, the other layers 3, 4 are provided by epitaxy, MOVPE in diis case. The chosen materials, diicknesses, doping levels, and compositions are as discussed wi reference to die first four Figures. After removal from the growing apparatus, a strip-shaped mesa 20 (see Fig. 6) is formed by means of a strip-shaped mask (not shown) of, for example, SiO 2 and an etching process, which mesa has the same shape as the mask and encloses a small angle, here an angle of 10°, wim the < 0.1-1 > direction in this case and extends down into the substrate 1. Further information on the etching process can be found in USP 5,266,518. A strip-shaped active region 4A to be formed is part of this mesa 20. After renewed placement in die growing apparatus (see Fig. 7), a fourth cladding layer 6, 6A is selectively applied on eidier side of die mesa 20. After removal from the growing apparatus, a furdier strip-shaped mesa 21 (see Fig. 8) is formed by means of a further strip-shaped mask (not shown), for example made of SiO 2 , and by etching, which mesa has die same shape as die furdier mask, whereby the strip-shaped active region 4A is given its final shape. The etching process is again described in die US Patent cited above. The shape of the furdier mask is such that an end of die strip-shaped active region 4A is provided with a tapering portion 40 of which a first side face 42 coincides with a side face 42 of die strip-shaped active region 4A outside the tapering portion 40 diereof, and a second side face 43 of the tapering portion 40 is given an acute angle relative to the peφendicular to me end faces 50, 51. According to the invention, the acute angle is chosen to lie between 0 and 30°, preferably between 0 and 10°, and preferably to be approximately 0°, as in the present example. Preferably, as in this example, the strip-shaped active region 4A is formed in two separate manufacturing steps: a first step in this example in which a strip-shaped region 4B which is still uninterrupted in longitudinal direction is formed in the active layer 4 (see Fig. 6), during the formation of me mesa 20 in this case, and a second step in which die strip- shaped active region 4B is provided with die tapering portion 40 by means of the further mask and etching, whereby die strip-shaped active region 4A is formed (see Fig. 8). Rounding of the tapering portion 40 dirough underetching is prevented or at least limited thereby as compared with a situation in which the strip-shaped active region 4A is formed in a single step. This is true in particular when a tapering portion 40 is formed which has a very shaφ tip, as in die present invention. The presence of die fourth cladding layer 6 on eidier side of the strip-shaped active region 4A (see Figs. 7 and 8) also contributes to die prevention of underetching and rounding during die formation of the second side face 43 (see Fig. 8), and thus to the prevention of an excessive overhang of die furdier strip-shaped mask beyond die further mesa 21 to be formed. Any irregularities in die material to be grown against the further mesa 21 in a later phase are counteracted thereby. Should any irregularities arise, diese will be present at die area of die fourth cladding layer 6, and accordingly not at the area of die strip-shaped active region 4 A, i.e. not in the radiation padi of the laser. The product is removed from the growing apparatus and the masks used for forming the mesas 20, 21 are removed, whereupon a fifth cladding layer 7 and a contact layer 8 are provided in a final growing process. Then die substrate thickness is reduced to approximately 100 μm by grinding, usual metal layers 11 , 12 are provided, and the end faces 50, 51 are formed by repeated cleaving and are provided with anti-reflection coatings. The peφendicular of die end faces 50, 51 was chosen to be die <0, 1 , -1 > direction in the present example, which is a preferred direction. Good results are also obtained, however, when the < 0, 1, 1 > direction is chosen for this peφendicular. A laser (amplifier) according to die invention has dius been obtained which is ready for use. When a grating is provided widiin the resonant cavity in die vicinity of the active layer 4A, the resulting laser is of the DFB (= Distributed Feed Back) type. The invention is not limited to the embodiments given since many modifications and variations are possible to diose skilled in die art widiin the scope of the invention. Thus diicknesses, semiconductor materials, compositions, or conductivity types other than those mentioned in die examples may be used. It is also possible to use a semi- insulating substrate. It is especially noted mat die invention may also be applied to die material systems GaAs/AlGaAs, InGaP/InAlGaP, and InP/AlGalnAs. The mesa structures used in d e examples were all manufactured by etching, but they may alternatively be manufactured by a selective growing process. The formation of die further mesa as in me present example may also be omitted. Manufacture is much simpler in mat case owing to the omission of a number of steps, among mem a growing process. The formation of the strip-shaped active region 4A according to die invention should preferably take place in two separate steps also in that case, however, because die advantage thereof discussed above is still obtained then. It is furdier noted that the invention is not limited to the SIPBH laser described. The use of alternative current-blocking cladding layers is possible. Thus a pnp triple layer structure may be used instead of an SI layer, comprising a reverse-bias, i.e. current-blocking pn junction. The invention may also be used to advantage in odier index- guided lasers such as diose of die, possibly buried, ridge type. The same is true for lasers of the gain-guided type, such as an oxide strip or proton bombarded laser. It is finally noted diat die growing process(es) used in a method according to the invention may comprise besides MOVPE also other processes such as LPE (= Liquid Phase Epitaxy), VPE (= Vapor Phase Epitaxy), or MBE (= Molecular Beam Epitaxy), or combinations thereof. Instead of d e wet-chemical etching processes referred to, RIE (= Reactive Ion Etching) may also be advantageously utilized.

Claims: Claims: 1. A semiconductor diode laser widi a semiconductor body (10) of III-V semiconductor materials comprising a substrate (1) and an overlaying semiconductor layer structure widi at least a first cladding layer (2) of a first conductivity type, a second cladding layer (3) of a second conductivity type opposed to die first, said cladding layers being provided widi current supply means (11, 12), and between the first and second cladding layers an active layer (4) and a pn junction which, given a sufficient current strengdi in the forward direction, is capable of amplifying or generating electromagnetic radiation in a strip-shaped active region (4 A) which forms part of the active layer (4), which lies within a resonance cavity formed between two parallel end faces (50,51), die longitudinal axis of said resonance cavity enclosing a small angle widi the peφendicular to die end faces (50,51), and which has at least one end (40) which is situated adjacent an end face (50,51) and is separated from said end face (50,51) by a diird cladding layer (5, 5 A) which is preferably current-blocking and which is provided with a tapering portion (40), as seen in projection, of which a first side face (42) coincides widi a side face (42) of the strip-shaped active region (4A) outside the tapering portion (40) and of which a second side face (43) encloses an acute angle with the peφendicular to die end face (50,51), characterized in diat the second side face (43) of said tapering portion (40) encloses an angle with the peφendicular to the end face (50,51) which lies between 0 and 30°. 2. A semiconductor diode laser as claimed in Claim 1, characterized in diat die second side face (43) of die tapering portion (40) of the strip-shaped active region (4A) encloses an angle widi die peφendicular to d e end face (50, 51) which lies between 0 and 10°, and which is preferably approximately 0°. 3. A semiconductor diode laser as claimed in Claim 1 or 2, characterized in diat die strip-shaped active region (4A) forms part of a strip-shaped mesa (20) which also comprises me first (2) and the second cladding layer (3), which coincides with the strip- shaped active region (4A) seen in projection, and which is surrounded by a further cladding layer (5, 5 A; 6,6A) which is current-blocking. 4. A semiconductor diode laser as claimed in Claim 3, characterized in diat die strip-shaped mesa (20) is bounded on either side by a fourth cladding layer (6,6A) which is current-blocking and forms a further strip-shaped mesa (21) dierewith which has a side face (43) coinciding widi the second side face (43) and which is surrounded by the mird cladding layer (5, 5 A). 5. A semiconductor diode laser as claimed in any one of the preceding Claims, characterized in diat die angle between the longitudinal axis of the strip-shaped active region (4A) and die end faces (50,51) lies between 0 and 20° and is preferably approximately 10°. 6. A semiconductor diode laser as claimed in any one of die preceding Claims, characterized in diat the semiconductor body (10) comprises materials of the InP/InGaAsP material system, and the end faces (50, 51) are provided with an anti-reflection layer. 7. A method of manufacturing a semiconductor diode laser with a semiconductor body (10) of III-V semiconductor materials, whereby a semiconductor layer structure is provided on a substrate (1) widi at least a first cladding layer (2) of a first conductivity type, an active layer (4), and a second cladding layer (3) of a second conductivity type opposed to the first, which cladding layers (2,3) are provided widi current supply means (11 , 12), while a strip-shaped active region (4 A) is formed within die active layer (4) so as to lie widiin two end faces (50,51) such that the longitudinal axis of die strip- shaped active region (4A) encloses a small angle with me peφendicular to die end faces (50,51) and at least one end (40) of die strip-shaped active region (4 A) is separated from an end face (50,51) by a third cladding layer (5), which is preferably current-blocking, and is provided widi a tapering portion (40), as seen in projection, such diat a first side face (42) thereof coincides with a side face (42) of die portion of die strip-shaped active region (4A) which lies outside die tapering portion (40) thereof, and a second side face (43) thereof encloses an acute angle with the peφendicular to the end face (50,51), characterized in diat an angle is chosen for the acute angle which is at most 30°, preferably at most 10°, and preferably approximately 0°. 8. A mediod as claimed in Claim 7, characterized in that a strip-shaped region (4B) is formed in die active layer (4) in one manufacturing step, after which in a furdier manufacturing step said strip-shaped region (4B) is provided with the tapering portion (40) so as to form the strip-shaped active region (4A) by means of etching with the use of a mask. 9. A method as claimed in Claim 7 or 8, characterized in that a strip-shaped mesa (20) is formed in die semiconductor layer structure, a fourth cladding layer (6,6A) which is current-blocking is provided on eidier side of the strip-shaped mesa (20), a further strip-shaped mesa (21) is formed which encompasses the strip-shaped mesa (20) and the adjoining portions (6,6A) of the four cladding layer (6,6A), whereupon the further strip- shaped mesa (21) is provided widi a tapering end (41) by means of etching wim the use of a mask, a first side face (44) of said end coinciding with a side face (44) of the furdier strip- shaped mesa (21) outside die tapering end (41) thereof and a second side face extending parallel to the peφendicular to an end face (50,51) to be formed, and subsequently die diird cladding layer (5, 5 A) is provided around die furdier strip-shaped mesa (21). 10. A method as claimed in Claim 7, 8 or 9, characterized in diat the semiconductor body (10) is formed in the InP/InGaAsP material system, and the end faces (50, 51) are provided with an anti-reflection layer.

Inventors: BINSMA JOHANNES JORDANUS MARIA, THIJS PETRUS JOHANNES ADRIANUS, TIEMEIJER LUKAS FREDERIK, BINSMA, JOHANNES, JORDANUS, MARIA, THIJS, PETRUS, JOHANNES, ADRIANUS, TIEMEIJER, LUKAS, FREDERIK
Applicants: PHILIPS ELECTRONICS NV, PHILIPS NORDEN AB, PHILIPS ELECTRONICS N.V.
Application year: 1996
Main classification: H01S3
IPC codes: H01S5