The present specification relates to enhancement-mode high-electron-mobility transistors (HEMTs).
A high-electron-mobility transistor (HEMT) includes a source contact terminal, a drain contact terminal, and a gate contact terminal to which a voltage may be applied to control the flow of electrical current between the source contact terminal and the drain contact terminal. A HEMT may be either a depletion-mode HEMT, which is normally in an “on” state at zero gate-source voltage, or an enhancement-mode HEMT, which is normally in an “off” state at zero gate-source voltage. The use of enhancement-mode HEMTs in circuit design eliminates the need for a negative-polarity voltage supply, and may be preferred in applications in which it is desirable that HEMTs fail in the “off” state.
According to an aspect of the specification, a method for fabricating an enhancement-mode high-electron-mobility transistor (HEMT) is provided. The method involves providing semiconductor layers capable of sustaining a two-dimensional electron sheet to enable electrical current to flow through the HEMT. The method further involves forming a series of trenches and fins in the semiconductor layer over an active area of the semiconductor layer on which a gate contact terminal is to be set down, the fins having widths equal to or less than about 30 nm across. The method further involves setting down the gate contact terminal across the fins.
According to another aspect of the specification, a method for fabricating a wafer containing enhancement-mode high-electron-mobility transistors (HEMTs) and depletion-mode HEMTs is provided. The method involves providing semiconductor layers capable of sustaining a two-dimensional electron sheet to enable electrical current to flow through the HEMTs. The method further involves, for each enhancement-mode HEMT, forming a series of trenches and fins in the semiconductor layer over an active area of the semiconductor layer on which a gate contact terminal of the enhancement-mode HEMT is to be set down, the fins having widths equal to or less than about 30 nm across; setting down the gate contact terminal across the fins; and setting down a source contact terminal and a drain contact terminal on either side of the gate contact terminal outside of the active area. The method further involves, for each depletion-mode HEMT, setting down a gate contact terminal, and a source contact terminal and a drain contact terminal on either side of the gate contact terminal.
According to yet another aspect of the specification, a high-electron-mobility transistor (HEMT) is provided. The HEMT includes a drain contact terminal, a source contact terminal, and semiconductor layers. The semiconductor layers are capable of sustaining a two-dimensional electron sheet to enable electrical current to flow through the HEMT. The semiconductor layers include an active area on which a gate contact terminal is to be set down, the active area including a series of trenches and fins, the fins having widths equal to or less than about 30 nm. The HEMT further includes a gate contact terminal set down across the fins.
High-electron-mobility transistors (HEMTs) may be designed to have a wide bandgap, high breakdown voltage, high peak electron drift velocity, and the high concentration of two-dimensional electron gas. Such characteristics may be provided by the use of semiconductor layers made of aluminum gallium nitride (AlGaN) and gallium nitride (GaN).
However, fabricating a HEMT with such characteristics in enhancement mode may be challenging. Previous attempts employed techniques such as barrier-thinning and fluoride-based plasma treatment, which may result in high gate-leakage current and the possibility of hysteresis in the gate characteristics of such enhancement-mode HEMTs. These drawbacks may be caused by surface damage and ease of tunnelling through a thinned-barrier, in the case of barrier-thinning, and/or by movement of fluorine ions, in the case of fluoride-based plasma treatment. Other techniques involve the reduction of the size of fins, but so far such fin features have only been fabricated at sizes as low as about 50 nanometers. At this size, such fin features result in HEMTs with positive threshold voltages nearly equal to about 0 volts, but this is unsatisfactory for the fabrication of reliable normally-off enhancement-mode HEMTs.
Described herein are methods to fabricate reliably normally-off enhancement-mode HEMT5 that involve the fabrication of fins at sizes equal to or less than about 30 nanometers. Such small fin feature sizes may be realized by the use of electron beam lithography and inductively coupled plasma-reactive ion etching (ICP-RIE). These fins are separated by trenches etched in the active area of the HEMT, the fins having widths less than or equal to about 30 nanometers. The reduced widths of the fins may cause the HEMT to reliably operate in enhancement-mode by the tri-gate concept and/or polarization relaxation.
The HEMT 100 further includes semiconductor layers 140 capable of sustaining a two-dimensional electron sheet to enable electrical current to flow through the HEMT 100. The semiconductor layers 140 comprises a first semiconductor layer, or barrier 142, of a first semiconductor material, and a second semiconductor layer, or channel 144, of a second semiconductor material underneath the barrier 142. The barrier 142 and channel 144 form layers that run continuously beneath the source contact terminal 110 and drain contact terminal 120 (the continuous path is not shown in the cross-section of
The second semiconductor material has a different band gap than the first semiconductor material, and thus a heterointerface 143 is formed between the barrier 142 and the channel 144. The channel 144 includes a region in which a two-dimensional electron sheet is formed, referred to herein as the two-dimensional electron sheet region 145. The two-dimensional electron sheet region 145 is in the channel 144 and adjacent to the heterointerface 143. The thickness of the two-dimensional electron sheet region 145 is exaggerated in the Figures for illustrative purposes, but it is to be understood that the thickness of the two-dimensional electron sheet region 145 may have a thickness of only about 1-2 nanometers. Further, it is to be understood that the channel 144 is an upper portion of a deeper layer of the second semiconductor material, below which may include the substrate wafer and any additional layer(s) epitaxially grown (not shown in
When a first voltage source is used to apply a voltage greater than a threshold voltage to the gate contact terminal 130, electrons accumulate in a two-dimensional electron sheet region 145 under the gate contact terminal 130 in the fins 154, thereby allowing electrical current to flow between the source contact terminal 110 and drain contact terminal 120, when a second voltage source is used to apply a voltage difference between the source and drain.
The second semiconductor material is selected to serve as a HEMT channel and the first semiconductor material is selected to serve as a HEMT barrier compatible with the channel. In the present example, the first semiconductor material includes aluminum gallium nitride (AlGaN) and the second semiconductor material may include gallium nitride (GaN).
As mentioned above, the semiconductor layers 140 includes the active area 150 on which a gate contact terminal 130 is to be set. The active area 150 includes a series of fins 154 having widths 153 (See
The gate contact terminal 130 is set down across the fins 154. The trenches 152 and fins 154 run perpendicular to the direction of the gate contact terminal 130, as shown in
Some segments of the gate contact terminal 130 rest on top of the barrier 142 or on a thin insulator layer (the latter not shown), forming either a Schottky contact or metal-insulator-semiconductor structure. Further, some segments of the gate contact terminal 130 that run down the trenches 152 rest adjacent to the inner side walls of the trenches 152, which may be of the barrier 142 or the channel 144. Further, some segments of the gate contact terminal 130 rest on the bottoms of the trenches 152 in the channel 144.
The trenches 152 extend through the semiconductor layer 140 past a depth at which the two-dimensional electron sheet is to be formed, or in other words, past the two-dimensional electron sheet region 145. Thus, in some examples, the trenches 152 may extend about 40 nanometers into the semiconductor layer 140, depending on the depth of the heterointerface 143.
As mentioned previously, the widths 153 of the fins 154 are equal to or less than about 30 nanometers.
At block 302, semiconductor layers capable of sustaining a two-dimensional electron sheet to enable electrical current to flow through the HEMI are provided. The semiconductor layers may be similar to the semiconductor layers 142 and 144 of semiconductor layers 140 of
Returning to
An example of semiconductor layers 440 with such trenches formed therein is shown in
The trenches 452 may be formed in the semiconductor layer 440 by a combination of electron beam lithography and dry etching, as described in greater detail in
Returning to
An example of semiconductor layers 440 with trenches 452 and fins 454 formed therein and a gate contact terminal 430 set down across the fins 454 is shown in
At block 502, the semiconductor layers are covered with an electrosensitive resist layer. The electrosensitive resist layer may include hydrogen silsesquioxane (HSQ).
At block 504, the series of fins are patterned using the electrosensitive resist layer by electron beam lithography, thereby forming a mask from the electrosensitive resist layer. The HSQ that is exposed to the electron beam of a sufficient dose is converted into silicon oxide. The unexposed HSQ can be removed as waste by an intermediate development step. The HSQ is a high-resolution resist, and is particularly well-suited for this application since the exposed resist provides a suitable mask for subsequent plasma etching of the semiconductor layer. A typical polymer resist layer may not withstand the subsequent plasma etching, and alternatively, the use of a sacrificial hard mask may introduce complexity and risk of damaging the semiconductor layers.
At block 506, the series of trenches is dry etched into the semiconductor layer through the mask. The trenches may be dry etched with chlorine-based dry etching and by inductively coupled plasma-reactive ion etching (ICP-RIE). Thus, small isolation features in the form of small fins spaced part by trenches may be fabricated, with the fins having widths equal to or less than about 30 nm.
At block 602, semiconductor layers capable of sustaining a two-dimensional electron sheet to enable electrical current to flow through the HEMTs is provided. The semiconductor layers may be similar to the semiconductor layers 140 of
At block 604, an enhancement-mode HEMT is fabricated into the semiconductor layers by the techniques discussed herein. That is, a series of trenches and fins is formed in the semiconductor layer in an active area of the semiconductor layer on which a gate contact terminal of the enhancement-mode HEMT is to be set down, the fins having widths equal to or less than about 30 nm across. The gate contact terminal is set down across the fins. Source contact terminal and drain contact terminals are set down on either side of the gate contact terminal outside of the area.
At block 606, a depletion-mode HEMT is fabricated into the semiconductor layers. Fabrication of the depletion-mode HEMT involves at least setting down a gate contact terminal, and a source contact terminal and a drain contact terminal on either side of the gate contact terminal.
Thus, a wafer containing both depletion-mode HEMTs and enhancement-mode HEMTs may be fabricated. Such parallel processing of depletion-mode HEMTs and enhancement-mode HEMTs may be particularly useful in HEMT-based logic circuits that features integrations of depletion-mode HEMTs and enhancement-mode HEMTs.
Thus, as described herein, a reliable normally-off HEMT may be produced. Such an HEMT may be produced with small fin isolation features and without the need for a separate sacrificial mask, thereby minimizing the risk of damage to the surface of the semiconductor layers. Such reliable normally-off HEMTs may be applicable in radio frequency, power electronics, and digital applications, and may be particularly useful in harsh environments such as automotive and aerospace engine controls, well logging in petroleum exploration, and nuclear reactors.
It should be recognized that features and aspects of the various examples provided above can be combined into further examples that also fall within the scope of the present disclosure. The scope of the claims should not be limited by the above examples but should be given the broadest interpretation consistent with the description as a whole.
Filing Document | Filing Date | Country | Kind |
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PCT/IB2020/058738 | 9/18/2020 | WO |
Number | Date | Country | |
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62903231 | Sep 2019 | US |