This invention is directed to optical devices and related methods. More particularly, the present invention provides a method and device for emitting electromagnetic radiation using nonpolar gallium containing substrates such as GaN, MN, InN, InGaN, AlGaN, and AlInGaN, and others. Merely by way of example, the invention can be applied to optical devices, lasers, light emitting diodes, solar cells, photoelectrochemical water splitting and hydrogen generation, photodetectors, integrated circuits, and transistors, among other devices.
In the late 1800's, Thomas Edison invented the light bulb. The conventional light bulb, commonly called the “Edison bulb,” has been used for over one hundred years for a variety of applications including lighting and displays. The conventional light bulb uses a tungsten filament enclosed in a glass bulb sealed in a base, which is screwed into a socket. The socket is coupled to an AC power or DC power source. The conventional light bulb can be found commonly in houses, buildings, and outdoor lightings, and other areas requiring light or displays. Unfortunately, drawbacks exist with the conventional Edison light bulb:
In 1960, the laser was first demonstrated by Theodore H. Maiman at Hughes Research Laboratories in Malibu. This laser utilized a solid-state flashlamp-pumped synthetic ruby crystal to produce red laser light at 694 nm. By 1964, blue and green laser output was demonstrated by William Bridges at Hughes Aircraft utilizing a gas laser design called an Argon ion laser. The Ar-ion laser utilized a noble gas as the active medium and produce laser light output in the UV, blue, and green wavelengths including 351 nm, 454.6 nm, 457.9 nm, 465.8 nm, 476.5 nm, 488.0 nm, 496.5 nm, 501.7 nm, 514.5 nm, and 528.7 nm. The Ar-ion laser had the benefit of producing highly directional and focusable light with a narrow spectral output, but the efficiency, size, weight, and cost of the lasers were undesirable.
As laser technology evolved, more efficient lamp pumped solid state laser designs were developed for the red and infrared wavelengths, but these technologies remained a challenge for blue and green lasers and blue lasers. As a result, lamp pumped solid state lasers were developed in the infrared, and the output wavelength was converted to the visible using specialty crystals with nonlinear optical properties. A green lamp pumped solid state lasers had 3 stages: electricity powers lamp, lamp excites gain crystal which lases at 1064 nm, 1064 nm goes into frequency conversion crystal which converts to visible 532 nm. The resulting green and blue lasers were called “lamp pumped solid state lasers with second harmonic generation” (LPSS with SHG) and were more efficient than Ar-ion gas lasers, but were still too inefficient, large, expensive, fragile for broad deployment outside of specialty scientific and medical applications. Additionally, the gain crystal used in the solid state lasers typically had energy storage properties which made the lasers difficult to modulate at high speeds, thereby limiting broader deployment.
To improve the efficiency of these visible lasers, high power diode (or semiconductor) lasers were utilized. These “diode pumped solid state lasers with SHG” (DPSS with SHG) had 3 stages: electricity powers 808 nm diode laser, 808 nm excites gain crystal which lases at 1064 nm, 1064 nm goes into frequency conversion crystal which converts to visible 532 nm. The DPSS laser technology extended the life and improved the efficiency of the LPSS lasers, and further commercialization ensue into more high end specialty industrial, medical, and scientific applications. The change to diode pumping, however, increased the system cost and required précised temperature controls, leaving the laser with substantial size and power consumption. Yet the technology did not address the energy storage properties, making the lasers difficult to modulate at high speeds.
As high power laser diodes evolved and new specialty SHG crystals were developed, it became possible to directly convert the output of the infrared diode laser to produce blue and green laser light output. These “directly doubled diode lasers” or SHG diode lasers had 2 stages: electricity powers 1064 nm semiconductor laser, 1064 nm goes into frequency conversion crystal which converts to visible 532 nm green light. These lasers designs are meant to improve the efficiency, cost and size compared to DPSS-SHG lasers, but the specialty diodes and crystals required make this challenging. Additionally, while the diode-SHG lasers have the benefit of being directly modulated, they suffer from severe sensitivity to temperature, limiting their application.
This invention provides techniques related generally to optical devices. More particularly, the invention provides a method and device for emitting electromagnetic radiation using nonpolar or semipolar gallium containing substrates such as GaN, MN, InN, InGaN, AlGaN, and AlInGaN, and others. In specific embodiments, the electromagnetic radiation has wavelengths of 405, 450, 485, 500, 520, nanometers. The invention can be applied to optical devices, lasers, light emitting diodes, solar cells, photoelectrochemical water splitting and hydrogen generation, photodetectors, integrated circuits, and transistors, among other devices.
In a specific embodiment, an optical device is provided which includes a gallium nitride substrate member having an m-plane nonpolar crystalline surface region characterized by an orientation of about −2 degrees to about 2 degrees towards (000-1) and less than about 0.5 degrees towards (11-20). The crystalline surface can be characterized as a miscut and does not include a cut orientation of zero degrees. The device also has a laser stripe region formed overlying a portion of the m-plane nonpolar crystalline orientation surface region. In a preferred embodiment, the laser stripe region is characterized by a cavity orientation that is substantially parallel to the c-direction, the laser strip region having a first end and a second end. The device includes a first cleaved c-face facet provided on the first end of the laser stripe region. The first cleaved c-face facet preferably includes a laser scribed region. The device also has a second cleaved c-face facet provided on the second end of the laser stripe region. In a specific embodiment, the second cleaved c-face facet is also characterized by including a laser scribed region.
In some embodiments, the optical device includes a gallium nitride substrate member having an m-plane nonpolar crystalline surface region characterized by an orientation of about −17 degrees to about 17 degrees towards a c-plane. The crystalline surface can be characterized as a miscut and does not include a cut orientation of zero degrees. The device also has a laser stripe region formed overlying a portion of the m-plane nonpolar crystalline orientation surface region or alternatively the semi-polar crystalline orientation surface region. In a preferred embodiment, the laser stripe region has a first end and a second end. The device includes a first cleaved face facet provided on the first end of the laser stripe region. In a specific embodiment, the first cleaved face facet is characterized by a laser scribed region. The device also has a second cleaved face facet provided on the second end of the laser stripe region. In a specific embodiment, the second cleaved face facet is characterized by a laser scribed region.
In an alternative specific embodiment, the present invention provides a method for forming an optical device. The method includes providing a gallium nitride substrate member having an m-plane nonpolar crystalline surface region characterized by an orientation of about −2 degrees to about 2 degrees towards (000-1) and less than about 0.5 degrees towards (11-20). In a specific embodiment, the crystalline surface can be characterized as a miscut and does not include a cut orientation of zero degrees. The device also has a laser stripe region formed overlying a portion of the m-plane nonpolar crystalline orientation surface region. The method includes forming a laser stripe region overlying a portion of the m-plane nonpolar crystalline orientation surface region. In a specific embodiment, the laser stripe region is characterized by a cavity orientation substantially parallel to the c-direction. In a specific embodiment, the laser strip region has a first end and a second end. The method preferably forms a pair of cleaved facets including a first cleaved c-face facet provided on the first end of the laser stripe region and a second cleaved c-face facet provided on the second end of the laser stripe region.
In other embodiments, the present invention includes a device and method configured on other gallium and nitrogen containing substrate orientations. In a specific embodiment, the gallium and nitrogen containing substrate is configured on a family of planes including a {20-21} crystal orientation. In a specific embodiment, {20-21} is 14.9 degrees off of the m-plane towards the c-plane (0001). As an example, the miscut or off-cut angle is +/−17 degrees from the m-plane towards c-plane or alternatively at about the {20-21} crystal orientation plane. As another example, the present device includes a laser stripe oriented in a projection of the c-direction, which is perpendicular to the a-direction (or alternatively on the m-plane, it is configured in the c-direction). In one or more embodiments, the cleaved facet would be the gallium and nitrogen containing face (e.g., GaN face) that is +/−5 degrees from a direction orthogonal to the projection of the c-direction (or alternatively, for the m-plane laser, it is the c-face). Of course, there can be other variations, modifications, and alternatives.
In yet other embodiments, the present invention provides a laser diode device. The laser diode device is provided on a crystal plane that is oriented between −8 degrees and 8 degrees from {20-21} towards the c-plane according to one or more embodiments. In one or more embodiments, the surface orientation of the crystal plane can be miscut from +/−5 degrees towards the a-plane. In a specific embodiment, the laser cavity is oriented in the projection of the c-direction and also uses cleaved facet mirrors. Depending upon the embodiment, the laser diode is operable in the 390-410 nm, 410-430 nm, 430-450 nm, 450-480 nm, 480-510 nm, 510-540 nm, 540-600 nm range, and other ranges. In other embodiments, the present method and structure can also be applied to light emitting diode devices, commonly known as LEDs or the like. Of course, there can be other variations, modifications, and alternatives.
Benefits are achieved over pre-existing techniques using the present invention. In particular, the present invention enables a cost-effective optical device for laser applications. In a specific embodiment, the present optical device can be manufactured in a relatively simple and cost effective manner. Depending upon the embodiment, the present apparatus and method can be manufactured using conventional materials and/or methods according to one of ordinary skill in the art. The present laser device uses a nonpolar gallium nitride material capable of achieve a laser having a wavelength of about 400 nanometers and 405 nanometers can greater, among others. In other embodiments, the device and method can achieve a wavelength of about 500 nanometers and greater including 520 nanometers. Depending upon the embodiment, one or more of these benefits may be achieved. These and other benefits may be described throughout the present specification and more particularly below.
The present invention achieves these benefits and others in the context of known process technology. However, a further understanding of the nature and advantages of the present invention may be realized by reference to the latter portions of the specification and attached drawings.
According to the present invention, techniques related generally to optical devices are provided. More particularly, the present invention provides a method and device for emitting electromagnetic radiation using non-polar or semipolar gallium containing substrates such as GaN, MN, InN, InGaN, AlGaN, and AlInGaN, and others. Merely by way of example, the invention can be applied to optical devices, lasers, light emitting diodes, solar cells, photoelectrochemical water splitting and hydrogen generation, photodetectors, integrated circuits, and transistors, among other devices.
In a specific embodiment, the device has a laser stripe region formed overlying a portion of the nonpolar crystalline orientation surface region. In a specific embodiment, the laser stripe region is characterized by a cavity orientation is substantially parallel to the c-direction. In a specific embodiment, the laser strip region has a first end 107 and a second end 109.
In a preferred embodiment, the device has a first cleaved c-face facet provided on the first end of the laser stripe region and a second cleaved c-face facet provided on the second end of the laser stripe region. In one or more embodiments, the first cleaved c-facet is substantially parallel with the second cleaved c-facet. Mirror surfaces are formed on each of the cleaved surfaces. The first cleaved c-facet comprises a first mirror surface. In a preferred embodiment, the first mirror surface is provided by a scribing and breaking process. The scribing process can use any suitable techniques, such as a diamond scribe or laser scribe or combinations. In a specific embodiment, the first mirror surface comprises a reflective coating. The reflective coating is selected from silicon dioxide, hafnia, and titaniatantalum pentoxidezirconia, including combinations, and the like. Depending upon the embodiment, the first mirror surface can also comprise an anti-reflective coating. Of course, there can be other variations, modifications, and alternatives.
Also in a preferred embodiment, the second cleaved c-facet comprises a second mirror surface. The second mirror surface is provided by a scribing and breaking process according to a specific embodiment. Preferably, the scribing is diamond scribed or laser scribed or the like. In a specific embodiment, the second mirror surface comprises a reflective coating, such as silicon dioxide, hafnia, titania, tantalum, pentoxide, zirconia, combinations, and the like. In a specific embodiment, the second mirror surface comprises an anti-reflective coating. Of course, there can be other variations, modifications, and alternatives.
In a specific embodiment, the laser stripe has a length and width. The length ranges from about 50 microns to about 3000 microns. The strip also has a width ranging from about 0.5 microns to about 50 microns, but can be other dimensions. In a specific embodiment, the width is substantially constant in dimension, although there may be slight variations. The width and length are often formed using a masking and etching process, which are commonly used in the art. Further details of the present device can be found throughout the present specification and more particularly below.
In a specific embodiment, the device is also characterized by a spontaneously emitted light is polarized in substantially perpendicular to the c-direction. That is, the device performs as a laser or the like. In a preferred embodiment, the spontaneously emitted light is characterized by a polarization ratio of greater than 0.1 to about 1 perpendicular to the c-direction. In a preferred embodiment, the spontaneously emitted light characterized by a wavelength ranging from about 405 nanometers to yield a blue emission, a green emission, and others. In a preferred embodiment, the spontaneously emitted light is highly polarized and is characterized by a polarization ratio of greater than 0.4. Of course, there can be other variations, modifications, and alternatives. Further details of the laser device can be found throughout the present specification and more particularly below.
In a specific embodiment, the device also has an overlying n-type gallium nitride layer 205, an active region 207, and an overlying p-type gallium nitride layer structured as a laser stripe region 209. In a specific embodiment, each of these regions is formed using at least an epitaxial deposition technique of metal organic chemical vapor deposition (MOCVD), molecular beam epitaxy (MBE), or other epitaxial growth techniques suitable for GaN growth. In a specific embodiment, the epitaxial layer is a high quality epitaxial layer overlying the n-type gallium nitride layer. In some embodiments the high quality layer is doped, for example, with Si or O to form n-type material, with a dopant concentration between about 1016 cm−3 and 1020 cm−3.
In a specific embodiment, an n-type AluInvGa1−u−vN layer, where 0≦u, v, u+v≦1, is deposited on the substrate. In a specific embodiment, the carrier concentration may lie in the range between about 1016 cm−3 and 1020 cm−3. The deposition may be performed using metalorganic chemical vapor deposition (MOCVD) or molecular beam epitaxy (MBE). Of course, there can be other variations, modifications, and alternatives.
As an example, the bulk GaN substrate is placed on a susceptor in an MOCVD reactor. After closing, evacuating, and back-filling the reactor (or using a load lock configuration) to atmospheric pressure, the susceptor is heated to a temperature between about 1000 and about 1200 degrees Celsius in the presence of a nitrogen-containing gas. In one specific embodiment, the susceptor is heated to approximately 1100 degrees Celsius under flowing ammonia. A flow of a gallium-containing metalorganic precursor, such as trimethylgallium (TMG) or triethylgallium (TEG) is initiated, in a carrier gas, at a total rate between approximately 1 and 50 standard cubic centimeters per minute (sccm). The carrier gas may comprise hydrogen, helium, nitrogen, or argon. The ratio of the flow rate of the group V precursor (ammonia) to that of the group III precursor (trimethylgallium, triethylgallium, trimethylindium, trimethylaluminum) during growth is between about 2000 and about 12000. A flow of disilane in a carrier gas, with a total flow rate of between about 0.1 and 10 sccm is initiated.
In a specific embodiment, the laser stripe region is made of the p-type gallium nitride layer 209. In a specific embodiment, the laser stripe is provided by an etching process selected from dry etching or wet etching. In a preferred embodiment, the etching process is dry, but can be others. As an example, the dry etching process is an inductively coupled process using chlorine bearing species or a reactive ion etching process using similar chemistries. Again as an example, the chlorine bearing species are commonly derived from chlorine gas or the like. The device also has an overlying dielectric region, which exposes 213 contact region. In a specific embodiment, the dielectric region is an oxide such as silicon dioxide or silicon nitride, but can be others. The contact region is coupled to an overlying metal layer 215. The overlying metal layer is a multilayered structure containing gold and platinum (Pt/Au), but can be others. Of course, there can be other variations, modifications, and alternatives.
In a specific embodiment, the laser device has active region 207. The active region can include one to twenty quantum well regions according to one or more embodiments. As an example following deposition of the n-type AluInvGa1−u−vN layer for a predetermined period of time, so as to achieve a predetermined thickness, an active layer is deposited. The active layer may comprise a single quantum well or a multiple quantum well, with 1-20 quantum wells. The quantum wells may comprise InGaN wells and GaN barrier layers. In other embodiments, the well layers and barrier layers comprise AlwInxGa1−w−xN and AlyInzGa1−y−zN, respectively, where 0≦w, x, y, z, w+x, y+z≦1, where w<u, y and/or x>v, z so that the bandgap of the well layer(s) is less than that of the barrier layer(s) and the n-type layer. The well layers and barrier layers may each have a thickness between about 1 nm and about 40 nm. In another embodiment, the active layer comprises a double heterostructure, with an InGaN or AlwInxGa1−w−xN layer about 10 nm to 100 nm thick surrounded by GaN or AlyInzGa1−y−zN layers, where w<u, y and/or x>v, z. The composition and structure of the active layer are chosen to provide light emission at a preselected wavelength. The active layer may be left undoped (or unintentionally doped) or may be doped n-type or p-type. Of course, there can be other variations, modifications, and alternatives.
In a specific embodiment, the active region can also include an electron blocking region, and a separate confinement heterostructure. In some embodiments, an electron blocking layer is preferably deposited. The electron-blocking layer may comprise AlsIntGa1−s−tN, where 0≦s, t, s+t≦1, with a higher bandgap than the active layer, and may be doped p-type. In one specific embodiment, the electron blocking layer comprises AlGaN. In another embodiment, the electron blocking layer comprises an AlGaN/GaN super-lattice structure, comprising alternating layers of AlGaN and GaN, each with a thickness between about 0.2 nm and about 5 nm. Of course, there can be other variations, modifications, and alternatives.
As noted, the p-type gallium nitride structure, which can be a p-type doped AlqInrGa1−q−rN, where 0≦q, r, q+r≦1, layer is deposited above the active layer. The p-type layer may be doped with Mg, to a level between about 1016 cm−3 and 1022 cm−3, and may have a thickness between about 5 nm and about 1000 nm. The outermost 1-50 nm of the p-type layer may be doped more heavily than the rest of the layer, so as to enable an improved electrical contact. In a specific embodiment, the laser stripe is provided by an etching process selected from dry etching or wet etching. In a preferred embodiment, the etching process is dry, but can be others. The device also has an overlying dielectric region, which exposes 213 contact region. In a specific embodiment, the dielectric region is an oxide such as silicon dioxide, but can be others. Of course, there can be other variations, modifications, and alternatives.
In a specific embodiment, the metal contact is made of suitable material. The reflective electrical contact may comprise at least one of silver, gold, aluminum, nickel, platinum, rhodium, palladium, chromium, or the like. The electrical contact may be deposited by thermal evaporation, electron beam evaporation, electroplating, sputtering, or another suitable technique. In a preferred embodiment, the electrical contact serves as a p-type electrode for the optical device. In another embodiment, the electrical contact serves as an n-type electrode for the optical device. Of course, there can be other variations, modifications, and alternatives. Further details of the cleaved facets can be found throughout the present specification and more particularly below.
A method of processing a laser device according to one or more embodiments may be outline as follows, see also
The above sequence of steps is used to form individual laser devices on a die from a substrate structure according to one or more embodiments of the present invention. In one or more preferred embodiments, the method includes cleaved facets substantially parallel to each other and facing each other in a ridge laser device configured on a non-polar gallium nitride substrate material. Depending upon the embodiment, one or more of these steps can be combined, or removed, or other steps may be added without departing from the scope of the claims herein. One of ordinary skill in the art would recognize other variations, modifications, and alternatives. Further details of this method are provided throughout the present specification and more particularly below.
In a specific embodiment, the carrier wafer is mounted to a lapping jig. An example of such lapping jig is made by Logitech Ltd. of the United Kingdom, or other vendor. The lapping jig helps maintain planarity of the substrates during the lapping process according to a specific embodiment. As an example, the starting thickness of the substrates are ˜325 um+/−20 um, but can be others. In a specific embodiment, the method laps or thins the substrates down to 70-80 um thickness, but can also be thinner or slightly thicker. In a preferred embodiment, the lapping jig is configured with a lapping plate, which is often made of a suitable material such as cast iron configured with a flatness of less than 5 um, but can be others. Preferably, the method uses a lapping slurry that is 1 part silicon carbide (SiC) and 10 parts water, but can also be other variations. In a specific embodiment, the SiC grit is about 5 um in dimension. In one or more embodiments, the lapping plate speed is suitable at about 10 revolutions per minute. Additionally, the method can adjust the lapping jig's down pressure to achieve a desired lapping rate, such as 2-3 um/min or greater or slightly less according to one or more embodiments.
In a specific embodiment, the present method includes a lapping process that may produce subsurface damage in the GaN material to cause generation of mid level traps or the like. The midlevel traps may lead to contacts having a Schottky characteristic. Accordingly, the present method includes one or more polishing processes such that ˜10 um of material having the damage is removed according to a specific embodiment. As an example, the method uses a Politex™ polishing pad of Rohm and Haas, but can be others, that is glued onto a stainless steel plate. A polishing solution is Ultraso1300 K manufactured by Eminess Technologies, but can be others. The Ultra-Sol 300 K is a high-purity colloidal silica slurry with a specially designed alkaline dispersion. It contains 70 nm colloidal silica and has a pH of 10.6. The solids content is 30% (by weight). In a specific embodiment, the lapping plate speed is 70 rpm and the full weight of the lapping jig is applied. In a preferred embodiment, the method includes a polishing rate of about ˜2 um/hour, but can be others. Of course, there can be other variations, modifications, and alternatives.
In other embodiments, the present invention provides a method for achieving high quality n-type contacts for m-plane GaN substrate material. In a specific embodiment, the method provides contacts that are rough to achieve suitable ohmic contact. In a specific embodiment, the roughness causes exposure of other crystal planes, which lead to good contacts. In a preferred embodiment, the present method includes a lapped surface, which is rough in texture to expose more than one or multiple different crystal planes. In other embodiments, lapping may be followed by etching such as dry etching and/or wet etching. In a specific embodiment, etching removes the subsurface damage, however, it is likely not to planarize the surface like polishing. Of course, there can be other variations, modifications, and alternatives.
As an example, the backside contact includes about 300 Å Al/3000 Å Au or other suitable materials. In a specific embodiment, the contact is a stack of metals that are deposited by e-beam evaporation or other suitable techniques. In a preferred embodiment and prior to the metal stack deposition, the method includes use of a wet etch such as an hydrofluoric acid wet etch to remove any oxides on the surface. In a specific embodiment, the metal stack is preferably not annealed or subjected to high temperature processing after its formation. Of course, there can be other variations, modifications, and alternatives.
Next, the method includes one or more scribing processes. In a specific embodiment, the method includes subjecting the substrates to a laser for pattern formation. In a preferred embodiment, the pattern is configured for the formation of a pair of facets for one or more ridge lasers. In a preferred embodiment, the pair of facets face each other and are in parallel alignment with each other. In a preferred embodiment, the method uses a UV (355 nm) laser to scribe the laser bars. In a specific embodiment, the laser is configured on a system, which allows for accurate scribe lines configured in one or more different patterns and profiles. In one or more embodiments, the scribing can be performed on the backside, frontside, or both depending upon the application. Of course, there can be other variations, modifications, and alternatives.
In a specific embodiment, the method uses backside scribing or the like. With backside scribing, the method preferably forms a continuous line scribe that is perpendicular to the laser bars on the backside of the GaN substrate. In a specific embodiment, the scribe is generally 15-20 um deep or other suitable depth. Preferably, backside scribing can be advantageous. That is, the scribe process does not depend on the pitch of the laser bars or other like pattern. Accordingly, backside scribing can lead to a higher density of laser bars on each substrate according to a preferred embodiment. In a specific embodiment, backside scribing, however, may lead to residue from the tape on one or more of the facets. In a specific embodiment, backside scribe often requires that the substrates face down on the tape. With frontside scribing, the backside of the substrate is in contact with the tape. Of course, there can be other variations, modifications, and alternatives.
In a preferred embodiment, the present method uses frontside scribing, which facilitates formation of clean facets. In a specific embodiment, the frontside scribing process is preferably used. In a specific embodiment, the method includes a scribe pattern to produce straight cleaves with minimal facet roughness or other imperfections. Further details of scribing are provided below.
Scribe Pattern: The pitch of the laser mask is about 200 um, but can be others. The method uses a 170 um scribe with a 30 um dash for the 200 um pitch. In a preferred embodiment, the scribe length is maximized or increased while maintaining the heat affected zone of the laser away from the laser ridge, which is sensitive to heat.
Scribe Profile: A saw tooth profile generally produces minimal facet roughness. It is believed that the saw tooth profile shape creates a very high stress concentration in the material, which causes the cleave to propogate much easier and/or more efficiently.
In a specific embodiment, the present method provides for a scribe suitable for fabrication of the present laser devices. As an example,
Referring now to
In a preferred embodiment, the method uses a suitable deposition system configured for deposition of each of the facets without breaking vacuum. The deposition system includes a dome structure with sufficient height and spatial volume. The system allows for the plurality of bars configured in a fixture to be flipped from one side to another side and to expose the back facet and the front facet according to a specific embodiment. In a preferred embodiment, the method allows for first deposition of the back facet, reconfiguring the bar fixture to expose the front facet, and second deposition of the front facet without breaking vacuum. In a preferred embodiment, the method allows for deposition of one or more films on front and back without breaking vacuum to save time and improve efficiency. Other embodiments can break vacuum. Of course, there can be other variations, modifications, and alternatives.
The device has a laser stripe region formed overlying a portion of the nonpolar crystalline orientation surface region. The laser stripe region is characterized by a cavity orientation is substantially parallel to the c-direction and has a first end and a second end. The device has a first cleaved c-face facet provided on the first end of the laser stripe region and a second cleaved c-face facet provided on the second end of the laser stripe region. The first cleaved c-facet is substantially parallel with the second cleaved c-facet. Mirror surfaces are formed on each of the cleaved surfaces. The first cleaved c-facet comprises a first mirror surface. The first mirror surface is provided by a scribing and breaking process such as the one described herein. The first mirror surface comprises a reflective coating, which is alumina and hafnia. The second cleaved c-facet comprises a second mirror surface. The second mirror surface is provided by a scribing and breaking process such as the one described herein. The second mirror surface comprises a reflective coating, such as silicon dioxide and hafnia. In a specific embodiment, the laser stripe has a length and width. The length is 400-1000 μm and the width is 1.4-4 μm. The width is substantially constant in dimension.
As shown, the device is also characterized by a spontaneously emitted light is polarized in substantially perpendicular to the c-direction. That is, the device performs as a laser. The spontaneously emitted light is characterized by a polarization ratio perpendicular to the c-direction. As also shown, the spontaneously emitted light characterized by a wavelength of about 405 nanometers to yield blue-violet emission. Other parameters included:
PowerCW>350 mW;
Ith<35 mA;
SE>1.0 W/A; and
Packaged on To-56 Header.
As shown, the graph illustrates a power and current relationship for the subject laser device at about 25 Degrees Celsius. Additionally, the wavelength is indicated at about 405 nanometers for the subject laser device. Again, the present device is merely an illustration and should not unduly limit the scope of the claims herein. One of ordinary skill in the art would recognize other variations, modifications, and alternatives.
In other embodiments, the present invention includes a device and method configured on other gallium and nitrogen containing substrate orientations. In a specific embodiment, the gallium and nitrogen containing substrate is configured on a family of planes including a {20-21} crystal orientation. In a specific embodiment, {20-21} is 14.9 degrees off of the m-plane towards the c-plane (0001). As an example, the miscut or off-cut angle is +/−17 degrees from the m-plane towards c-plane or alternatively at about the {20-21} crystal orientation plane. As another example, the present device includes a laser stripe oriented in a projection of the c-direction, which is perpendicular to the a-direction (or alternatively on the m-plane, it is configured in the c-direction). In one or more embodiments, the cleaved facet would be the gallium and nitrogen containing face (e.g., GaN face) that is +/−5 degrees from a direction orthogonal to the projection of the c-direction (or alternatively, for the m-plane laser, it is the c-face). Of course, there can be other variations, modifications, and alternatives.
While the above is a full description of the specific embodiments, various modifications, alternative constructions and equivalents may be used. Therefore, the above description and illustrations should not be taken as limiting the scope of the present invention which is defined by the appended claims.
This application claims priority to U.S. Ser. No. 61/168,926 filed Apr. 13, 2009, and U.S. Ser. No. 61/243,502 filed Sep. 17, 2009, each of which is commonly assigned and hereby incorporated by reference.
Number | Name | Date | Kind |
---|---|---|---|
4318058 | Mito et al. | Mar 1982 | A |
4341592 | Shortes et al. | Jul 1982 | A |
4860687 | Frijlink | Aug 1989 | A |
4911102 | Manabe et al. | Mar 1990 | A |
5331654 | Jewell et al. | Jul 1994 | A |
5334277 | Nakamura | Aug 1994 | A |
5366953 | Char et al. | Nov 1994 | A |
5527417 | Lida et al. | Jun 1996 | A |
5607899 | Yoshida et al. | Mar 1997 | A |
5632812 | Hirabayashi | May 1997 | A |
5647945 | Matsuse et al. | Jul 1997 | A |
5696389 | Ishikawa et al. | Dec 1997 | A |
5760484 | Lee et al. | Jun 1998 | A |
5821555 | Saito et al. | Oct 1998 | A |
5888907 | Tomoyasu et al. | Mar 1999 | A |
5926493 | O'Brien et al. | Jul 1999 | A |
5951923 | Horie et al. | Sep 1999 | A |
6069394 | Hashimoto et al. | May 2000 | A |
6072197 | Horino et al. | Jun 2000 | A |
6147953 | Duncan | Nov 2000 | A |
6153010 | Kiyoku et al. | Nov 2000 | A |
6195381 | Botez et al. | Feb 2001 | B1 |
6239454 | Glew et al. | May 2001 | B1 |
6379985 | Cervantes et al. | Apr 2002 | B1 |
6451157 | Hubacek | Sep 2002 | B1 |
6489636 | Goetz et al. | Dec 2002 | B1 |
6586762 | Kozaki | Jul 2003 | B2 |
6635904 | Goetz et al. | Oct 2003 | B2 |
6639925 | Niwa et al. | Oct 2003 | B2 |
6680959 | Tanabe et al. | Jan 2004 | B2 |
6734461 | Shiomi et al. | May 2004 | B1 |
6755932 | Masuda et al. | Jun 2004 | B2 |
6809781 | Setlur et al. | Oct 2004 | B2 |
6814811 | Ose | Nov 2004 | B2 |
6833564 | Shen et al. | Dec 2004 | B2 |
6858081 | Biwa et al. | Feb 2005 | B2 |
6858882 | Tsuda et al. | Feb 2005 | B2 |
6920166 | Akasaka et al. | Jul 2005 | B2 |
7009199 | Hall | Mar 2006 | B2 |
7019325 | Li et al. | Mar 2006 | B2 |
7033858 | Chai et al. | Apr 2006 | B2 |
7053413 | D'Evelyn et al. | May 2006 | B2 |
7063741 | D'Evelyn | Jun 2006 | B2 |
7128849 | Setlur et al. | Oct 2006 | B2 |
7220324 | Baker et al. | May 2007 | B2 |
7303630 | Motoki et al. | Dec 2007 | B2 |
7312156 | Granneman et al. | Dec 2007 | B2 |
7323723 | Ohtsuka et al. | Jan 2008 | B2 |
7338828 | Imer et al. | Mar 2008 | B2 |
7358542 | Radkov et al. | Apr 2008 | B2 |
7358543 | Chua et al. | Apr 2008 | B2 |
7390359 | Miyanaga et al. | Jun 2008 | B2 |
7470555 | Matsumura | Dec 2008 | B2 |
7483466 | Uchida et al. | Jan 2009 | B2 |
7483468 | Tanaka | Jan 2009 | B2 |
7489441 | Scheible et al. | Feb 2009 | B2 |
7491984 | Koike et al. | Feb 2009 | B2 |
7555025 | Yoshida | Jun 2009 | B2 |
7598104 | Teng et al. | Oct 2009 | B2 |
7691658 | Kaeding et al. | Apr 2010 | B2 |
7709284 | Iza et al. | May 2010 | B2 |
7727332 | Habel et al. | Jun 2010 | B2 |
7733571 | Li | Jun 2010 | B1 |
7749326 | Kim et al. | Jul 2010 | B2 |
7806078 | Yoshida | Oct 2010 | B2 |
7858408 | Mueller et al. | Dec 2010 | B2 |
7862761 | Okushima et al. | Jan 2011 | B2 |
7923741 | Zhai et al. | Apr 2011 | B1 |
7939354 | Kyono et al. | May 2011 | B2 |
7968864 | Akita et al. | Jun 2011 | B2 |
7976630 | Poblenz et al. | Jul 2011 | B2 |
8017932 | Okamoto et al. | Sep 2011 | B2 |
8044412 | Murphy et al. | Oct 2011 | B2 |
8124996 | Raring et al. | Feb 2012 | B2 |
8126024 | Raring | Feb 2012 | B1 |
8143148 | Raring et al. | Mar 2012 | B1 |
8242522 | Raring | Aug 2012 | B1 |
8247887 | Raring et al. | Aug 2012 | B1 |
8254425 | Raring | Aug 2012 | B1 |
8259769 | Raring et al. | Sep 2012 | B1 |
8284810 | Sharma et al. | Oct 2012 | B1 |
8294179 | Raring | Oct 2012 | B1 |
8314429 | Raring et al. | Nov 2012 | B1 |
8350273 | Vielemeyer | Jan 2013 | B2 |
8351478 | Raring et al. | Jan 2013 | B2 |
8355418 | Raring et al. | Jan 2013 | B2 |
8416825 | Raring | Apr 2013 | B1 |
8422525 | Raring et al. | Apr 2013 | B1 |
8427590 | Raring et al. | Apr 2013 | B2 |
8451876 | Raring et al. | May 2013 | B1 |
8634442 | Raring et al. | Jan 2014 | B1 |
9356430 | Raring | May 2016 | B2 |
20010048114 | Morita et al. | Dec 2001 | A1 |
20020027933 | Tanabe et al. | Mar 2002 | A1 |
20020050488 | Nikitin et al. | May 2002 | A1 |
20020085603 | Okumura | Jul 2002 | A1 |
20020105986 | Yamasaki | Aug 2002 | A1 |
20020171092 | Goetz et al. | Nov 2002 | A1 |
20030000453 | Unno et al. | Jan 2003 | A1 |
20030001238 | Ban | Jan 2003 | A1 |
20030012243 | Okumura | Jan 2003 | A1 |
20030020087 | Goto et al. | Jan 2003 | A1 |
20030129810 | Barth et al. | Jul 2003 | A1 |
20030140846 | Biwa et al. | Jul 2003 | A1 |
20030178617 | Appenzeller et al. | Sep 2003 | A1 |
20030200931 | Goodwin | Oct 2003 | A1 |
20030216011 | Nakamura et al. | Nov 2003 | A1 |
20040025787 | Selbrede et al. | Feb 2004 | A1 |
20040060518 | Nakamura et al. | Apr 2004 | A1 |
20040099213 | Adomaitis et al. | May 2004 | A1 |
20040104391 | Maeda et al. | Jun 2004 | A1 |
20040146264 | Auner et al. | Jul 2004 | A1 |
20040151222 | Sekine | Aug 2004 | A1 |
20040196877 | Kawakami et al. | Oct 2004 | A1 |
20040222357 | King et al. | Nov 2004 | A1 |
20040233950 | Furukawa et al. | Nov 2004 | A1 |
20040247275 | Vakhshoori et al. | Dec 2004 | A1 |
20040262624 | Akita et al. | Dec 2004 | A1 |
20050040384 | Tanaka et al. | Feb 2005 | A1 |
20050072986 | Sasaoka | Apr 2005 | A1 |
20050168564 | Kawaguchi et al. | Aug 2005 | A1 |
20050214992 | Chakraborty et al. | Sep 2005 | A1 |
20050218413 | Matsumoto et al. | Oct 2005 | A1 |
20050224826 | Keuper et al. | Oct 2005 | A1 |
20050229855 | Raaijmakers | Oct 2005 | A1 |
20050230701 | Huang | Oct 2005 | A1 |
20050247260 | Shin et al. | Nov 2005 | A1 |
20050285128 | Scherer et al. | Dec 2005 | A1 |
20050286591 | Lee | Dec 2005 | A1 |
20060030738 | Vanmaele et al. | Feb 2006 | A1 |
20060033009 | Kobayashi et al. | Feb 2006 | A1 |
20060037529 | D'Evelyn | Feb 2006 | A1 |
20060038193 | Wu et al. | Feb 2006 | A1 |
20060060131 | Atanackovic | Mar 2006 | A1 |
20060066319 | Dallenbach et al. | Mar 2006 | A1 |
20060077795 | Kitahara et al. | Apr 2006 | A1 |
20060078022 | Kozaki et al. | Apr 2006 | A1 |
20060078024 | Matsumura | Apr 2006 | A1 |
20060079082 | Bruhns et al. | Apr 2006 | A1 |
20060086319 | Kasai et al. | Apr 2006 | A1 |
20060118799 | D'Evelyn et al. | Jun 2006 | A1 |
20060126688 | Kneissl | Jun 2006 | A1 |
20060144334 | Yim et al. | Jul 2006 | A1 |
20060175624 | Sharma et al. | Aug 2006 | A1 |
20060189098 | Edmond | Aug 2006 | A1 |
20060193359 | Kuramoto | Aug 2006 | A1 |
20060205199 | Baker et al. | Sep 2006 | A1 |
20060213429 | Motoki et al. | Sep 2006 | A1 |
20060216416 | Sumakeris et al. | Sep 2006 | A1 |
20060256482 | Araki et al. | Nov 2006 | A1 |
20060288928 | Eom et al. | Dec 2006 | A1 |
20070081857 | Yoon | Apr 2007 | A1 |
20070086916 | LeBoeuf et al. | Apr 2007 | A1 |
20070093073 | Farrell, Jr. et al. | Apr 2007 | A1 |
20070101932 | Schowalter et al. | May 2007 | A1 |
20070110112 | Sugiura | May 2007 | A1 |
20070120141 | Moustakas et al. | May 2007 | A1 |
20070153866 | Shchegrov et al. | Jul 2007 | A1 |
20070163490 | Habel et al. | Jul 2007 | A1 |
20070166853 | Guenther et al. | Jul 2007 | A1 |
20070184637 | Haskell et al. | Aug 2007 | A1 |
20070217462 | Yamasaki | Sep 2007 | A1 |
20070242716 | Samal et al. | Oct 2007 | A1 |
20070252164 | Zhong et al. | Nov 2007 | A1 |
20070259464 | Bour et al. | Nov 2007 | A1 |
20070272933 | Kim et al. | Nov 2007 | A1 |
20070280320 | Feezell et al. | Dec 2007 | A1 |
20080029152 | Milshtein et al. | Feb 2008 | A1 |
20080087919 | Tysoe et al. | Apr 2008 | A1 |
20080092812 | McDiarmid et al. | Apr 2008 | A1 |
20080094592 | Shibazaki | Apr 2008 | A1 |
20080095492 | Son et al. | Apr 2008 | A1 |
20080121916 | Teng et al. | May 2008 | A1 |
20080124817 | Bour et al. | May 2008 | A1 |
20080149949 | Nakamura et al. | Jun 2008 | A1 |
20080149959 | Nakamura et al. | Jun 2008 | A1 |
20080164578 | Tanikella et al. | Jul 2008 | A1 |
20080173735 | Mitrovic et al. | Jul 2008 | A1 |
20080191192 | Feezle et al. | Aug 2008 | A1 |
20080191223 | Nakamura et al. | Aug 2008 | A1 |
20080198881 | Farrell et al. | Aug 2008 | A1 |
20080210958 | Senda et al. | Sep 2008 | A1 |
20080217745 | Miyanaga et al. | Sep 2008 | A1 |
20080232416 | Okamoto et al. | Sep 2008 | A1 |
20080251020 | Franken et al. | Oct 2008 | A1 |
20080283851 | Akita | Nov 2008 | A1 |
20080285609 | Ohta et al. | Nov 2008 | A1 |
20080291961 | Kamikawa et al. | Nov 2008 | A1 |
20080298409 | Yamashita et al. | Dec 2008 | A1 |
20080303033 | Brandes | Dec 2008 | A1 |
20080308815 | Kasai et al. | Dec 2008 | A1 |
20080315179 | Kim et al. | Dec 2008 | A1 |
20090021723 | De Lega | Jan 2009 | A1 |
20090058532 | Kikkawa et al. | Mar 2009 | A1 |
20090061857 | Kazmi | Mar 2009 | A1 |
20090066241 | Yokoyama | Mar 2009 | A1 |
20090078944 | Kubota et al. | Mar 2009 | A1 |
20090080857 | St. John-Larkin | Mar 2009 | A1 |
20090081857 | Hanser et al. | Mar 2009 | A1 |
20090081867 | Taguchi et al. | Mar 2009 | A1 |
20090141765 | Kohda et al. | Jun 2009 | A1 |
20090153752 | Silverstein | Jun 2009 | A1 |
20090159869 | Ponce et al. | Jun 2009 | A1 |
20090229519 | Saitoh | Sep 2009 | A1 |
20090250686 | Sato et al. | Oct 2009 | A1 |
20090267100 | Miyake et al. | Oct 2009 | A1 |
20090273005 | Lin | Nov 2009 | A1 |
20090301387 | D'Evelyn | Dec 2009 | A1 |
20090301388 | D'Evelyn | Dec 2009 | A1 |
20090309110 | Raring et al. | Dec 2009 | A1 |
20090309127 | Raring et al. | Dec 2009 | A1 |
20090310640 | Sato et al. | Dec 2009 | A1 |
20090316116 | Melville et al. | Dec 2009 | A1 |
20090320744 | D'Evelyn | Dec 2009 | A1 |
20090321778 | Chen et al. | Dec 2009 | A1 |
20100001300 | Raring et al. | Jan 2010 | A1 |
20100003492 | D'Evelyn | Jan 2010 | A1 |
20100006546 | Young et al. | Jan 2010 | A1 |
20100006873 | Raring et al. | Jan 2010 | A1 |
20100025656 | Raring et al. | Feb 2010 | A1 |
20100031875 | D'Evelyn | Feb 2010 | A1 |
20100044718 | Hanser et al. | Feb 2010 | A1 |
20100096615 | Okamoto et al. | Apr 2010 | A1 |
20100104495 | Kawabata et al. | Apr 2010 | A1 |
20100140630 | Hamaguchi et al. | Jun 2010 | A1 |
20100140745 | Khan et al. | Jun 2010 | A1 |
20100151194 | D'Evelyn | Jun 2010 | A1 |
20100195687 | Okamoto et al. | Aug 2010 | A1 |
20100220262 | DeMille et al. | Sep 2010 | A1 |
20100276663 | Enya et al. | Nov 2010 | A1 |
20100295054 | Okamoto et al. | Nov 2010 | A1 |
20100302464 | Raring | Dec 2010 | A1 |
20100309943 | Chakraborty et al. | Dec 2010 | A1 |
20100316075 | Raring et al. | Dec 2010 | A1 |
20100327291 | Preble et al. | Dec 2010 | A1 |
20110031508 | Hamaguchi et al. | Feb 2011 | A1 |
20110056429 | Raring et al. | Mar 2011 | A1 |
20110057167 | Ueno et al. | Mar 2011 | A1 |
20110064100 | Raring et al. | Mar 2011 | A1 |
20110064101 | Raring et al. | Mar 2011 | A1 |
20110064102 | Raring et al. | Mar 2011 | A1 |
20110073888 | Ueno et al. | Mar 2011 | A1 |
20110075694 | Yoshizumi et al. | Mar 2011 | A1 |
20110103418 | Hardy et al. | May 2011 | A1 |
20110129669 | Fujito et al. | Jun 2011 | A1 |
20110150020 | Haase et al. | Jun 2011 | A1 |
20110164637 | Yoshizumi et al. | Jul 2011 | A1 |
20110170569 | Tyagi et al. | Jul 2011 | A1 |
20110180781 | Raring et al. | Jul 2011 | A1 |
20110182056 | Trottier et al. | Jul 2011 | A1 |
20110186874 | Shum | Aug 2011 | A1 |
20110186887 | Trottier et al. | Aug 2011 | A1 |
20110188530 | Lell et al. | Aug 2011 | A1 |
20110216795 | Hsu et al. | Sep 2011 | A1 |
20110247556 | Raring et al. | Oct 2011 | A1 |
20110281422 | Wang et al. | Nov 2011 | A1 |
20110286484 | Raring et al. | Nov 2011 | A1 |
20120104359 | Felker et al. | May 2012 | A1 |
20120178198 | Raring et al. | Jul 2012 | A1 |
20120187371 | Raring et al. | Jul 2012 | A1 |
20120314398 | Raring et al. | Dec 2012 | A1 |
20130016750 | Raring et al. | Jan 2013 | A1 |
20130022064 | Raring et al. | Jan 2013 | A1 |
20130044782 | Raring | Feb 2013 | A1 |
20130064261 | Sharma et al. | Mar 2013 | A1 |
20160006217 | Raring et al. | Jan 2016 | A1 |
Number | Date | Country |
---|---|---|
101009347 | Mar 1987 | CN |
1538534 | Oct 2004 | CN |
1702836 | Nov 2005 | CN |
1781195 | May 2006 | CN |
101079463 | Nov 2007 | CN |
101099245 | Jan 2008 | CN |
101171692 | Apr 2008 | CN |
101079463 | Sep 2009 | CN |
3-287770 | Dec 1991 | JP |
2007-173467 | Jul 2007 | JP |
2007-068398 | Apr 2008 | JP |
2008-205231 | Sep 2008 | JP |
2008-300547 | Dec 2008 | JP |
2008-306062 | Dec 2008 | JP |
2008-311640 | Dec 2008 | JP |
WO 2004084275 | Sep 2004 | WO |
2008041521 | Apr 2008 | WO |
WO 2010120819 | Oct 2010 | WO |
Entry |
---|
Park (“Crystal orientation effects on electronic properties of wurtzite InGaN/GaN quantum wells”, JAP, vol. 91, No. 12, Jun. 15, 2002). |
International Search Report and Written Opinion for PCT application PCT/US2010/030939 (Jun. 16, 2010). |
International Search Report of PCT Application No. PCT/US2009/047107, dated Sep. 29, 2009, 4 pages total. |
International Search Report of PCT Application No. PCT/US2009/046786, dated May 13, 2010, 2 pages total. |
International Search Report of PCT Application No. PCT/US2009/52611, dated Sep. 29, 2009, 3 pages total. |
International Search Report & Written Opinion of PCT Application No. PCT/US2010/049172, dated Nov. 17, 2010, 7 pages total. |
International Search Report of PCT Application No. PCT/US2011/037792, dated Sep. 8, 2011, 2 pages total. |
USPTO Office Action for U.S. Appl. No. 12/759,273 dated Nov. 21, 2011. |
USPTO Office Action for U.S. Appl. No. 12/573,820 dated Oct. 11, 2011. |
Office action for U.S. Appl. No. 12/573,820 (Oct. 11, 2011). |
Office action for U.S. Appl. No. 12/749,466 (Feb. 3, 2012). |
Office action for U.S. Appl. No. 13/046,565 (Feb. 2, 2012). |
Office action for U.S. Appl. No. 13/046,565 (Nov. 7, 2011). |
Office action for U.S. Appl. No. 12/484,924 (Oct. 31, 2011). |
Office action for U.S. Appl. No. 12/497,289 (Feb. 2, 2012). |
Office action for U.S. Appl. No. 12/762,269 (Oct. 12, 2011). |
Office action for U.S. Appl. No. 12/762,271 (Dec. 23, 2011). |
Office action for U.S. Appl. No. 12/778,718 (Nov. 25, 2011). |
Notice of Allowance for U.S. Appl. No. 12/762,278 (Nov. 7, 2011). |
Abare “Cleaved and Etched Facet Nitride Laser Diodes,” IEEE Journal of Selected Topics in Quantum Electronics, vol. 4, No. 3, pp. 505-509 (May 1998). |
Asif Khan “Cleaved cavity optically pumped InGaN—GaN laser grown on spinel substrates,” Appl. Phys. Lett. 69 (16), pp. 2418-2420 (Oct. 14, 1996). |
Lin et al.“Influence of Separate Confinement Heterostructure Layer on Carrier Distribution in InGaAsP Laser Diodes with Nonidentical Multiple Quantum Wells,” Japanese Journal of Applied Physics, vol. 43, No. 10, pp. 7032-7035 (2004). |
Okamoto et al. In “High-Efficiency Continuous-Wave Operation of Blue-Green Laser Diodes Based on Nonpolar m-Plane Gallium Nitride,” The Japan Society of Applied Physics, Applied Physics Express 1 (Jun. 2008). |
Park, “Crystal orientation effects on electronic properties of wurtzite InGaN/GaN quantum wells,”,Journal of Applied Physics vol. 91, No. 12, pp. 9904-9908 (Jun. 2002). |
Romanov “Strain-induced polarization in wurtzite III-nitride semipolar layers,” Journal of Applied Physics 100, pp. 023522-1 through 023522-10 (Jul. 25, 2006). |
Schoedl “Facet degradation of GaN heterostructure laser diodes,” Journal of Applied Physics vol. 97, issue 12, pp. 123102-1 to 123102-8 (2005). |
Chinese Office Action From Chinese Patent Application No. 200980134723.8 dated Nov. 1, 2012, 22 pgs. (With Translation). |
Founta et al., ‘Anisotropic Morphology Of Nonpolar a-Plane GaN Quantum Dots And Quantum Wells,’ Journal of Applied Physics, vol. 102, vol. 7, 2007, pp. 074304-1-074304-6. |
Franssila, ‘Tools for CVD and Epitaxy’, Introduction to Microfabrication, 2004, pp. 329-336. |
USPTO Office Action for U.S. Appl. No. 12/481,543 dated Jun. 27, 2011. |
USPTO Office Action for U.S. Appl. No. 12/482,440 dated Feb. 23, 2011. |
USPTO Office Action for U.S. Appl. No. 12/482,440 dated Aug. 12, 2011. |
USPTO Office Action for U.S. Appl. No. 12/484,924 dated Apr. 14, 2011. |
USPTO Office Action for U.S. Appl. No. 12/491,169 dated Oct. 22, 2010. |
USPTO Office Action for U.S. Appl. No. 12/491,169 dated May 11, 2011. |
USPTO Notice of Allowance for U.S. Appl. No. 12/497,289 dated May 22, 2012. |
USPTO Office Action for U.S. Appl. No. 12/502,058 dated Dec. 8, 2010. |
USPTO Office Action for U.S. Appl. No. 12/502,058 dated Aug. 19, 2011. |
USPTO Notice of Allowance for U.S. Appl. No. 12/502,058 dated Apr. 16, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/502,058 dated Jul. 19, 2012. |
USPTO Office Action for U.S. Appl. No. 12/534,829 dated Apr. 19, 2011. |
USPTO Notice of Allowance for U.S. Appl. No. 12/534,829 dated Oct. 28, 2011. |
USPTO Notice of Allowance for U.S. Appl. No. 12/534,829 dated Dec. 5, 2011. |
USPTO Notice of Allowance for U.S. Appl. No. 12/534,829 dated Dec. 21, 2011. |
USPTO Office Action for U.S. Appl. No. 12/573,820 dated Mar. 2, 2011. |
USPTO Office Action for U.S. Appl. No. 12/749,466 dated Jun. 29, 2011. |
USPTO Office Action for U.S. Appl. No. 12/749,466 dated Jul. 3, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/762,269 dated Apr. 23, 2012. |
USPTO Office Action for U.S. Appl. No. 12/762,271 dated Jun. 6, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/762,271 dated Aug. 8, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/778,718 dated Apr. 3, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/778,718 dated Jun. 13, 2012. |
USPTO Office Action for U.S. Appl. No. 12/789,303 dated Sep. 24, 2012. |
USPTO Office Action for U.S. Appl. No. 12/859,153 dated Sep. 25, 2012. |
USPTO Office Action for U.S. Appl. No. 12/868,441 dated Apr. 30, 2012. |
USPTO Office Action for U.S. Appl. No. 12/880,803 dated Feb. 22, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/880,803 dated Jul. 18, 2012. |
USPTO Office Action for U.S. Appl. No. 12/883,093 dated Mar. 13, 2012. |
USPTO Office Action for U.S. Appl. No. 12/883,093 dated Aug. 3, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/883,093 dated Nov. 21, 2012. |
USPTO Office Action for U.S. Appl. No. 12/883,652 dated Apr. 17, 2012. |
USPTO Office Action for U.S. Appl. No. 12/884,993 dated Mar. 16, 2012. |
USPTO Office Action for U.S. Appl. No. 12/884,993 dated Aug. 2, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/884,993 dated Nov. 26, 2012. |
USPTO Office Action for U.S. Appl. No. 12/995,946 dated Mar. 28, 2012. |
USPTO Office Action for U.S. Appl. No. 13/014,622 dated Nov. 28, 2011. |
USPTO Office Action for U.S. Appl. No. 13/014,622 dated Apr. 30, 2012. |
USPTO Office Action for U.S. Appl. No. 13/046,565 dated Apr. 13, 2012. |
USPTO Office Action for U.S. Appl. No. 13/046,565 dated Jul. 19, 2012. |
USPTO Office Action for U.S. Appl. No. 13/354,639 dated Nov. 7, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 13/354,639 dated Dec. 14, 2012. |
Non-Final Office Action of Nov. 20, 2013 for U.S. Appl. No. 13/549,335, 12 pages. |
Feezell et al. ‘Development of nonpolar and semipolar InGaN/GaN visible light-emitting diodes’, MRS Bulletin, vol. 34, May 2009, pp. 318-323. |
International Search Report of PCT Application No. PCT/US2010/030939, dated Jun. 16, 2010, 9 pages total. |
Communication from the Chinese Patent Office re 200980134723.8 dated Jun. 27, 2013, 19 pages. |
USPTO Notice of Allowance for U.S. Appl. No. 12/868,441 dated Sep. 18, 2013, 13 pages. |
USPTO Office Action for U.S. Appl. No. 13/114,806 dated Aug. 26, 2013, 22 pages. |
International Preliminary Report & Written Opinion of PCT Application No. PCT/US2011/037792, dated Sep. 8, 2011, 13 pages total. |
Tyagi et al., ‘Semipolar (1011) InGaN/GaN Laser Diodes On Bulk GaN Substrates,’ Japanese Journal of Applied Physics, vol. 46, No. 19, 2007, pp. L444-L445. |
USPTO Office Action for U.S. Appl. No. 12/995,946 dated Jan. 29, 2013. |
USPTO Office Action for U.S. Appl. No. 12/534,838 dated May 3, 2011. |
USPTO Office Action for U.S. Appl. No. 12/534,838 dated Jan. 13, 2012. |
USPTO Office Action for U.S. Appl. No. 12/534,838 dated Mar. 20, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/534,838 dated Jun. 8, 2012. |
USPTO Office Action for U.S. Appl. No. 12/859,153 dated Feb. 26, 2013. |
USPTO Office Action for U.S. Appl. No. 12/942,817 dated Feb. 20, 2013. |
USPTO Notice of Allowance for U.S. Appl. No. 13/108,645 dated Jan. 28, 2013. |
USPTO Office Action for U.S. Appl. No. 13/291,922 dated Feb. 20, 2013. |
USPTO Office Action for U.S. Appl. No. 13/425,354 dated Feb. 14, 2013. |
USPTO Office Action for U.S. Appl. No. 13/548,312 dated Mar. 12, 2013. |
USPTO Office Action for U.S. Appl. No. 13/606,894 dated Feb. 5, 2013. |
Adesida et al., ‘Characteristics of chemically assisted ion beam etching of gallium nitride’, Applied Physics Letters, vol. 65, No. 7, 1994, pp. 889-891. |
Behfar et al., ‘Progress in Etched Facet Technology for GaN and Blue Lasers’, Proc. of SPIE., vol. 6473, 64731F, 2007, pp. 1-8. |
International Preliminary Report & Written Opinion of PCT Application No. PCT/US2011/060030 dated Mar. 21, 2012, 11 pgs. total. |
USPTO Notice of Allowance for U.S. Appl. No. 12/749,466 dated Jan. 2, 2013. |
USPTO Office Action for U.S. Appl. No. 12/787,343 dated Dec. 17, 2012. |
USPTO Notice of Allowance for U.S. Appl. No. 12/787,343 dated Jun. 10, 2013. |
USPTO Notice of Allowance for U.S. Appl. No. 12/789,303 dated Dec. 21, 2012. |
USPTO Office Action for U.S. Appl. No. 12/868,441 dated Dec. 18, 2012. |
USPTO Office Action for U.S. Appl. No. 13/114,806 dated Apr. 12, 2013. |
USPTO Office Action for U.S. Appl. No. 13/291,922 dated Jun. 18, 2013. |
USPTO Office Action for U.S. Appl. No. 13/548,635 dated Jun. 14, 2013. |
USPTO Notice of Allowance for U.S. Appl. No. 13/606,894 dated May 24, 2013. |
Notice of Allowance of Mar. 20, 2014 for U.S. Appl. No. 13/549,335, 19 pages. |
Non-Final Office Action of Jun. 19, 2014 for U.S. Appl. No. 14/134,244 21 pages. |
Notice of Allowance of Oct. 22, 2014 for U.S. Appl. No. 14/229,738 16 pages. |
U.S. Appl. No. 14/754,043, Notice of Allowance mailed Feb. 4, 2016, 8 pages. |
U.S. Appl. No. 12/942,817 unpublished, filed Nov. 9, 2010, Pfister at al. |
U.S. Appl. No. 12/963,238 unpublished, filed Sep. 20, 2010, Raring et al. |
U.S. Appl. No. 12/880,803 unpublished, filed Sep. 13, 2010, Raring et al. |
U.S. Appl. No. 12/880,889 unpublished, filed Sep. 13, 2010, Raring et al. |
U.S. Appl. No. 12/749,466 unpublished, filed Mar. 29, 2010, Raring et al. |
U.S. Appl. No. 12/749,476 unpublished, filed Mar. 29, 2010, Poblenz et al. |
U.S. Appl. No. 12/727,148 unpublished, filed Mar. 18, 2010, Raring. |
U.S. Appl. No. 12/573,820 unpublished, filed Oct. 5, 2009 Raring et al. |
U.S. Appl. No. 12/502,382 unpublished, filed Jul. 14, 2009, Raring et al. |
U.S. Appl. No. 12/502,058 unpublished, filed Jul. 13, 2009, Raring et al. |
U.S. Appl. No. 12/497,289 unpublished, filed Jul. 2, 2009, Raring et al. |
Aoki et al., InGaAs/InGaAsP MQW Electroabsorption Modulator Integrated with a DFB Laser Fabricated by Band-Gap Energy Control Selective Area MOCVD, 1993, IEEE J Quantum Electronics, vol. 29, pp. 2088-2096. |
Asano et al., “100-mW kink-Free Blue-Violet Laser Diodes with Low Aspect Ratio,” 2003, IEEE Journal of Quantum Electronics, vol. 39, No. 1, pp. 135-140. |
Bernardini et al., “Spontaneous Polarization and Piezoelectric Constants of III-V Nitrides,” 1997, Physical Review B, vol. 56, No. 16, pp. 10024-10027. |
Caneau et al., “Studies on Selective OMVPE of (Ga,In)/(As,P),” 1992, Journal of Crystal Growth, vol. 124, pp. 243-248. |
Chen et al., “Growth and Optical Properties of Highly Uniform and Periodic InGaN Nanostructures,” 2007, Advanced Materials, vol. 19, pp. 1707-1710. |
D'Evelyn et al., “Bulk GaN Crystal Growth by the High-Pressure Arnmonotherrnal Method,” Journal of Crystal Growth, 2007, vol. 300, pp. 11-16. |
Fujii et al., “Increase in the Extraction Efficiency of GaN-based Light-Emitting Diodes Via Surface Roughening,” 2004, Applied Physics Letters, vol. 84, No. 6, pp. 855-857. |
Funato et al., “Blue, Green, and Amber InGaN/GaN Light-Emitting Diodes on Semipolar (1122) GaN Substrates,” 2006, Journal of Japanese Applied Physics, vol. 45, No. 26, pp. L659-L662. |
Funato et al., “Monolithic Polychromatic Light-Emitting Diodes Based on InGaN Microfacet Quantum Wells toward Tailor-Made Solid-State Lighting,” 2008, Applied Physics Express, vol. 1, pp. 011106-1-011106-3. |
Gardner et al. “Blue-emitting InGaN—GaN double-heterostructure light-emitting diodes reaching maximum quantum efficiency above 200 a/ cm2”, Applied Physics Letters 91, 243506 (2007). |
hap ://techon.nikkeibp. co jp/english/NEWS—EN/20080122/146009. |
Hiramatsu et al., Selective Area Growth and Epitaxial Lateral Overgrowth of GaN by Metalorganic Vapor Phase Epitaxy and Hydride Vapor Phase Epitaxy. Materials Science and Engineering B, vol. 59, May 6, 1999. pp 104-111. |
Iso et al., “High Brightness Blue InGaN/GaN Light Emitting Diode on Nonpolar m-plane Bulk GaN Substrate,” 2007, Japanese Journal of Applied Physics, vol. 46, No. 40, pp. L960-L962. |
Kendall et al., “Energy Savings Potential of Solid State Lighting in General Lighting Applications,” 2001, Report for the Department of Energy, pp. 1-35. |
Kim et al, “Improved Electroluminescence on Nonpolar m-plane InGaN/GaN Qantum Well LEDs”, 2007, Physica Status Solidi (RRL), vol. 1, No. 3, pp. 125-127. |
Kuramoto et al., “Novel Ridge-Type InGaN Multiple-Quantum-Well Laser Diodes Fabricated by Selective Area Re-Growth on n-GaN Substrates,” 2007, Journal of Japanese Applied Physics, vol. 40, pp. 925-927. |
Masui et al. “Electrical Characteristics of Nonpolar InGaN-Based Light-Emitting Diodes Evaluated at Low Temperature,” Jpn. J. Appl. Phys. 46 pp. 7309-7310 (2007). |
Michiue et al. “Recent development of nitride LEDs and LDs,” Proceedings of SPIE, vol. 7216, 72161Z (2009). |
Nakamura et al., “InGaN/Gan/AlGaN-based Laser Diodes with Modulation-doped Strained-layer Superlattices Grown on an Epitaxially Laterally Grown GaN Substrate”, 1998, Applied Physics Letters, vol. 72, No. 12, pp. 211-213. |
Nam et al., “Later Epitaxial Overgrowth of GaN films on SiO2 Areas Via Metalorganic Vapor Phase Epitaxy,” 1998, Journal of Electronic Materials, vol. 27, No. 4, pp. 233-237. |
Okamoto et al., “Pure Blue Laser Diodes Based on Nonpolar m-Plane Gallium Nitride with InGaN Waveguiding Layers,” 2007, Journal of Japanese Applied Physics, vol. 46, No. 35, pp. 820-822. |
Okamoto et. al “Continuous-Wave Operation of m-Plane InGaN Multiple Quantum Well Laser Diodes” The Japan Society of I Applied Physics JJAP Express LEtter, vol. 46, no. 9, 2007 pp. L 187-L 189. |
Purvis, “Changing the Crystal Face of Gallium Nitride.” The Advance Semiconductor Magazine, vol. 18, No. 8, Nov. 2005. |
Sato et al., “High Power and High Efficiency Green Light Emitting Diode on free-Standing Semipolar (1122) Bulk GaN Substrate,” 2007.Physica Status Solidi (RRL), vol. 1, pp. 162-164. |
Sato et al., “Optical Properties of Yellow Light-Emitting-Diodes Grown on Semipolar (1122) Bulk GaN Substrate,” 2008, Applied Physics Letter, vol. 92, No. 22, pp. 221110-1-221110-3. |
Schmidt et al., “Demonstration of Nonpolar m-plane InGaN/GaN Laser Diodes,” 2007, Journal of Japanese Applied Physics, vol. 46, No. 9, pp. 190-191. |
Schmidt et al., “High Power and High External Efficiency m-plane InGaN Light Emitting Diodes,” 2007, Japanese Journal of Applied Physics, vol. 46, No. 7, pp. L126-L128. |
Shchekin et al., “High Performance Thin-film Flip-Chip InGaN—GaN Light-emitting Diodes,” 2006, Applied Physics Letters, vol. 89, pp. 071109-071109-3. |
Shen et al. “Auger recombination in InGaN measured by photoluminescence,” Applied Physics Letters, 91, 141101 (2007). |
Sizov et al., “500-nm Optical Gain Anisotropy of Semipolar (1122) InGaN Quantum Wells,” 2009, Applied Physics Express, vol. 2, pp. 071001-1-071001-3. |
Tomiya et. al. Dislocation related issues in the degradation of GaN-based laser diodes, IEEE Journal of Selected Topics in Quantum Electronics vol. 10, No. 6 (2004). |
Tyagi et al., “High Brightness Violet InGaN/GaN Light Emitting Diodes on Semipolar (1011) Bulk GaN Substrates,” 2007, Japanese Journal of Applied Physics, vol. 46, No. 7, pp. L129-L131. |
Uchida et al.,“Recent Progress in High-Power Blue-violet Lasers,” 2003, IEEE Journal of Selected Topics in Quantum Electronics, vol. 9, No. 5, pp. 1252-1259. |
Waltereit et al., “Nitride Semiconductors Free of Electrostatic Fields for Efficient White Light-emitting Diodes,” 2000, Nature: International Weekly Journal of Science, vol. 406, pp. 865-868. |
Wierer et al., “High-power AlGaInN Flip-chip Light-emitting Diodes,” 2001, Applied Physics Letters, vol. 78, No. 22, pp. 3379-3381. |
Yamaguchi, A. Atsushi, “Anisotropic Optical Matrix Elements in Strained GaN-quantum Wells with Various Substrate Orientations,” 2008, Physics Status Solidi (PSS), vol. 5, No. 6, pp. 2329-2332. |
Yoshizumi et al. “Continuous-Wave operation of 520 nm Green InGaN-Based Laser Diodes on Semi-Polar {20-21} GaN Substrates,” Applied Physics Express 2 (2009). -1310 1410. |
Yu et al., “Multiple Wavelength Emission from Semipolar InGaN/GaN Quantum Wells Selectively Grown by MOCVD,” in Conference on Lasers and Electro-Optics/Quantum Electronics and Laser Science Conference and Photonic Applications Systems Technologies, OSA Technical Digest (CD) (Optical Society of America, 2007), paper JTuA92. |
Zhong et al., “Demonstration of High Power Blue-Green Light Emitting Diode on Semipolar (1122) Bulk GaN Substrate,” 2007, Electron Letter, vol. 43, No. 15, pp. 825-826. |
Zhong et al., “High Power and High Efficiency Blue Light Emitting Diode on Freestanding Semipolar (1122) Bulk GaN Substrate,” 2007, Applied Physics Letter, vol. 90, No. 23, pp. 233504-233504-3. |
Non-Final Office Action received in U.S. Appl. No. 14/736,939, dated Oct. 21, 2016, 40 pages. |
Number | Date | Country | |
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20100316075 A1 | Dec 2010 | US |
Number | Date | Country | |
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61168926 | Apr 2009 | US | |
61243502 | Sep 2009 | US |