JPH02114538A - High frequency high power field effect transistor - Google Patents

High frequency high power field effect transistor

Info

Publication number
JPH02114538A
JPH02114538A JP63268604A JP26860488A JPH02114538A JP H02114538 A JPH02114538 A JP H02114538A JP 63268604 A JP63268604 A JP 63268604A JP 26860488 A JP26860488 A JP 26860488A JP H02114538 A JPH02114538 A JP H02114538A
Authority
JP
Japan
Prior art keywords
region
impurity concentration
drain region
gate electrode
back gate
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP63268604A
Other languages
Japanese (ja)
Inventor
Toshikazu Manno
万野 寿和
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
NEC Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Corp filed Critical NEC Corp
Priority to JP63268604A priority Critical patent/JPH02114538A/en
Publication of JPH02114538A publication Critical patent/JPH02114538A/en
Pending legal-status Critical Current

Links

Landscapes

  • Junction Field-Effect Transistors (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Abstract] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、高周波高出力電界効果トランジスタの構造に
関し、特に縦型MO3構造を有する電界効果トランジス
タの構造に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to the structure of a high frequency, high power field effect transistor, and particularly to the structure of a field effect transistor having a vertical MO3 structure.

〔従来の技術〕[Conventional technology]

従来、この種の高電力MO8FETは高耐圧設計を行っ
てもさほどオン抵抗が大きくならず、かつ単位チップ面
積当りのゲート幅が大きくとれるという利点を有する縦
型MO8構造が広く用いられている。この構造は、第2
図に示すように、高不純物濃度基板6上に同導電型のド
レイン領域2を有し、このドレイン領域2に逆導電型の
バックゲート領域1と基板6と同導電型のソース領域5
とを有し、ゲート電極4をソース領域5とドレイン領域
2との間にゲート酸化膜7を介して設け、ソース電極9
をソース領域5とバックゲート領域lとに接続して形成
していた。かかる縦型MO3構造を用いて高周波化を図
るには、第2図に示すように、バックゲート1並びにソ
ース領域5をゲート電極4に対して自己整合で拡散ある
いはイオン注入により形成することで、ソース領域5と
ゲート電極4との重なり容量を低減する手法が一般的で
あった。この際、ドレイン領域2は、ゲート電極4に対
して自己整合で形成されないのでバックゲート領域lは
ゲート電極4よりドレイン領域2側にできるだけはみ出
ないようにバックゲート領域1の拡散時間を制御してい
た。この種の構造を用いた例としては、たとえば、IE
DM 84−447〜450 ”A 900MHz 1
00W VD−MOSFET WITH5ILICID
E GATE 5ELF−ALIGNED CANNE
L”に示されている。
Conventionally, this type of high-power MO8FET has been widely used with a vertical MO8 structure, which has the advantage that the on-resistance does not increase significantly even when designed with a high breakdown voltage, and the gate width per unit chip area can be increased. This structure is the second
As shown in the figure, a drain region 2 of the same conductivity type is provided on a highly impurity-concentrated substrate 6, and this drain region 2 includes a back gate region 1 of an opposite conductivity type and a source region 5 of the same conductivity type as the substrate 6.
A gate electrode 4 is provided between a source region 5 and a drain region 2 with a gate oxide film 7 interposed therebetween, and a source electrode 9 is provided between the source region 5 and the drain region 2.
is connected to the source region 5 and the back gate region l. In order to achieve high frequency using such a vertical MO3 structure, as shown in FIG. 2, the back gate 1 and source region 5 are formed by diffusion or ion implantation in self-alignment with the gate electrode 4. A common method has been to reduce the overlap capacitance between the source region 5 and the gate electrode 4. At this time, since the drain region 2 is not formed in self-alignment with the gate electrode 4, the diffusion time of the back gate region 1 is controlled so that the back gate region l does not protrude from the gate electrode 4 toward the drain region 2 as much as possible. Ta. An example using this kind of structure is, for example, IE
DM 84-447~450”A 900MHz 1
00W VD-MOSFET WITH5ILICID
E GATE 5ELF-ALIGNED CANNE
It is shown in "L".

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上述した従来の縦型MO8FETの構造では、拡散のバ
ラツキを考慮して、バックゲート領域1は、ゲート電極
4の内側に約0.5μm程度までしか延ばさないので、
ゲート−ドレイン間の帰還容量は設計値としである程度
見込まねばならず、これが利得帯域幅積の低下を招いて
いた。また、高出力トランジスタの場合、チップ面積が
太きくなるので、バックゲート領域1の拡散長のバラツ
キとゲート電極4の長さとのバラツキの両者が原因で単
位トランジスタのチャネル長と帰還容量のバラツキが出
るので合成損失が増大するという欠点があった。
In the structure of the conventional vertical MO8FET described above, the back gate region 1 extends only to about 0.5 μm inside the gate electrode 4 in consideration of diffusion variations.
A certain amount of feedback capacitance between the gate and the drain must be assumed as a design value, which causes a decrease in the gain-bandwidth product. In addition, in the case of high-output transistors, the chip area becomes large, so variations in the channel length and feedback capacitance of the unit transistor are caused by both variations in the diffusion length of the back gate region 1 and variations in the length of the gate electrode 4. This has the disadvantage that the synthesis loss increases.

〔課題を解決するための手段〕[Means to solve the problem]

本発明によれば、ゲート電極よりドレイン領域にせり出
したバックゲート領域と、せり出したバックゲート領域
の表面にドレイン領域と同程度の不純物濃度の真性ドレ
イン領域を有する縦型構造の高周波高出力電界効果トラ
ンジスタを得る。
According to the present invention, the high-frequency, high-output electric field effect of the vertical structure has a back gate region that protrudes from the gate electrode to the drain region, and an intrinsic drain region that has the same impurity concentration as the drain region on the surface of the protruded back gate region. Get a transistor.

〔実施例〕〔Example〕

次に、本発明について図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.

第1図は本発明の一実施例による縦型MO3FETの構
造断面図を示す。バックゲート領域1並びにソース領域
5は、ゲート電極4に対して自己整合で形成されている
。更にバックゲート領域lは、ソース領域5からみてゲ
ート電極4よりドレイン領域2側にせり出ており、かつ
、このせり出たバックゲート領域1の表面には、ゲート
電極4に対して自己整合で、ドレイン領域2の不純物と
同程度の濃度を有する真性ドレイン領域3を有する。こ
こで、真性ドレイン領域3の不純物濃度をドレイン領域
2の不純物濃度と同程度にした理由は、真性ドレイン部
による耐圧の劣化を防ぐためである。上記の構造をとる
ことで、チャネル長はゲート電極4でのみ決定され、か
つ、ゲート電極4.ドレイン領域2間の帰還容量も、真
性ドレイン領域3の横広がりで決定されるので、バラツ
キが少なく、かつ、高周波特性の優れたFETを作るこ
とができる。
FIG. 1 shows a structural cross-sectional view of a vertical MO3FET according to an embodiment of the present invention. Back gate region 1 and source region 5 are formed in self-alignment with gate electrode 4 . Furthermore, the back gate region 1 protrudes from the gate electrode 4 toward the drain region 2 side when viewed from the source region 5, and the surface of this protruding back gate region 1 has a surface that is self-aligned with the gate electrode 4. , has an intrinsic drain region 3 having an impurity concentration comparable to that of the drain region 2. Here, the reason why the impurity concentration of the intrinsic drain region 3 is made to be approximately the same as that of the drain region 2 is to prevent the breakdown voltage from deteriorating due to the intrinsic drain portion. By adopting the above structure, the channel length is determined only by the gate electrode 4, and the channel length is determined only by the gate electrode 4. Since the feedback capacitance between the drain regions 2 is also determined by the lateral extent of the intrinsic drain region 3, an FET with little variation and excellent high frequency characteristics can be manufactured.

次に、上記実施例の効果を数値例で示す。縦型構造の場
合、チャネル部は拡散で形成されるので、チャネル長は
通常3μm以下で設計するのが通常である。
Next, the effects of the above embodiment will be shown using numerical examples. In the case of a vertical structure, since the channel portion is formed by diffusion, the channel length is usually designed to be 3 μm or less.

従来技術の第2図に示す構造の場合、チャネル長を2.
5 μm、ゲート幅を20cmで耐圧を100V以上を
目標に設計を行うと、利得帯域幅積は次に示す様な結果
となる。このとき、ゲート・ドレイン間の重なりは、拡
散でのバラツキと、ゲート電極長変換差バラツキを考慮
に入れなければならないので、1.5μm程度必要とな
る。利得帯域幅積(fT)は、 1:’τ二)で干0〒う品4τ°譜早屏3を炙′ん)で
表される。上記の条件では、c、、=300 pF。
In the case of the conventional structure shown in FIG. 2, the channel length is 2.
When designing with a target of 5 μm, gate width of 20 cm, and breakdown voltage of 100 V or more, the gain-bandwidth product results as shown below. At this time, the overlap between the gate and the drain must be approximately 1.5 μm, since it is necessary to take into account variations in diffusion and variations in gate electrode length conversion difference. The gain-bandwidth product (fT) is expressed as: 1:'τ2); Under the above conditions, c, , = 300 pF.

g、、=2.  c、d=l OOpF、R,=lΩと
なり、利得帯域幅積f1は300MHzとなる。
g,,=2. c, d=l OOpF, R,=lΩ, and the gain bandwidth product f1 is 300 MHz.

一方、第1図に示した一実施例の構造を同じデイメンジ
ョンで行うと、ゲート・ドレイン間の重なりは、0.3
μm程度に低減されるので、C,d21pFとなり、利
得帯域幅積fTは470MHz程度まで上昇する。
On the other hand, if the structure of the embodiment shown in FIG. 1 is constructed with the same dimension, the overlap between the gate and drain will be 0.3
Since it is reduced to approximately μm, C, d becomes 21 pF, and the gain bandwidth product fT increases to approximately 470 MHz.

尚、ゲート電極4の材質については、ソース領域5ある
いは真性ドレイン領域3を形成する際にマスクと成り得
る材質であり、かつ、バックゲート領域1を形成する際
の高温熱処理に耐え得る材質であれば、特に制約はない
。通常は、ポリシリコン、モリブデンやタングステン又
は前記材質の化合物を用いるのが一般的である。
The material for the gate electrode 4 may be any material that can serve as a mask when forming the source region 5 or the intrinsic drain region 3 and that can withstand high-temperature heat treatment when forming the back gate region 1. There are no particular restrictions. Usually, polysilicon, molybdenum, tungsten, or a compound of the above materials is used.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明は、縦型MO8FETにお
いて、バックゲート領域をソース領域からみてゲート電
極よりドレイン領域にせり出した構造にし、かつ、ゲー
ト電極よりドレイン領域の表面にドレイン領域と同程度
の真性ドレイン領域をゲート電極に対して自己整合で形
成することにより、チャネル長を、ゲート電極長のみで
制御でき、かつ、帰還容量を低減できるので、合成損失
を低減しかつ利得帯域幅積を広くとれるという効果を有
する。
As explained above, the present invention provides a vertical MO8FET with a structure in which the back gate region protrudes from the gate electrode toward the drain region when viewed from the source region, and the surface of the drain region from the gate electrode has the same extent as the drain region. By forming the intrinsic drain region in self-alignment with the gate electrode, the channel length can be controlled only by the gate electrode length, and feedback capacitance can be reduced, reducing combined loss and widening the gain bandwidth product. It has the effect of being removed.

5・・・・・・ソース領域、6・・・・・・高不純物濃
度基板、7・・・・・・ゲート酸化膜、8・・・・・・
層間絶縁膜、9・・・・・ソース電極。
5...Source region, 6...High impurity concentration substrate, 7...Gate oxide film, 8...
Interlayer insulating film, 9...source electrode.

Claims (1)

【特許請求の範囲】[Claims] 第一導電型で高不純物濃度の半導体基板上に前記第一導
電型で低不純物濃度の半導体層を設け、該低不純物濃度
の半導体層をドレイン領域とし、該低不純物濃度の半導
体層の表面側にバックゲート領域、ソース領域を形成し
た縦型構造の電界効果トランジスタにおいて、前記バッ
クゲート領域を前記ソース領域からみて前記ゲート電極
より前記ドレイン領域側にせり出した構造になっており
、かつ、前記ゲート電極より前記ドレイン領域側にせり
出した前記バックゲート領域の表面に、前記低不純濃度
領域と同程度の不純物濃度の真性ドレイン領域を前記ゲ
ート電極に対して自己整合で形成したことを特徴とする
高周波高出力電界効果トランジスタ。
A semiconductor layer of a first conductivity type and a low impurity concentration is provided on a semiconductor substrate of a first conductivity type and a high impurity concentration, the semiconductor layer of the low impurity concentration is used as a drain region, and the surface side of the semiconductor layer of the low impurity concentration is provided. In a field effect transistor having a vertical structure in which a back gate region and a source region are formed, the back gate region has a structure in which the back gate region protrudes from the gate electrode toward the drain region side when viewed from the source region, and A high frequency device characterized in that an intrinsic drain region having an impurity concentration similar to that of the low impurity concentration region is formed on the surface of the back gate region protruding from the electrode toward the drain region in a self-aligned manner with respect to the gate electrode. High power field effect transistor.
JP63268604A 1988-10-24 1988-10-24 High frequency high power field effect transistor Pending JPH02114538A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63268604A JPH02114538A (en) 1988-10-24 1988-10-24 High frequency high power field effect transistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63268604A JPH02114538A (en) 1988-10-24 1988-10-24 High frequency high power field effect transistor

Publications (1)

Publication Number Publication Date
JPH02114538A true JPH02114538A (en) 1990-04-26

Family

ID=17460844

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63268604A Pending JPH02114538A (en) 1988-10-24 1988-10-24 High frequency high power field effect transistor

Country Status (1)

Country Link
JP (1) JPH02114538A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10457178B2 (en) 2015-08-04 2019-10-29 Ts Tech Co., Ltd. Armrest device

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10457178B2 (en) 2015-08-04 2019-10-29 Ts Tech Co., Ltd. Armrest device
US10994639B2 (en) 2015-08-04 2021-05-04 Ts Tech Co., Ltd. Armrest device
US11535135B2 (en) 2015-08-04 2022-12-27 Ts Tech Co., Ltd. Armrest device
US11827132B2 (en) 2015-08-04 2023-11-28 Ts Tech Co., Ltd. Armrest device

Similar Documents

Publication Publication Date Title
US6667516B2 (en) RF LDMOS on partial SOI substrate
JPH022179A (en) Metal semiconductor fet
US5977588A (en) Radio frequency power MOSFET device having improved performance characteristics
US6087697A (en) Radio frequency power MOSFET device having improved performance characteristics
JP2002343960A (en) Semiconductor device
JP3185441B2 (en) High frequency high power field effect transistor
JPH11168099A (en) Semiconductor device
US20070145415A1 (en) High-frequency semiconductor device
JPH02114538A (en) High frequency high power field effect transistor
US6207508B1 (en) Method for fabricating a radio frequency power MOSFET device having improved performance characteristics
JPH02231771A (en) vertical field effect transistor
US20020167044A1 (en) Semiconductor component with an edge termination that is suitable for high voltage
JPH0493083A (en) Semiconductor device and its manufacturing method
US6893923B2 (en) Reduced mask count process for manufacture of mosgated device
JPH051083Y2 (en)
JP2914411B2 (en) Field effect transistor
US20240204065A1 (en) High frequency transistor
CN118281049B (en) A semiconductor device
JPH01111378A (en) Vertical mosfet
JP2638776B2 (en) Semiconductor device
JPH065858A (en) Insulated gate type semiconductor device
US9502557B2 (en) LDMOS for high frequency power amplifiers
JP2507030B2 (en) Field effect transistor
JPH03238831A (en) Compound semiconductor field effect transistor
JP2867420B2 (en) Compound semiconductor device