WO1997011497A1 - Fabrication method of vertical field effect transistor - Google Patents
Fabrication method of vertical field effect transistor Download PDFInfo
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- WO1997011497A1 WO1997011497A1 PCT/JP1995/001885 JP9501885W WO9711497A1 WO 1997011497 A1 WO1997011497 A1 WO 1997011497A1 JP 9501885 W JP9501885 W JP 9501885W WO 9711497 A1 WO9711497 A1 WO 9711497A1
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- WIPO (PCT)
- Prior art keywords
- arsenic
- epi layer
- layer
- concentration
- effect transistor
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- 238000004519 manufacturing process Methods 0.000 title claims abstract description 26
- 230000005669 field effect Effects 0.000 title claims abstract description 24
- 238000000034 method Methods 0.000 title claims description 18
- 229910052785 arsenic Inorganic materials 0.000 claims abstract description 55
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 claims abstract description 55
- 239000012535 impurity Substances 0.000 claims abstract description 38
- 239000000758 substrate Substances 0.000 claims abstract description 35
- 238000009826 distribution Methods 0.000 claims abstract description 32
- 238000005468 ion implantation Methods 0.000 claims abstract description 14
- 239000004065 semiconductor Substances 0.000 claims description 11
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 claims description 8
- 229910052796 boron Inorganic materials 0.000 claims description 8
- 230000000694 effects Effects 0.000 claims description 3
- 230000005684 electric field Effects 0.000 claims 2
- 239000002699 waste material Substances 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 13
- 230000015556 catabolic process Effects 0.000 description 11
- 150000002500 ions Chemical class 0.000 description 9
- 230000008569 process Effects 0.000 description 8
- 230000006378 damage Effects 0.000 description 6
- 238000002513 implantation Methods 0.000 description 6
- 230000008859 change Effects 0.000 description 5
- 238000009792 diffusion process Methods 0.000 description 5
- 238000010438 heat treatment Methods 0.000 description 5
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 4
- 238000005516 engineering process Methods 0.000 description 4
- 238000000407 epitaxy Methods 0.000 description 4
- 229910052698 phosphorus Inorganic materials 0.000 description 4
- 239000011574 phosphorus Substances 0.000 description 4
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 3
- 229920005591 polysilicon Polymers 0.000 description 3
- 238000004364 calculation method Methods 0.000 description 2
- 230000003071 parasitic effect Effects 0.000 description 2
- 230000009467 reduction Effects 0.000 description 2
- 230000008901 benefit Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 210000004709 eyebrow Anatomy 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 238000000206 photolithography Methods 0.000 description 1
- 238000009827 uniform distribution Methods 0.000 description 1
Classifications
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/60—Insulated-gate field-effect transistors [IGFET]
- H10D30/64—Double-diffused metal-oxide semiconductor [DMOS] FETs
- H10D30/66—Vertical DMOS [VDMOS] FETs
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/01—Manufacture or treatment
- H10D30/021—Manufacture or treatment of FETs having insulated gates [IGFET]
- H10D30/028—Manufacture or treatment of FETs having insulated gates [IGFET] of double-diffused metal oxide semiconductor [DMOS] FETs
- H10D30/0291—Manufacture or treatment of FETs having insulated gates [IGFET] of double-diffused metal oxide semiconductor [DMOS] FETs of vertical DMOS [VDMOS] FETs
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/60—Insulated-gate field-effect transistors [IGFET]
- H10D30/64—Double-diffused metal-oxide semiconductor [DMOS] FETs
- H10D30/66—Vertical DMOS [VDMOS] FETs
- H10D30/662—Vertical DMOS [VDMOS] FETs having a drift region having a doping concentration that is higher between adjacent body regions relative to other parts of the drift region
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/13—Semiconductor regions connected to electrodes carrying current to be rectified, amplified or switched, e.g. source or drain regions
- H10D62/149—Source or drain regions of field-effect devices
- H10D62/151—Source or drain regions of field-effect devices of IGFETs
- H10D62/156—Drain regions of DMOS transistors
- H10D62/157—Impurity concentrations or distributions
Definitions
- the present invention relates to a vertical field effect transistor, and more particularly to a method for manufacturing a vertical field effect transistor having high output and high-speed switching characteristics.
- Japanese Patent Application Laid-Open No. 63-175754 / 78 discloses that an N ion implanted layer is formed by ion implantation to not only increase the concentration of only the surface but also make the entire N + connection region uniform. It has an O degree distribution to reduce the on-resistance.
- n-type impurity ions are implanted to form an n + connection region.
- Implanted impurity ions, or low port n- A method is described in which a conductive type drain region is formed by epitaxial growth, a high-concentration n + connection region is grown, and a low-concentration n-conductive region is formed by epitaxy growth. It is described that the parasitic capacitance is reduced and the resistance during conduction is reduced by these methods. Disclosure of the invention
- Japanese Unexamined Patent Publication No. 63-175574 / 98 discloses that not only the concentration on the surface alone is increased, but also the N ions which can make the entire N + connection region have a uniform distribution. Since high-energy ions are implanted, the port on the substrate surface could not be sufficiently lowered, and it was not possible to reduce the return volume S between the gate and drain.
- the realization method is to reduce the n-one conductivity type drain region.
- the method of implanting n-type impurity ions to form an n + contact region after forming by epitaxial growth, and then implanting p-type impurity ions requires two ion implantation steps.
- the n-type impurity ion concentration near the substrate surface is made to be isotopically low by offsetting by the p-type impurity ion, so that the carrier is small in spite of the fact that the amount of impurities including np is very large.
- n + connection region is formed at the same depth as immediately below the gate even in the source region, so that latch-up due to breakdown in the case of avalanche breakdown is sufficiently suppressed. There was also a problem that it was not done.
- the present invention provides a manufacturing method in which the n-type impurity concentration in the vicinity of the substrate surface immediately below the gate is sufficiently reduced, and the impurity concentration distribution is increased toward the inside of the substrate in one step. Aim.
- Another object of the present invention is to provide a vertical field effect transistor that suppresses latchup.
- the surface concentration is equal to or less than the concentration of the N-epi layer, and the peak concentration is N. 500 ke so that the range in the depth direction of the region above the concentration of the N-epi layer and above the concentration of the N-epi layer is located between the surface of the N-epi layer and the lower end of the channel region.
- Arsenic is ion-implanted with ⁇ energy of V or more. In this method, since arsenic is used as an impurity, impurity diffusion is small, and the concentration near the substrate surface does not increase.
- the surface concentration is equal to or less than the concentration of the N-epi layer, and the range in the depth direction of the region where the portability of the N-epi layer is equal to or more than the N-epi layer is N-epi.
- a vertical field-effect transistor having an arsenic distribution located therein is formed by ion implantation of arsenic with an energy of 500 keV or more using the gate polysilicon and the resist as a mask. in this case, Since the breakdown current path changes depending on the arsenic distribution directly below the channel, the latch-up phenomenon is suppressed.
- FIG. 1 is a sectional view of a vertical field-effect transistor according to the present invention.
- FIG. 2 is a view showing an impurity distribution along a depth direction of a cut surface at the center of a gate electrode.
- FIG. 3 is a conceptual diagram of Embodiment 1 of the manufacturing method.
- FIG. 4 is a conceptual diagram of Embodiment 1 of the manufacturing method.
- FIG. 5 is a conceptual diagram of Embodiment 1 of the manufacturing method.
- FIG. 6 is a conceptual diagram of Embodiment 2 of the manufacturing method.
- FIG. 7 is a conceptual diagram of Embodiment 2 of the manufacturing method.
- Fig. 8 is a conceptual diagram of Embodiment 2 of the manufacturing method.
- FIG. 9 is a diagram showing a change in on-resistance when the dose of the ⁇ energy arsenic implantation is changed.
- FIG. 10 is a diagram showing a change in the feedback capacitance S with respect to the impurity distribution shape immediately below the gate.
- FIG. 11 is a diagram showing a conventional impurity distribution.
- FIG. 12 is a diagram showing a conventional impurity distribution.
- FIG. 13 is a view showing a conventional impurity distribution.
- FIG. 14 is a view showing a vertical field effect transistor structure according to the present invention.
- FIG. 15 is a diagram showing a conventional structure for avoiding destruction due to latch-up.
- FIG. 16 shows a method for manufacturing a vertical field-effect transistor structure according to the present invention.
- FIG. 17 is a view showing a method of manufacturing a vertical field-effect transistor structure according to the present invention.
- FIG. 18 is a diagram showing a breakdown current path in the embodiment according to the present invention.
- FIG. 19 is a diagram showing a breakdown current path in the conventional structure.
- FIG. 1 is a sectional view of a vertical field-effect transistor according to an embodiment of the present invention.
- the structure shown in Fig. 1 has a structure in which an N-epi layer 4 is laminated on the surface of an N-substrate 5, and in addition to the channel region 3 and the N + source region 2 inside the N-epi layer 4, Implanted layer 1 is formed.
- a gate electrode 6 is formed on the N-epi layer 4 via an oxide film.
- the surface concentration of the high-energy arsenic-implanted layer 1 becomes less than the concentration of the N-epi layer 4 and the peak concentration is more than the concentration of the N-epi layer 4
- the distribution in the depth direction in which the S-degree of the N-epi layer 4 is equal to or more than the S degree is a distribution located between the surface of the N-epi scrap 4 and the lower end 10 of the channel region.
- This high-energy arsenic implanted layer 1 is formed on the entire surface of the N-epi layer 4 by using high-energy ion implantation of 500 keV or more.
- FIG. 2 shows the impurity distribution along the depth direction 11 of the cut surface at the center of the gate electrode 6 in FIG.
- the horizontal axis in FIG. 2 represents the depth direction 11 and the vertical axis represents the impurity concentration.
- an N-epi layer and a high energy arsenic implanted layer 1 are formed on an N substrate 5. As shown in Fig.
- the surface concentration is lower than the concentration of the N-epi layer
- the peak concentration is higher than the concentration of the N-epi layer
- the range is a distribution located between the surface of the N-epi layer and the bottom of the channel region.
- the impurity concentration of the N-epi layer 4 and the impurity concentration of the N-connection region 8 do not always match, but in the present invention, the impurity concentration of the N-epi layer 4 and the impurity concentration of the N-connection region 8 are different. The impurity concentrations are completely consistent.
- FIG. 3 One embodiment of the manufacturing method for the embodiment shown in FIG. 1 is shown in FIG. 3, FIG. 4, and FIG.
- FIGS. 3, 4, and 5 One embodiment of the manufacturing method for the embodiment shown in FIG. 1 is shown in FIGS. 3, 4, and 5.
- the N-epi layer 4 is seeded on the N substrate 5 by epitaxial growth (Fig. 3).
- phosphorus is doped to make the N-epi layer N-type.
- a high-energy arsenic implanted layer 1 is formed using high-energy ion implantation of 500 keV or more (Fig. 4). After the above steps, a channel region 3 and an N + source region 2 are formed (FIG. 5).
- the channel region 3 is formed by implanting boron into the substrate 5 after forming a predetermined mask, and further diffusing boron by heat treatment.
- the lower end of the channel region 3 is located deeper than the lower end of the high-energy arsenic implanted layer 1.
- the N + source region 2 is formed by implanting arsenic after forming a predetermined mask. In the arsenic distribution formed in Fig. 4, the diffusion coefficient of arsenic is different. It is not changed by the heat treatment shown in Fig. 5 because it is smaller than the impurity by one order of magnitude.
- FIG. 6, FIG. 7, and FIG. The channel region 3 is formed after the N-epi layer 4 is laminated on the N substrate 5 by epitaxial growth (FIG. 6).
- phosphorus is doped to make the N-epi layer N-type.
- the channel region 3 is formed by implanting po- ron into the substrate 5 after forming a predetermined mask, and further diffusing boron by heat treatment.
- a high-energy arsenic implanted layer 1 is formed using high-energy ion implantation of 500 keV or more (Fig. 7).
- the lower end of the channel region 3 is located deeper than the lower end of the high-energy arsenic implanted layer 1.
- an N + source region 2 is formed (FIG. 8).
- the N + source region 2 is formed by implanting arsenic after forming a predetermined mask. Since the diffusion coefficient of arsenic is one order of magnitude lower than that of other impurities, the impurity distribution formed in Fig. 7 does not change due to the heat treatment in Fig. 8.
- FIG. 9 shows a change in on-resistance when the dose of the high-energy arsenic implantation is changed in the embodiment shown in FIG. Fig. 9 shows the calculation results using a device simulator.
- the horizontal axis in FIG. 9 shows the arsenic dose, and the vertical axis shows the on-resistance. From Fig. 9, it can be seen that if arsenic is implanted at 1.0E16 (cm-2), a low resistance with an on-resistance of 100m ⁇ mm2 or less can be obtained. This value is at the same level as when only N + connection region 7 is formed.
- FIG. 10 shows a change in the feedback capacitance with respect to the impurity distribution shape immediately below the gate.
- FIG. 10 shows a calculation result using a device simulator.
- the axis represents the impurity distribution shape just below the gate, and the vertical axis represents the feedback capacitance. It can be seen that the feedback capacitance can be reduced when the high energy arsenic implanted layer 1 is formed, as compared with the case where only the N + connection region 7 is formed. When the N + connection region 7 is not formed, the feedback capacitance S can be further reduced, but as shown in FIG. 9, the on-resistance becomes as high as about 120 m ⁇ mm 2. From FIGS. 9 and 10, it can be seen that this embodiment is effective not only in reducing the conventional two steps to one step but also in reducing the resistance and the feedback capacitance. Due to the reduction of the resistance and the reduction of the return capacitance, the vertical field effect transistor according to the present embodiment has a high output and a high speed switching characteristic.
- FIGS. 11, 12 and 13 show differences in impurity distribution between the conventional technology and the high-energy arsenic-implanted layer 1 according to the embodiment of the present invention.
- the horizontal axis in FIGS. 11, 12, and 13 represents the depth direction 11, and the vertical axis represents the impurity concentration.
- N + connection region 7 is formed by N + epi layer 1 101 on top of N-epi layer 4, and N-connection region 8 is further formed by N-epi layer 1
- An example in the case of forming with 102 is shown.
- the diffusion coefficient of arsenic is at least one order of magnitude smaller than that of other impurities, so that there is a flat portion of the impurity distribution.
- an N + connection region 7 is formed on the N-epi layer 4 by the N + epi layer 1 101, and the surface of the N + connection region 7 is opposite to arsenic.
- An embodiment in which the N-connection region 8 is formed by forming a conductive type polon diffusion layer 1221 will be described.
- boron is introduced to form the N-connection region 8. When the high energy arsenic implanted layer 1 is used, no boron exists in the N-connection region 8.
- FIGS. 11 and 12 require two steps to form the N + connection region 7 and the N ⁇ connection region 8.
- the N + connection region 7 and the N ⁇ connection region 8 can be formed in one step, so that the cost per chip is reduced.
- FIG. 13 shows an embodiment in which high-energy ion implantation is used to flatten the impurity concentration of the N + connection region 7.
- the surface concentration of the N + connection region 7 formed by the high-energy ion-implanted layer 1301 shown in FIG. 13 is higher than the concentration of the N-epi layer 4. Furthermore, in order to form such a distribution, it is necessary to use phosphorus instead of arsenic.
- FIG. 15 shows an embodiment of the prior art.
- the N-epi layer 4 is removed above the N-substrate 5, and the channel region 3, N + source region 2, N + connection region 7, N + -The connection area 8 is formed.
- a P + connection region 9 is formed to avoid destruction due to latch-up.
- a total of three steps are required to form the N + connection region 7, the N- connection region 8, and the P + connection region 9. The reason why the conventional P + connection region 9 is effective in avoiding latch-up will be described with reference to FIG. FIG.
- the vertical field effect transistor has an edge portion of the gate electrode 6 in the channel region 3.
- the base turns on and a large current flows. This phenomenon is We call it top. If the vertical field-effect transistor latches up, the device will be destroyed. In order to prevent latch-up, it is necessary to suppress the voltage rise at the edge of the gate electrode 6.
- the P + connection region 9 is a technology that suppresses an increase in compressibility at the edge of the gate electrode 6 due to a voltage drop by reducing the resistance of the channel portion 3.
- an N + connection region, an N ⁇ connection region, and a P + connection region are formed in a total of three steps.
- FIG. 14 shows an embodiment of the present invention.
- Fig. 14 shows an N + connection region, an N- connection region, and a device structure that enables a structure to avoid latch-up to be formed in a single process, which was conventionally formed in three processes. It is.
- an N-epi layer 4 is laminated on an N substrate 5, and a channel region 3 and an N + source region 2 are formed in the region of the N-epi layer 4.
- the surface area in the depth direction where the surface concentration is less than the concentration of the N-epi layer 4 and higher than the portability of the N-epi layer 4 is N-
- the arsenic distribution located between the surface of the epitaxial layer 4 and the lower end 10 of the channel region, and the area directly below the channel region 10 in the depth direction where the concentration of the N-epi layer is higher than the lower end of the channel region 1 It has a rectangular high-energy arsenic implanted layer 12 which simultaneously constitutes an arsenic distribution located between 0 and the N substrate 5.
- the arsenic distribution directly under the gate 3 ⁇ 4 pole 6 of the rectangular high-energy arsenic implanted layer 12 plays a role in obtaining high output and high switching characteristics, and the arsenic distribution directly under the channel region 10 avoids damage due to latch-up. Play a role.
- the reason why the arsenic distribution immediately below the channel region 10 avoids destruction due to latch-up will be described with reference to FIG. In the prior art shown in FIG. 19, the avalanche breakdown occurs near the left end of the gate electrode 6 in the channel region 3. On the other hand, in the embodiment shown in FIG. + Source area 2 Occurs near the left end. Therefore, the breakdown current flows along the path 1801.
- FIGS. 16 and 17 show the manufacturing method of the embodiment shown in FIG.
- the manufacturing method shown in Fig. 16 and Fig. 17 makes it possible to form the N + connection area, N-connection area, and P + connection area in one process, which were conventionally formed in three processes.
- An N-epi layer 4 is formed on the substrate 5 and a channel region 3 and an N + source region 2 are formed in the N-epi layer 4 (FIG. 16).
- phosphorus is doped to make the N-epi layer N-type.
- the channel region 3 is formed by implanting boron into the substrate 5 after forming a predetermined mask, and further diffusing boron by heat treatment.
- the N + source region 2 is formed by implanting arsenic after forming a predetermined mask.
- a resist 1701 is applied on the polysilicon, and the resist 1701 is applied only to a predetermined region by photolithography. Remove and remove. By etching the polysilicon after removing the resist 1701, the structure shown in Fig. 17 can be formed.
- a rectangular high-energy arsenic implanted layer 12 is formed by high-energy arsenic implantation 1702.
- a rectangular high energy arsenic implanted layer 12 is formed.
- the lower end of the arsenic distribution directly below the gate 3 ⁇ 4 pole 6 is located above the lower end of the channel region 3, and the upper end of the arsenic distribution immediately below the channel region 3 is located below the lower end of the channel region 3.
- the positions of the arsenic distribution directly below the gate electrode 6 and the arsenic distribution directly below the channel region 3 in the depth direction 11 can be separately specified by the resist film thickness and the implantation energy.
- high-energy arsenic implantation 1702 By using high-energy arsenic implantation 1702, a structure that conventionally required three processes can be configured by the ⁇ process.
- N + connection region and the N ⁇ connection region which are conventionally formed in two steps, can be formed in one step, and the cost per chip can be made equal to the case where only the N + connection region is formed.
- Another advantage of the present invention is that the N + connection region conventionally formed in three steps, The structure to avoid destruction due to N-connection area and latch-up can be formed in one process, and the unit cost of the chip can be reduced to less than the conventional one.
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- Insulated Gate Type Field-Effect Transistor (AREA)
Abstract
Description
明 細 書 Specification
縱型電界効果 トランジス夕の製造方法 Manufacturing method of vertical field effect transistor
技術分野 Technical field
本発明は、 縱型電界効果 トラ ンジスタに関し、 特に、 高出力及び高速 度スィ ツチング特性をもつ縱型電界 トランジス夕の製造方法に関する。 The present invention relates to a vertical field effect transistor, and more particularly to a method for manufacturing a vertical field effect transistor having high output and high-speed switching characteristics.
背景技術 Background art
一般用あるいは工業用に使用される電源装置、 例えば、 スイ ッチング レギュレータなどは周波数を高くすることにより、 益々小型化及び低価 格化の傾向が強くなり、 これらに使用されるスイ ツチング用 トランジス 夕に対しても、 低価格で且つ高出力、 高速度スイ ッチング性能が要求さ れてきている。 通常、 この種の トランジスタには、 半導体基板表面に複 数のソース及びゲー トを設け、 これらを並列に接続し、 裏面に ドレイ ン ¾極を設けることによって高出力、 高速度スィ ッチング電流が得られる 構造の縱型電界効果 トランジスタが使用されている。 しかし、 本 トラン ジスタは導通時抵抗 (オン抵抗) が高く、 また、 ゲー 卜 · ドレイ ン間の 帰還容量が大きいことから、 高出力スィ ツチング電流が得られにく いと ともに高速スィ ッチングが得られないという問題があり、 種々の改善提 案がなされてきた。 Power supplies used for general or industrial use, such as switching regulators, have a tendency to become smaller and lower in price by increasing the frequency, and switching transistors used for these are increasingly used. In addition, low-cost, high-output, high-speed switching performance is required. Normally, this type of transistor has a high output and high speed switching current by providing multiple sources and gates on the surface of the semiconductor substrate, connecting them in parallel, and providing a drain electrode on the back. A vertical field-effect transistor having a structure is used. However, this transistor has a high resistance during conduction (on-resistance) and a large feedback capacitance between the gate and the drain. There is no problem, and various improvement proposals have been made.
特開昭 6 3 - 1 7 5 4 7 8号公報は、 Nイオン注入層を髙エネルギーィ オン打ち込みで形成し、 表面のみの濃度を高くするだけではなく、 N +接 続領域全体を均一な澳度分布とし、 オン抵抗の低減を図ったものである。 特開平 1 — 2 5 3 9 6 6号公報では、 n—導電型 ドレイ ン領域をェピタ キシャル成長により形成した後、 n型不純物イオンを注入して n +接続領 域を形成し、 その後、 p型不純物イオンを注入する方法や、 低港度の n— 導電型 ドレイ ン領域をェピタキシャル成長により形成した後、 高濃度の n +接続領域を成長し、 さらに低濃度の n—導 ¾型領域をェピタキシャル成 長により形成する方法が記載されている。 そして、 これらの方法により 寄生容量を小さ くするとともに導通時抵抗を低くする旨が記載されてい る。 発明の開示 Japanese Patent Application Laid-Open No. 63-175754 / 78 discloses that an N ion implanted layer is formed by ion implantation to not only increase the concentration of only the surface but also make the entire N + connection region uniform. It has an O degree distribution to reduce the on-resistance. In Japanese Patent Application Laid-Open No. 1-2536966, after forming an n-conductivity type drain region by epitaxial growth, n-type impurity ions are implanted to form an n + connection region. Implanted impurity ions, or low port n- A method is described in which a conductive type drain region is formed by epitaxial growth, a high-concentration n + connection region is grown, and a low-concentration n-conductive region is formed by epitaxy growth. It is described that the parasitic capacitance is reduced and the resistance during conduction is reduced by these methods. Disclosure of the invention
しかしながら、 特開昭 6 3 — 1 7 5 4 7 8号公報は、 表面のみの濃度 を高くするだけではなく、 N +接続領域全体を均一な澳度分布とすること ができるような Nイオンを高エネルギーイオン打ち込んでいるため、 基 板表面での港度を十分に低くすることができず、 ゲー ト . ドレイ ン間の 帰還容 Sを低減しょうとしても不可能であった。 However, Japanese Unexamined Patent Publication No. 63-175574 / 98 discloses that not only the concentration on the surface alone is increased, but also the N ions which can make the entire N + connection region have a uniform distribution. Since high-energy ions are implanted, the port on the substrate surface could not be sufficiently lowered, and it was not possible to reduce the return volume S between the gate and drain.
また、 特開平 1 — 2 5 3 9 6 6号公報では、 寄生容量を小さ くすると ともに導通時抵抗を低くすることが可能ではあるが、 その実現方法が、 n 一導電型 ドレイ ン領域をェピタキシャル成長により形成した後、 n型不純 物イオンを注入して n +接铳領域を形成し、 その後、 p型不純物イオンを 注入する方法の場合には、 イオン注入の工程が 2回必要であり、 また、 基板表面付近での n型不純物ィォン濃度は、 p型不純物ィォンによる相 殺によって等偭的に低濃度にされているので n pを合わせた不純物量が 非常に多い割にキヤ リァが少ないという状況になるので、 この部分での 抵抗値はあまり小さ くならないという問題があった。 さ らに、 n pの相 殺による低港度化は港度の微調整が難しいので、 トランジスタの V t hを 制御しにくいという問題もあった。 また、 低濃度の n—導電型 ドレイ ン領 域をェピタキシャル成長により形成した後、 高港度の n +接続領域を成長 し、 さ らに低濃度の n—導電型領域をェピタキシャル成長により形成する 方法では、 ェピタキシャル成長が 3回も行われるため、 工程数が増加す る問題があつた。 Also, in Japanese Patent Application Laid-Open No. 1-253936, it is possible to reduce the parasitic capacitance and the resistance at the time of conduction, but the realization method is to reduce the n-one conductivity type drain region. The method of implanting n-type impurity ions to form an n + contact region after forming by epitaxial growth, and then implanting p-type impurity ions, requires two ion implantation steps. In addition, the n-type impurity ion concentration near the substrate surface is made to be isotopically low by offsetting by the p-type impurity ion, so that the carrier is small in spite of the fact that the amount of impurities including np is very large. Therefore, there was a problem that the resistance value in this part did not become too small. In addition, since lowering the port by canceling np makes it difficult to fine-tune the port, there is also a problem that it is difficult to control the V th of the transistor. After forming a low-concentration n-conductivity-type drain region by epitaxy, a high-port n + connection region is grown, and a low-concentration n-conductivity-type region is formed by epitaxy. Form In the method, epitaxy was performed three times, and the number of steps increased.
また、 他の問題として、 上記従来技術では n +接続領域がソース領域に おいてもゲー ト直下と同じ深さに形成されているため、 アバランシェ降 伏した場合のブレイクダウンによるラッチァップが十分に抑制されない という問題もあった。 Another problem is that, in the above-described conventional technology, the n + connection region is formed at the same depth as immediately below the gate even in the source region, so that latch-up due to breakdown in the case of avalanche breakdown is sufficiently suppressed. There was also a problem that it was not done.
そこで、 本発明では、 ゲー ト直下の基板表面近傍の n型不純物濃度を 十分に低く し、 基板内部に向けて濃度を高く した不純物濃度分布を 1ェ 程で形成する製造方法を提供することを目的とする。 Therefore, the present invention provides a manufacturing method in which the n-type impurity concentration in the vicinity of the substrate surface immediately below the gate is sufficiently reduced, and the impurity concentration distribution is increased toward the inside of the substrate in one step. Aim.
本発明の他の目的と しては、 ラッチァップを抑制する縱型電界効果 ト ランジスタを提供することを目的とする。 Another object of the present invention is to provide a vertical field effect transistor that suppresses latchup.
上記目的を達成するための本発明の一実施例では、 N -のェピ層を形成 後も しく はチャネル層形成後に、 表面濃度が N -ェピ層の濃度以下、' ピー ク濃度が N -ェピ層の濃度以上、 且つ、 N -ェピ層の濃度以上になる領域の 深さ方向の範囲が N -ェピ層表面とチャネル領域下端の間に位置するよう に、 5 0 0 k e V以上の髙エネルギーでヒ素をイオン打ち込みする。 この方法 では、 ヒ素を不純物としているので不純物拡散が小さ く、 基板表面近傍 の濃度が髙くならない。 In one embodiment of the present invention for achieving the above object, after forming the N-epi layer or after forming the channel layer, the surface concentration is equal to or less than the concentration of the N-epi layer, and the peak concentration is N. 500 ke so that the range in the depth direction of the region above the concentration of the N-epi layer and above the concentration of the N-epi layer is located between the surface of the N-epi layer and the lower end of the channel region. Arsenic is ion-implanted with 髙 energy of V or more. In this method, since arsenic is used as an impurity, impurity diffusion is small, and the concentration near the substrate surface does not increase.
また、 本発明の他の実施例では、 ゲー ト直下では、 表面濃度が N -ェピ 層の濃度以下となり、 N -ェピ層の港度以上になる領域の深さ方向の範囲 が N -ェピ層表面からチャネル領域下端の間に位置するヒ素分布と、 チヤ ネル直下では、 N -ェピ層の濃度以上になる領域の深さ方向の範囲がチャ ネル領域下端と基板との間に位置するヒ素分布とを有する縱型茧界効果 トランジスタを、 ゲー トポリ シリ コン及びレジス トをマスクとして 5 0 0 k e V以上のヒ素髙エネルギーイオン打ち込みにより形成する。 この場合は、 チャネル直下のヒ素分布によりブレイクダウン電流経路が変わるので、 ラ ッチアツプ現象が抑制される。 図面の簡単な説明 Further, in another embodiment of the present invention, immediately below the gate, the surface concentration is equal to or less than the concentration of the N-epi layer, and the range in the depth direction of the region where the portability of the N-epi layer is equal to or more than the N-epi layer is N-epi. The arsenic distribution located between the surface of the epitaxial layer and the bottom of the channel region, and immediately below the channel, the range in the depth direction of the region where the concentration of the N-epi layer exceeds the concentration between the bottom of the channel region and the substrate A vertical field-effect transistor having an arsenic distribution located therein is formed by ion implantation of arsenic with an energy of 500 keV or more using the gate polysilicon and the resist as a mask. in this case, Since the breakdown current path changes depending on the arsenic distribution directly below the channel, the latch-up phenomenon is suppressed. BRIEF DESCRIPTION OF THE FIGURES
第 1 図は、 本発明による縱型電界効果 トラ ンジスタの断面図である。 第 2図は、 ゲー ト電極中心における切断面の深さ方向に添った不純物 分布を示す図である。 FIG. 1 is a sectional view of a vertical field-effect transistor according to the present invention. FIG. 2 is a view showing an impurity distribution along a depth direction of a cut surface at the center of a gate electrode.
第 3図は、 製造方法の一実施例 1 の概念図である。 FIG. 3 is a conceptual diagram of Embodiment 1 of the manufacturing method.
第 4図は、 製造方法の一実施例 1 の概念図である。 FIG. 4 is a conceptual diagram of Embodiment 1 of the manufacturing method.
第 5図は、 製造方法の一実施例 1 の概念図である。 FIG. 5 is a conceptual diagram of Embodiment 1 of the manufacturing method.
第 6図は、 製造方法の一実施例 2の概念図である。 FIG. 6 is a conceptual diagram of Embodiment 2 of the manufacturing method.
第 7図は、 製造方法の一実施例 2の概念図である。 FIG. 7 is a conceptual diagram of Embodiment 2 of the manufacturing method.
第 8図は、 製造方法の一実施例 2の概念図 Fig. 8 is a conceptual diagram of Embodiment 2 of the manufacturing method.
第 9図は、 髙エネルギーヒ素打ち込み ドーズ量を変化させた時のオン 抵抗の変化を示す図である。 FIG. 9 is a diagram showing a change in on-resistance when the dose of the 髙 energy arsenic implantation is changed.
第 1 0図は、 ゲー ト直下の不純物分布形状に対する帰還容 Sの変化を 示す図である。 FIG. 10 is a diagram showing a change in the feedback capacitance S with respect to the impurity distribution shape immediately below the gate.
第 1 1図は、 従来技術の不純物分布を示す図である。 FIG. 11 is a diagram showing a conventional impurity distribution.
第 1 2図は、 従来技術の不純物分布を示す図である。 FIG. 12 is a diagram showing a conventional impurity distribution.
第 1 3図は、 従来技術の不純物分布を示す図である。 FIG. 13 is a view showing a conventional impurity distribution.
第 1 4図は、 本発明による縱型電界効果トランジスタ構造を示す図で ある。 FIG. 14 is a view showing a vertical field effect transistor structure according to the present invention.
第 1 5図は、 ラッチアップによる破壊を回避するための従来構造を示 す図である。 FIG. 15 is a diagram showing a conventional structure for avoiding destruction due to latch-up.
第 1 6図は、 本発明による縱型電界効果 トラ ンジスタ構造の製造方法 を示す図である。 FIG. 16 shows a method for manufacturing a vertical field-effect transistor structure according to the present invention. FIG.
第 1 7図は、 本発明による縱型電界効果トラ ンジスタ構造の製造方法 を示す図である。 FIG. 17 is a view showing a method of manufacturing a vertical field-effect transistor structure according to the present invention.
第 1 8図は、 本発明による実施例におけるブレイクダウン電流経路を 示す図である。 FIG. 18 is a diagram showing a breakdown current path in the embodiment according to the present invention.
第 1 9図は、 従来構造におけるブレイクダウン電流経路を示す図であ る。 発明を実施するための最良の形態 FIG. 19 is a diagram showing a breakdown current path in the conventional structure. BEST MODE FOR CARRYING OUT THE INVENTION
以下、 実施例により本発明をより詳細に説明する。 Hereinafter, the present invention will be described in more detail with reference to examples.
本発明の一実施例である縱型電界効果トラ ンジスタの断面図を第 1図 に示す。 第 1図に示す構造は、 N基板 5の表面に、 N-ェピ層 4を積層し、 N-ェピ層 4内部にチャネル領域 3、 N+ソース領域 2に加えて、 高工ネル ギーヒ素打ち込み層 1が形成されている。 N-ェピ層 4上層には、 酸化膜 を介してゲー ト電極 6が形成されている。 高エネルギーヒ素打ち込み層 1 は、 N-ェピ層 4を形成後もしくはチャネル層 3形成後に、 表面濃度が N -ェピ層 4の濃度以下となり、 ピーク濃度が N-ェピ層 4の濃度以上となり 且つ、 N-ェピ層 4の S度以上になる深さ方向の範囲が、 N-ェピ屑 4表面 とチャネル領域下端 1 0の間に位置する分布となっている。 この高エネ ルギーヒ素打ち込み層 1 は、 500keV以上の高エネルギーイオン打ち込み を用いて、 N-ェピ層 4全面に形成されている。 通常これらに加えて、 P + 接続領域 9を形成するが、 本実施例では図への記述を省略する。 本実施 例では、 N-ェピ層 4表面か N-接続領域 8 となり、 N-ェピ層 4の港度よ り高い部分が N +接続領域 7 となり、 一工程で N +接続領域と N—接続領 域が形成さる。 第 2図は、 第 1 図のゲー ト電極 6の中心での切断面の深さ方向 1 1 に 添った不純物分布を示す。 第 2図の横軸は深さ方向 1 1を表し、 縱軸は 不純物濃度を表している。 第 2図において、 N基板 5上に N -ェピ層及び 高エネルギーヒ素打ち込み層 1が形成されている。 第 2図に示すように、 表面濃度が N -ェピ層の濃度以下となり、 ピーク濃度が N -ェピ層の濃度以 上となり且つ、 N -ェピ層の濃度以上になる深さ方向の範囲が、 N -ェピ層 表面とチヤネル領域下端の間に位置する分布となつている。 従来技術で は、 N -ェピ層 4の不純物濃度と N -接続領域 8の不純物澳度が必ずしも一 致しないが、 本発明では N -ェピ層 4の不純物濃度と N -接続領域 8の不純 物濃度は完全に一致する。 高エネルギーヒ素打ち込み層 1 を形成するこ とにより、一工程で N -接続領域及び N +接続領域 7形成できる。 FIG. 1 is a sectional view of a vertical field-effect transistor according to an embodiment of the present invention. The structure shown in Fig. 1 has a structure in which an N-epi layer 4 is laminated on the surface of an N-substrate 5, and in addition to the channel region 3 and the N + source region 2 inside the N-epi layer 4, Implanted layer 1 is formed. A gate electrode 6 is formed on the N-epi layer 4 via an oxide film. After the N-epi layer 4 or the channel layer 3 is formed, the surface concentration of the high-energy arsenic-implanted layer 1 becomes less than the concentration of the N-epi layer 4 and the peak concentration is more than the concentration of the N-epi layer 4 In addition, the distribution in the depth direction in which the S-degree of the N-epi layer 4 is equal to or more than the S degree is a distribution located between the surface of the N-epi scrap 4 and the lower end 10 of the channel region. This high-energy arsenic implanted layer 1 is formed on the entire surface of the N-epi layer 4 by using high-energy ion implantation of 500 keV or more. Usually, in addition to these, a P + connection region 9 is formed, but in the present embodiment, the description in the figure is omitted. In this embodiment, the surface of the N-epi layer 4 or the N-connection region 8 becomes the N-epi layer 4, and the portion of the N-epi layer 4 higher than the port degree becomes the N + connection region 7. —Connection area is formed. FIG. 2 shows the impurity distribution along the depth direction 11 of the cut surface at the center of the gate electrode 6 in FIG. The horizontal axis in FIG. 2 represents the depth direction 11 and the vertical axis represents the impurity concentration. In FIG. 2, an N-epi layer and a high energy arsenic implanted layer 1 are formed on an N substrate 5. As shown in Fig. 2, the surface concentration is lower than the concentration of the N-epi layer, the peak concentration is higher than the concentration of the N-epi layer, and is higher than the concentration of the N-epi layer. The range is a distribution located between the surface of the N-epi layer and the bottom of the channel region. In the prior art, the impurity concentration of the N-epi layer 4 and the impurity concentration of the N-connection region 8 do not always match, but in the present invention, the impurity concentration of the N-epi layer 4 and the impurity concentration of the N-connection region 8 are different. The impurity concentrations are completely consistent. By forming the high-energy arsenic-implanted layer 1, the N-connection region and the N + connection region 7 can be formed in one step.
第 1 図に示す実施例に対する製造方法の一実施例を第 3図、 第 4図、 第 5図に示す。 One embodiment of the manufacturing method for the embodiment shown in FIG. 1 is shown in FIG. 3, FIG. 4, and FIG.
第 1図に示す実施例に対する製造方法の一実施例を第 3図, 第 4図, 第 5図に示す。 N基板 5の上部にェピタキシャル成長により, N -ェピ層 4を 種展する (第 3図) 。 N基板 5には, 低抵抗化しやすいヒ素 ドープ基板を 用いる。 N -ェピ層 4形成時には, ェピ層を N導電型にするためにリ ンを ドープする。 次に, 5 00 k e V以上の高エネルギーイオン打ち込みを用いて, 高エネルギーヒ素打ち込み層 1 を形成する (第 4図) 。 以上の工程終了 後, チャネル領域 3及び N +ソース領域 2を形成する (第 5図) 。 チヤネ ル領域 3は, 所定のマスク形成後にボロンを基板 5中に打ち込み, 更に 熱処理によりボロンを拡散させることにより形成する。 チヤネル領域 3 の下端部は, 高エネルギーヒ素打ち込み層 1 の下端部と比較し, 深部に 位置する。 N +ソース領域 2は, 所定のマスク形成後にヒ素を打ち込むこ とにより形成する。 第 4図で形成したヒ素分布は, ヒ素の拡散係数が他 の不純物と比較し一桁以上小さいことより, 第 5図での熱処理により変 化しない。 高エネルギーヒ素打ち込み層 1を形成することにより, ーェ 程で N-接続領域 8及び N +接続領域 7形成できる。 One embodiment of the manufacturing method for the embodiment shown in FIG. 1 is shown in FIGS. 3, 4, and 5. The N-epi layer 4 is seeded on the N substrate 5 by epitaxial growth (Fig. 3). As the N-substrate 5, an arsenic-doped substrate that easily reduces resistance is used. When forming the N-epi layer 4, phosphorus is doped to make the N-epi layer N-type. Next, a high-energy arsenic implanted layer 1 is formed using high-energy ion implantation of 500 keV or more (Fig. 4). After the above steps, a channel region 3 and an N + source region 2 are formed (FIG. 5). The channel region 3 is formed by implanting boron into the substrate 5 after forming a predetermined mask, and further diffusing boron by heat treatment. The lower end of the channel region 3 is located deeper than the lower end of the high-energy arsenic implanted layer 1. The N + source region 2 is formed by implanting arsenic after forming a predetermined mask. In the arsenic distribution formed in Fig. 4, the diffusion coefficient of arsenic is different. It is not changed by the heat treatment shown in Fig. 5 because it is smaller than the impurity by one order of magnitude. By forming the high-energy arsenic implanted layer 1, the N-connection region 8 and the N + connection region 7 can be formed in the process.
第 1 図に示す実施例に対する製造方法の他の実施例を第 6図, 第 7図, 第 8図に示す。 N基板 5の上部にェピタキシャル成長により, N-ェピ層 4 を積層した後チャネル領域 3を形成する (第 6図) 。 基板 5には, 低抵 抗化しゃすいヒ素ドープ基板を用いる。 N-ェピ層 4形成時には, ェピ層 を N導電型にするためにリ ンを ドープする。 チャネル領域 3は, 所定の マスク形成後にポロンを基板 5中に打ち込み, 更に熱処理によりボロン を拡散させることにより形成する。 次に, 500keV以上の高エネルギーィ オン打ち込みを用いて, 高エネルギーヒ素打ち込み層 1 を形成する (第 7図) 。 チャネル領域 3の下端部は, 高エネルギーヒ素打ち込み層 1の 下端部と比較し, 深部に位置する。 以上の工程終了後, N+ソース領域 2 を形成する (第 8図) 。 N+ソース領域 2は, 所定のマスク形成後にヒ素 を打ち込むことにより形成する。 ヒ素は他の不純物と比較して拡散係数 が一桁以上小さいので, 第 7図で形成した不純物分布は, 第 8図での熱 処理により変化しない。 Another embodiment of the manufacturing method for the embodiment shown in FIG. 1 is shown in FIG. 6, FIG. 7, and FIG. The channel region 3 is formed after the N-epi layer 4 is laminated on the N substrate 5 by epitaxial growth (FIG. 6). As the substrate 5, a low-resistance arsenic-doped substrate is used. When the N-epi layer 4 is formed, phosphorus is doped to make the N-epi layer N-type. The channel region 3 is formed by implanting po- ron into the substrate 5 after forming a predetermined mask, and further diffusing boron by heat treatment. Next, a high-energy arsenic implanted layer 1 is formed using high-energy ion implantation of 500 keV or more (Fig. 7). The lower end of the channel region 3 is located deeper than the lower end of the high-energy arsenic implanted layer 1. After the above steps, an N + source region 2 is formed (FIG. 8). The N + source region 2 is formed by implanting arsenic after forming a predetermined mask. Since the diffusion coefficient of arsenic is one order of magnitude lower than that of other impurities, the impurity distribution formed in Fig. 7 does not change due to the heat treatment in Fig. 8.
第 9図に、 第 1図に示す実施例において高エネルギーヒ素打ち込みの ドーズ量を変化させた時のオン抵抗の変化を示す。 第 9図は、 デバイス シミ ュレータを用いた計算結果である。 第 9図の横軸はヒ素の ドーズ量、 縱軸はオン抵抗を表す。 第 9図より、 ヒ素を 1.0E16 (cm- 2)打ち込めば. オン抵抗 100m Ω mm2以下の低抵抗を得ることができることが分かる。 こ の値は、 N +接続領域 7のみを形成する場合と同レベルである。 第 1 0図 に、 ゲー ト直下の不純物分布形状に対する帰還容量の変化を示す。 第 1 0図は、 デバイスシ ミ ュ レータを用いた計算結果である。 第 1 0図の横 軸はゲー ト直下の不純物分布形状、 縱軸は帰還容量を表している。 高工 ネルギーヒ素打ち込み層 1形成した場合、 N +接続領域 7のみを形成した 場合と比較して、 帰還容量を低減できることが分かる。 N +接続領域 7を 形成しない場合は、 帰還容 Sをさ らに低減できるが、 第 9図に示すよう に、 オン抵抗が 1 20 m Ω mm 2程度の高抵抗になってしまう。 第 9図及び第 1 0図より、 本実施例は、 従来の二工程を一工程にできるだけでなく 、 抵抗低減、 帰還容量低減に有効であることが分かる。 この抵抗低減、 帰 還容量低滅により、 本実施例による縱型電界効果 トランジスタは、 高出 力及び高速度スィ ツチング特性を持つ。 FIG. 9 shows a change in on-resistance when the dose of the high-energy arsenic implantation is changed in the embodiment shown in FIG. Fig. 9 shows the calculation results using a device simulator. The horizontal axis in FIG. 9 shows the arsenic dose, and the vertical axis shows the on-resistance. From Fig. 9, it can be seen that if arsenic is implanted at 1.0E16 (cm-2), a low resistance with an on-resistance of 100mΩ mm2 or less can be obtained. This value is at the same level as when only N + connection region 7 is formed. FIG. 10 shows a change in the feedback capacitance with respect to the impurity distribution shape immediately below the gate. FIG. 10 shows a calculation result using a device simulator. Next to Fig. 10 The axis represents the impurity distribution shape just below the gate, and the vertical axis represents the feedback capacitance. It can be seen that the feedback capacitance can be reduced when the high energy arsenic implanted layer 1 is formed, as compared with the case where only the N + connection region 7 is formed. When the N + connection region 7 is not formed, the feedback capacitance S can be further reduced, but as shown in FIG. 9, the on-resistance becomes as high as about 120 mΩ mm 2. From FIGS. 9 and 10, it can be seen that this embodiment is effective not only in reducing the conventional two steps to one step but also in reducing the resistance and the feedback capacitance. Due to the reduction of the resistance and the reduction of the return capacitance, the vertical field effect transistor according to the present embodiment has a high output and a high speed switching characteristic.
第 1 1 図、 第 1 2図、 第 1 3図を用いて、 従来技術と本発明の実施例 である高エネルギーヒ素打ち込み層 1 との不純物分布の相異点を示す。 第 1 1 図、 第 1 2図、 第 1 3図の横軸は深さ方向 1 1を表し、 縱軸は不 純物濃度を表している。 第 1 1図には、 N -ェピ層 4の上部に、 N +接続領 域 7を N +ェピ層 1 1 0 1 により形成し、 更に N -接続領域 8を N -ェピ層 1 1 0 2により形成した場合の実施例を示す。 N +ェピ層 1 1 0 1 にヒ素 を用いた場合は、 ヒ素の拡散係数が他の不純物と比較し一桁以上小さい ので、 不純物分布の平坦な部分が存在する。 高エネルギーヒ素打ち込み 眉 1 を用いた場合には、 このような平坦部は存在しない。 また、 N +ェピ 層 1 1 0 1の N -ェピ層 1 1 0 2 と N -ェピ層 4の不純物 ¾度は、 必ずしも 一致していない。 第 1 2図には、 N -ェピ層 4の上部に、 N +接続領域 7を N +ェピ層 1 1 0 1 により形成し、 更に N +接続領域 7の表面部に、 ヒ素と 逆導電型のポロン拡散層 1 2 0 1 を形成することにより N -接続領域 8を 形成した場合の実施例を示す。 第 1 2図に示す実施例では、 N -接続領域 8を形成するために、 ボロンが導入されている。 高エネルギーヒ素打ち 込み層 1 を用いた場合には、 N -接続領域 8にはボロ ンは存在しない。 第 1 1 図及び第 1 2図に示す従来技術では共に、 N +接続領域 7及び N -接続 領域 8を形成するために二工程必要となる。 高エネルギーヒ素打ち込み 層 1 を用いた場合には、 一工程で N +接続領域 7及び N -接続領域 8が形成 できるためチップ単価が安くなる。 第 1 3図に、 N +接続領域 7の不純物 濃度を平坦化するため、 高エネルギーィォン打ち込みを用いた場合の実 施例を示す。 第 1 3図に示す高エネルギーイオン打ち込み層 1 3 0 1 に より形成した N +接続領域 7の表面濃度は、 N -ェピ層 4の濃度と比較し高 くなつている。 更に、 このような分布を形成するためには、 ヒ素ではな く リ ンを用いる必要がある。 FIGS. 11, 12 and 13 show differences in impurity distribution between the conventional technology and the high-energy arsenic-implanted layer 1 according to the embodiment of the present invention. The horizontal axis in FIGS. 11, 12, and 13 represents the depth direction 11, and the vertical axis represents the impurity concentration. In FIG. 11, N + connection region 7 is formed by N + epi layer 1 101 on top of N-epi layer 4, and N-connection region 8 is further formed by N-epi layer 1 An example in the case of forming with 102 is shown. When arsenic is used for the N + epi layer 1101, the diffusion coefficient of arsenic is at least one order of magnitude smaller than that of other impurities, so that there is a flat portion of the impurity distribution. When using high-energy arsenic implantation eyebrow 1, such a flat part does not exist. In addition, the impurity concentrations of the N-epi layer 1102 of the N + epi layer 1101 and the N-epi layer 4 do not always match. In FIG. 12, an N + connection region 7 is formed on the N-epi layer 4 by the N + epi layer 1 101, and the surface of the N + connection region 7 is opposite to arsenic. An embodiment in which the N-connection region 8 is formed by forming a conductive type polon diffusion layer 1221 will be described. In the embodiment shown in FIG. 12, boron is introduced to form the N-connection region 8. When the high energy arsenic implanted layer 1 is used, no boron exists in the N-connection region 8. No. Both the prior art shown in FIGS. 11 and 12 require two steps to form the N + connection region 7 and the N − connection region 8. When the high-energy arsenic-implanted layer 1 is used, the N + connection region 7 and the N − connection region 8 can be formed in one step, so that the cost per chip is reduced. FIG. 13 shows an embodiment in which high-energy ion implantation is used to flatten the impurity concentration of the N + connection region 7. The surface concentration of the N + connection region 7 formed by the high-energy ion-implanted layer 1301 shown in FIG. 13 is higher than the concentration of the N-epi layer 4. Furthermore, in order to form such a distribution, it is necessary to use phosphorus instead of arsenic.
第 1 5図及び第 1 9図を用いて、 ラ ッチアツプによる破壊を回避する ための従来技術を説明する。 第 1 5図は、 従来技術の一実施例を示す。 第 1 5図では、 N基板 5の上部に N -ェピ層 4を穑屑し、 N -ェピ層 4の領 域にチャネル領域 3、 N +ソース領域 2、 N +接続領域 7、 N -接続領域 8を 形成している。 第 1 5図に示す実施例では、 ラ ッチアップによる破壊を 回避するために P +接続領域 9が形成されている。 本実施例では、 N +接続 領域 7、 N -接続領域 8、 P +接続領域 9を形成するために計三工程必要と なる。 第 1 9図を用いて、 従来技術の P +接続領域 9がラ ッチアップ回避 に有効である理由を説明する。 第 1 9図には、 縱型電界効果 トランジス 夕が、 アバランシ 降伏した際のブレイクダウン電流の経路 1 8 0 1 を 示している。 チヤネル領域 3内のブレイクダウン電流経路 1 8 0 1 に添 つて電流が流れると、 チャネル領域 3のゲー ト電極 6エツ ジ部の電圧が 上昇する。 縱型電界効果 トラ ンジスタは、 N +ソース領域 2、 チャネル領 域 3、 及び N -ェピ層 4が N P Nのバイポーラ トラ ンジスタを形成している ため、 チャネル領域 3のゲー 卜電極 6エツ ジ部の電圧上昇により、 ベー スがオンした状態になり、 大電流が流れてしまう。 この現象をラ ッチァ ップと呼ぶ。 縱型電界効果 トラ ンジスタが、 ラッチアップすると、 素子 が破壊されてしまう。 ラ ッチアップを防ぐためには、 ゲー ト電極 6エツ ジ部の電圧上昇を抑制する必要がある。 P +接続領域 9は、 チャネル部 3 を低抵抗化することにより、 電圧降下によるゲー ト電極 6エッジ部の罨 圧上昇を抑制する技術である。 本技術を用いた場合、 N +接続領域、 N— 接铳領域、 及び P +接続領域を計三工程で形成する。 A conventional technique for avoiding destruction by latch-up will be described with reference to FIGS. 15 and 19. FIG. FIG. 15 shows an embodiment of the prior art. In FIG. 15, the N-epi layer 4 is removed above the N-substrate 5, and the channel region 3, N + source region 2, N + connection region 7, N + -The connection area 8 is formed. In the embodiment shown in FIG. 15, a P + connection region 9 is formed to avoid destruction due to latch-up. In this embodiment, a total of three steps are required to form the N + connection region 7, the N- connection region 8, and the P + connection region 9. The reason why the conventional P + connection region 9 is effective in avoiding latch-up will be described with reference to FIG. FIG. 19 shows the path 1801 of the breakdown current when the vertical field-effect transistor is subjected to avalanche breakdown. When a current flows along the breakdown current path 1801 in the channel region 3, the voltage at the edge of the gate electrode 6 in the channel region 3 increases. Since the N + source region 2, the channel region 3, and the N-epi layer 4 form an NPN bipolar transistor, the vertical field effect transistor has an edge portion of the gate electrode 6 in the channel region 3. When the voltage rises, the base turns on and a large current flows. This phenomenon is We call it top. If the vertical field-effect transistor latches up, the device will be destroyed. In order to prevent latch-up, it is necessary to suppress the voltage rise at the edge of the gate electrode 6. The P + connection region 9 is a technology that suppresses an increase in compressibility at the edge of the gate electrode 6 due to a voltage drop by reducing the resistance of the channel portion 3. When the present technology is used, an N + connection region, an N − connection region, and a P + connection region are formed in a total of three steps.
第 1 4図に、 本発明の一実施例を示す。 第 1 4図は、 従来三工程で形 成していた N +接続領域、 N—接続領域、 及びラッチアップを回避する構 造を一工程で形成することを可能とする素子構造を示したものである。 第 1 4図では、 N基板 5の上部に N -ェピ層 4を積層し、 N -ェピ層 4の領 域にチャネル領域 3、 N +ソース領域 2を形成している。 第 1 4図の構造 は、 ゲー ト 極 6直下では、 表面濃度が N -ェピ層 4の濃度以下となり、 N -ェピ層 4の港度以上になる深さ方向の範囲が、 N -ェピ層 4表面からチヤ ネル領域下端 1 0の間に位置するヒ素分布と、 チャネル領域 1 0直下で は、 N -ェピ層の濃度以上になる深さ方向の範囲が、 チャネル領域下端 1 0 と N基板 5との間に位置するヒ素分布を同時に構成している矩形高工 ネルギーヒ素打ち込み層 1 2を有する。 矩形高エネルギーヒ素打ち込み 層 1 2のゲー ト¾極 6直下のヒ素分布は、 高出力及び高スイ ッチング特 性を得る役割、 またチャネル領域 1 0直下のヒ素分布はラ ッチアップに よる破壊を回避する役割をはたす。 チャネル領域 1 0直下のヒ素分布が、 ラ ッチアップによる破壊を回避する理由を第 1 8図を用いて説明する。 第 1 9図に示す従来技術では、 アバランシェ降伏がチャネル領域 3のゲ 一ト電極 6左端付近で起こるのに対して、 第 1 4図に示す実施例では、 アバランシ X降伏はチヤネル領域 3の N +ソース領域 2左端付近で起きる。 従ってブレイクダウン電流は経路 1 8 0 1 に添って流れる。 ブレイ クダ ゥン電流経路 1 8 0 1 は、 従来技術と比較し短くなっているため、 電圧 降下によるチャネル領域 3のゲー ト電極 6エツジ部での電圧上昇が起こ りにくい。 従って、 ラッチアツプが起こ りにく く なつている。 単に、 N - ェピ層 4の濃度を上昇させただけでは、 第 1 9図に示すブレイクダウン 電流経路 1 8 0 2 となり、 ラ ッチアツプを回避できない。 FIG. 14 shows an embodiment of the present invention. Fig. 14 shows an N + connection region, an N- connection region, and a device structure that enables a structure to avoid latch-up to be formed in a single process, which was conventionally formed in three processes. It is. In FIG. 14, an N-epi layer 4 is laminated on an N substrate 5, and a channel region 3 and an N + source region 2 are formed in the region of the N-epi layer 4. The structure shown in Fig. 14 shows that immediately below the gate pole 6, the surface area in the depth direction where the surface concentration is less than the concentration of the N-epi layer 4 and higher than the portability of the N-epi layer 4 is N- The arsenic distribution located between the surface of the epitaxial layer 4 and the lower end 10 of the channel region, and the area directly below the channel region 10 in the depth direction where the concentration of the N-epi layer is higher than the lower end of the channel region 1 It has a rectangular high-energy arsenic implanted layer 12 which simultaneously constitutes an arsenic distribution located between 0 and the N substrate 5. The arsenic distribution directly under the gate ¾ pole 6 of the rectangular high-energy arsenic implanted layer 12 plays a role in obtaining high output and high switching characteristics, and the arsenic distribution directly under the channel region 10 avoids damage due to latch-up. Play a role. The reason why the arsenic distribution immediately below the channel region 10 avoids destruction due to latch-up will be described with reference to FIG. In the prior art shown in FIG. 19, the avalanche breakdown occurs near the left end of the gate electrode 6 in the channel region 3. On the other hand, in the embodiment shown in FIG. + Source area 2 Occurs near the left end. Therefore, the breakdown current flows along the path 1801. Blake Kuda Since the pin current path 1801 is shorter than that of the related art, a voltage drop at the edge of the gate electrode 6 of the channel region 3 due to a voltage drop does not easily occur. Therefore, latch-up is less likely to occur. Simply increasing the concentration of the N-epi layer 4 results in the breakdown current path 1802 shown in FIG. 19, and cannot avoid latch-up.
第 1 6図, 第 1 7図は, 第 1 4図に示す実施例の製造方法を示す。 第 1 6図, 第 1 7図に示す製造方法は, 従来三工程で形成していた N +接続領 域, N—接続領域, 及び P +接続領域を一工程で形成することを可能とする c 基板 5の上部に N -ェピ層 4を穡層し, N -ェピ層 4の領域にチャネル領 域 3 , N +ソース領域 2を形成する (第 1 6図) 。 N基板 5には, 低抵抗化 しゃすいヒ素 ドープ基板を用いる。 N -ェピ層 4形成時には, ェピ層を N 導電型にするためにリ ンを ドープする。 チャネル領域 3 は, 所定のマス ク形成後にポロ ンを基板 5中に打ち込み, 更に熱処理によ りボロンを拡 散させることにより形成する。 N +ソース領域 2は, 所定のマスク形成後 にヒ素を打ち込むこ とにより形成する。 次に, ゲー ト電極 6を形成する ために, レジス ト 1 7 0 1 をポ リ シ リ コ ン上に塗布し, ホ ト リ ソグラ フィ によ り レジス ト 1 7 0 1 を所定の領域のみ残し除去する。 レジス ト 1 7 0 1 除去後にポリ シ リ コ ンをエッチングすることによ り, 第 1 7図 に示す構造を形成することができる。 第 1 7図に示す構造を形成後, 高 エネルギーヒ素打ち込み 1 7 0 2により, 矩形高エネルギーヒ素打ち込 み層 1 2を形成する。 矩形高エネルギーヒ素打ち込み層 1 2を構成する。 ゲー ト¾極 6直下のヒ素分布の下端部は, チャネル領域 3の下端部の上 部に, 且つチャネル領域 3直下のヒ素分布の上端部は, チャネル領域 3 の下端部の下部に位置する。 ゲー ト電極 6直下のヒ素分布とチャネル領 域 3直下のヒ素分布の深さ方向 1 1 の位置は, レジス ト膜厚及び打ち込 みエネルギーよ り別々に指定することができる。 高エネルギーヒ素打ち 込み 1 7 0 2を用いることによ り, 従来三工程を必要と した構造をーェ 程で構成することができる。 FIGS. 16 and 17 show the manufacturing method of the embodiment shown in FIG. The manufacturing method shown in Fig. 16 and Fig. 17 makes it possible to form the N + connection area, N-connection area, and P + connection area in one process, which were conventionally formed in three processes. c An N-epi layer 4 is formed on the substrate 5 and a channel region 3 and an N + source region 2 are formed in the N-epi layer 4 (FIG. 16). As the N-substrate 5, a low-resistance arsenic-doped substrate is used. When the N-epi layer 4 is formed, phosphorus is doped to make the N-epi layer N-type. The channel region 3 is formed by implanting boron into the substrate 5 after forming a predetermined mask, and further diffusing boron by heat treatment. The N + source region 2 is formed by implanting arsenic after forming a predetermined mask. Next, in order to form the gate electrode 6, a resist 1701 is applied on the polysilicon, and the resist 1701 is applied only to a predetermined region by photolithography. Remove and remove. By etching the polysilicon after removing the resist 1701, the structure shown in Fig. 17 can be formed. After forming the structure shown in Fig. 17, a rectangular high-energy arsenic implanted layer 12 is formed by high-energy arsenic implantation 1702. A rectangular high energy arsenic implanted layer 12 is formed. The lower end of the arsenic distribution directly below the gate ¾ pole 6 is located above the lower end of the channel region 3, and the upper end of the arsenic distribution immediately below the channel region 3 is located below the lower end of the channel region 3. The positions of the arsenic distribution directly below the gate electrode 6 and the arsenic distribution directly below the channel region 3 in the depth direction 11 can be separately specified by the resist film thickness and the implantation energy. By using high-energy arsenic implantation 1702, a structure that conventionally required three processes can be configured by the ェ process.
本発明の効果の一つは、 従来二工程で形成していた N +接続領域と N— 接続領域を一工程で形成でき、 チップ単価を N +接続領域のみ形成する場 合と等しく できる。 One of the effects of the present invention is that the N + connection region and the N − connection region, which are conventionally formed in two steps, can be formed in one step, and the cost per chip can be made equal to the case where only the N + connection region is formed.
本発明のもう一つの効果は、 従来三工程で形成していた N +接続領域、 N—接続領域、 ラ ッチアツプによる破壊を回避するための構造を一工程で 形成でき、 チップ単価を従来以下にできる。 Another advantage of the present invention is that the N + connection region conventionally formed in three steps, The structure to avoid destruction due to N-connection area and latch-up can be formed in one process, and the unit cost of the chip can be reduced to less than the conventional one.
Claims
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| PCT/JP1995/001885 WO1997011497A1 (en) | 1995-09-20 | 1995-09-20 | Fabrication method of vertical field effect transistor |
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| PCT/JP1995/001885 WO1997011497A1 (en) | 1995-09-20 | 1995-09-20 | Fabrication method of vertical field effect transistor |
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| JP2014063949A (en) * | 2012-09-24 | 2014-04-10 | Sumitomo Electric Ind Ltd | Silicon carbide semiconductor device and method of manufacturing the same |
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