US20230411518A1 - Semiconductor device comprising a lateral super junction field effect transistor - Google Patents
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 28
- 230000005669 field effect Effects 0.000 title claims abstract description 4
- 239000000758 substrate Substances 0.000 claims abstract description 18
- 230000003247 decreasing effect Effects 0.000 claims description 2
- 230000005684 electric field Effects 0.000 description 10
- 230000015556 catabolic process Effects 0.000 description 8
- 238000005468 ion implantation Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000001419 dependent effect Effects 0.000 description 1
- 238000002513 implantation Methods 0.000 description 1
- 229920002120 photoresistant polymer Polymers 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
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- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
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- H01L29/68—Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/80—Field effect transistors with field effect produced by a PN or other rectifying junction gate, i.e. potential-jump barrier
- H01L29/808—Field effect transistors with field effect produced by a PN or other rectifying junction gate, i.e. potential-jump barrier with a PN junction gate, e.g. PN homojunction gate
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- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/78—Field effect transistors with field effect produced by an insulated gate
- H01L29/7831—Field effect transistors with field effect produced by an insulated gate with multiple gate structure
- H01L29/7832—Field effect transistors with field effect produced by an insulated gate with multiple gate structure the structure comprising a MOS gate and at least one non-MOS gate, e.g. JFET or MESFET gate
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- H01L29/0611—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices
- H01L29/0615—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices by the doping profile or the shape or the arrangement of the PN junction, or with supplementary regions, e.g. junction termination extension [JTE]
- H01L29/063—Reduced surface field [RESURF] pn-junction structures
- H01L29/0634—Multiple reduced surface field (multi-RESURF) structures, e.g. double RESURF, charge compensation, cool, superjunction (SJ), 3D-RESURF, composite buffer (CB) structures
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- H01L29/08—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions with semiconductor regions connected to an electrode carrying current to be rectified, amplified or switched and such electrode being part of a semiconductor device which comprises three or more electrodes
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- H01L29/1066—Gate region of field-effect devices with PN junction gate
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- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/66007—Multistep manufacturing processes
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- H01L29/66227—Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials the devices being controllable only by the electric current supplied or the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched, e.g. three-terminal devices
- H01L29/66409—Unipolar field-effect transistors
- H01L29/66893—Unipolar field-effect transistors with a PN junction gate, i.e. JFET
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- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/68—Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/78—Field effect transistors with field effect produced by an insulated gate
- H01L29/7801—DMOS transistors, i.e. MISFETs with a channel accommodating body or base region adjoining a drain drift region
- H01L29/7816—Lateral DMOS transistors, i.e. LDMOS transistors
- H01L29/7825—Lateral DMOS transistors, i.e. LDMOS transistors with trench gate electrode
Definitions
- the stack of alternating n- and p-layers will, if they are matched in charge, completely deplete each other and a uniform electric field can be formed in the material with almost op-timal use of the material in terms of breakdown voltage.
- the stack of alternating n- and p-layers needs to be terminated at the bottom and the field needs to turn 90 degrees since the substrate is grounded and have constant potential along the whole drift region. This will increase the electric field locally and this increase in field will induce an electric breakdown lowerthan the breakdown in the stack.
- US 2011/0127606 A1 suggests an n-buffer layer ( 160 ) that is located under the bottom channel all the way between the source and drain, or partially ( 160 - 1 ) between the source and drain. Another suggestion is to place a floating n+region ( 661 ) in the substrate under the drain to shield the drain from the high field.
- US 2017/0222043 A1 suggests a diffused p-region ( 253 ) and/or a diffused n-region ( 252 ) under the source and drain respectively, also to shape the electric field and decrease the maximum electric field.
- US 2019/0198609 A1 suggests a region ( 202 ) with linear or non-linear increasing thickness going from the source to the drain. This is also with the intention to shape the electric field.
- the stack of n- and p-layers is previously demonstrated in several places in the above cited documents.
- the bottom channel is abruptly ended at the drain and under the channel the substrate is acting as a bottom gate and also a substrate that should support the breakdown voltage of the device.
- the electric field is perfectly lateral but under the drain it has to turn to a vertical field since the backside is grounded. This means that the field has to turn 90 degrees under the bottom channel in the substrate. If nothing is done, the electric field profile from source to drain will form a U-shape with highest field near the drain.
- the U-shape means that the field is not uniformly distributed, and the breakdown voltage will be lower than is possible.
- the present invention relates to a semiconductor device comprising a lateral super junction field effect transistor, JFET, that can be implemented by placing a plurality of alternating n- and p-type layers on top of each other and connecting them in parallel.
- JFET lateral super junction field effect transistor
- the object of the present invention is to reduce the above drawbacks and to obtaining a higher breakdown voltage.
- FIG. 1 shows a first embodiment of the invention
- FIG. 2 shows a second embodiment of a further development of the invention.
- FIG. 1 shows the invention, starting with a highly doped substrate 1 of first conductivity type which is connected to a grounded back contact. On the substrate is a thick, low-doped layer 2 of first conductivity type epitaxially grown. The thickness of the epitaxial layer should be large enough to support the breakdown voltage of the device. On the low-doped layer 2 of first conductivity type is a layer n1 of second conductivity type epitaxially grown. On the epitaxial layer n1 is an implantation mask placed and ion implantation is done forming a masked layer p1 of first conductivity type.
- first conductivity type p2 By partitioning the layer and varying the lengths and distances of the resulting p-regions in the masked layer of first conductivity type p1, the effective amount of charges of first conductivity type will decrease towards to the drain side D of the structure. This will decrease the electric field near drain and thus a more uniform electric field is achieved and a higher breakdown voltage.
- an epitaxial layer of second conductivity type n2 placed and a first gate of the first conductivity type is either implanted or epitaxially grown on the channel n2.
- a semiconductor device according to the invention can be combined with a further isolated region X arranged over the substrate, comprising logics and analogue control functions, isolated with deep polycrystalline trenches of the first conductivity type 4, on both sides thereof, to the left of the parts shown in the figure.
- a semiconductor device is e.g. described in U.S. Pat. No. 11,031,480 B2.
- consecutive dots 5 of different lengths have decreasing lengths in direction towards the drain side D of the structure, and the distances 6 between the dots 5 increase in the direction towards the drain side D of the structure.
- the whole structure is mirrored around the line of symmetry L which allows for high voltage on the drain trench.
- FIG. 2 shows a modified device where the gate layers p2-p5 are made with ion implantation through a photoresist mask creating interruptions 7 in the layers p2-p5 of first conductivity type.
- the doping is the same as in the adjacent channel regions n2-n5 of second conductivity type.
- the interruptions 7 are evenly distributed along the drift region.
- the interruptions 7 in the layer will divide the region in several shorter regions 8 of first conductivity type.
- the leftmost region of the shorter regions is connected to the ground as described earlier and the other regions are floating.
- the floating regions of first conductivity type will deplete the channel region less than a long p-gate which is grounded along the whole drift region. This will increase the current through the device for low drain voltages. For higher voltages a current will flow through the shorter regions and connecting them together.
- the length of the interruptions 7 should not be too large.
- the distance 7 between the regions 8 can be about 0.3 ⁇ m, and the length of the regions 8 can be about 5 ⁇ m.
- the device according to the invention has been described when the first conductivity type is p-type, and the second conductivity type is n-type.
- the device according to the invention can also be implemented so that the first conductivity type is n-type, and the second conductivity type is p-type.
Abstract
Disclosed is a semiconductor device, including: a substrate of a first conductivity type that is a base for the semiconductor device; a high voltage junction field effect transistor, JFET, over the substrate, wherein the JFET including a plurality of parallel conductive layers; and a first conductive layer of the second conductivity type of the parallel conductive layers stretching over the substrate. On top of the first conductive layer of the second conductivity type is arranged a plurality of layers forming the parallel conductive layers with channels formed by a plurality of doped epitaxial layers of the second conductivity type with a plurality of gate layers of the first conductivity type on both sides thereof; wherein a lowermost layer of the first conductivity type is arranged in the form of consecutive dots with different lengths and distances between them.
Description
- Such devices have previously been described in many patent documents, e.g. in U.S. Pat. No. 11,031,480 B2, US 2019/0198609 A1, US 2017/0222043 A1, and US 2011/0127606 A1.
- The stack of alternating n- and p-layers will, if they are matched in charge, completely deplete each other and a uniform electric field can be formed in the material with almost op-timal use of the material in terms of breakdown voltage. The stack of alternating n- and p-layers needs to be terminated at the bottom and the field needs to turn 90 degrees since the substrate is grounded and have constant potential along the whole drift region. This will increase the electric field locally and this increase in field will induce an electric breakdown lowerthan the breakdown in the stack. Several different attempts to shape the electric field have been demonstrated.
- US 2011/0127606 A1 suggests an n-buffer layer (160) that is located under the bottom channel all the way between the source and drain, or partially (160-1) between the source and drain. Another suggestion is to place a floating n+region (661) in the substrate under the drain to shield the drain from the high field.
- US 2017/0222043 A1 suggests a diffused p-region (253) and/or a diffused n-region (252) under the source and drain respectively, also to shape the electric field and decrease the maximum electric field. US 2019/0198609 A1 suggests a region (202) with linear or non-linear increasing thickness going from the source to the drain. This is also with the intention to shape the electric field.
- The stack of n- and p-layers is previously demonstrated in several places in the above cited documents. Normally the bottom channel is abruptly ended at the drain and under the channel the substrate is acting as a bottom gate and also a substrate that should support the breakdown voltage of the device. In the channels the electric field is perfectly lateral but under the drain it has to turn to a vertical field since the backside is grounded. This means that the field has to turn 90 degrees under the bottom channel in the substrate. If nothing is done, the electric field profile from source to drain will form a U-shape with highest field near the drain. The U-shape means that the field is not uniformly distributed, and the breakdown voltage will be lower than is possible.
- The present invention relates to a semiconductor device comprising a lateral super junction field effect transistor, JFET, that can be implemented by placing a plurality of alternating n- and p-type layers on top of each other and connecting them in parallel.
- The object of the present invention is to reduce the above drawbacks and to obtaining a higher breakdown voltage.
- This object is obtained by the device according to the present invention, where a lowermost layer of the first conductivity type is arranged in the form of consecutive dots with different lengths and distances between deep polycrystalline trenches of the second conductivity type in the bottom part of the JFET.
- Further improvements can be obtained through the devices defined in the dependent claims.
- The invention will now be explained with the help of a couple of non-limiting embodiments of a semiconductor device, focusing on the JFET part as shown on the accompanying drawings, in which:
-
FIG. 1 shows a first embodiment of the invention, and -
FIG. 2 shows a second embodiment of a further development of the invention. -
FIG. 1 . shows the invention, starting with a highly dopedsubstrate 1 of first conductivity type which is connected to a grounded back contact. On the substrate is a thick, low-dopedlayer 2 of first conductivity type epitaxially grown. The thickness of the epitaxial layer should be large enough to support the breakdown voltage of the device. On the low-dopedlayer 2 of first conductivity type is a layer n1 of second conductivity type epitaxially grown. On the epitaxial layer n1 is an implantation mask placed and ion implantation is done forming a masked layer p1 of first conductivity type. By partitioning the layer and varying the lengths and distances of the resulting p-regions in the masked layer of first conductivity type p1, the effective amount of charges of first conductivity type will decrease towards to the drain side D of the structure. This will decrease the electric field near drain and thus a more uniform electric field is achieved and a higher breakdown voltage. On top of the structure is now an epitaxial layer of second conductivity type n2 placed and a first gate of the first conductivity type is either implanted or epitaxially grown on the channel n2. These two layers are then repeated upwards as demonstrated in several earlier publications, e.g. in the above cited patent documents. - From the surface are deep trenches etched and then filled with highly doped silicon. In the figure is shown two filled
trenches 3 that are of second conductivity type and connecting the channels of second conductivity type n2-n6. The filledtrench 4 of first conductivity type is used to connect the layers of first conductivity type p1-p5. The gates p2-p5 are connected to ground in the third dimension, for example by making interruptions in the source trench as demonstrated in U.S. Pat. No. 11,031,480 B2, or by making filled trench pillars of first conductivity type as shown in US 2019/0198609 A1 and US 2017/0222043 A1. - A semiconductor device according to the invention can be combined with a further isolated region X arranged over the substrate, comprising logics and analogue control functions, isolated with deep polycrystalline trenches of the
first conductivity type 4, on both sides thereof, to the left of the parts shown in the figure. Such a semiconductor device is e.g. described in U.S. Pat. No. 11,031,480 B2. - Preferably the
consecutive dots 5 of different lengths have decreasing lengths in direction towards the drain side D of the structure, and thedistances 6 between thedots 5 increase in the direction towards the drain side D of the structure. - The whole structure is mirrored around the line of symmetry L which allows for high voltage on the drain trench.
-
FIG. 2 shows a modified device where the gate layers p2-p5 are made with ion implantation through a photoresistmask creating interruptions 7 in the layers p2-p5 of first conductivity type. In the interruptions the doping is the same as in the adjacent channel regions n2-n5 of second conductivity type. Theinterruptions 7 are evenly distributed along the drift region. Theinterruptions 7 in the layer will divide the region in severalshorter regions 8 of first conductivity type. The leftmost region of the shorter regions is connected to the ground as described earlier and the other regions are floating. For small drain voltages the floating regions of first conductivity type will deplete the channel region less than a long p-gate which is grounded along the whole drift region. This will increase the current through the device for low drain voltages. For higher voltages a current will flow through the shorter regions and connecting them together. - For this to happen the length of the
interruptions 7 should not be too large. E.g. thedistance 7 between theregions 8 can be about 0.3 μm, and the length of theregions 8 can be about 5 μm. - In the drawings the device according to the invention has been described when the first conductivity type is p-type, and the second conductivity type is n-type. However, the device according to the invention can also be implemented so that the first conductivity type is n-type, and the second conductivity type is p-type.
Claims (20)
1. A semiconductor device, comprising:
a substrate of a first conductivity type that is a base for the semiconductor device;
a high voltage junction field effect transistor, JFET, over the substrate, wherein the JFET comprising a plurality of parallel conductive layers, the JFET being isolated with a deep polycrystalline trench of a first conductivity type on a source side of the JFET;
a first conductive layer of the second conductivity type of the parallel conductive layers stretching over the substrate;
wherein on top of the first conductive layer of the second conductivity type is arranged a plurality of layers forming the parallel conductive layers with channels formed by a plurality of doped epitaxial layers of the second conductivity type with a plurality of gate layers of the first conductivity type on both sides thereof;
wherein,
a lowermost layer of the first conductivity type is arranged in the form of consecutive dots with different lengths and distances between them.
2. A semiconductor device according to claim 1 ,
wherein
the consecutive dots of different lengths have decreasing lengths in direction towards the drain side of the structure, and the distances between the dots increase in the direction towards the drain side of the structure.
3. A semiconductor device according to claim 1 , wherein
the conductive layers of the first conductivity type above the first conductive layer of the first conductive type are comprised of consecutive regions with different lengths and distances between each of the regions and the deep polycrystalline trenches of the second conductivity type.
4. A semiconductor device according to claim 1 , wherein
a further isolated region is arranged over the substrate, comprising logics and analogue control functions, isolated with deep polycrystalline trenches of the first conductivity type on both sides thereof.
5. A semiconductor device according to claim 1 , wherein
the first conductivity type is p-type and the second conductivity type is n-type.
6. A semiconductor device according to claim 1 , wherein
the first conductivity type is n-type and the second conductivity type is p-type.
7. A semiconductor device according to claim 2 , wherein
the conductive layers of the first conductivity type above the first conductive layer of the first conductive type are comprised of consecutive regions with different lengths and distances between each of the regions and the deep polycrystalline trenches of the second conductivity type.
8. A semiconductor device according to claim 2 , wherein
a further isolated region is arranged over the substrate, comprising logics and analogue control functions, isolated with deep polycrystalline trenches of the first conductivity type on both sides thereof.
9. A semiconductor device according to claim 3 , wherein
a further isolated region is arranged over the substrate, comprising logics and analogue control functions, isolated with deep polycrystalline trenches of the first conductivity type on both sides thereof.
10. A semiconductor device according to claim 7 , wherein
a further isolated region is arranged over the substrate, comprising logics and analogue control functions, isolated with deep polycrystalline trenches of the first conductivity type on both sides thereof.
11. A semiconductor device according to claim 2 , wherein
the first conductivity type is p-type and the second conductivity type is n-type.
12. A semiconductor device according to claim 3 , wherein
the first conductivity type is p-type and the second conductivity type is n-type.
13. A semiconductor device according to claim 4 , wherein
the first conductivity type is p-type and the second conductivity type is n-type.
14. A semiconductor device according to claim 7 , wherein
the first conductivity type is p-type and the second conductivity type is n-type.
15. A semiconductor device according to claim 8 , wherein
the first conductivity type is p-type and the second conductivity type is n-type.
16. A semiconductor device according to claim 9 , wherein
the first conductivity type is p-type and the second conductivity type is n-type.
17. A semiconductor device according to claim 10 , wherein
the first conductivity type is p-type and the second conductivity type is n-type.
18. A semiconductor device according to claim 2 , wherein
the first conductivity type is n-type and the second conductivity type is p-type.
19. A semiconductor device according to claim 3 , wherein
the first conductivity type is n-type and the second conductivity type is p-type.
20. A semiconductor device according to claim 4 , wherein
the first conductivity type is n-type and the second conductivity type is p-type.
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US17/845,789 US11837658B1 (en) | 2022-06-21 | 2022-06-21 | Semiconductor device comprising a lateral super junction field effect transistor |
PCT/SE2023/050602 WO2023249538A1 (en) | 2022-06-21 | 2023-06-15 | A semiconductor device comprising a lateral super junction field effect transistor |
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US20170222043A1 (en) * | 2016-01-29 | 2017-08-03 | Infineon Technologies Austria Ag | Semiconductor Device Including a Lateral Transistor |
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US8575695B2 (en) | 2009-11-30 | 2013-11-05 | Alpha And Omega Semiconductor Incorporated | Lateral super junction device with high substrate-drain breakdown and built-in avalanche clamp diode |
US11031480B2 (en) | 2019-09-13 | 2021-06-08 | K. Eklund Innovation | Semiconductor device, comprising an insulated gate field effect transistor connected in series with a field effect transistor |
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