SEMICONDUCTOR DEVICE HAVING SUPER JUNCTION METAL OXIDE SEMICONDUCTOR STRUCTURE AND FABRICATION METHOD FOR THE SAME

Abstract

A semiconductor device includes: a first base layer; a drain layer disposed on the back side surface of the first base layer; a second base layer formed on the surface of the first base layer; a source layer formed on the surface of the second base layer; a gate insulating film disposed on the surface of both the source layer and the second base layer; a gate electrode disposed on the gate insulating film; a column layer formed in the first base layer of the lower part of both the second base layer and the source layer by opposing the drain layer; a drain electrode disposed in the drain layer; and a source electrode disposed on both the source layer and the second base layer, wherein heavy particle irradiation is performed to the column layer to form a trap level locally.

Claims

1. A semiconductor device, comprising: a first base layer of a first conductivity type; a drain layer of the first conductivity type formed on a back side surface of the first base layer; a second base layer of a second conductivity type formed in a surface side of the first base layer; a source layer of the first conductivity type formed in a surface side of the second base layer; a gate insulating film disposed on a surface of both the source layer and the second base layer; a gate electrode disposed on the gate insulating film; a column layer of the second conductivity type formed in the first base layer directly below both the second base layer and the source layer by opposing the drain layer so that a long-side direction of the column layer is vertical to a principal surface of the drain layer; a drain electrode disposed on the drain layer; and a source electrode disposed on both the source layer and the second base layer, wherein the column layer and the first base layer are alternately-arranged repeatedly in a direction parallel to the principal surface of the drain layer, and a bottom surface of the column layer and a top surface of the drain layer are separated from each other, a space is defined between a bottom surface of the column layer and the upper surface of the drain layer, the bottom surface of the column layer or an upper portion of the space is subjected to a charged particle irradiation, and a resistance value of the upper portion of the space is higher than a resistance value of a lower portion of the space.

2. The semiconductor device according to claim 1, wherein the charged particle irradiation is performed to a lower part of the column layer to form a trap level locally.

3. The semiconductor device according to claim 2, wherein the trap level is due to the charged particle irradiation.

4. The semiconductor device according to claim 1, wherein the charged particle irradiation is applied at a target position that is between a first position and a second position between the bottom surface of the column layer and the top surface of the drain layer, the first position corresponds to a first distance from the bottom surface of the column layer at which reverse recovery time is shorter than a predetermined time period, and the second position corresponds to a second distance from the bottom surface of the column layer at which a saturation current between the drain electrode and the source electrode is lower than a predetermined saturation current.

5. The semiconductor device according to claim 1, wherein an amount of dosage of the charged particle irradiation is 5×10.sup.10/cm.sup.2 to 5×10.sup.12/cm.sup.2.

6. The semiconductor device according to claim 1, wherein a planar pattern on the basis of one of a rectangle and a hexagon is disposed being checkered lattice-like or zigzagged checkered lattice-like, in the first base layer, the second base layer, and the source layer.

7. The semiconductor device according to claim 1, wherein the bottom surface of the column layer and the drain layer are separated by the first base layer.

8. The semiconductor device according to claim 2, wherein the trap level extends over the column layer and the first base layer.

9. The semiconductor device according to claim 1, wherein a distance between two neighboring column layers is smaller than a width of each of the column layers.

10. The semiconductor device according to claim 1, wherein the charged particle irradiation is one of .sup.3He.sup.++ and .sup.4He.sup.++ and is applied to the column layer so that a peak position having a highest resistivity is formed at a bottom surface portion of the column layer.

11. A fabrication method for a semiconductor device, comprising: forming a first base layer of a first conductivity type; forming a drain layer of the first conductivity type on a back side surface of the first base layer; forming a second base layer of a second conductivity type in a surface side in the first base layer; forming a source layer of the first conductivity type in a surface side in the second base layer; forming a gate insulating film on a surface of both the source layer and the second base layer; forming a gate electrode on the gate insulating film; forming a column layer of the second conductivity type in the first base layer directly below both the second base layer and the source layer by opposing the drain layer so that a long-side direction of the column layer is vertical to a principal surface of the drain layer; forming a drain electrode on the drain layer, forming a source electrode on both the source layer and the second base layer; and performing a charged particle irradiation to a bottom surface of the column layer or an upper portion of a space, the space being defined between the bottom surface of the column layer and an upper surface of the drain layer, a resistance value of the upper portion of the space being higher than a resistance value of a lower portion of the space, wherein the column layer and the first base layer are alternately-arranged repeatedly in a direction parallel to the principal surface of the drain layer, and a bottom surface of the column layer and a top surface of the drain layer are separated from each other.

12. The fabrication method for the semiconductor device according to claim 11, wherein the charged particle irradiation is performed to a lower part of the column layer to form a trap level locally.

13. The fabrication method for the semiconductor device according to claim 12, wherein the trap level is due to the charged particle irradiation.

14. The fabrication method for the semiconductor device according to claim 12, wherein the trap level is formed by: determining a first position between the bottom surface of the column layer and the top surface of the drain layer, by obtaining a first distance from the bottom surface of the column layer so that reverse recovery time is shorter than a predetermined time period, on the basis of the bottom surface of the column layer; determining a second position between the bottom surface of the column layer and the top surface of the drain layer, by obtaining a second distance from the bottom surface of the column layer so that a saturation current between the drain electrode and the source electrode is lower than a predetermined saturation current; and performing the charged particle irradiation so that an attenuation peak position is included between the first position and the second position.

15. The fabrication method for the semiconductor device according to claim 11, wherein an amount of dosage of the charged particle irradiation is 5×10.sup.10/cm.sup.2 to 5×10.sup.12/cm.sup.2.

16. The fabrication method for the semiconductor device according to claim 11, wherein a planar pattern on the basis of one of a rectangle and a hexagon is disposed being checkered lattice-like or zigzagged checkered lattice-like, in the first base layer, the second base layer, and the source layer.

17. The fabrication method for the semiconductor device according to claim 12, wherein the trap level is formed both along the first direction and along a second direction parallel to the principal surface of the drain layer so as to contact both the column layer and the first base layer.

18. The fabrication method for the semiconductor device according to claim 11, wherein the charged particle irradiation is one of .sup.3He.sup.++ and .sup.4He.sup.++ and is applied to the column layer so that a peak position having a highest resistivity is formed at a bottom surface portion of the column layer.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0020] FIG. 1 A schematic cross-sectional configuration diagram of a semiconductor device according to a first embodiment of the present invention.

[0021] FIG. 2 A schematic bird's-eye view of the semiconductor device according to the first embodiment of the present invention.

[0022] FIG. 3 A schematic planar pattern configuration diagram of the semiconductor device according to the first embodiment of the present invention.

[0023] FIG. 4 An alternative schematic planar pattern configuration diagram of the semiconductor device according to the first embodiment of the present invention.

[0024] FIG. 5 An example of a switching waveform of a comparative example of the semiconductor device according to the first embodiment of the present invention.

[0025] FIG. 6 The schematic cross-sectional configuration diagram explaining the relation between the irradiation target position and the device structure, in the case of .sup.3He.sup.++ ion irradiation to the semiconductor device according to the first embodiment of the present invention from a back side surface.

[0026] FIG. 7 A diagram showing the relation between a saturation current I.sub.DSS between the drain and the source and a distance from a bottom surface of a column layer, in the semiconductor device according to the first embodiment of the present invention.

[0027] FIG. 8 A diagram showing the relation between the reverse recovery time trr and the distance from the bottom surface of the column layer, in the semiconductor device according to the first embodiment of the present invention.

[0028] FIG. 9 A schematic diagram showing the relation between the reverse recovery time trr and the saturation current I.sub.DSS between the drain and the source and the distance from the bottom surface of the column layer, in the semiconductor device according to the first embodiment of the present invention.

[0029] FIG. 10 A diagram showing the relation between impurity concentration N, resistivity and sheet resistance R and the distance from the bottom surface of the column layer, in the semiconductor device related to the first embodiment of the present invention.

[0030] FIG. 11 A schematic bird's-eye view of a semiconductor device according to a conventional example.

[0031] FIG. 12 An example of a switching waveform of the semiconductor device according to the conventional example.

DESCRIPTION OF EMBODIMENTS

[0032] Next, embodiments of the present invention will be described with reference to drawings. It explains simple by attaching the same reference numeral as the same block or element to below, in order to avoid duplication of description. However, the drawings are schematic and it should care about differing from an actual thing. Of course, the part from which the relation or ratio between the mutual sizes differ also in mutually drawings may be included.

[0033] The embodiments shown in the following exemplifies the device and method for materializing the technical idea of the present invention, and the embodiments of the present invention does not specify assignment of each component parts, etc. as the following. Various changes can be added to the technical idea of the present invention in scope of claims.

First Embodiment

(Element Structure)

[0034] FIG. 1 shows a schematic cross-section structure of a semiconductor device according to a first embodiment of the present invention. Moreover, FIG. 2 shows a schematic bird's-eye view structure of the semiconductor device according to the first embodiment. As shown in FIG. 1 to FIG. 2, the semiconductor device according to the first embodiment includes: an n type impurity doped high resistivity first base layer 12; an n type impurity doped drain layer 10 disposed on the back side surface of the first base layer 12; a p type impurity doped second base layer 16 famed on the surface of the first base layer 12; an n type impurity doped source layer 18 famed on the surface of the second base layer 16; a gate insulating film 20 disposed on the surface of both the source layer 18 and the second base layer 16; a gate electrode 22 disposed on the gate insulating film 20; a p type impurity doped column layer 14 famed in the first base layer 12 of the lower part of both the second base layer 16 and the source layer 18 by opposing the drain layer 10; a drain electrode 28 disposed in the drain layer 10; and a source electrode 26 disposed on both the source layer 18 and the second base layer 16. An interlayer insulating film 24 is disposed on the gate electrode 22. Dashed lines shown in FIG. 1 indicate current which flows between the drain and the source. As clearly illustrated in FIGS. 1 and 2, the column layer 14 extends in a first direction vertical to a principal surface of the drain layer 10, a length of the column layer 14 in the first direction being larger than a length thereof in a second direction that is parallel to the principal surface of the drain layer 10. The column layer 14 and the first base layer 12 are repeatedly alternately-arranged in the second direction.

[0035] In the semiconductor device according to the first embodiment, a trap level (see “TR” in FIG. 1) is formed locally by performing heavy particle irradiation to the column layer 14. Thus, as illustrated in FIG. 1, the trap level is formed below the second base layer 16.

[0036] P, As, Sb, etc. can be applied as the n type impurity, and B, Al, Ga, etc. can be applied as the p type impurity, for example. The above-mentioned impurities can be doped on each layer using diffusion technology or ion implantation technology.

[0037] A silicon dioxide film, a silicon nitride film, a silicon oxynitride film, a hafnium oxide film, an alumina film, a tantalum oxide film, etc. can be applied, for example, as the gate insulating film 20.

[0038] Polysilicon can be applied as the gate electrode 22, and aluminum can be applied to both the drain electrode 28 and the source electrode 26, for example.

[0039] A silicon dioxide film, a silicon nitride film, a tetraethoxy silane (TEOS) film, etc. are applicable, for example, as the interlayer insulating film 24.

[0040] In the example of FIG. 2, the schematic planar pattern configuration of the semiconductor device according to the first embodiment shows an example which is disposed being checkered lattice-like on the basis of a rectangular pattern. On the other hand, as shown in FIG. 3, the planar pattern configuration may be disposed being zigzagged checkered lattice-like on the basis of a rectangular pattern, for example. Alternatively, as shown in FIG. 4, the planar pattern configuration may be disposed being zigzagged checkered lattice-like on the basis of a hexagonal pattern, for example. Moreover, the planar pattern configuration is not limited to the rectangle or the hexagon. That is, the planar pattern configuration is also effective on the basis of circular, an oval figure, a pentagon, a polygon greater than heptagon, etc. Each of FIG. 3 and FIG. 4 shows schematically the pattern of semiconductor layers, such as the first base layer 12, the column layer 14, the second base layer 16, and the source layer 18. However, illustrating of the gate electrode 22, the source electrode 26, etc. is omitted.

[0041] FIG. 5 shows an example of a switching waveform in the comparative example which does not control life time by the heavy particle irradiation, in the semiconductor device according to the first embodiment. The reverse recovery time trr is 160 nsec according to a result shown in FIG. 5, and is longer than the reverse recovery time being 130 nsec of the conventional example shown in FIG. 12.

[0042] FIG. 6 shows a schematic cross-section structure for explaining the relation between an irradiation target position and device structure, in the case of performing .sup.3He.sup.++ ion irradiation (IR) to the semiconductor device according to the first embodiment from the back side surface.

[0043] In FIG. 6, WA denotes the thickness of the drain layer 10 measured from the back side surface of the semiconductor device. Also, WB denotes the distance to the bottom surface of the column layer 14 measured from the back side surface of the semiconductor device. In the example shown in FIG. 6, it is WA=208 μm, and is WB=220 μm.

[0044] Moreover, as shown in FIG. 6, a coordinate system is defined by applying the direction of the source electrode 26 into a positive direction and applying the direction of the drain layer 10 into a negative direction on the basis of the bottom surface of the column layer 14. The irradiation target position can be defined as an attenuation peak position of the range of the heavy ion irradiated from the back side surface of the semiconductor device, and can be indicated on the above-mentioned coordinate system.

(Result of Experiment)

[0045] FIG. 7 shows the relation between the saturation current I.sub.DSS between the drain and the source and the distance from the bottom surface of the column layer 14 corresponding to the attenuation peak position, in the semiconductor device according to the first embodiment. FIG. 7 shows the case of the amount of dosage of .sup.3He ion is set to 1×10.sup.12/cm.sup.2, and is set to 5×10.sup.12/cm.sup.2.

[0046] Moreover, FIG. 8 shows the relation between the reverse recovery time trr and the distance from the bottom surface of the column layer 14 corresponding to the attenuation peak position, in the semiconductor device according to the first embodiment. FIG. 8 also shows the case of the amount of dosage of .sup.3He.sup.++ ion is set to 1×10.sup.12/cm.sup.2, cm and is set to 5×10.sup.12/cm.sup.2.

[0047] As clearly from FIG. 7, the value of the saturation current I.sub.DSS between the drain and the source tends to decrease as the distance from the bottom surface of the column layer 14 corresponding to the attenuation peak position increases. On the other hand, as clearly from FIG. 8, the reverse recovery time trr tends to increase as the distance from the bottom surface of the column layer 14 corresponding to the attenuation peak position increases.

[0048] FIG. 9 shows schematically the relation between: the reverse recovery time trr and the saturation current I.sub.DSS between the drain and the source; and the distance from the bottom surface of the column layer 14, in the semiconductor device according to the first embodiment.

[0049] In the semiconductor device according to the first embodiment, the heavy particle irradiation is performed so that the attenuation peak position of the heavy particle irradiation may be included between: the first position PB obtained from the relation between the distance from the bottom surface of the column layer 14 and the reverse recovery time trr on the basis of the bottom surface of the column layer 14; and the second position PA obtained from the relation between the distance from the bottom surface of the column layer 14 and the saturation current I.sub.DSS between the drain and the source, and thereby it can be obtained of the semiconductor device having the reverse recovery time trr shorter than the reverse recovery time t.sub.0, and having the saturation current I.sub.DSS between the drain and the source smaller than the saturation current I.sub.0 between the drain and the source. In FIG. 9, the curve D denotes the attenuation peak curve of the heavy particle irradiation for obtaining the semiconductor device having the reverse recovery time trr shorter than the reverse recovery time t.sub.0, and having the saturation current I.sub.DSS between the drain and the source smaller than the saturation current I.sub.0 between the drain and the source.

[0050] Here, the first position PB is the attenuation peak position of the heavy particle irradiation corresponding to the reverse recovery time t.sub.0. Moreover, the second position PA is the attenuation peak position of the heavy particle irradiation corresponding to the saturation current I.sub.0 between the drain and the source. For example, when the reverse recovery time t.sub.0 is set to 80 nsec and the saturation current I.sub.0 between the drain and source is set to 1 μA, it can be obtained of the semiconductor device whose the reverse recovery time trr<t.sub.0=80 nsec, and the saturation current between the drain and the source I.sub.DSS<I.sub.0=1 μA.

[0051] Here, a proton, .sup.3He.sup.++, or .sup.4He.sup.++ can be used for the particle species for performing the heavy particle irradiation, for example. When using .sup.4He.sup.++ as the particle species for performing the heavy particle irradiation, it is preferable to use the drain layer 10 composed of a thin substrate.

[0052] The amount of dosage of the heavy particle irradiation can be set as the scope of 5×10.sup.10/cm.sup.2 to 5×10.sup.12/cm.sup.2, for example.

[0053] FIG. 10 shows the relation between the impurity concentration N, the resistivity p, and sheet resistance R and the distance from the bottom surface of the column layer 14, in the semiconductor device according to the first embodiment. Corresponding to the tendency of the attenuation peak curve of heavy particle irradiation, the peak characteristics that the resistivity p and sheet resistance R increase are shown, and the peak characteristics that the impurity concentration N decreases are shown.

(Fabrication Method)

[0054] As shown in FIG. 1 to FIG. 2, a fabrication method of the semiconductor device according to the first embodiment includes: the step of forming a high resistivity first base layer 12 of a first conductivity type; the step of forming a drain layer 10 of the first conductivity type on the back side surface of the first base layer 12; the step of forming a second base layer 16 of a second conductivity type on the surface of the first base layer 12; the step of forming a source layer 18 of the first conductivity type on the surface of the second base layer 16; the step of forming a gate insulating film 20 on the surface of both the source layer 18 and the second base layer 16; the step of forming a gate electrode 22 on the gate insulating film 20; the step of forming a column layer 14 of the second conductivity type in the first base layer 12 of the lower part of both the second base layer 16 and the source layer 18 by opposing the drain layer 10; the step of forming a drain electrode 28 in the drain layer 10; the step of forming a source electrode in both the source layer and the second base layer; and the step of performing heavy particle irradiation to the column layer 14 and forming a trap level locally.

[0055] As shown in FIG. 9, the step of forming the trap level locally includes: the step of determining a first position PB based on the relation between the distance from the bottom surface of the column layer 14 and the reverse recovery time trr on the basis of the bottom surface of the column layer 14; the step of determining a second position PA obtained from the relation between the distance from the bottom surface of the column layer 14 and the saturation current I.sub.DSS between the drain and the source; and the step of performing the heavy particle irradiation so that an attenuation peak position may be included between the first position PB and the second position PA.

[0056] According to the first embodiment, it can achieve controlling degradation of both the saturation current I.sub.DSS between the drain and the source and the threshold value voltage between the gate and the source, and improving the reverse recovery characteristics of a built-in diode. Thus, it is possible to reduce the switching power loss, and reduce the diode reverse recovery loss.

[0057] According to the first embodiment, it can be provided of the semiconductor device including the super junction MOS structure where the reverse recovery time trr can be shortened without increasing the leakage current between the drain and the source, and can be provided of the fabrication method for such semiconductor device.

OTHER EMBODIMENTS

[0058] The present invention has been described by the first embodiment, as a disclosure including associated description and drawings to be construed as illustrative, not restrictive. With the disclosure, a person skilled in the art might easily think up alternative embodiments, embodiment examples, or application techniques.

[0059] Thus, the present invention includes various embodiments etc. which have not been described in this specification.

INDUSTRIAL APPLICABILITY

[0060] The semiconductor device according to the present invention is applicable to a bridge circuit, a LCD inverter, a motor, automotive High Intensity Discharge lamp (HID) headlight lighting apparatus, etc. which use a high breakdown voltage MOSFET.

REFERENCE SIGNS LIST

[0061] 10: Drain layer; [0062] 12: First base layer; [0063] 14: Column layer; [0064] 16: Second base layer; [0065] 18: Source layer; [0066] 20: Gate insulating film; [0067] 22: Gate electrode; [0068] 24: Interlayer insulating film; [0069] 26: Source electrode; and [0070] 28: Drain electrode.