This present application relates to a power device, and more particularly to a power device having a grading interlayer doped with carbon.
Recently, group III nitride semiconductor such as gallium nitride (GaN) develops rapidly for the high power devices because of its wider band gap, high breakdown field strength, and high electron saturation velocity. In a heterostructure of aluminum gallium nitride (AlGaN)/gallium nitride (GaN) formed on a substrate, two-dimensional electron gas (2DEG) is generated at a heterointerface due to spontaneous polarization and piezoelectric polarization. Particular attention has been drawn to Schottky barrier diodes (SBDs) and field effect transistors (FETs) using a high concentration 2DEG as a carrier.
If GaN-based nitride semiconductors are formed on a hetero-substrate, since the lattice constant and the coefficient of thermal expansion of the substrate are different from those of the nitride semiconductors, problems such as bowing and cracks are likely to occur.
A power device comprises a substrate, a first semiconductor layer formed on the substrate, a second semiconductor layer formed on the first semiconductor layer and comprising a first element of group III, a third semiconductor layer formed on the second semiconductor layer and a plurality of first interlayers formed in the third semiconductor layer and comprising a second element of III group. The first element of III group and the second element of III group are the same. The second semiconductor layer and the plurality of first interlayers are doped with carbon.
A power device comprises a substrate, a first semiconductor layer formed on the substrate, a second semiconductor layer formed on the first semiconductor layer, a third semiconductor layer formed on the second semiconductor layer, a plurality of first interlayers formed in the third semiconductor layer and comprising a first lattice constant, and a plurality of second interlayers formed in the third semiconductor layer and comprising a second lattice constant. The first lattice constant is less than the second lattice constant
The substrate 11 may be made of a material suitable for growing nitride semiconductor, such as Si, SiC, GaN or sapphire. The first semiconductor layer 12 having a thickness of 150 nm can be a nucleation layer and comprises a first element of group III. The second semiconductor layer 13 having a thickness range between 700˜800 nm can be a grading layer and comprises a second element of group III which is same as the first element, such as Al. The third semiconductor layer 14 having a thickness of 4 μm can be a buffer layer.
The first interlayers 101a˜101c can also be buffer layers used to adjust the stress and coefficient of thermal expansion of the substrate 11 and increase the thickness of the buffer layer. The first interlayers 101a˜101c may comprise MN or AlGaN, and every first interlayer has a thickness range between 1 nm˜100 nm, wherein the thickness of the first interlayer is preferably 20 nm.
The second semiconductor layer 13, third semiconductor layer 14 or/and the first interlayers 101a˜101c may be doped with carbon to prevent the leakage current of the substrate 11, increase the resistance of buffer layer and raise the breakdown voltage. A range of the doping concentration may be between 1×1017 to 1×1020 cm−3 and a doping type comprises grading type, step type and contact type.
The power device 10 further comprises a channel layer 15, a supplying layer 16, a source electrode 17, a drain electrode 18, and a gate electrode 19. The channel layer 15 having a thickness range between 50˜300 nm is formed on the third semiconductor layer 14. The supplying layer 16 having a thickness range between 20˜30 nm is formed on the channel layer 15, wherein the piezoelectric polarization and the spontaneous polarization occur at an interface between the channel layer 15 and the supplying layer 16 by the different lattice constant, and then a two dimensional electron gas (2DEG) can be generated by heterostructural interface of channel layer 15 and supplying layer 16.
The gate electrode 17 is formed on the supplying layer 16 and in schottky contact with the supplying layer 16. The source electrode 18 and the drain electrode 19 are formed in both lateral regions of the gate electrode 17 and in ohmic contact with the supplying layer 16.
Then, the channel layer 15 made of undoped GaN and having a thickness of 100 nm is grown on the sublayer 14d, as shown in
Subsequently, as shown in
Although the power device and the method of manufacturing the power device of the first embodiment have been described above, the present disclosure is not limited to the first embodiment. For example, the number of the first interlayers is not limited to the first embodiment, more than three first interlayers can be formed in the third semiconductor layer 14.
The second interlayers 201a˜201c are formed in the third semiconductor layer 14 and can also be buffer layers used to adjust the stress and coefficient of thermal expansion of the substrate 11 and increase the thickness of the buffer layer. The second interlayers 201a˜201c may comprise AlGaN or AlInGaN, and every second interlayer has a thickness range between 1 nm˜100 nm, wherein the thickness of the second interlayer is preferably 20 nm. In the second embodiment, the first interlayers 101a˜101c comprise a first lattice constant and the second interlayers 201a˜201c comprise a second lattice constant, wherein the first lattice constant is smaller than the second lattice constant.
As shown in
Furthermore, the plurality of second interlayers 201 comprises a third element of III group which is same as the second element of the first interlayers 101, such as Al. A variance type of a content of the third element comprises grading type, step type, and contact type. In the second embodiment, a content of Al of the second interlayers 201a˜201c is decreased in a direction away from the adjacent first interlayers 101a˜101c, respectively. For example, a content of Al of the second interlayer 201a is decreased in a direction away from the adjacent first interlayer 101a.
In other words, a variance type of the second lattice constant comprises grading type, step type, and contact type. The second lattice constant of the second interlayers 201a˜201c is increased in a direction away from the adjacent first interlayers 101a˜101c, respectively.
In the fourth embodiment, the power device structure of the fourth embodiment is similar to that of the second embodiment, except that the second semiconductor layer 13, third semiconductor layer 14, the first interlayers 101a˜101C or/and the second interlayers 201a˜201c may be doped with carbon to prevent the leakage current of the substrate 11, increase the resistance of buffer layer, and raise the breakdown voltage. A range of the doping concentration may be between 1×1017 to 1×1020 cm−3 and a doping type comprises grading type, step type, and contact type.
In the fifth embodiment, the power device structure of the fifth embodiment is similar to that of the third embodiment, except that the second semiconductor layer 13, third semiconductor layer 14, the first interlayers 101a˜101C or/and the second interlayers 201a˜201c, 202a˜202c may be doped with carbon. A range of the doping concentration may be between 1×1017 to 1×1020 cm−3 and a doping type comprises grading type, step type and contact type.
Table 1 shows the experimental result of the comparable sample and samples A˜C in different carbon concentrations when the working voltage is 600V, wherein the leakage current is lower while the carbon concentration is higher, and the leakage current is over limit while the compared sample is un-doped. This obviously shows that the second semiconductor layer, the third semiconductor layer and interlayers doped with carbon is beneficial to reduce the leakage current.
Table 2 shows the experimental results of the comparable sample and samples A˜C in different thicknesses when the working current is 1 mA, wherein a thickness is a sum of a thickness from the first semiconductor layer to the supplying layer. The breakdown voltage is higher while the thickness is thicker. Thus, it is useful to increase thicknesses of GaN-based nitride semiconductors to raise the breakdown voltage.
It should be noted that the proposed various embodiments are not for the purpose to limit the scope of the disclosure. Any possible modifications without departing from the spirit of the disclosure may be made and should be covered by the disclosure.