Patent Application
20220415671
The present invention relates to a method for efficiently extract heat from a semiconductor surface emitting device by employing a selective area growth of the semiconductor in diamond patterned structure.
Semiconductor surface emitting devices constitute a very important class of light emitting devices that comprise vertical cavity surface emitting lasers (VCSEL's), optically pumped disk lasers, micro-LED's and a plethora of mixed devices. Major advantages of such devices include high light extraction efficiency, built-in scalability, light mode quality inter alia. However, for high power applications, these devices lack proper heat extraction mechanism. This is due to their basic configuration: the physical contact between the device and the substrate is substantially smaller than for edge emitting devices. Moreover, the active region, where the heat is generated, is usually relatively far from the substrate, being separated from this substrate by a large number of layers, such as Bragg mirrors for example. Finally, since III-V crystals display relatively poor heat conductivity, heat is accumulated within the device and deteriorates its output (GaAs thermal conductivity coefficient is 0.55 W cm1° C.−1 compared to 1.3 W cm1° C.−1 for silicon).
This situation strongly hampers the development of high power devices and reduces the quality of the emitted light (mode distortion).
Currently, the state of the art for heat removal is either to mount them directly, or with a highly heat conductive heat-spreader, on a copper heat-sink.
Recently, to further improve heat extraction, new VECSEL designs have been proposed by employing two diamond heat-spreaders top and bottom (diamond-sandwich approach), either by diamond deposition or bonding. However, for both approaches, heat must diffuse through the whole structure in order to reach the bottom or the top of the device, from where it can be extracted.
For high power emission these approaches are not sufficient and more efficient heat extraction has to be provided.
The present invention seeks to provide a method to embed semiconductor light emitting devices in a diamond surrounding so that each region of the device is in close contact with diamond. Since diamond is the best heat-spreader, this method leads to optimal heat extraction.
The present invention provides an approach for producing a semiconductor surface emitting device with highly efficient heat extraction in order to enable high output, high quality power emitting device.
In order to do so, a diamond layer is grown on a semiconductor substrate. Reference is made to
Starting from a semiconductor substrate 101, a dielectric material (such as silicon oxide, silicon nitride or any other material suitable for seeding with diamond particles) layer is deposited (102) and then a photoresist (PR) (or any other material that can be patterned by lithography) layer is deposited and patterned by lithography (103), determining areas with PR and areas without PR on the dielectric material surface. Next, a diamond seeding layer, such as diamond slurry, is deposited on the wafer (104). The photoresist is then removed, leaving a patterned diamond seeded surface on the wafer (105).
A diamond layer is deposited, for example by chemical vapor deposition technique (CVD). It should be noted that the diamond will grow preferentially on the regions that have been seeded. Residual growth might occur on the non-seeded regions, however with a very sparse density (islands-like growth), which is easy to remove in the following processes.
Deposition of diamond is done at high temperature range (>650° C.), which is not applicable on a semiconductor device without protection, as the semiconductor (such as GaAs, InP, GaSb) surface thermally decomposes. Therefore, the dielectric layer has a dual purpose: prevent diamond growth on non-seeded regions on the wafer, and act as nucleation areas for diamond particles in the seeded areas (106).
Then, using an etching process, the dielectric layer in the non-seeded areas is removed, leaving an intact semiconductor surface. This process finally results in open semiconductor substrate selected areas surrounded by a diamond layer (107). It should be noted that thick diamond layers can be deposited in this way.
Following this, semiconductor layers are grown, for example using MOCVD (metal organic chemical vapor deposition) or MBE (molecular beam epitaxy) techniques (108). The growth is selective, being effective only in the selected areas where the semiconductor surface is open, free from diamond. The epitaxial layers are grown on the semiconductor surface (e.g. GaAs, InP, GaSb, GaN and alloys of these) and not on the diamond surface. According to the growth conditions, the epitaxial structure might be in contact with the diamond or very close. For thermal conduction, this is less critical than for electric conduction. and the diamond layer which will act as a heat spread layer.
Another issue arises from the fact that the grown diamond layer surface may be hydrogen terminated, as a result of the hydrogen rich growth environment. The hydrogenation of the diamond surface may result in negative electron affinity, pulling the vacuum level below the conduction band minimum (up to −1.3 eV). This can result in charge transfer between the valence band of the diamond and conduction band of the device layer, thus turning the diamond into a P-type semiconductor and injecting unwanted electrons into the device layers. Possible methods to prevent this charge transfer include:
1. Surface oxidation, which will result in a diamond surface with a positive electron affinity of 1.7 eV, as shown by Ristein (J., Surface science of diamond: Familiar and amazing. Surface Science, 2006. 600(18): p. 3677-3689).
2. Deposition of a thin insulating layer with large band gap and sufficiently small electron affinity, such as SiO2.
This technique enables a near-contact to full contact of the semiconductor side walls and the diamond layer which will act as a heat spread layer.
This technique enables a highly efficient heat extraction needed for high power devices, as heat generated in the active region of the device is very close to the diamond heat sink layer, resulting in a higher heat extraction efficiency compared to other techniques where the heat sink is located at a much higher distance from the active region.
The diamond layer is then connected to a heat exchanger or a thermoelectric cooler.
In order to remove heat efficiently, it is preferable to connect the diamond covered areas to a heat exchanger located at close proximity. A convenient way to do so is through vias filled with a thermally conducting material such as copper, indium or diamond.
The process is illustrated in
After optionally thinning the wafer, starting from the grown device 201, a protective layer such as photoresist is deposited on the grown side of the wafer in order to protect the structures (202). Then a photoresist layer is deposited on the other side of the wafer and is patterned so as to leave holes that are correspondingly in front of the regions where the diamond has been grown previously (203). The wafer is then etched until the diamond layer is reached (204). The holes (204) are then filled with the thermally conducting material (205). The protective layer can then be removed (206). The wafer can then be cut into individual devices, and each device can be put in thermal contact with a passive or active heat sink.
It should be noted that the thermally conducting material can be a metal, such as copper. In such a case, this layer can be pattern by itself in order to provide electric contact to the devices.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/IB2020/062432 | 12/24/2020 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 62953558 | Dec 2019 | US |
