Doping activation and ohmic contact formation in SiC electronic devices and SiC electronic devices

Abstract

To provide a method for manufacturing a SiC-based electronic device (50).SOLUTION: The manufacturing method includes: implanting, at a front side (52a) of a solid body (52) of SiC having a conductivity of N type, dopant species of P type, thus forming an implanted region (59') that extends in depth in the solid body starting from the front side (52a) and has a top surface co-planar with the front side (52a); and generating a laser beam (82) directed towards the implanted region (59') in order to generate heating of the implanted region (59') to a temperature between 1500°C and 2600°C, so as to form one or more carbon-rich layers, e.g., graphene and / or graphite layers, in the implanted region (59'), and, simultaneously, activate the dopant species of P type.SELECTED DRAWING: Figure 2

Description

[Technical Field]

[0001] The present invention relates to a method for fabricating a SiC electronic device and the SiC electronic device so fabricated. In particular, the present invention relates to a method for activating doping in a SiC electronic device and simultaneously forming an ohmic contact. [Background technology]

[0002] As is known, a wide band gap, especially a band gap energy value Eg higher than 1.1 eV, and a low on-state resistance (R ON Semiconductor materials that exhibit high thermal conductivity, high operating frequencies, and high saturation of charge carriers are ideal for the fabrication of electronic components such as diodes or transistors, especially for power applications. A material that possesses these properties and is designed to be used for the fabrication of electronic components is silicon carbide (SiC). In particular, silicon carbide, in its different polytypes (e.g., 3C-SiC, 4H-SiC, 6H-SiC), is more preferable than silicon as far as the aforementioned properties are concerned.

[0003] Electronic devices built on silicon carbide substrates offer numerous advantages over similar devices built on silicon substrates, including lower output resistance in conduction, lower leakage current, higher operating temperatures, and higher operating frequencies. In particular, SiC Schottky diodes exhibit higher switching performance, making SiC electronic devices particularly suitable for high-frequency applications. Current applications impose requirements on electrical characteristics and on the long-term reliability of the devices.

[0004] FIG. 1 shows a known type of merged PIN Schottky (MPS) device 1 in cross section in an X, Y, Z (three-axis) Cartesian coordinate system.

[0005] The MPS device 1 comprises a substrate 3 of N-type SiC having a surface 3a opposite a surface 3b, a thickness of about 350 μm, and a first doping concentration; a drift layer 2 (epitaxially grown) made of N-type SiC and having a second doping concentration lower than the first doping concentration, extending over the surface 3a of the substrate 3, and having a thickness of between 5 and 15 μm; and an ohmic contact region 6 (e.g., made of nickel silicide) extending over the surface 3b of the substrate 3. anode metallization 8 extending over the upper surface 2 a of the drift layer 2; multi-junction barrier (JB) elements 9 in the drift layer 2 facing the upper surface 2 a of the drift layer 2 and each including a respective implanted region 9′ of P type and an ohmic contact 9″ of metallic material; and optional end termination regions or guard rings 10 loosely surrounding the JB elements 9 and being specifically implanted regions of P type.

[0006] The Schottky diode 12 is formed at the interface between the drift layer 2 and the anode metallization 8. In particular, a Schottky junction (between semiconductor and metal) is formed by portions of the drift layer 2 in direct electrical contact with respective portions of the anode metallization 8.

[0007] The region of the MPS 1 containing the JB element 9 and the Schottky diode 12 (ie, the region contained within the guard ring 10) is the active area 4 of the MPS device 1.

[0008] The steps for fabricating the MPS device 1 of FIG. 1 include a masked implantation of dopant species (e.g., boron or aluminum) having a second conductivity type (P) to form implanted region 9′ and end termination region 10. A thermal annealing step is then performed to allow diffusion and activation of the so-implanted dopant species. The thermal annealing is performed, for example, at a temperature greater than 1600° C. (e.g., between 1700° C. and 1900° C., and in some cases even higher). After the thermal treatment, implanted region 9′ has a size of approximately 1×10 17 〜1×10 20 atoms / cm 3 The dopant species has a concentration between 0.01 and 0.1.

[0009] Then, a step is carried out to carry out the formation of the ohmic contacts 9" which involves the deposition of nickel exclusively in the implanted regions 9', using in particular a silicon oxide mask to cover the surface areas of the drift layer 2 other than the implanted regions 9'. A subsequent thermal annealing at high temperature (between 900°C and 1000°C for a time period of 1 to 120 minutes) allows the formation of nickel silicide ohmic contacts 9" by chemical reaction between the deposited nickel and the silicon of the drift layer 2. In fact, the deposited nickel reacts with the surface material of the drift layer 2 to form NiSi (i.e., ohmic contacts), while the nickel in contact with the oxide of the mask does not react. Then, a step is carried out to remove the unreacted metal and the mask.

[0010] The steps described above require several thermal annealing steps, first for doping activation and then for ohmic contact formation. Furthermore, the deposition step of the metal that reacts with the drift layer 2 to form the ohmic contact 9" is critical in that an optimal match is required between the implanted region 9' and the deposited metal; indeed, a possible mismatch between the metal contact useful for forming the ohmic contact 9" and the region of the Schottky diode 12 can cause device malfunction. Indeed, ohmic contacts formed on SiC epitaxy can form resistors and no longer diodes, or else Schottky contacts with very low barrier heights. In either case, the devices so formed are unusable due to high leakage in reverse bias. Summary of the Invention [Problem to be solved by the invention]

[0011] SUMMARY OF THE INVENTION An object of the present invention is to provide a method for manufacturing an electronic device and a corresponding SiC electronic device that can overcome the drawbacks of the prior art. [Means for solving the problem]

[0012] According to the present invention, there is provided a method of manufacturing an electronic device and a corresponding SiC electronic device, as defined in the claims. For a better understanding of the present invention, preferred embodiments thereof will now be described, purely by way of non-limiting example, with reference to the accompanying drawings, in which: [Brief explanation of the drawings]

[0013] [Figure 1] 1 is a schematic cross-sectional view of an MPS device according to one known embodiment. [Figure 2] 1 is a schematic cross-sectional view of an MPS device according to one embodiment of the present invention. [Figure 3]3A-3C are schematic cross-sectional views illustrating certain steps in fabricating the device of FIG. 2 in accordance with one embodiment of the present invention. [Figure 4] 3A-3C are schematic cross-sectional views illustrating certain steps in fabricating the device of FIG. 2 in accordance with one embodiment of the present invention. [Figure 5] 3A-3C are schematic cross-sectional views illustrating certain steps in fabricating the device of FIG. 2 in accordance with one embodiment of the present invention. [Figure 6] 3A-3C are schematic cross-sectional views illustrating certain steps in fabricating the device of FIG. 2 in accordance with one embodiment of the present invention. [Figure 7] 4 is a graph illustrating the voltage-current curve of a device made in accordance with the present invention. DETAILED DESCRIPTION OF THE INVENTION

[0014] Although the present invention will be described with particular reference to merged PIN Schottky (MPS) devices, it will be apparent from the following description that the invention is generally applicable to any SiC-based electronic device, such as a MOSFET.

[0015] FIG. 2 shows a cross-sectional view of an MPS device 50 in an X, Y, Z (three-axis) Cartesian coordinate system according to one aspect of the present invention.

[0016] The MPS device 50 comprises a substrate 53 made of N-type SiC having a first doping concentration, a surface 53a opposite a surface 53b, and a thickness between 50 μm and 350 μm, more particularly between 160 μm and 200 μm, e.g., 180 μm; a drift layer 52 (epitaxially grown) made of N-type SiC having a second doping concentration lower than the first doping concentration and extending on the surface 53a of the substrate 53, the drift layer 52 having a thickness between 5 μm and 15 μm, e.g., 5 μm; an ohmic contact region or layer 56 (made of, e.g., nickel silicide) extending on the surface 53b of the substrate 53; and a semiconductor layer 56 extending on the ohmic contact region 56. anode metallization 58 extending over the upper surface 52 a of the drift layer 52 and made of, for example, Ti / AlSiCu or Ni / AlSiCu; a passivation layer 69 on the anode metallization 58 for protecting the anode metallization 58; multi-junction barrier (JB) elements 59 in the drift layer 52 facing the upper surface 52 a of the drift layer 52 and each including a respective P-type implanted region 59′ and ohmic contact 59″; and optional end termination regions or guard rings 60, which are P-type implanted regions completely surrounding the JB elements 89.

[0017] Laterally with respect to the implantation region 59′, one or more Schottky diodes 62 are formed at the interface between the drift layer 52 and the anode metallization 58. In particular, Schottky junctions (of the semiconductor-metal type) are formed by respective portions of the drift layer 52 in direct electrical contact with respective portions of the anode metallization 58.

[0018] The region of MPS device 50 that includes JB element 59 and Schottky diode 62 (ie, the region contained within guard ring 60 ) is the active area 54 of MPS device 50 .

[0019] According to one aspect of the present invention, each ohmic contact 59″ is formed by one or more carbon-rich layers, including, for example, a graphite layer or a graphene multilayer. More specifically, each ohmic contact 59″ has, at the surface 52 a, an amorphous SiC layer in which the number of carbon atoms is predominant (e.g., at least two times higher, particularly two to one hundred times higher) relative to the number of silicon atoms due to phase separation between silicon atoms and carbon atoms in the SiC substrate. Beneath this amorphous layer, each ohmic contact 59″ may provide a layer including carbon clusters (e.g., a graphite layer) having a thickness greater than that of the amorphous layer. The formation of such ohmic contacts 59″ results from the thermal decomposition of silicon carbide as a result of the manufacturing process described below.

[0020] According to a further aspect of the invention, the ohmic contact 59" is self-aligned with the implanted region 59' at the surface 52a (i.e., in plan view in the plane XY, the ohmic contact 59" has the same shape and extent as the implanted region 59'). In this case, electrical contact between the anode metallization 58 and the implanted region 59' occurs exclusively via the ohmic contact 59".

[0021] Furthermore, in accordance with a further aspect of the present invention, ohmic contact 59" does not extend along the Z axis beyond surface 52a; i.e., ohmic contact 59" has an upper surface 52a that is coplanar with surface 52a (i.e., aligned along axis X) and extends a depth (along Z) within ohmic contact 59' for a depth of between 1 nanometer and tens of nanometers (e.g., between 1 nm and 20 nm) measured starting from surface 52a.

[0022] The steps for forming ohmic contacts 59" are described below with particular reference to the steps for fabricating MPS device 50 (FIGS. 3-6).

[0023] Referring to FIG. 3, a wafer 100 is provided that includes a SiC substrate 53 (specifically, 4H—SiC, although other polytypes such as, but not limited to, 2H—SiC, 3C—SiC, 6H—SiC, etc., may also be used).

[0024] The substrate 53 has a first conductivity type (in this example, N-type doping) and has a front surface 53a and a back surface 53b, which are opposite each other along the Z axis. 19 and 1×10 22 atoms / cm 3 The doping concentration is between 0.01 and 0.1.

[0025] The front side of wafer 100 corresponds to front surface 53a, and the back side of wafer 100 corresponds to back surface 53b. The resistivity of substrate 30 is, for example, between 2 mΩ·cm and 40 mΩ·cm.

[0026] A silicon carbide drift layer 52 is formed on the front surface 53a of the substrate 53, for example by epitaxial growth, and the drift layer 52 has a first conductivity type (N) and a lower doping concentration than that of the substrate 53, for example 1×10 14 ~5×10 16 atoms / cm 3 The drift layer 52 is composed of SiC, specifically 4H—SiC, although other polytypes such as 2H, 6H, 3C, or 15R may also be used.

[0027] Drift layer 52 has a thickness defined between top side 52a and bottom side 52b (which is in direct contact with front surface 53a of substrate 53).

[0028] Next (FIG. 4), a hard mask 70 is formed on the upper side 52a of the drift layer 52, for example by depositing photoresist, or TEOS, or another material designed for that purpose. The hard mask 70 has a thickness between 0.5 μm and 2 μm, or in any case a thickness that will block implants described below, again with reference to FIG. 4. The hard mask 70 extends into the region of the wafer 100 where the active area 54 of the MPS device 50 will be formed in a later step.

[0029] In a top plan view in plane XY, the hard mask 70 covers the areas of the upper sides 52 a of the drift layer 52 that will form the Schottky cells (diodes 62) and leaves exposed the areas of the upper sides 52 a of the drift layer 52 that will form the implanted regions 59′ already identified with reference to FIG. 6 .

[0030] Then, using the hard mask 70, an implantation step of a dopant species (e.g., boron or aluminum) having a second conductivity type (here, P-type conductivity) is carried out (the implantation is represented in the figure by arrows 72). During the step of Figure 4, the guard ring 60, if present, is also formed.

[0031] In one embodiment given by way of example, the implantation step of FIG. 18 atoms / cm 3 To form implanted region 59' having a doping concentration higher than 1×10 12 atoms / cm 3 〜1×10 15 atoms / cm 3 The implanted region includes one or more implants of a dopant species having the second conductivity type at a dose between 0.4 μm and 1 μm and at an implant energy between 30 keV and 400 keV, such that an implanted region is formed having a depth measured from surface 52 a between 0.4 μm and 1 μm.

[0032] 5, mask 70 is removed, and in FIG. 6, a heat treatment is performed on surface 52a to render it suitable for the development of one or more carbon-rich layers (e.g., graphene and / or graphite layers) as previously described in the implanted region 59′.

[0033] For that purpose, a laser source 80 is used, configured to generate a beam 82 that locally heats the surface 52a (in particular the implanted region 59') to a temperature of approximately 1500° C. to 2600° C. Given the maximum depth of the implanted region 59', a temperature of approximately 2000° C. at the level of the surface 52a is sufficient to ensure a temperature within the aforementioned range even at the maximum depth reached by the implanted region 59' (e.g., 1 μm).

[0034] This temperature favors the formation of a carbon-rich ohmic contact compound exclusively in the implanted region 59', and not in the surface 52a where the implanted region 59' is not present. This effect is of a known type and is described, for example, in Maxime G. Lemitre, "Low-temperature, site-selective graphitization of SiC via ion implantation and pulsed laser annealing," APPLIED PHYSICS LETTERS 100, 193105 (2012).

[0035] In one embodiment, conversion of a portion of implanted region 59' to ohmic contact 59'' occurs by heating the entire wafer 100 by moving laser 80 accordingly.

[0036] In a further embodiment, the conversion of the surface portion of implanted region 59′ to ohmic contact 59″ occurs by heating the useful surface of wafer 100. Here, “useful surface” refers to the surface portion of drift layer 52 that includes implanted region 59′ that is outwardly bounded by edge termination region 10, for example, and may not correspond to the entire surface of wafer 100 (e.g., excluding potentially some portion of wafer 100 lateral to active area 54 that is not of interest during use of MPS device 50 in that it does not participate in charge transport).

[0037] According to a further embodiment, a mask can be provided above (in contact with or at a distance from) surface 52a having areas transparent to beam 82 (i.e., areas through which beam 82 passes) and areas opaque to beam 82 (i.e., areas through which beam 82 does not pass or passes in an attenuated manner so as not to cause significant heating of the underlying portion of wafer 100). The transparent areas of the mask are aligned with implanted regions 59' to allow for the formation of respective ohmic contacts 59".

[0038] Regardless of the embodiment employed, implanted region 59' (particularly, about 1×10 17 atoms / cm 3 〜1×10 20 atoms / cm 3 59"。 Furthermore, since the ohmic contacts are formed exclusively on the implanted regions 59', even in the absence of a mask, there is self-alignment between the implanted regions 59' and the respective ohmic contacts 59".

[0039] In implanted region 59', a localized surface increase in temperature causes the formation of ohmic contact 59", while laterally with respect to implanted region 59', this effect is not significant. The conversion of P-type SiC to graphene occurs between 1200°C and 2600°C, more particularly at temperatures above 1600°C. According to the invention, these temperatures are achieved in the surface portion (a few nanometers, e.g., 1 to 20 nm) of implanted region 59'. At greater depths, the temperature decreases to a value that no longer causes the conversion of silicon carbide to a carbon-rich layer (graphene and / or graphite layer). Therefore, the formation of the ohmic contact 59" is self-limiting. As a result, the ohmic contact 59" does not extend through the thickness of the respective implanted region, but is solely at its surface level.

[0040] The laser 80 is, for example, a UV excimer laser. Other types of lasers can also be used, among them lasers with wavelengths in the visible light range.

[0041] The configuration and activation parameters of the laser 80 that have been optimized for the purposes of the present invention, i.e., that allow the formation of a graphene ohmic contact in the injection region 59', are as follows:

[0042] The wavelength is between 290 and 370 nm, in particular 310 nm.

[0043] The pulse duration is between 100 ns and 300 ns, in particular 160 ns.

[0044] The number of pulses is between 1 and 10, in particular 4.

[0045] Energy density is (2) 1.6 to 4 J / cm 3 Especially (3) 2.6 J / cm 3 (considered at the level of surface 52a).

[0046] The temperature is between 1400° C. and 2600° C., in particular 1800° C. (considered at the level of the surface 52a).

[0047] The spot area of ​​the beam 82 at the level of the surface 52a is, for example, 0.7 to 1.5 cm 2 It is between.

[0048] One or more scans of the laser 80 are performed in plane XY (e.g., multiple scans parallel to each other and to axis X and / or axis Y) to cover the entire wafer 100 or a sub-region of the wafer 100 to be heated.

[0049] However, as has been discovered by the present invention, the aforementioned parameters result in the desired electrical behavior of MPS device 50. Figure 7 illustrates experimental data in this regard, showing the change in conduction current as a function of the voltage applied between the anode and cathode of MPS device 50. Curve S1 relates to electrical measurements on the PiN diode before laser treatment, while curve S2 relates to electrical measurements on the PiN diode after laser treatment and thus ohmic contact formation. The profiles of curves S1 and S2 confirm that the expected behavior is achieved.

[0050] In view of the properties of the present invention obtained based on this disclosure, the advantages achieved by the present invention are clear.

[0051] While specific embodiments of the present invention have been described in detail above, the present invention is not limited to these specific embodiments, and various modifications and alterations can be made without departing from the scope of the present invention. In particular, as already mentioned above, the present invention is not limited to ohmic contact formation in MPS devices, but also extends to ohmic contact formation in general vertical conduction electron devices such as Schottky diodes, JBS diodes, MOSFETs, IGBTs, JFETs, and DMOSs.

Claims

1. 1. A method of manufacturing a SiC-based electronic device (50), the electronic device (50) including a merged PiN Schottky (MPS) diode, the method comprising: forming a solid body of SiC including providing an N-type SiC substrate having an N-type SiC solid body with opposed front and back sides, and epitaxially growing an N-type SiC drift layer (52) on the front side of the substrate; implanting in a front side (52a) of a solid body (52) of SiC having an N-type conductivity type and a P-type dopant species and forming an implanted region (59'), the implanted region starting from the front side (52a) of the solid body and extending to a depth into the solid body and having an upper surface flush with the front side (52a) of the solid body; generating a laser beam (82) directed toward the implanted region (59') to generate heating of the implanted region (59') to a temperature between 1500°C and 2600°C to activate the P-type dopant species while simultaneously forming an ohmic contact region (59") comprising one or more carbon-rich layers, particularly graphene and / or graphite layers, within the implanted region (59'), the ohmic contact region (59") configured to form a Schottky diode with the drift layer (52); A way of embracing that.

2. The laser beam (82) wavelengths between 290 nm and 370 nm, a pulse duration between 100 and 300 ns, a number of pulses between 1 and 10, 1.6 to 4 J / cm ２ The energy density between 2. The method of claim 1, wherein the parameter is generated under the following conditions:

3. 3. A method according to claim 1 or 2, wherein the heating of the implanted region (59') is carried out along the direction (Z) of the implanted region (59') throughout its thickness.

4. 4. The method of claim 1, wherein forming the ohmic contact region (59") comprises forming the one or more carbon-rich layers starting from the front side (52a) and into the implanted region (59').

5. The method of claim 4, wherein the ohmic contact region (59") has an upper surface thereof coincident with an upper surface of the implanted region (59').

6. 6. The method of any one of claims 1 to 5, wherein the ohmic contact region (59") has a thickness between 1 nm and 20 nm.

7. 7. A method according to any one of claims 1 to 6, wherein the material of the solid body is one of 4H-SiC, 6H-SiC, 3C-SiC, 15R-SiC.

8. forming a first electrical terminal (58) electrically contacting the implanted region (59') through the ohmic contact region (59") and directly electrically contacting the drift layer (52) laterally with respect to the implanted region (59') to form a junction barrier (JB) diode with the implanted region (59') and a Schottky diode with the drift layer (52); forming a second electrical terminal (57) on the back side of the substrate; 2. The method of claim 1, comprising:

9. A SiC-based electronic device (50), said electronic device (50) comprising a merged PiN Schottky (MPS) diode; The combined PiN Schottky (MPS) diode is a solid body (52) of SiC having N-type conductivity, the solid body having opposite front and back sides, the solid body including an N-type SiC substrate and an N-type SiC drift layer (52) on the front side of the substrate; an implanted region (59') in the front side (52a) of the solid body (52), the implanted region (59') containing a P-type dopant species, extending from the front side (52a) into the solid body to a depth, and having an upper surface coplanar with the front side (52a) of the solid body; an ohmic contact region (59") extending into the injection region (59'), the ohmic contact region (59") including one or more carbon-rich layers, in particular graphene and / or graphite layers, the ohmic contact region (59") forming a Schottky diode with the drift layer (52); An electronic device comprising:

10. 10. The electronic device of claim 9, wherein the ohmic contact region (59") has the one or more carbon-rich layers extending exclusively within the implanted region starting from the front side (52a) of the solid body.

11. 11. The electronic device of claim 10, wherein the ohmic contact region (59") has its upper surface coinciding with the upper surface of the implanted region (59').

12. 12. The electronic device according to any one of claims 9 to 11, wherein the ohmic contact region (59") has a thickness between 1 nm and 20 nm.

13. 13. The electronic device according to any one of claims 9 to 12, wherein the material of the solid body is one of 4H-SiC, 6H-SiC, 3C-SiC, and 15R-SiC. a first electrical terminal (58) electrically contacting the injection region (59') through the ohmic contact region (59") and electrically contacting the drift layer (52) laterally with respect to the injection region (59') directly to form a junction barrier (JB) diode with the injection region (59') and a Schottky diode with the drift layer (52); and a second electrical terminal (57) on the back side of the substrate; 14. The electronic device of any one of claims 9 to 13, further comprising:

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