Semiconductor substrate, light-emitting device, and method for producing the same

Information

  • Patent Grant
  • 6294440
  • Patent Number
    6,294,440
  • Date Filed
    Friday, April 9, 1999
    25 years ago
  • Date Issued
    Tuesday, September 25, 2001
    23 years ago
Abstract
A method for producing a semiconductor substrate of the present invention, includes the steps: forming a first patterned mask containing a material having a growth suppressing effect on a lower substrate; growing a semiconductor crystal on the lower substrate via the first patterned mask to form a first semiconductor crystal layer; forming a second patterned mask containing a material having a growth suppressing effect on or above the lower substrate, the second patterned mask at least having a surface which is positioned at a level different from a level of a surface of the first patterned mask, with respect to a surface of the lower substrate; and growing a semiconductor crystal on or above the lower substrate via the second patterned mask to form a second semiconductor crystal layer.
Description




BACKGROUND OF THE INVENTION




1. Field of the Invention




The present invention relates to a method for growing, on a lower substrate, a crystal of high quality having a lattice constant different from that of a lower substrate, and a semiconductor substrate obtained by such a method. The present invention further relates to a method for growing a crystal to obtain a highly reliable device with high performance by producing a light-emitting element and an electronic element on a semiconductor substrate, and a device obtained by such a method. In particular, the present invention relates to a method for growing a crystal preferably used for producing a gallium nitride (GaN) type blue light emitting element having a high efficiency and high reliability and a light-emitting element obtained by such a method.




2. Description of the Related Art




An optoelectronic integrated circuit (OEIC) is a device which is capable of processing a large amount of information at a high speed by integrating an optical element and an Si-type LSI on the same substrate. The OEIC is expected as an indispensable device in an advanced information society and has been studied for such a reason.




In the field of an Si-type LSI, SOI, SIMOX, and the like are suggested as an ultra-fast next generation integrated circuits with low power consumption, and there is an increasing demand for technical development of SOI, SIMOX, and the like.




The main purpose in the field of an optical element is to develop a technique of producing an AlGaAs laser structure on an Si substrate. However, a difference in a lattice constant and a difference in a coefficient of thermal expansion between an AlGaAs crystal and an Si crystal of a substrate is large, thereby making it very difficult to grow an AlGaAs crystal having good crystallinity on an Si substrate. In realizing such a semiconductor device, characteristics of an underlying crystal layer for producing a device and a substrate are important.




In particular, a gallium nitride (GaN) type semiconductor is applied to a short-wavelength light-emitting element (blue light emitting element) and an electronic element which operates at a high temperature and a high speed. In production of such a GaN type semiconductor device, a substrate made of a material (e.g., sapphire and SiC) which is different from a GaN type semiconductor is used as a substitute substrate. Basically, it is desirable to use a substrate made of GaN for a substrate on which a GaN type semiconductor crystal is grown. However, a GaN type semiconductor has a large decompression pressure, so that a large-scale bulk crystal made of a GaN type semiconductor cannot be produced; thus, such a substitute substrate is used.




In the case of using a substitute substrate as described above, a difference in a lattice constant or a difference in a coefficient of thermal expansion between a crystal of a substrate material and a GaN type semiconductor crystal is large, so that it is difficult to epitaxially grow a crystal having good crystallinity and having a small crystal defect or a crystal dislocation density on the substitute substrate. For example, in the case of using a sapphire substrate as a substitute substrate for growing a GaN semiconductor crystal, it is known that there will be a threading dislocation of about 10


9


to 10


10


/cm


2


in the GaN semiconductor crystal layer grown on the sapphire substrate. Furthermore, in the case where the thickness of the GaN semiconductor crystal layer exceeds about 10 μm, crystal cracks and lattice strains in the GaN semiconductor crystal layer become large.




In order to overcome the above-mentioned problems, for example, the following two methods for growing a crystal are suggested. As the first conventional example, a method for growing a crystal in Extended Abstracts 2p-Q-14, No. 1 (1997), p. 265 (The 58th Meeting, 1997); The Japan Society of Applied Physics will be described. Referring to

FIG. 14

, according to this method, an SiO


2


pattern


901


, with openings


902


, is formed on a sapphire substrate


900


, and then, a GaN single crystal film


903


is grown by a metal organic chemical vapor deposition (MOCVD) method, using the SiO


2


pattern


901


as a mask. In the first conventional example, the growth of the GaN single crystal starts from the opening


902


, not from a portion covered with the SiO


2


pattern


901


of the sapphire substrate


900


. Thus, strains, which are caused by a difference in a lattice constant and/or a difference in a coefficient of thermal expansion and which may cause threading dislocation, can be prevented from being generated in the vicinity of an interface between the sapphire substrate


900


and the GaN single crystal film


903


. According to this method, the SiO


2


pattern is effective for allowing a GaN crystal to be selectively grown (i.e., an effect of suppressing the growth of a crystal defect), so that a defect density is measured (about 10


5


to about 10


6


/cm


2


) only in a GaN single crystal


904


above the SiO


2


pattern


901


in the GaN single crystal film


903


. According to this method, a value of a defect density is decreased by 4 orders of magnitude, compared with a GaN single crystal in the case where a GaN signal crystal film is directly grown on a sapphire substrate.




Furthermore, a method for growing a crystal in Extended Abstracts 2p-Q-14, No. 1 (1997), p. 266 (The 58th Meeting, 1997); The Japan Society of Applied Physics will be described. Referring to

FIG. 15

, according to this method, a GaN single crystal film


911


is grown on a sapphire substrate


910


by an MOCVD method, an SiO


2


pattern


912


with openings


913


is formed on the GaN single crystal film


911


, and a GaN single crystal film


914


is grown by an HVPE (hydride vapor phase epitaxy) method, using the SiO


2


pattern


912


as a mask. According to this method, a value of a defect density of the GaN single crystal film


914


can be decreased for the same reason as that of the first conventional example. A defect density in the vicinity of the surface of the GaN single crystal film


914


is measured to be about 6×10


7


/cm


2


. According to this method, a value of a defect density is decreased by three orders of magnitude, compared with a GaN single crystal in the case where a GaN single crystal film is grown directly on a sapphire substrate without using an SiO


2


pattern.




A semiconductor substrate having as its surface a GaN single crystal film produced by one of the above-mentioned first and second conventional methods is used as a substrate for growing a GaN type semiconductor device, whereby it is expected to realize an electronic device with higher performance.




However, a semiconductor substrate having as its surface a GaN single crystal film obtained by using one of the above-mentioned first and second conventional methods is not sufficient for obtaining a highly reliable semiconductor laser or an LED, or electronic elements such as an FET. For example, in order to enhance a life-span of a product in a semiconductor laser device, a defect density in the vicinity of a light-emitting region is required to be about 10


5


/cm


2


or less, and a defect density is desired to be equal to or lower than the order of 10


4


/cm


2


of another III-V group (e.g., GaAs, etc.) semiconductor substrate.




A GaN single crystal layer produced by the first and second conventional methods has a defect density of about 10


5


to about 10


7


/cm


2


, and therefore, does not satisfy the above-mentioned condition. A light-emitting element produced on a GaN single crystal layer having lattice strains and a number of crystal defects has lower reliability. For example, a semiconductor laser device produced on such a GaN single crystal layer is confirmed to have a life-span of only about 900 hours at a continuous oscillation under the condition of room temperature and an output of 3 mW.




According to the first conventional method, a high quality GaN crystal having a reduced defect density is limited to that grown in a region above an SiO


2


pattern. A crystal grown in the other region has quality equal to that of a crystal according to the conventional method without using an SiO


2


pattern. To use a semiconductor substrate including a GaN crystal layer having a locally reduced defect density as a substrate for growing a crystal is not practical for the reason of a limited degree of freedom of a device design.




According to the second conventional method, since an HVPE method is used, a crystal layer which is relatively thick (about several 10 μm) for an epitaxial growth film can be obtained. The effect of the SiO


2


pattern is relaxed in the vicinity of the surface of the GaN crystal layer by increasing the thickness of the crystal layer, so that defects will be uniformly distributed in the entire surface. Accordingly, the problem that crystal quality of the GaN crystal layer is locally improved as in the first conventional example can be solved. However, in terms of the defect density, the second conventional example is inferior to the first conventional example.




In addition, according to the first and second conventional methods, a GaN single crystal layer is produced by using an SiO


2


pattern in the shape of a stripe. Thus, lattice strains are decreased in a direction vertical to the stripe of the SiO


2


pattern; however, lattice strains in a plane parallel to the stripe remain substantially equal to that of a crystal according to the conventional method without using an SiO


2


pattern. When a GaN type semiconductor layer is grown on a GaN crystal layer in which lattice strains having a particular directivity are introduced, lattice strains having anisotropy are propagated to the GaN type semiconductor layer.




Alternatively, it is also possible to grow a thicker GaN crystal layer (about 50 μm) on a sapphire substrate, and remove the sapphire substrate from the reverse surface of the GaN crystal layer, thereby obtaining a GaN substrate. However, crystal defects (more than on the order of 10


5


/cm


2


) remain even in the GaN substrate thus obtained, and lattice strains having anisotropy cannot be relaxed.




SUMMARY OF THE INVENTION




A method for producing a semiconductor substrate of the present invention, includes the steps: forming a first patterned mask containing a material having a growth suppressing effect on a lower substrate; growing a semiconductor crystal on the lower substrate via the first patterned mask to form a first semiconductor crystal layer; forming a second patterned mask containing a material having a growth suppressing effect on or above the lower substrate, the second patterned mask at least having a surface which is positioned at a level different from a level of a surface of the first patterned mask, with respect to a surface of the lower substrate; and growing a semiconductor crystal on or above the lower substrate via the second patterned mask to form a second semiconductor crystal layer.




In one embodiment of the present invention, the second patterned mask is positioned on the first semiconductor crystal layer.




In another embodiment of the present invention, the first and second patterned masks are patterned in such a manner that a combination of the first and second patterned masks covers the entire surface of the lower substrate, and an area of the lower substrate covered with the second patterned mask is larger than an area of the lower substrate covered with the first patterned mask.




In another embodiment of the present invention, the second patterned mask includes a first portion and a second portion, the first and second portions have different widths in a direction vertical to the surface of the lower substrate, and the step of forming the first semiconductor crystal layer and the step of forming the second semiconductor crystal layer are conducted during the same crystal growth step.




In another embodiment of the present invention, the first portion of the second patterned mask is at least partially positioned on the first patterned mask, and the second patterned mask has an L-shape.




In another embodiment of the present invention, the first portion of the second patterned mask is at least partially positioned on the lower substrate, and the second patterned mask has a T-shape.




In another embodiment of the present invention, a growth direction of the second semiconductor crystal layer is at least partially different from a growth direction of the first semiconductor crystal layer.




In another embodiment of the present invention, the first semiconductor crystal layer is formed in the vicinity of openings in the first patterned mask, whereby the first semiconductor crystal layer has openings on the lower substrate and the first patterned mask.




In another embodiment of the present invention, the lower substrate includes a sapphire substrate and a lower semiconductor crystal layer provided on an upper side of the sapphire substrate in a crystal growth direction.




In another embodiment of the present invention, the material having a growth suppressing effect is selected from the group consisting of SiO


2


and SiN


x


, and the first and second patterned masks are independently selected from the group consisting of SiO


2


and SiN


x


.




In another embodiment of the present invention, the first and second semiconductor crystal layers are selected from the group consisting of GaN, InGaN, and AlGaN.




A semiconductor substrate of the present invention, includes: a first patterned mask containing a material having a growth suppressing effect, provided on a lower substrate; a first semiconductor crystal layer grown on the lower substrate via the first patterned mask; a second patterned mask containing a material having a growth suppressing effect, provided on or above the lower substrate, at least having a surface which is positioned at a level different from a level of a surface of the first patterned mask, with respect to a surface of the lower substrate; and a second semiconductor crystal layer grown on or above the lower substrate via the second patterned mask.




A method for producing a semiconductor substrate of the present invention, includes the steps of: forming an n-th patterned mask containing a material having a growth suppressing effect on or above a lower substrate, wherein n is an integer of 1 or more; growing a nitride semiconductor crystal on or above the lower substrate via the n-th patterned mask to form an n-th nitride semiconductor crystal layer; forming an (n+1)-th patterned mask containing a material having a growth suppressing effect on or above the lower substrate, the (n+1)-th patterned mask at least having a surface which is positioned at a level different from a level of a surface of the n-th patterned mask, with respect to a surface of the lower substrate; and growing a nitride semiconductor crystal on or above the lower substrate via the (n+1)-th patterned mask to form an (n+1)-th nitride semiconductor crystal layer.




In one embodiment of the present invention, the first to (n+1)-th patterned masks are patterned in such a manner that a combination of the first to(n+1)-th patterned masks covers the entire surface of the lower substrate.




In another embodiment of the present invention, the n-th patterned mask and the (n+1)-th patterned mask are respectively patterned in a stripe shape, and a direction of the stripe of the n-th patterned mask is twisted from a direction of the stripe of the (n+1)-th patterned mask.




In another embodiment of the present invention, the direction of the stripe of the n-th patterned mask and the direction of the stripe of the (n+1)-th patterned mask have an angle difference of about 120°.




In another embodiment of the present invention, the direction of the stripe of the n-th patterned mask and the direction of the stripe of the (n+1)-th patterned mask have an angle difference of about 90°.




In another embodiment of the present invention, a width of the stripe of the (n+1)-th patterned mask is equal to or larger than a width of the stripe of the n-th patterned mask.




In another embodiment of the present invention, the material having a growth suppressing effect is made of SiO


2


or SiN


x


, and the first to (n+1)-th patterned masks are independently made of SiO


2


or SiN


x


.




In another embodiment of the present invention, the lower substrate includes at least a lower nitride semiconductor crystal layer provided on an upper surface of the lower substrate, and a direction of the stripe of the n-th patterned mask is equal to a <1-100> direction or a <11-20> direction of a crystal of the nitride semiconductor crystal layer.




In another embodiment of the present invention, the lower substrate includes at least a lower nitride semiconductor crystal layer provided on an upper side of the lower substrate in a crystal growth direction, the semiconductor substrate includes the first, second and third nitride semiconductor crystal layers, and a combination of directions of the first, second and third patterned masks consists of a combination of [1-100], [10—10], and [01-10] directions of a crystal of the nitride semiconductor crystal.




In another embodiment of the present invention, the n-th nitride semiconductor crystal layer is made of Al


x


In


y


Ga


z


N (where x+y+z=1, 0≦x≦1, 0≦y≦1, and 0≦z≦1).




In another embodiment of the present invention, the n-th nitride semiconductor crystal layer or the (n+1)-th nitride semiconductor crystal layer has a thickness of about 5 μm or more.




In another embodiment of the present invention, the lower substrate includes a substrate body and a lower nitride semiconductor crystal layer provided on an upper side of the substrate body in a crystal growth direction, the method further including the step of removing at least the substrate body from a crystal structure including the (n+1)-th nitride semiconductor crystal layer after the step of forming the (n+1)-th nitride semiconductor crystal layer.




A semiconductor substrate of the present invention, includes: an n-th patterned mask containing a material having a growth suppressing effect provided on or above a lower substrate, wherein n is an integer of 1 or more; an n-th nitride semiconductor crystal layer grown on or above the lower substrate via the n-th mask; an (n+1)-th patterned mask containing a material having a growth suppressing material provided on or above the lower substrate, the (n+1)-th mask at least having a surface which is positioned at a level different from a level of a surface of the n-th mask, with respect to a surface of the lower substrate; and an (n+1)-th nitride semiconductor crystal layer grown on or above the lower substrate via the (n+1)-th patterned mask.




A light-emitting device produced by using the above-mentioned semiconductor substrate is provided.




Thus, the invention described herein makes possible the advantages of (1) providing a semiconductor substrate including a nitride semiconductor crystal layer with a crystal defect density and a threading dislocation surface density sufficiently reduced, and a method for producing the same; (2) providing a semiconductor substrate including a nitride semiconductor crystal layer with no lattice strains having anisotropy introduced thereto, and a method for producing the same; and (3) providing a highly reliable semiconductor device with high performance, using a semiconductor substrate including a nitride semiconductor crystal layer with improved crystallinity as a substrate for growth, and a method for producing the same.




These and other advantages of the present invention will become apparent to those skilled in the art upon reading and understanding the following detailed description with reference to the accompanying figures.











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

is a cross-sectional view of a semiconductor substrate in Embodiment 1 of the present invention.





FIG. 2

is a cross-sectional view of a semiconductor substrate in Embodiment 2 of the present invention.





FIG. 3

is a cross-sectional view of a semiconductor substrate in Embodiment 3 of the present invention.





FIG. 4

is a cross-sectional view of a semiconductor substrate in Embodiment 4 of the present invention.





FIG. 5

is a cross-sectional view of a semiconductor substrate in Embodiment 5 of the present invention.





FIG. 6

is a cross-sectional view of a semiconductor laser device in Embodiment 6 of the present invention.





FIGS. 7A and 7B

are views illustrating the steps of producing semiconductor substrates in Embodiments 7 and 8 of the present invention.





FIG. 8

is a view illustrating the steps of producing the semiconductor substrates in Embodiments 7 and 8 of the present invention.





FIGS. 9A and 9B

are views illustrating the steps of producing the semiconductor substrates in Embodiments 7 and 8 of the present invention.





FIGS. 10A and 10B

are views each illustrating the steps of producing the semiconductor substrate in Embodiment 7 of the present invention.





FIGS. 11A and 11B

are views each illustrating a semiconductor substrate in Embodiment 9 of the present invention.





FIGS. 12A and 12B

are views illustrating a semiconductor substrate in Embodiment 10 of the present invention.





FIG. 13

is a cross-sectional view of a semiconductor laser device in Embodiment 11 of the present invention.





FIG. 14

is a cross-sectional view of a semiconductor substrate having a GaN crystal film on its surface in a first conventional example.





FIG. 15

is a cross-sectional view of a semiconductor substrate having a GaN crystal film on its surface in a second conventional example.











DESCRIPTION OF THE PREFERRED EMBODIMENTS




The present invention will be described by way of illustrative embodiments with reference to the drawings.




The term “growth suppressing effect” used in the specification and the attached claims of the present application refers to “an effect of suppressing a crystal growth on a mask”. In addition, the term “twisted” is used herein to refer to a positional relationship in which two lines are disposed, without crossing in the same plane, so as to be not in parallel to each other.




Embodiment 1




A method for growing a crystal in the present embodiment will be described.




First, a GaN layer


101


is grown to a thickness of about 4 μm, using trimethyl gallium (TMG) and ammonia (NH


3


) as materials, on a sapphire substrate


100


having a C-plane as its surface placed in a predetermined growth chamber. The sapphire substrate


100


and the GaN layer


101


are included in a lower substrate. The GaN layer


101


is a lower semiconductor crystal layer as well as a lower nitride semiconductor crystal layer.




Then, in order to form a first patterned mask, a film (thickness: about 200 nm) made of a growth suppressing material (SiO


2


) is formed on the GaN layer


101


by sputtering. A method for forming the SiO


2


film is not limited to sputtering. Other methods, such as vacuum vapor deposition and chemical vapor deposition (CVD), may be used. Furthermore, as a growth suppressing material, oxides such as Al


2


O


3


and TiO


2


and SiN


x


can be used in place of SiO


2


. Then, the SiO


2


film is patterned to a periodic stripe (width: about 7 μm; pitch: about 10 μm) by a conventional photolithography method, whereby a first SiO


2


mask


102


is formed. The direction of the stripe is desirably a <1-100> direction of a crystal of the GaN layer


101


.




By using the lower substrate thus obtained, a GaN crystal film


103


is grown by a metal-organic-vapor-phase epitaxy (MOVPE) method. More specifically, the GaN crystal film


103


is grown to a thickness of about 3 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in a predetermined growth chamber. The GaN crystal film


103


starts growing from openings in the first mask, and is flatly grown over substantially the entire surface of the lower substrate due to anisotropy (i.e., a growth speed in a direction horizontal to the lower substrate is higher than that in a direction vertical to the lower substrate).




A defect density on the first mask is about 10


5


/cm


2


or less; however, a defect density on the sapphire substrate in the opening portions of the first mask is about 10


7


/cm


2


. In the conventional example, although a laser device is formed avoiding such portions, reliability and yield are not sufficient.




Then, a second mask is formed on the GaN crystal film


103


. More specifically, an SiO


2


film (thickness: about 200 nm) is formed by sputtering in the same way as in the first mask, and a second SiO


2


mask


104


with a periodic stripe pattern (width: about 8 μm; pitch: about 10 μm) is formed by a photolithography method. At this time, it is important that the position of the second mask is matched with the openings in the first mask.




Then, a GaN single crystal film


105


is grown on the second SiO


2


film by a MOVPE method. More specifically, GaN is grown to a thickness of about 3 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in a predetermined growth chamber. Thus, a semiconductor substrate is completed.




In the GaN single crystal film


105


grown in the present embodiment, a defect density is decreased to about 1500/cm


2


or less, and crystallinity is remarkably improved.




In the case where the first mask and the second mask have a stripe width of about 4 μm and a pitch of about 10 μm, and the first and second masks are positioned so as to be shifted by a half pitch (in the case where the stripe width of the second mask is smaller than each opening of the first mask) in the present embodiment, a defect density becomes about 5000/cm


2


. Thus, an effect of a sufficient decrease in crystal defects is observed when compared with the case of using only the first mask in the conventional example. A defect density becomes relatively small in the case where the stripe width of the second mask is larger than each opening of the first mask, and the first and second masks completely cover crystal threading dislocation extending upward from the sapphire substrate


100


. Accordingly, it is confirmed that it is important to form the second mask so as to completely cover the openings of the first mask.




On the other hand, the following is found according to X-ray diffraction measurement: in the case where the stripe width of the second mask is smaller than each opening of the first mask, a defect density is decreased to some degree (about 5000/cm


2


), and a c-axis alignment of a GaN continuous film is improved. The following is confirmed in the case where the stripe width of the second mask is larger than each opening of the first mask, a ω value (full width at half maximum) of X-ray diffraction representing alignment variation is about 4 to 6 arcminutes: however, in the case where the stripe width of the second mask is smaller than each opening of the first mask, alignment variation (ω value) of a crystal is reduced to 2 arcminutes in a wafer plane. Thus, in the case where an LED, a semiconductor laser device, or the like is produced under the condition that the stripe width of the second mask is smaller than each opening of the first mask, a light-emitting efficiency is degraded compared with the case where the stripe width of the second mask is larger than each opening of the first mask; however, a light-emitting efficiency in a wafer plane and uniformity of a threshold current of a laser are improved, which enhances the production yield of a device. Accordingly, it is important to select the relationship between the size of each opening of the first mask and the stripe width of the second mask, depending upon required characteristics of a light-emitting device. Furthermore, if the first and second masks are formed of the same material, the same vapor deposition apparatus can be used, and quality of crystal films can be stabilized by the same growth suppressing effect (in the case of giving a high priority to a light-emitting efficiency, the stripe width of the second mask should be prescribed to be larger than each opening of the first mask; in the case of giving a high priority to uniformity of characteristics and yield, the stripe width of the second mask should be prescribed to be smaller than each opening of the first mask).




Embodiment 2





FIG. 2

shows the second embodiment. The second embodiment is different from the first embodiment in that a GaN crystal film


203


grown by using a first mask is not a continuous film, and a second mask is formed on the GaN crystal film


203


grown in the shape of an island.




First, a GaN layer


201


is grown to a thickness of about 4 μm on a sapphire substrate


200


in the same way as in Embodiment 1. In the case of the second embodiment, a first GaN crystal film


203


grown by using a first SiO


2


mask


202


is prescribed to have a thickness of about 1 μm, a width of about 7 μm, and a pitch of about 10 μm. Then, a second GaN single crystal film


205


(thickness: about 4 μm) is grown by using a second SiO


2


mask


204


(thickness: about 200 nm). A defect density is about 800/cm


2


or less. Thus, a satisfactory crystal is obtained. This is an effect that the GaN single crystal film


205


grows only from side surfaces


206


where there are few defects in the first GaN crystal.




Embodiment 3




The third embodiment will be described with reference to FIG.


3


. In Embodiment 1, it is required to conduct crystal growth of GaN for a patterned mask by two steps; however, in Embodiment 3, one step of crystal growth suffices, which results in a cost advantage.




First, an SiO


2


film is formed to a thickness of about 200 nm on a sapphire substrate


300


with a GaN layer


301


formed thereon, by sputtering in the same way as in Embodiment 1. The SiO


2


film is etched to a stripe shape (width: about 4 μm; pitch: about 8 μm) by a conventional photolithography method, whereby a first SiO


2


mask


302


is formed. Then, an SiO


2


film is formed on the resultant substrate in the same way as the above, whereby a second lower SiO


2


mask


303


in the shape of a stripe (width: about 2 μm; pitch: about 8 μm) is formed on the first SiO


2


mask


302


. Then, a portion other than the lower SiO


2


mask


303


is covered with a photoresist film by conventional photolithography. More specifically, a photoresist such as AZ (produced by SHIPLEY is spin-coated over the entire surface of the GaN layer


301


, the first SiO


2


mask


302


, and the lower SiO


2


mask


303


. Then, only the lower SiO


2


mask


303


is exposed to light and developed, and the photoresist film is removed. Furthermore, an SiO


2


film is formed to obtain a second upper SiO


2


mask


304


in the shape of a stripe (width: about 5 μm; pitch: about 8 μm). Thereafter, the above-mentioned photoresist film is removed with a solvent such as acetone. The second lower SiO


2


mask


303


and the second upper SiO


2


mask


304


form a second mask in the shape of a letter “L”. GaN is grown by a MOVPE method by using the resultant substrate. More specifically, a GaN single crystal film


305


is grown to a thickness of about 3 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in a predetermined growth chamber. Thus, a semiconductor substrate is completed.




Herein, crystal growth of the GaN single crystal film


305


starts from openings of the first SiO


2


mask


302


. Then, the crystal growth in a direction vertical to the substrate stops at the second upper SiO


2


mask


304


. Thereafter, the crystal growth proceeds in a direction parallel to the substrate. The crystal growth also starts from openings of the second upper SiO


2


mask


304


in a direction vertical to the substrate. Finally, a crystal is grown uniformly over the entire surface of the substrate.




In the present embodiment, dislocation in a direction vertical to the substrate, which is generated from the interface between the GaN layer


301


and the sapphire substrate


300


, stops at the second upper SiO


2


mask


304


, and dislocation in a direction horizontal to the substrate stops at the second lower SiO


2


mask


303


. Thus, the obtained GaN single crystal film


305


is of satisfactory quality (i.e., a defect density is about 600/cm


2


or less).




Embodiment 4




The fourth embodiment will be described with reference to FIG.


4


.




First, an SiO


2


film is formed to a thickness of about 200 nm on a sapphire substrate


400


with a GaN layer


401


formed thereon, by sputtering in the same way as in Embodiment 1. The SiO


2


film is etched to a stripe shape (width: about 4 μm; pitch: about 8 μm) by a conventional photolithography method, whereby a first SiO


2


mask


402


is formed. Then, a second lower SiO


2


mask


403


is formed to a stripe shape (width: about 2 μm; pitch: about 8 μm) on the GaN layer


401


. Then, a portion other than the lower SiO


2


mask


403


is covered with a photoresist film by conventional photolithography. More specifically, a photoresist such as AZ (produced by SHIPLEY) is spin-coated over the entire surface of the GaN layer


401


and the first SiO


2


mask


402


. Then, only the lower SiO


2


mask


403


is exposed to light and developed, and the photoresist film is removed. Furthermore, a second upper SiO


2


mask


404


in the shape of a stripe (width: about 5 μm; pitch: about 8 μm) is formed on the second lower SiO


2


mask


403


. Thereafter, the above-mentioned photoresist film is removed with a solvent such as acetone. The second lower SiO


2


mask


403


and the second upper SiO


2


mask


404


form a second mask in the shape of a letter “T”. GaN is grown by a MOVPE method by using the resultant substrate. More specifically, a GaN single crystal film


405


is grown to a thickness of about 3 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in a predetermined growth chamber. Thus, a semiconductor substrate is completed.




Herein, crystal growth of the GaN single crystal film


405


starts from openings of the first SiO


2


mask


402


. Then, the crystal growth in a direction vertical to the substrate stops at the second upper SiO


2


mask


404


. Thereafter, the crystal growth proceeds in a direction parallel to the substrate. The crystal growth also starts from openings of the second upper SiO


2


mask


404


in a direction vertical to the substrate. Finally, a crystal is grown uniformly over the entire surface of the substrate.




In the present embodiment, dislocation in a direction vertical to the substrate, which is generated from the interface between the GaN layer


401


and the sapphire substrate


400


, stops at the second upper SiO


2


mask


404


, and dislocation in a direction horizontal to the substrate stops at the second lower SiO


2


mask


403


. Thus, the obtained GaN single crystal film


405


is of satisfactory quality (i.e., a defect density is about 800/cm


2


or less).




Embodiment 5




The fifth embodiment will be described with reference to FIG.


5


.




First, in order to form a first patterned mask, a film made of a growth suppressing material (SiO


2


) is formed to a thickness of about 200 nm by sputtering on a sapphire substrate


500


having a C-plane as its surface on which a GaN layer


501


is formed. A method for forming the SiO


2


film is not limited to sputtering. Another method, such as vacuum vapor deposition or CVD, may be used. Furthermore, as a growth suppressing material, oxides such as Al


2


O


3


and TiO


2


and SiN


x


can be used in place of SiO


2


. Then, openings in the shape of a stripe (width: about 3 μm; pitch: about 100 μm) are provided in the SiO


2


film by a conventional photolithography method, whereby a first SiO


2


mask


502


is formed. The direction of the stripes is desirably <1-100> with respect to the GaN layer


501


.




GaN is grown by a MOVPE method by using the resultant substrate. More specifically, GaN


503


is grown to a thickness of about 0.5 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in a predetermined growth chamber. The GaN


503


is grown only at edge portions of the first SiO


2


mask


502


without burying the first SiO


2


mask


502


. The edge portions have a low potential with respect to other portions, so that the GaN


503


is of satisfactory quality without any defects.




Then, a second mask is formed on the resultant substrate. More specifically, SiO


2


is deposited to a thickness of about 200 nm by sputtering in the same way as in the first SiO


2


mask


502


, whereby a second SiO


2


mask


504


is formed in the shape of a stripe (width: 5 μm; pitch: 100 μm) by a photolithography method. It is important that the positions of light-blocking portions are substantially matched with the openings of the first SiO


2


mask


502


.




Then, a GaN single crystal film


505


is grown by a MOVPE method, by using the resultant substrate. More specifically, GaN is grown to a thickness of about 3 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in a predetermined growth chamber. Thus, a semiconductor substrate is completed.




In the GaN single crystal film


505


grown in the present embodiment, a defect density is decreased to about 1000/cm


2


or less over the entire surface thereof, and crystallinity is remarkably improved.




Herein, it is important that the light-blocking portions of the second SiO


2


mask


504


cover the openings of the first SiO


2


mask


502


.




Embodiment 6




The sixth embodiment will be described with reference to FIG.


6


. Herein, the same reference numerals as those in Embodiment 1 denote the same elements as those herein.




A semiconductor laser device in the present embodiment includes an n-GaN contact layer


106


, an n-Al


0.1


Ga


0.9


N cladding layer


107


, an n-GaN guide layer


108


, a multi quantum-well structure active layer


109


including 5 In


0.2


Ga


0.8


N quantum-well layers and 6 In


0.05


Ga


0.95


N barrier layers, an Al


0.2


Ga


0.8


N evaporation preventing layer


110


, a p-GaN guide layer


111


, a p-Al


0.1


Ga


0.9


N cladding layer


112


, a p-GaN contact layer


113


, a p-type electrode


114


, an n-type electrode


115


, and an SiO


2


insulating film


116


.




According to the present invention, the surface of the sapphire substrate


100


may have another orientation, such as an a-plane, an r-plane, and an m-plane. Furthermore, a GaN substrate, an SiC substrate, a spinnel substrate, an MgO substrate, an Si substrate, and a GaAs substrate can be used in place of a sapphire substrate. Particularly in the case of using a GaN substrate, compared with the case of using a sapphire substrate, at least the following advantages are obtained: a difference in a lattice constant between the substrate and a gallium nitride type semiconductor material deposited on the substrate is smaller, and a film with satisfactory crystallinity can be obtained. Furthermore, the GaN substrate is more likely to be cleaved, so that it is easier to produce a laser resonator by cleavage. The cladding layer


107


and the cladding layer


112


may be made of a mixed crystal containing three elements (AlGaN) having an Al mole fraction other than Al


0.1


Ga


0.9


N. In this case, when an Al mole fraction is increased, a difference in an energy gap and a difference in a refractive index between the active layer and the cladding layer becomes larger, so that carriers and light are confined in the active layer, which further decreases an oscillation threshold current and improves temperature characteristics. Furthermore, when an Al mole fraction is decreased to such a degree that carriers and light can be confined, the mobility of carriers in the cladding layer becomes large. Therefore, the resistance of a semiconductor laser device can be decreased. Furthermore, the cladding layers


107


and


112


may be made of a mixed crystal semiconductor containing a trace amount of another element in addition to the above-mentioned three elements, and the mole fractions of a mixed crystal are not required to be the same between the cladding layer


107


and the cladding layer


112


.




The guide layers


108


and


111


may be made of any material which allows an energy gap therebetween to have a value between an energy gap of the quantum-well layers included in the active layer


109


and a energy gap of the cladding layers


107


and


112


. For example, a mixed crystal containing three elements (e.g., InGaN or AlGaN) may be used. Furthermore, it is not necessary to dope a donor or an acceptor over the entire guide layers


108


and


111


, and only a portion thereof on the side of the active layer


109


may be non-doped. Furthermore, the entire guide layers


108


and


111


may be non-doped. In this case, there is an advantage that the number of carriers present in the guide layers


108


and


111


becomes small, light absorption by free carriers is decreased, and an oscillation threshold current can be further reduced.




With the quantum-well layers and the barrier layers included in the active layer


109


, mole fractions should be set in accordance with a required laser oscillation wavelength. In the case where it is desirable to make an oscillation wavelength longer, the In mole fraction of the quantum-well layers is increased. In the case where it is desired to shorten an oscillation wavelength, the In mole fraction of the quantum-well layers is decreased. Furthermore, the quantum-well layers and the barrier layers may be made of a mixed crystal semiconductor containing four or more elements including a trace amount of another element in addition to a mixed crystal containing three elements (InGaN). The barrier layers may be made of GaN.




In the present embodiment, the evaporation preventing layer


110


is formed in contact with the active layer


109


. The purpose of this is to prevent the active layer


109


from evaporating during an increase in a growth temperature. Therefore, any material can be used for the evaporation preventing layer


110


as long as it protects the active layer


109


. For example, a mixed crystal containing three elements (AlGaN) having another Al mole fraction and GaN maybe used. Furthermore, Mg may be doped into the evaporation preventing layer


110


. In this case, there is an advantage that holes can be easily injected from the guide layer


111


and the cladding layer


112


. Furthermore, in the case where the In mole fraction of the quantum-well layers included in the active layer


109


is small, the quantum-well layers are not evaporated, so that the evaporation preventing layer


110


is not required to be formed. Even if the evaporation preventing layer


110


is not formed, characteristics of a gallium nitride type semiconductor laser device in the present embodiment will not be impaired.




Hereinafter, a method for producing the above-mentioned gallium nitride type semiconductor laser device will be described with reference to FIG.


6


.




In the following description, the case of using a MOVPE method is shown. However, any method which is capable of epitaxially growing GaN may be used. For example, another vapor growth method such as molecular beam epitaxy (MBE) or HVPE can be used.




First, the contact layer


106


doped with Si is grown to a thickness of about 3 μm at a growth temperature of about 1050° C., using TMG, NH


3


, and a silane gas (SiH


4


) as materials, on the substrate produced in Embodiment 1 placed in a predetermined growth chamber. Then, trimethyl aluminum (TMA) is added to the materials, and the cladding layer


107


doped with Si is grown to a thickness of about 0.4 μm at a growth temperature of about 1050° C. TMA is removed from the materials, and the guide layer


108


doped with Si is grown to a thickness of about 0.1 μm at a growth temperature of about 1050° C.




Next, the growth temperature is lowered to about 750° C., and 5 barrier layers (thickness: about 5 nm) and 5 quantum-well layers (thickness: about 2 nm) are alternately grown and the barrier layer (thickness: about 5 nm) is grown, using TMG, NH


3


and trimethyl indium (TMI), whereby the active layer


109


(total thickness: about 40 nm) is produced. Then, the evaporation preventing layer


110


is grown to a thickness of about 20 nm at a growth temperature of about 750° C., using TMG, TMA, and NH


3


as materials.




Next, the growth temperature is raised to about 1050° C., and the guide layer


111


doped with Mg is grown to a thickness of about 0.1 μm, using TMG, NH


3


, and bisethylcyclopentadienyl magnesium (EtCP


2


Mg) as materials. TMA is added to the materials, and the cladding layer


112


is grown to a thickness of about 0.4 μm at a growth temperature of about 1050° C. TMA is removed from the materials, and the contact layer


113


doped with Mg is grown to a thickness of about 0.2 μm at a growth temperature of about 1050° C. Thus, a gallium nitride type epitaxial wafer is completed. Thereafter, the wafer is annealed in a nitrogen gas atmosphere at about 800° C., whereby the Mg-doped p-type layers are rendered low-resistant.




Furthermore, etching is conducted from the top surface of the contact layer


113


so as to obtain a stripe shape (width: about 200 μm) by using conventional photolithography and dry etching until the contact layer


106


is exposed, whereby amesa structure is produced. Next, using the photolithography and dry etching similar to the above, the remaining contact layer


113


and the cladding layer


112


are etched. At this time, a stripe-shaped ridge structure should be positioned about 3 μm or more away from both ends of the mesa structure with a width of about 200 μm. In the present embodiment, the ridge structure is formed about 10 μm away from the end of the mesa structure on the side where the n-type electrode


115


is to be formed. If the ridge structure is positioned so as to be close to the n-type electrode


115


as described above, the electric resistance of the device is decreased, and the working voltage is reduced. Furthermore, the dry etching is stopped so as not to etch the active layer


109


. Thus, the active layer


109


is protected from etching damage, which prevents a decrease in reliability and an increase in an oscillation threshold current.




The insulating film


116


is formed to a thickness of about 200 nm as a current blocking layer on the side surfaces of the ridge structure and on the surface of the p-type layer excluding the ridge. The p-type electrode


114


made of nickel and gold is formed on the surface of the insulating layer


116


and the contact layer


113


, and the n-type electrode


115


made of titanium and aluminum is formed on the surface of the contact layer


106


exposed by etching. Thus, a gallium nitride type laser device wafer is completed.




Thereafter, the wafer thus obtained is cleaved in a direction vertical to the ridge stripe to form a resonance plane, and the wafer is divided into chips. Each chip is mounted on a stem, and each electrode is connected to each lead terminal by wire bonding. Thus, a gallium nitride type semiconductor laser device is completed.




In the semiconductor laser device produced as described above, satisfactory laser characteristics (oscillation wavelength: about 410 nm; oscillation threshold value: about 20 mA) are obtained. Furthermore, due to a decrease in crystal defects, the semiconductor laser device thus obtained is highly reliable (about 10


5


hours at about 60° C.). Furthermore, a ratio of laser devices having crystal defects is remarkably decreased, with a yield being about 80% or higher.




In the present embodiment, thicknesses of each quantum-well layer and each barrier layer included in the active layer


109


are about 2 nm and about 5 nm, respectively. However, as long as the thickness of each quantum-well layer and each barrier layer is prescribed to be about 10 nm or less, the same effects can be obtained irrespective of embodiments. Furthermore, the number of quantum-well layers in the active layer


109


may be 2, 3 or 4. Alternatively, a single quantum-well structure active layer may be used.




In the present embodiment, sapphire, which is an insulator, is used for the substrate, so that the n-type electrode


115


is formed on the surface of the contact layer


106


exposed by etching. However, if GaN, SiC, Si, GaAs, or the like having an n-type insulating property is used, the n-type electrode


115


may be formed on the reverse surface of the substrate. In this case, the mesa structure with a width of about 200 μm should be positioned at least about 3 μm away from both ends of the semiconductor laser device chip. P-type structures and n-type structures may be reversed.




Embodiment 7




Referring to

FIG. 7A

, a method for growing a crystal in Embodiment 7 will be described.

FIG. 7A

is a cross-sectional view of a nitride semiconductor to be formed.




First, a GaN layer


601


is grown to a thickness of about 2 μm, using TMG and NH


3


as materials, on a sapphire substrate


600


having a C-plane as its surface placed in a predetermined growth chamber. The sapphire substrate


600


and the GaN layer


601


are included in a lower substrate. The GaN layer


601


is a lower semiconductor crystal layer as well as a lower nitride semiconductor crystal layer.




Then, in order to form a first mask pattern, a film (thickness: about 100 nm) made of a growth suppressing material (SiO


2


) is formed on the GaN layer


601


by sputtering. A method for forming the SiO


2


film is not limited to sputtering. Another method, such as CVD, electron beam (EB) vapor deposition, or vacuum vapor deposition, may be used. Furthermore, as a growth suppressing material, oxides such as Al


2


O


3


and TiO


2


and SiN


x


can be used in place of SiO


2


. Then, the SiO


2


film is patterned to a periodic stripe (width w: about 7 μm; pitch d: about 10 μm) by a conventional photolithography method, whereby a first mask pattern


602


is formed.

FIG. 7B

is a plan view of a nitride semiconductor to be formed. As shown in

FIG. 7B

, the direction of the stripe is prescribed to be a [1-100] direction of a GaN crystal.




By using the substrate with the first mask pattern thus obtained, a first GaN film


604


is grown by a MOVPE method. More specifically, the first GaN film


604


is grown to a thickness of about 5 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in a predetermined growth chamber. Thus, the first step is completed. The first GaN film


604


starts growing from openings


605


in the first mask pattern


602


, and is flatly grown over substantially the entire surface of the sapphire substrate due to anisotropy (i.e., a growth speed in a direction horizontal to the substrate, particularly, in a <11-20> direction with respect to a GaN crystal, is higher than that in a direction vertical to the substrate).




Portions of the first GaN film


604


on the first mask pattern


602


grown in a direction vertical to the stripe of the first mask pattern


602


have a very weak inter-atom bond with respect to the first mask pattern


602


(i.e., these portions are not epitaxially grown from the first mask pattern


602


); therefore, lattice strains are not caused in these portions. However, lattice strains remain in a direction parallel to the stripe due to a difference in a lattice constant between the GaN layer


601


and the sapphire substrate


600


, and the lattice strains are also reflected onto the first GaN film


604


. During the first step, problems of lattice strains and a high threading dislocation density are not overcome. Thus, when a semiconductor laser is formed on the first GaN film


604


including the lattice strains and having a high threading dislocation density, a continuous oscillation time of the device at room temperature is about 900 hours. This oscillation life does not satisfy reliability of the device.




Furthermore, as described above, since the portions of the first GaN film


604


immediately above the first mask pattern


602


have a very weak inter-atom bond with respect to the first mask pattern


602


, these portions are unlikely to be influenced by thermal strains from the underlying layer (i.e., the sapphire substrate


600


). However, a GaN crystal above the openings in the first mask pattern


602


is more strongly influenced by thermal strains from the underlying layer (i.e., the sapphire substrate


600


).




The portions of the first GaN film


604


immediately above the first mask pattern


602


has a threading dislocation density of the order of 10


4


to 10


5


/cm


2


. The portions of the first GaN film


604


immediately above the openings of the first mask pattern


602


have a threading dislocation density of the order of 10


7


to 10


8


/cm


2


. In the conventional example, a laser device is formed avoiding the portions including lattice strains, thermal strains, and the like, which makes reliability and yield of the device insufficient.




Then, a second mask pattern


606


(

FIG. 8

) made of SiO


2


is formed on the surface of the first GaN film


604


. More specifically, an SiO


2


film (thickness: about 100 nm) formed by the same method as that of the first mask pattern


602


is subjected to conventional photolithography and etching, whereby the periodic second mask pattern


606


(width: about 8 μm; pitch: about 10 μm) made of SiO


2


is formed. Furthermore, under the condition that the stripe direction of the second mask pattern


606


is observed from above the wafer, the stripe direction of the second mask pattern


606


is prescribed to be a [01-10] direction of a GaN crystal so that it forms an angle of about 120° with respect to the stripe direction of the first mask pattern


602


.

FIG. 8

is a plan view of the semiconductor device in this state. For description,

FIG. 8

shows the mask patterns as seen from the top.




The second mask pattern


606


is formed to have a width larger than that of the first mask pattern


602


by about 1 μm, so that the second mask pattern


606


covers the surface of the underlying first GaN film


604


more widely than the first mask pattern


602


.




Next, a second GaN film


607


(

FIG. 9A

) is grown over the entire surface of the first GaN film


604


with the second mask pattern


606


formed thereon by an MOCVD method. Thus, the second step is completed. The growth of the second GaN film


607


is conducted at a substrate temperature of about 1050° C., using TMG and NH


3


as materials. The second GaN film


607


has a thickness of about 5 μm. Accordingly, the second GaN film


607


is grown uniformly over the entire surface of the wafer including upper portions of the second mask pattern


606


, and the surface of the second GaN film


607


becomes substantially flat.

FIG. 9A

is across-sectional view taken along a line a-a′ parallel to the second mask pattern


606


in

FIG. 8

, and

FIG. 9B

is across-sectional view taken along a line b-b′ parallel to the first mask pattern


602


in FIG.


8


. The cross-section taken along the line b-b′ is obtained from an opening portion of the first mask pattern


602


, and hence, the first mask pattern


602


cannot be observed in FIG.


9


B.




Lattice strains in the second GaN film


607


grown during the second step are reduced in a direction vertical to the stripe of the second mask pattern


606


in the same way as in the first step, compared with the case where there is no second mask pattern


606


. Lattice strains in a direction parallel to the stripe of the second mask pattern


606


become similar to that of the first GaN film


604


. Lattice strains in the first GaN film


604


are reduced in a direction vertical to the first mask pattern


602


during the first step. Therefore, in the second GaN film


607


, lattice strains are reduced in two directions, i.e., in a direction vertical to the stripe of the first mask pattern


602


and in a direction vertical to the stripe of the second mask pattern


606


.




Furthermore, a threading dislocation density of the second GaN film


607


produced during the second step is decreased to the order of 10


3


/cm


2


in portions


608


immediately above the first and second mask patterns


602


and


606


, and crystallinity is remarkably improved. Furthermore, a threading dislocation density of portions


609


of the second GaN film


607


grown from the opening portions of the first mask pattern


602


is on the order of 10


5


/cm


2


due to lateral growth caused by the second mask pattern


606


. Furthermore, a threading dislocation density of portions


610


immediately above the first mask pattern


602


is on the order of about 10


4


/cm


2


.




Furthermore, as the third step, a GaN crystal is grown on the second GaN film


607


by using a periodic stripe-shaped mask similar to those used during the first and second steps. First, an SiO


2


film (thickness: about 100 nm) is formed on the second GaN film


607


by the same method as that of the first step. The SiO


2


film is formed into a periodic stripe by conventional photolithography and etching, whereby a third mask pattern


611


with a width of about 8 μm and a period of about 10 μm is obtained. The third mask pattern


611


is disposed in such a manner that the stripe direction thereof forms an angle of about 120° with respect to any direction of the first and second mask patterns


602


and


606


. That is, the stripe direction of the third mask pattern


611


is a [10—10] direction.

FIG. 10A

is a plan view of the semiconductor device in this state. For description,

FIG. 10A

shows the mask patterns as seen from the top.




Next, a third GaN film


612


(thickness: about 5 μm) is grown on the second GaN film


607


with the third mask pattern


611


formed thereon in the same way as in the first and second steps. Thus, the third step is completed. The third GaN film


612


is also grown over the entire surface of the third mask pattern


611


made of SiO


2


, and exhibits a single film having a substantially flat surface. Furthermore, in the third GaN film


612


formed during the third step, lattice strains in a direction vertical to the stripe of the third mask pattern


611


are further reduced, compared with the second GaN film


607


.

FIG. 10B

is a view showing the semiconductor device, taken along a line a-a′ in FIG.


10


A.




As described above, the third GaN film


612


on the uppermost surface produced through three steps is obtained by growing a GaN crystal above three kinds of mask patterns


602


,


606


, and


611


which form an angle of about 120° with respect to each other. During the respective steps, lattice strains in a direction vertical to the stripes of the respective mask patterns are relaxed. Thus, the third GaN film


612


has strains reduced isotropically by three kinds of mask patterns which form the same angle with each other. As a result, a semiconductor substrate including the third GaN film


612


having substantially no strains in any in-plane direction is realized.




Furthermore, in the present embodiment, the stripe directions of the first mask pattern


602


, the second mask pattern


606


, and the third mask pattern


611


are prescribed to be [1-100], [01-10], and [10—10]. The present invention is not limited thereto. If the stripe directions of the first, second, and third mask patterns are a <1-100> direction, and the respective stripe directions have an angle difference of about 120°, there is an effect that substantially no strains are present in any in-plane direction. By prescribing the stripe direction of one of the first to third masks to be <1-100> and prescribing the stripe directions of the other mask patterns so that they have an angle difference of about 120°, an equivalent strain relaxing function is exhibited in a nitride semiconductor, and lateral growth of a crystal is promoted, whereby the mask patterns can be efficiently buried. Therefore, a decrease in a threading dislocation density and strain relaxation can be maximized.




A threading dislocation density on the surface of the third GaN film


612


is checked, revealing that a threading dislocation extending straight upward from the sapphire substrate


600


is covered with any of the first to third mask patterns, whereby a threading dislocation is prevented from extending through the masks. Therefore, a threading dislocation density on the surface of the third GaN film


612


can be reduced by one or more orders of magnitude (i.e., about 10


3


/cm


2


to about 10


4


/cm


2


), compared with the conventional technique. Although portions


613


in the third GaN film


612


grown from the opening portions of the first mask pattern


602


are not covered with three kinds of mask patterns, their ratio with respect to the entire area is less than about 10%, and a threading dislocation is not increased in these portions. This may be because a threading dislocation is dispersed to the right and left during the step of forming a GaN film to a total of about 15 μm or more, and a threading dislocation is substantially uniformly distributed on the surface of the third GaN film


612


formed during the third step.




The first, second, and third mask patterns have the same thickness and are made of the same growth suppressing material (SiO


2


) in Embodiment 7. However, these mask patterns may have different thicknesses and be made of different growth suppressing materials. In particular, if the same grown suppressing material is used for these mask patterns, the same growth chamber can be used, which is advantageous in terms of productivity, and the same growth suppressing effect is obtained, resulting in good controllability of growth. As a method for growing a nitride semiconductor, an HVPE method or an MBE method may be used in place of the above-mentioned MOVPE method.




Furthermore, in the present embodiment, the first to third nitride semiconductor crystal layers are formed by using the first to third masks. However, the present invention is not limited thereto. For example, it may be possible that the n-th nitride semiconductor crystal layer is formed on the n-th mask, and the (n+1)-th mask and the (n+1)-th nitride semiconductor crystal layer are formed in the same way as in the n-th step. Herein, n is an integer of 1 or more. Accordingly, by successively conducting a series of steps, crystal strains in a nitride semiconductor film during each step (strains caused by a difference in a lattice constant or a difference in a coefficient of thermal expansion between the substrate and the nitride semiconductor crystal) are reduced. Furthermore, a dislocation generated from the interface of the substrate will not emerge on the surface of a grown crystal film.




Even in the above case, in the same way as in the present embodiment, it is preferable that the first to (n+1)-th masks are combined with each other and patterned so as to cover the entire surface of the lower substrate. Because of this, a dislocation generated from the opening portions of the first mask pattern formed on the substrate or the nitride semiconductor film grown on the substrate is blocked with any of (n+1) mask patterns. Thus, a density of a threading dislocation which reaches the surface of the n-th nitride semiconductor film is remarkably reduced.




Furthermore, it is preferable that the n-th mask and the (n+1)-th mask are patterned to be striped, and the stripe directions of the n-th mask and the (n+1)th mask are disposed so as to be twisted from each other. Because of this, a nitride semiconductor film crystal covering portions immediately above a mask pattern is unlikely to grow, due to selective growth, directly on the mask pattern, and the nitride semiconductor film crystal covering portions immediately above a mask pattern is laterally grown from the opening portions of the mask pattern in a direction vertical to the stripe direction of the mask pattern. Thus, portions of the (n+1)-th nitride semiconductor film on the (n+1)-th mask pattern grown in a direction vertical to the stripe of the (n+1)-th mask pattern have a very weak inter-atom bond with respect to the (n+1)-th mask pattern, so that lattice strains are not caused in these portions. However, in a direction parallel to a stripe, lattice strains are transferred from the underlying layer formed during or prior to the nth step to the (n+)-th nitride semiconductor film. This is also applicable to thermal strains.




Due to the twisted positional relationship among the mask patterns as described above, an effect of strains from the underlying layer can be canceled in various directions, as well as in one direction. The above-mentioned relaxation of strains has an effect of suppressing an edge dislocation from being generated.




Furthermore, it is preferable that the stripe directions of the n-th mask and the (n+1)-th mask are twisted from each other so as to have an angle difference of about 120°. A nitride semiconductor mainly has a wurtzite structure, so that there are three kinds of equivalent directions. These three directions have an angle difference of 1200 from each other. By disposing the mask patterns produced during the above-mentioned steps so that they have an angle difference of about 120° from each other, these mask patterns have selection characteristics equivalent to each other, and strains can be relaxed by an equivalent strain relaxing function.




It is preferable that the stripe width of the (n+1)-th mask is equal to or larger than that of the n-th mask. If the stripe width of a mask pattern is increased with the increase in the number of the above-mentioned steps (i.e., an increase in n), a nitride semiconductor film produced during each step will have a decreased density of a threading dislocation generated from the substrate to the crystal layering direction.




A growth suppressing material may be SiO


2


or SiN


x


, and the first to (n+1)-th masks may be independently made of SiO


2


or SiN


x


. A mask pattern made of SiO


2


or SiN


x


has a sufficient growth suppressing effect.




The stripe direction of the n-th mask preferably agrees with a <1-100> direction or a <11-20> direction of a crystal of the nitride semiconductor crystal layer. In the case where the stripe direction of the mask pattern is <1-100>, a nitride semiconductor film formed particularly by an MOVPE method is laterally grown in a <11-20> direction vertical to the stripe direction, so that it is possible to bury the mask pattern with the nitride semiconductor thin film. Furthermore, depending upon growth characteristics, a threading dislocation hardly appears on the mask pattern. It is understood from these characteristics that the <1-100> stripe direction is very important for selective growth (lateral growth).




In the case where the stripe direction of the mask pattern is prescribed to be <11-20>, a nitride semiconductor crystal is laterally grown in a direction of <1-100>. In this case, a lateral growth speed of the nitride semiconductor crystal is lower than that in the case where the stripe direction of the mask pattern is set to be <1-100>. Furthermore, a threading dislocation which comes from the opening portions of a mask is bent in the direction of the mask, and is combined with another threading dislocation to extend in the crystal growth direction. Thus, compared with the case where the stripe direction of the mask pattern is prescribed to be <1-100>, a number of threading dislocations are generated even in portions on the mask. However, this does not mean that a new dislocation is generated immediately above the mask, but that a threading dislocation which comes from the opening portions of the mask is dispersed. As a result, a threading dislocation density is reduced in the same way as in the case where the stripe direction is prescribed to be <1-100>. According to one embodiment, the stripe direction of the mask pattern is prescribed to be <1-100> or <11-20>, whereby a lateral growth is promoted and the mask pattern is buried efficiently; thus, a decrease in a threading dislocation density and strain relaxation can be realized.




The n-th nitride semiconductor crystal layer may be made of Al


x


In


y


Ga


z


N (x+y+z=1, 0≦x≦1, 0≦y≦1, and 0≦z≦1). Such a crystal is suitable for the growth method of the present invention due to its anisotropy (lateral growth).




It is preferable that the n-th nitride semiconductor crystal layer or the (n+1)-th nitride semiconductor crystal layer has a thickness of about 5 μm or more. A threading dislocation generated from the substrate is blocked by a mask pattern, and enters a nitride semiconductor film from the openings of the mask. However, by forming a thick nitride semiconductor crystal layer, the mask pattern can be covered with a GaN film, and a threading dislocation which is not blocked can be reduced by the thick nitride semiconductor crystal layer.




Embodiment 8




In Embodiment 8, the GaN film


607


formed during the second step in Embodiment 7 is evaluated for characteristics, in the case where the GaN film


607


is used as an underlying film of a device. More specifically, in Embodiment 7, mask formation and crystal growth on a mask are repeated three times. Herein, the effect of the present invention will be described, in the case where mask formation and crystal growth on a mask are repeated twice. In this case, the first and second mask patterns are formed so as to have an angle difference of about 120° from each other, so that lattice strains are reduced in two directions vertical to the stripe directions of two mask patterns. However, a small number of lattice strains remain in a direction (i.e., in a horizontal on the drawing surface of

FIG. 8

) which bisects an angle of about 120° formed by two mask patterns.




Furthermore, a threading dislocation density of the second GaN film


607


positioned immediately above the first and second mask patterns is reduced to about 10


3


/cm


2


, and a threading dislocation density of the portions


609


in the second GaN film


607


grown from the opening portions of the first mask pattern is about 10


5


/cm


2


. An average threading dislocation density on the entire surface of the second GaN film


607


is about 3×10


4


/cm


2


, which is a reduction of a threading dislocation by about one order of magnitude, compared with the conventional example. Regarding strains, as described in Embodiment 7, more satisfactory relaxation effect is obtained compared with the conventional example (only the first step), by conducting the second step of the present invention.




Embodiment 9




Embodiment 9 is an altered example of Embodiment 8. Embodiment 9 is the same as Embodiment 8, except that the stripe direction of the first mask pattern formed during the first step and the stripe direction of the second mask pattern formed during the second step have an angle difference of about 90°.

FIG. 11A

is a plan view of a GaN film formed in Embodiment 9. For description,

FIG. 11A

shows mask patterns as seen from the top. As shown in

FIG. 11A

, the stripe direction of a first mask pattern


702


and the stripe direction of a second mask pattern


704


form an angle of about 90°. The first and second mask patterns


702


and


704


are formed in a <11-20> direction and a <1-100> direction of a GaN crystal, respectively. It is preferable that the first and second mask patterns


702


and


704


are formed in a <11-20> direction and a <1-100> direction, respectively. However, the present invention is not limited thereto.





FIG. 11B

is a cross-sectional view taken along a line a-a′ in FIG.


11


A. First, a sapphire substrate


700


having a C-plane is placed in an MOVPE growth chamber, and a GaN layer


701


is grown to a thickness of about 2 μm, using TMG and NH


3


as materials. Then, in order to form a first patterned mask, an SiO


2


film having a thickness of about 100 nm is formed by an EB vapor deposition method. Then, the SiO


2


film is patterned to a periodic stripe (width: about 3 μm; pitch: about 7 μm) by a conventional photolithography method, whereby a first mask pattern


702


is formed. As shown in

FIG. 11A

, The stripe direction of the first mask pattern


702


is prescribed to be <11-20> of a GaN crystal.




By using the substrate with the first mask pattern thus obtained, a first GaN film


703


is grown by a MOVPE method. More specifically, the first GaN film


703


is grown to a thickness of about 10 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in a predetermined growth chamber. Thus, the first step is completed. The first GaN film


703


starts growing from opening portions


706


of the first mask pattern


702


, and is laterally grown in a direction horizontal to the substrate surface. Although a lateral growth speed is lower, compared with the case where the stripe direction of the mask pattern is prescribed to be <1-100> as in Embodiment 7 or 8, the GaN film


703


having a thickness of about 10 μm is grown flat, covering the first mask pattern


702


.




A threading dislocation density of the first GaN film


703


is on the order of about 10


6


/cm


2


in the portions immediately above the first mask pattern


702


. However, a threading dislocation density of the first GaN film


703


is on the order of about 10


7


/cm


2


in the portions immediately above the openings


706


of the first mask pattern


702


. Compared with the case where the stripe direction of a mask pattern is prescribed to be <1-100>, a threading dislocation density in portions immediately above the mask pattern is larger by one to two orders of magnitude. Strains are relaxed in a direction vertical to the stripe of the mask pattern in the same way as in Embodiments 7 and 8.




Next, a second mask pattern


704


is formed on the first GaN film


703


. More specifically, an SiO


2


film having a thickness of about 100 nm is formed by an EB vapor deposition method in the same way as in the first mask pattern


702


. The SiO


2


film is patterned to a periodic stripe (width: about 5 μm; pitch: about 7 μm) by a conventional photolithography method, whereby a second mask pattern


704


is formed. As shown in

FIG. 11A

, the stripe direction of the second mask pattern


704


is prescribed to be <1-100>. Furthermore, the stripe width of the second mask pattern


704


is prescribed to be larger by about 2 μm than that of the first mask pattern


702


.




Then, a second GaN film


705


is grown to a thickness of about 5 μm at a growth temperature of about 1050° C., using TMG and NH


3


as materials, in an MOVPE growth chamber. Thus, the second step is completed. The GaN film


705


is grown uniformly over the entire surface of the wafer.




A threading dislocation density of the entire second GaN film


705


is on the order of 10


5


/cm


2


, which is slightly lower than that of the conventional example. The direction of strains (including thermal strains) caused in the first mask pattern


702


corresponds to the direction in which strains are relaxed in the second mask pattern


704


. Similarly, the direction of strains caused in the second mask pattern


704


corresponds to the direction in which strains are relaxed in the first mask pattern


702


. Thus, in Embodiment 9, there is a larger effect of removing strains, compared with Embodiments 7 and 8. Furthermore, as described above in Embodiment 9, only the first and second steps are conducted. However, a third step may be conducted: a third mask pattern can be formed on the second GaN film


705


so as to cover the portions which cannot be covered with the first and second mask patterns, and a third GaN film can be formed. This can reduce a threading dislocation density from on the order of 10


5


/cm


2


to a threading dislocation density on the order of 10


4


/cm


2


.




In the present embodiment, the stripe directions of these mask patterns are not equivalent. Therefore, equivalent selectivity and an equivalent relaxation function as in Embodiment 7 cannot be expected. However, since the stripe directions of the mask patterns form an angle of about 90°, there is a large effect of strain relaxation.




Embodiment 10




The purpose of Embodiment 10 is to form a thick GaN film on a GaN film having a mask pattern with a growth suppressing effect. In the prior art, a GaN substrate, which has an appropriate size and satisfactory surface morphology intended for production of a nitride semiconductor device, has not been provided. Embodiment 10 provides a crack-free GaN substrate





FIG. 12A

is a cross-sectional view showing a structure of a nitride semiconductor including a thick GaN film produced in Embodiment 10. Reference numeral


800


denotes a nitride semiconductor (e.g., a GaN film) including a substrate produced by conducting n steps, using a method for forming a GaN film described in Embodiments 7 to 9, and an uppermost surface


801


of the nitride semiconductor


800


denotes the n-th nitride semiconductor film (e.g., a GaN film) produced during the n-th step. Reference numeral


802


denotes a thick GaN film produced by an HVPE method. The thick GaN film


802


may be produced by an MOVPE method, instead of the HVPE method. As shown in

FIG. 12A

, the nitride semiconductor structure is composed of the nitride semiconductor


800


including a substrate and the thick GaN film


802


.




In Embodiment 10, the GaN film produced in Embodiment 7 will be exemplified as the nitride semiconductor


800


produced by n steps. The nitride semiconductor


800


including a sapphire substrate produced in Embodiment 7 is set in an HVPE apparatus. Then, in order to grow the thick GaN film


802


, a V-group gas (which is a mixture of a NH


3


gas and a carrier H


2


gas) and a III-group gas (which is obtained by supplying an HCl gas onto Ga metal held in an HVPE apparatus at about 850° C. and mixing a III-group chloride (reaction product of Ga and an HCl gas with a carrier H


2


gas) are respectively supplied to an HVPE growth chamber in which the nitride semiconductor


800


is set. Thus, the thick GaN film


802


is grown to a thickness of about 350 μm. The thick GaN film


802


is grown flat, and observation of the surface thereof with an optical microscope shows that there are no cracks. Thus, a nitride semiconductor structure is formed.




A threading dislocation density of the thick GaN film


802


produced in Embodiment 10 is on the order of 10


3


to 10


4


/cm


2


which is substantially the same or slightly lower than that of the GaN film which is the nitride semiconductor


800


produced in Embodiment 7. The same results as those in Embodiment 7 are obtained with respect to strains.




In Embodiment 10, the uppermost surface


801


of the nitride semiconductor (e.g., GaN film)


800


including a substrate produced during the n-th step is the n-th nitride semiconductor film (e.g., GaN film). However, as shown in

FIG. 12B

, the thick GaN film


802


may be formed directly on the n-th mask pattern


803


. For example, in the case of using the nitride semiconductor


800


produced as in Embodiment 7, the thick GaN film is directly on the third mask pattern, and in the case of using the nitride semiconductor


800


produced as in Embodiment 8 or 9, the thick GaN film is directly on the second mask pattern. Characteristics of these crystals are the same as those in Embodiment 10.




A semiconductor structure including a sapphire substrate produced in Embodiment 10 can also be used as a substrate. Also, the sapphire substrate may be peeled off from the semiconductor structure by grinding or etching, or by utilizing thermal strains, and the remaining structure can be used as a GaN substrate. When such a GaN substrate is used, the thick GaN film


802


may be used as a substrate. Furthermore, a GaN substrate, which is obtained by removing the sapphire substrate and grinding or etching a part of the nitride semiconductor structure, may be used. For example, the n-th nitride semiconductor film which is the uppermost surface can be used as a substrate.




In the prior art, it is difficult to provide a nitride semiconductor substrate having an appropriate size and satisfactory surface morphology intended for device production. However, by removing at least the sapphire substrate from a crystal structure including a nitride semiconductor crystal layer, it becomes possible to provide a nitride semiconductor substrate which satisfies the requirements of device production by simple procedure.




Furthermore, the crystal growth method including the above-mentioned steps has an effect of relaxing strains, in addition to decreasing a threading dislocation density. The strains are caused by a difference in a coefficient of thermal expansion as well as a difference in a lattice constant between the substrate and the nitride semiconductor crystal. For example, it is known that in the case where a thick nitride semiconductor is grown directly on a sapphire substrate, cracks (about 20 μm) are formed during a temperature decrease step at the end of crystal growth due to a difference in a coefficient of thermal expansion. However, by using the above-mentioned crystal growth method of the present invention, a thick nitride semiconductor film can be formed on a sapphire substrate without forming cracks.




Embodiment 11





FIG. 13

shows a structure of a semiconductor laser device produced in Embodiment 11. The elements denoted by reference numerals


600


to


612


shown in

FIG. 13

are the same as those in Embodiment 7.




The semiconductor laser device in the present embodiment includes an n-GaN contact layer


650


, an n-Al


0.1


Ga


0.9


N cladding layer


614


, an n-GaN optical guide layer


615


, a multi quantum-well structure active layer


616


including 5 In


0.2


Ga


0.8


N quantum-well layers and 6 In


0.05


Ga


0.95


N barrier layers, an Al


0.2


Ga


0.8


N evaporation preventing layer


617


, a p-GaN optical guide layer


618


, a p-Al


0.1


Ga


0.9


N cladding layer


619


, a p-GaN contact layer


620


, a p-type electrode


621


, an n-type electrode


622


, and an SiO


2


insulating film


623


.




According to the present invention, the surface of the sapphire substrate


600


may have another orientation, such as an a-plane, an r-plane, and an m-plane. Furthermore, a GaN substrate, an SiC substrate, a spinnel substrate, an MgO substrate, an Si substrate, and a GaAs substrate can be used in place of a sapphire substrate. Particularly in the case of using a GaN substrate, compared with the case of using a sapphire substrate, at least the following advantages are obtained: a difference in a lattice constant between the substrate and a gallium nitride type semiconductor material deposited on the substrate is smaller, and a film with satisfactory crystallinity can be obtained. Furthermore, the GaN substrate is more likely to be cleaved, so that it is easier to produce a laser resonator by cleavage. The cladding layers


614


and


619


maybe made of a mixed crystal containing three elements (AlGaN) having an Al mole fraction other than Al


0.1


Ga


0.9


N. In this case, when an Al mole fraction is increased, a difference in an energy gap and a difference in a refractive index between the active layer and the cladding layer becomes larger, so that carriers and light are confined in the active layer, which further decreases an oscillation threshold current and improves temperature characteristics. Furthermore, when an Al mole fraction is decreased to such a degree that carriers and light can be confined, the mobility of carriers in the cladding layer becomes large. Therefore, the resistance of a semiconductor laser device can be decreased. Furthermore, the cladding layers


614


and


619


may be made of a mixed crystal semiconductor containing a trace amount of another element in addition to the above-mentioned three elements, and the mole fractions of a mixed crystal are not required to be the same between the cladding layer


614


and the cladding layer


619


.




The optical guide layers


615


and


618


may be made of any material which allows an energy gap therebetween to have a value between an energy gap of the quantum-well layers included in the active layer


616


and a energy gap of the cladding layers


614


and


619


. For example, a mixed crystal containing three elements (e.g., InGaN or AlGaN) may be used. Furthermore, it is not necessary to dope a donor or an acceptor over the entire optical guide layers


615


and


618


, and only a portion thereof on the side of the active layer


616


may be non-doped. Furthermore, the entire guide layers


615


and


618


may be non-doped. In this case, there is an advantage in that the number of carriers present in the optical guide layers


615


and


618


becomes small, light absorption by free carriers is decreased, and an oscillation threshold current can be further reduced.




With the quantum-well layers and the barrier layers included in the active layer


616


, mole fractions should be set in accordance with a required laser oscillation wavelength. In the case where it is desirable to make an oscillation wavelength longer, the In mole fraction of the quantum-well layers is increased. In the case where it is desired to shorten an oscillation wavelength, the In mole fraction of the quantum-well layers is decreased. Furthermore, the quantum-well layers and the barrier layers may be made of a mixed crystal semiconductor containing four or more elements including a trace amount of another element in addition to a mixed crystal containing three elements (InGaN). The barrier layers may be made of GaN.




In the present embodiment, the evaporation preventing layer


617


is formed in contact with the active layer


616


. The purpose of this is to prevent In contained in the active layer


616


from evaporating during an increase in growth temperature. Therefore, any material can be used for the evaporation preventing layer


617


as long as it protects the active layer


616


. For example, a mixed crystal containing three elements (AlGaN) having another Al mole fraction and GaN may be used. Furthermore, Mg may be doped into the evaporation preventing layer


617


. In this case, there is an advantage that holes can be easily injected from the optical guide layer


618


and the cladding layer


619


. Furthermore, in the case where the In mole fraction of the quantum-well layers included in the active layer


616


is small, a change in the In mole fraction in the active layer


616


due to evaporation of In is small, so that the evaporation preventing layer


617


is not required to be formed. Even if the evaporation preventing layer


617


is not formed, characteristics of a gallium nitride type semiconductor laser device in the present embodiment will not be impaired.




Hereinafter, a method for producing the above-mentioned gallium nitride type semiconductor laser device will be described with reference to FIG.


13


.




In the following description, the case of using a MOVPE method is shown. However, any method which is capable of epitaxially growing GaN may be used. For example, another crystal growth method such as MBE or HVPE can be used.




First, the contact layer


650


doped with Si is grown to a thickness of about 3 μm at a growth temperature of about 1050° C., using TMG, NH


3


, and SiH


4


as materials, on the substrate produced in Embodiment 7 placed in a predetermined growth chamber. Then, TMA is added to the materials, and the cladding layer


614


doped with Si is grown to a thickness of about 0.4 μm at a growth temperature of about 1050° C. TMA is removed from the materials, and the optical guide layer


615


doped with Si is grown to a thickness of about 0.1 μm at a growth temperature of about 1050° C.




Next, the growth temperature is lowered to about 750° C., and 5 barrier layers (thickness: about 3 nm) and 5 quantum-well layers (thickness: about 2 nm) are alternately grown and the barrier layer (thickness: about 3 nm) is grown, using TMG, NH


3


and TMI, whereby the active layer


616


(total thickness: about 28 nm) is produced. Then, the evaporation preventing layer


617


is grown to a thickness of about 30 nm at a growth temperature of about 750° C., using TMG, TMA, and NH


3


as materials.




Next, the growth temperature is raised to about 1050° C., and the optical guide layer


618


doped with Mg is grown to a thickness of about 0.1 μm, using TMG, NH


3


, and bisethylcyclopentadienyl magnesium (EtCP


2


Mg) as materials. TMA is added to the materials, and the cladding layer


619


doped with Mg is grown to a thickness of about 0.4 μm at a growth temperature of about 1050° C. TMA is removed from the materials, and the contact layer


620


doped with Mg is grown to a thickness of about 0.5 μm at a growth temperature of about 1050° C. Thus, an epitaxial wafer having a gallium nitride type laser device structure is completed. Thereafter, the wafer is annealed in a nitrogen gas atmosphere at about 800° C., whereby the Mg-doped p-type layers are rendered low-resistant.




Furthermore, etching is conducted from the top surface of the contact layer


620


so as to obtain a stripe shape (width: about 200 μm) by using conventional photolithography and dry etching until the contact layer


650


is exposed, whereby amesa structure is produced. Next, using the photolithography and dry etching similar to the above, the remaining contact layer


620


and the cladding layer


619


are etched. At this time, a stripe-shaped ridge structure should be positioned about 3 μm or more away from both ends of the mesa structure with a width of about 200 μm. In the present embodiment, the ridge structure is formed about 10 μm away from the end of the mesa structure on the side where the n-type electrode


622


is to be formed. If the ridge structure is positioned so as to be close to the n-type electrode


622


as described above, the electric resistance of a device is decreased, and the working voltage is reduced. Furthermore, the dry etching is stopped so as not to etch the active layer


616


. Thus, the active layer


616


is protected from etching damage, which prevents a decrease in reliability and an increase in an oscillation threshold current.




The insulating film


623


is formed to a thickness of about 200 nm as a current blocking layer on the side surfaces of the ridge structure and on the surface of the p-type layer excluding the ridge. The p-type electrode


621


made of nickel and gold is formed on the surface of the insulating layer


623


and the contact layer


620


, and the n-type electrode


622


made of titanium and aluminum is formed on the surface of the contact layer


650


exposed by etching. Thus, a gallium nitride type laser device wafer is completed.




Thereafter, the wafer thus obtained is cleaved in a direction vertical to the ridge stripe to form a resonance plane, and the wafer is divided into chips. Each chip is mounted on a stem, and each electrode is connected to each lead terminal by wire bonding. Thus, a gallium nitride type semiconductor laser device is completed.




In the semiconductor laser device produced as described above, satisfactory laser characteristics (oscillation wavelength: about 410 nm; oscillation threshold value: about 50 mA) are obtained. Furthermore, due to a decrease in crystal defects, the semiconductor laser device thus obtained is highly reliable (about 900 hours at about 60° C.). Furthermore, a ratio of laser devices having crystal defects is remarkably decreased, with a yield being about 80% or higher.




In the present embodiment, thicknesses of each quantum-well layer and each barrier layer included in the active layer


616


are about 2 nm and about 3 nm, respectively. However, as long as the thickness of each quantum-well layer and each barrier layer is prescribed to be about 10 nm or less, the same effects can be obtained irrespective of embodiments. Furthermore, the number of quantum-well layers in the active layer


616


may be 3 or 4. Alternatively, a single quantum-well structure active layer may be used.




In the present embodiment, sapphire, which is an insulator, is used for the substrate, so that the n-type electrode


622


is formed on the surface of the contact layer


650


exposed by etching. However, if GaN, SiC, Si, GaAs, or the like having an n-type conductivity is used, the n-type electrode


622


may be formed on the reverse surface of the substrate. In this case, the mesa structure with a width of about 200 μm should be positioned at least about 3 μm away from both ends of the semiconductor laser device chip. P-type structures and n-type structures may be reversed.




Furthermore, GaN used in the crystal growth method of the present invention can also be applied to a power device dealing with a large current (i.e., a device in the field of hard electronics such as a GaN FET device and an AlGaN/GaN HEMT device). In the case where a nitride semiconductor is applied to a power device, thermal strains caused by heat generation due to a large current are combined with strains present in the device, which has an adverse effect to reliability of the device. Therefore, in particular, the crystal growth method of the present invention is advantageous.




As described above, in a semiconductor substrate including a gallium nitride crystal layer produced according to the present invention, a film made of a growth suppressing material and a nitride semiconductor film are formed on different surfaces, using a reverse mask pattern, so that growth of a threading dislocation is prevented. Thus, a crystal having very small crystal defect density (about 10


4


/cm


2


or less) is obtained. A gallium nitride semiconductor laser device using such a crystal can be produced with highly reliability and good yield at a low production cost.




Alternatively, in a semiconductor substrate including a gallium nitride crystal layer produced according to the present invention, films made of a growth suppressing material and nitride semiconductor films are alternately formed. Thus, a crystal with little strains and a very small threading dislocation density (about 10


4


/cm


2


or less) is obtained. A gallium nitride semiconductor laser using such a crystal can also be produced with high reliability and good yield.




Various other modifications will be apparent to and can be readily made by those skilled in the art without departing from the scope and spirit of this invention. Accordingly, it is not intended that the scope of the claims appended hereto be limited to the description as set forth herein, but rather that the claims be broadly construed.



Claims
  • 1. A method for producing a semiconductor substrate, comprising the steps:forming a first patterned mask containing a material having a growth suppressing effect on a lower substrate; growing a semiconductor crystal on the lower substrate via the first patterned mask to form a first semiconductor crystal layer; forming a second patterned mask containing a material having a growth suppressing effect on or above the lower substrate, the second patterned mask at least having a surface which is positioned at a level different from a level of a surface of the first patterned mask, with respect to a surface of the lower substrate; and growing a semiconductor crystal on or above the lower substrate via the second patterned mask to form a second semiconductor crystal layer.
  • 2. A method for producing a semiconductor substrate according to claim 1, wherein the second patterned mask is positioned on the first semiconductor crystal layer.
  • 3. A method for producing a semiconductor substrate according to claim 1, wherein the first and second patterned masks are patterned in such a manner that a combination of the first and second patterned masks covers the entire surface of the lower substrate, and an area of the lower substrate covered with the second patterned mask is larger than an area of the lower substrate covered with the first patterned mask.
  • 4. A method for producing a semiconductor substrate according to claim 1, wherein the second patterned mask includes a first portion and a second portion, the first and second portions have different widths in a direction vertical to the surface of the lower substrate, and the step of forming the first semiconductor crystal layer and the step of forming the second semiconductor crystal layer are conducted during the same crystal growth step.
  • 5. A method for producing a semiconductor substrate according to claim 4, wherein the first portion of the second patterned mask is at least partially positioned on the first patterned mask, and the second patterned mask has an L-shape.
  • 6. A method for producing a semiconductor substrate according to claim 5, wherein the first portion of the second patterned mask is at least partially positioned on the lower substrate, and the second patterned mask has a T-shape.
  • 7. A method for producing a semiconductor substrate according to claim 1, wherein a growth direction of the second semiconductor crystal layer is at least partially different from a growth direction of the first semiconductor crystal layer.
  • 8. A method for producing a semiconductor substrate according to claim 1, wherein the first semiconductor crystal layer is formed in the vicinity of openings in the first patterned mask, whereby the first semiconductor crystal layer has openings on the lower substrate and the first patterned mask.
  • 9. A method for producing a semiconductor substrate according to claim 1, wherein the lower substrate includes a sapphire substrate and a lower semiconductor crystal layer provided on an upper side of the sapphire substrate in a crystal growth direction.
  • 10. A method for producing a semiconductor substrate according to claim 1, wherein the material having a growth suppressing effect is selected from the group consisting of SiO2 and SiNx, and the first and second patterned masks are independently selected from the group consisting of SiO2, SiNx, TiO2 and Al2O3.
  • 11. A method for producing a semiconductor substrate according to claim 1, wherein the first and second semiconductor crystal layers are selected from the group consisting of GaN, InGaN, and AlGaN.
  • 12. A method for producing a semiconductor substrate, comprising the steps of:forming an n-th patterned mask containing a material having a growth suppressing effect on or above a lower substrate, wherein n is an integer of 1 or more; growing a nitride semiconductor crystal on or above the lower substrate via the n-th patterned mask to form an n-th nitride semiconductor crystal layer; forming an (n+1)-th patterned mask containing a material having a growth suppressing effect on or above the lower substrate, the (n+1)-th patterned mask at least having a surface which is positioned at a level different from a level of a surface of the n-th patterned mask, with respect to a surface of the lower substrate; and growing a nitride semiconductor crystal on or above the lower substrate via the (n+1)-th patterned mask to form an (n+1)-th nitride semiconductor crystal layer.
  • 13. A method for producing a semiconductor substrate according to claim 12, wherein the first to (n+1)-th patterned masks are patterned in such a manner that a combination of the first to(n+1)-th patterned masks covers the entire surface of the lower substrate.
  • 14. A method for producing a semiconductor substrate according to claim 12, wherein the n-th patterned mask and the (n+1)-th patterned mask are respectively patterned in a stripe shape, and a direction of the stripe of the n-th patterned mask is twisted from a direction of the stripe of the (n+1)-th patterned mask.
  • 15. A method for producing a semiconductor substrate according to claim 14, wherein the direction of the stripe of the n-th patterned mask and the direction of the stripe of the (n+1)-th patterned mask have an angle difference of about 120°.
  • 16. A method for producing a semiconductor substrate according to claim 14, wherein the direction of the stripe of the n-th patterned mask and the direction of the stripe of the (n+1)-th patterned mask have an angle difference of about 90°.
  • 17. A method for producing a semiconductor substrate according to claim 14, wherein a width of the stripe of the (n+1)-th patterned mask is equal to or larger than a width of the stripe of the n-th patterned mask.
  • 18. A method for producing a semiconductor substrate according to claim 12, wherein the material having a growth suppressing effect is made of SiO2 or SiNx, and the first to (n+1)-th patterned masks are independently made of SiO2, SiNx, TiO2 and Al2O3.
  • 19. A method for producing a semiconductor substrate according to claim 14, wherein the lower substrate includes at least a lower nitride semiconductor crystal layer provided on an upper surface of the lower substrate, and a direction of the stripe of the n-th patterned mask is equal to a <1-100> direction or a <11-20> direction of a crystal of the nitride semiconductor crystal layer.
  • 20. A method for producing a semiconductor substrate according to claim 14, wherein the lower substrate includes at least a lower nitride semiconductor crystal layer provided on an upper side of the lower substrate in a crystal growth direction, the semiconductor substrate includes the first, second and third nitride semiconductor crystal layers, and a combination of directions of the first, second and third patterned masks consists of a combination of [1-100], [10—10], and [01-10] directions of a crystal of the nitride semiconductor crystal.
  • 21. A method for producing a semiconductor substrate according to claim 12, wherein the n-th nitride semiconductor crystal layer is made of AlxInyGazN (where x+y+z=1, 0≦x≦1, 0≦y≦1, and 0≦z≦1).
  • 22. A method for producing a semiconductor substrate according to claim 12, wherein the n-th nitride semiconductor crystal layer or the (n+1)-th nitride semiconductor crystal layer has a thickness of about 5 μm or more.
  • 23. A method for producing a semiconductor substrate according to claim 12, wherein the lower substrate includes a substrate body and a lower nitride semiconductor crystal layer provided on an upper side of the substrate body in a crystal growth direction,the method further comprising the step of removing at least the substrate body from a crystal structure including the (n+1)-th nitride semiconductor crystal layer after the step of forming the (n+1)-th nitride semiconductor crystal layer.
  • 24. A method for producing a semiconductor substrate, comprising the steps of:forming a first patterned mask containing a material having a growth suppressing effect on a lower substrate; growing a semiconductor crystal on the lower substrate via the first patterned mask to form a first semiconductor crystal layer; forming a second patterned mask containing a material having a growth suppressing effect on or above the lower substrate, the second patterned mask at least having a surface which is positioned at a level different from a level of a surface of the first patterned mask, with respect to a surface of the lower substrate; and growing a semiconductor crystal on or above the lower substrate via the second patterned mask to form a second semiconductor crystal layer, wherein the second patterned mask is formed in a position with respect to a position of the first patterned mask so that the second semiconductor crystal layer has a lower defect density than the first semiconductor crystal layer.
  • 25. A method for producing a semiconductor substrate, comprising the steps of:forming an n-th patterned mask containing a material having a growth suppressing effect on or above a lower substrate, wherein n is an integer of 1 or more; growing a semiconductor crystal on or above the lower substrate via the n-th patterned mask to form an n-th semiconductor crystal layer; forming an (n+1)-th patterned mask at least having a surface which is positioned at a level different from a level of a surface of the n-th patterned mask, with respect to a surface of the lower substrate; and growing a semiconductor crystal on or above the lower substrate via the (n+1)-th patterned mask to form an (n+1)-th semiconductor crystal layer; whereby the (n+1)-th patterned mask is formed in a position with respect to a position of the n-th patterned mask so that the (n+1)-th semiconductor crystal layer has a lower defect density than the n-th semiconductor crystal layer.
  • 26. A method according to claim 1, wherein the second semiconductor crystal layer is prescribed to have a defect density of less than about 105/cm2.
  • 27. A method according to claim 12, wherein the (n+1)-th semiconductor crystal layer is prescribed to have a defect density of less than about 105/cm2.
  • 28. A method according to claim 2, wherein the second mask is formed so as to cover openings of the first mask.
  • 29. A method according to claim 1, wherein a stripe width of the second mask is smaller than each opening of the first mask.
  • 30. A method according to claim 1, wherein the first and second masks are formed of the same material.
  • 31. A method according to claim 12, wherein the n-th, and (n+1)-th are formed of the same material.
  • 32. A method according to claim 12, wherein the thickness of the n-th and (n+1)-th masks are the same as each other.
  • 33. A method according to claim 12, wherein the lower substrate is GaN.
Priority Claims (2)
Number Date Country Kind
10-098841 Apr 1998 JP
10-183468 Jun 1998 JP
US Referenced Citations (2)
Number Name Date Kind
4999314 Pribat et al. Mar 1991
5362682 Bozler et al. Nov 1994
Non-Patent Literature Citations (4)
Entry
Usui, A. et al., “Thick GaN epitaxial growth with low dislocation density by hydride vapor phase epitaxy”, Jpn. J. Appl. Phys. vol. 36 Part 2 No. 7B pp. L899-L992, Jul. 1997.*
Sunakawa et al. “Thick GaN crystal growth with low defect density by hydride vapor phase epitaxy” Ext. Abstract. (The 58th Autumn Meeting) J. Soc. of Appl. Phys. (1997) No. 1 266 2p-Q-15. English language translation included herein.
Tanaka et al. “Reduced dislocation densities in selectivity-grown nitride materials” Ext. Abstract. (The 58th Autumn Meeting) J. Soc. of Appl. Phys. (1997) No. 1 265 2p-Q-14. English language translation included herein.
Usui et al. “Thick GaN epitaxial growth with Low dislocation density by hydride vapor phase epitaxy” 1997) Jpn. J. Appl. Phys. 36:(2), No. 7B L899-L902.