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JPH069254B2 - Method for manufacturing semiconductor radiation detecting element - Google Patents
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JPH069254B2 - Method for manufacturing semiconductor radiation detecting element - Google Patents

Method for manufacturing semiconductor radiation detecting element

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Publication number
JPH069254B2
JPH069254B2 JP62310514A JP31051487A JPH069254B2 JP H069254 B2 JPH069254 B2 JP H069254B2 JP 62310514 A JP62310514 A JP 62310514A JP 31051487 A JP31051487 A JP 31051487A JP H069254 B2 JPH069254 B2 JP H069254B2
Authority
JP
Japan
Prior art keywords
film
boron
substrate
amorphous silicon
detecting element
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.)
Expired - Lifetime
Application number
JP62310514A
Other languages
Japanese (ja)
Other versions
JPH01151242A (en
Inventor
則忠 佐藤
敏和 鈴木
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Corporate Research and Development Ltd
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 Fuji Electric Corporate Research and Development Ltd filed Critical Fuji Electric Corporate Research and Development Ltd
Priority to JP62310514A priority Critical patent/JPH069254B2/en
Publication of JPH01151242A publication Critical patent/JPH01151242A/en
Publication of JPH069254B2 publication Critical patent/JPH069254B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Measurement Of Radiation (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)
  • Light Receiving Elements (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は熱中性子線を含む放射線を検出する半導体放射
線検出素子の製造方法に関する。
The present invention relates to a method for manufacturing a semiconductor radiation detecting element for detecting radiation including thermal neutron rays.

〔従来の技術〕[Conventional technology]

半導体放射線検出素子は、その代表例を第2図に示すよ
うにp形の高比抵抗シリコン板21に酸化膜23をマスクと
してのりん拡散によってn領域22を形成し、このpn接
合に対する逆電圧の印加によって生ずる空乏層10内に放
射線が入射した際発生する電子−正孔対に基づき、両面
の両電極24,25間に流れる電流によって放射線を検出す
るものである。しかし中性子線は電荷をもっていないの
で、格反応以外には軌道電子や原子核のクーロン場には
なんらの作用も及ぼさず、従って電子−正孔対が生じな
い。このため、中性子線を中性子吸収断面積の大きい物
質を透過させ、中性子核変換反応によりα線を発生さ
せ、このα線によって空乏層内に電子−正孔対を生成さ
せる。
As shown in FIG. 2, a semiconductor radiation detecting element has a typical n-type region 22 formed on a p-type high resistivity silicon plate 21 by phosphorus diffusion using an oxide film 23 as a mask. The radiation is detected by the current flowing between the electrodes 24 and 25 on both sides, based on the electron-hole pairs generated when the radiation enters the depletion layer 10 caused by the application of. However, since the neutron beam has no charge, it has no effect on the Coulomb field of orbital electrons and nuclei except for the case reaction, and therefore electron-hole pairs do not occur. Therefore, a neutron beam is transmitted through a substance having a large neutron absorption cross section, an α ray is generated by a neutron transmutation reaction, and an electron-hole pair is generated in the depletion layer by the α ray.

第3図は特開昭61−17477号公報により開示された熱中
性子検出可能の半導体放射線検出素子の断面構造を示す
もので、n形シリコン基板1,ほう素被膜2,電極31,3
2から構成されている。基板1のほう素被膜に接する部
分にp形ドーピング層4が形成されている。この検出素
子にpn接合への逆電圧−Vを印加した状態で熱中性
子線11が入射するとほう素被膜2において、10B+n→
7Li+αの中性子核変換反応によりα粒子12と7Li核13が
発生し、このα粒子と7Li核によって空乏層10に電子−
正孔対が生成され、これが増幅回路15を通して検出され
る。
FIG. 3 shows a cross-sectional structure of a semiconductor radiation detecting element capable of detecting thermal neutrons, which is disclosed in Japanese Patent Laid-Open No. 61-17477. The n-type silicon substrate 1, the boron coating 2, the electrodes 31, 3 are shown.
It consists of two. A p-type doping layer 4 is formed on a portion of the substrate 1 which is in contact with the boron film. When a thermal neutron beam 11 is incident on the detection element with a reverse voltage −V B applied to the pn junction, 10 B + n →
7 Li + alpha particles 12 and 7 Li nucleus 13 by neutron transmutation reaction of alpha is generated, electrons in the depletion layer 10 by the alpha particles and 7 Li nucleus -
Hole pairs are generated, which are detected through the amplification circuit 15.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

第4図(a)〜(e)は、第3図に示した検出素子の製造工程
の概要を示すもので、n形シリコン基板1の表面に熱酸
化膜またはCVD酸化膜23を被着したのち(a図)、ホト
エッチング工程で窓26をあけ(b図)、プラズマCVD法
によりこの窓上にマスク27を通してほう素被膜2を形成
する(c図)。次いで、このシリコン基板を赤外線照射ア
ニール炉に挿入して、例えば900℃で10秒間乾燥窒素中
でアニールを行い、シリコン基板1中に浸入したほう素
28をさらに電気的に活性化し、P領域4を形成する(d
図)。次に、マスク27より100〜200μm口径の小さいマ
スク29を通して、例えばアルミニウムの真空蒸着法でほ
う素被膜2の表面上に電極31を、またシリコン基板1の
裏面に電極32を形成する(e図)。
4 (a) to 4 (e) show an outline of the manufacturing process of the detection element shown in FIG. 3, in which a thermal oxide film or a CVD oxide film 23 is deposited on the surface of the n-type silicon substrate 1. After that (FIG. A), the window 26 is opened by a photo-etching process (FIG. B), and the boron film 2 is formed on this window through the mask 27 by the plasma CVD method (FIG. C). Then, this silicon substrate is inserted into an infrared irradiation annealing furnace, and is annealed in dry nitrogen at 900 ° C. for 10 seconds, for example, and boron is immersed in the silicon substrate 1.
28 is further electrically activated to form P + region 4 (d
(Figure). Next, an electrode 31 is formed on the surface of the boron coating 2 and an electrode 32 is formed on the back surface of the silicon substrate 1 by, for example, a vacuum evaporation method of aluminum through a mask 29 having a diameter of 100 to 200 μm smaller than that of the mask 27 (e figure). ).

上述の製造工程は、熱酸化膜またはCVD酸化膜を形成
するための酸化膜生成装置,赤外線照射アニール炉,ホ
トエッチング装置およびプラズマCVD装置,真空蒸着
装置を少なくとも必要とする。したがって、放射線検出
素子の製造には多くの工程と日数を要し、そのほかに高
価な酸化膜生成装置やホトエッチング装置はその取扱い
に高度の技術を要するという欠点があった。
The above-described manufacturing process requires at least an oxide film generation device for forming a thermal oxide film or a CVD oxide film, an infrared irradiation annealing furnace, a photoetching device, a plasma CVD device, and a vacuum deposition device. Therefore, the manufacturing of the radiation detecting element requires many steps and days, and in addition, the expensive oxide film generating apparatus and photoetching apparatus have a drawback that a high technique is required for handling them.

本発明の目的は上述の欠点を除き、比較的簡単な製造設
備と短期間の技術教育で、熱中性子線の検出も可能で特
性良好な半導体放射線検出素子の製造方法を提供するこ
とを目的とする。
The object of the present invention is to provide a method for manufacturing a semiconductor radiation detecting element which is capable of detecting thermal neutron rays and has good characteristics, with relatively simple manufacturing equipment and short-term technical education, except for the above-mentioned drawbacks. To do.

〔問題点を解決するための手段〕[Means for solving problems]

上記の目的を達成するために、本発明の方法は、n形半
導体基板の一面の所定の領域にほう素膜を被着し、その
半導体基板にほう素被膜と接触するp形領域を設けて半
導体基板本来の部分との間にpn接合を形成するに際
し、n形半導体基板の一面にシリコン化合物ガスを用い
てのプラズマCVD法により非晶質シリコン膜を被着し
たのち、エッチング用ガスを用いてのプラズマエッチン
グにより非晶質シリコン膜をマスクを介して選択的に除
去し、次いでほう素化合物ガスを用いてのプラズマCV
D法により基板面の非晶質シリコン膜除去部にほう素膜
を被着すると共に、ほう素原子を基板内に侵入させてp
層を形成するものとする。
In order to achieve the above object, the method of the present invention comprises depositing a boron film on a predetermined region of one surface of an n-type semiconductor substrate and providing the semiconductor substrate with a p-type region in contact with the boron coating. In forming a pn junction with the original portion of the semiconductor substrate, an amorphous silicon film is deposited on one surface of the n-type semiconductor substrate by a plasma CVD method using a silicon compound gas, and then an etching gas is used. The amorphous silicon film is selectively removed through a mask by plasma etching, and then plasma CV is performed using a boron compound gas.
A boron film is deposited on the removed portion of the amorphous silicon film on the substrate surface by the D method, and boron atoms are allowed to penetrate into the substrate to p
A layer shall be formed.

〔作用〕[Action]

プラズマCVD法により形成後プラズマエッチングでパ
ターニングされた非晶質シリコン膜が従来の酸化膜に代
わってp層形成のマスクとして働き、プラズマCVD法
によるほう素膜の被着と同時にグロー放電による基板の
温度上昇によりほう素のドーピングが行われる。従っ
て、各工程が同一のプラズマ反応装置で実施可能であ
る。
The amorphous silicon film formed by plasma CVD and then patterned by plasma etching acts as a mask for forming a p-layer instead of a conventional oxide film, and a boron film is deposited by plasma CVD and at the same time a substrate is formed by glow discharge. Boron is doped by increasing the temperature. Therefore, each process can be performed by the same plasma reactor.

〔実施例〕〔Example〕

以下図を引用して本発明の一実施例について説明する。
第5図は本発明の実施に用いられるプラズマ反応装置を
示し、真空容器51内に対向する電極52,53が配置され、
電源54に接続されている。一方の電極53の下には、電極
上に載置される半導体基板1を加熱できるように電源55
に接続されたヒータ56を備えている。真空排気系57は真
空計59で測定される容器内圧力調整のためのバルブ58を
介して真空容器51に接続され、一方各種のガスのボンベ
61,62,63はガスの圧力と流量を調整するための調整回路
64を介して真空容器に接続されている。この装置を用い
ての製造工程を第1図(a)〜(d)に示す。まず、比抵抗10
00Ωcmのn形シリコン基板1を鏡面を上にして負電極53
の上に載置し、例えば水素で10%に希釈したSiH4ガスを
ボンベ61から真空容器51に導入し、ガス圧力1〜10Torr
で電極52,53間に600〜800Vの電圧を印加してグロー放
電を発生させ、ヒータ56により200℃に加熱された基板
の表面に厚さ1μmの非晶質シリコン膜5を被着させる
(a図)。次に所定の形状の金属マスク6を前記非晶質
シリコン膜5上に配置したのち、ボンベ62からSF6ガス
を前記真空容器1に導入し、ガス圧力0.2Torrで800Vの
放電電圧でグロー放電を発生させると、金属マスクで覆
われていない窓の部分はSF6ガスと反応して非晶質シリ
コン膜5の領域7がドライエッチングによって除去され
る(b図)。次いで、例えばほう素の同位元素10Bを94%
以上含有したジボラン(B2H6)を水素で1000ppmに希釈し
たガスをボンベ63から真空容器51に導入してガス圧力2
〜6Torrで400〜700Vの放電電圧により同様にグロー放
電を発生させ、膜厚0.6μmのほう素被膜2を温度200℃
のシリコン基板1の領域7の上に被着させる。このほう
素被膜形成時にほう素原子はn形シリコン基板1に侵入
し、表面濃度:1〜3×1015原子/cm3,深さ:約0.3μ
mのP形ドーピング層4が生じ、pn接合が形成される
(c図)。
An embodiment of the present invention will be described below with reference to the drawings.
FIG. 5 shows a plasma reactor used for carrying out the present invention, in which electrodes 52 and 53 facing each other are arranged in a vacuum chamber 51.
Connected to power supply 54. Below the one electrode 53, a power supply 55 is provided so that the semiconductor substrate 1 placed on the electrode can be heated.
And a heater 56 connected to the. The vacuum evacuation system 57 is connected to the vacuum container 51 through a valve 58 for adjusting the pressure inside the container, which is measured by a vacuum gauge 59.
61, 62, 63 are adjusting circuits for adjusting gas pressure and flow rate
It is connected to the vacuum vessel via 64. A manufacturing process using this apparatus is shown in FIGS. 1 (a) to (d). First, the specific resistance 10
Negative electrode 53 with 00Ωcm n-type silicon substrate 1 with the mirror surface facing up
Placed on the top of the container, for example, SiH 4 gas diluted with hydrogen to 10% is introduced into the vacuum container 51 from the cylinder 61, and the gas pressure is 1 to 10 Torr.
Then, a voltage of 600 to 800 V is applied between the electrodes 52 and 53 to generate glow discharge, and a 1 μm thick amorphous silicon film 5 is deposited on the surface of the substrate heated to 200 ° C. by the heater 56 ( (Figure a). Next, a metal mask 6 having a predetermined shape is placed on the amorphous silicon film 5, SF 6 gas is introduced from the cylinder 62 into the vacuum vessel 1, and a glow discharge is performed at a gas pressure of 0.2 Torr and a discharge voltage of 800 V. Is generated, the portion of the window which is not covered with the metal mask reacts with SF 6 gas and the region 7 of the amorphous silicon film 5 is removed by dry etching (FIG. 7B). Then, for example, boron isotope 10 B is added to 94%
Gas containing diborane (B 2 H 6 ) contained above diluted to 1000 ppm with hydrogen is introduced into the vacuum vessel 51 from the cylinder 63 and the gas pressure is set to 2
Glow discharge is similarly generated by a discharge voltage of 400 to 700 V at -6 torr, and the boron coating 2 having a thickness of 0.6 μm is heated at a temperature of 200 ° C.
On the area 7 of the silicon substrate 1. At the time of forming the boron film, boron atoms penetrate into the n-type silicon substrate 1 and have a surface concentration of 1 to 3 × 10 15 atoms / cm 3 and a depth of about 0.3 μm.
A P-type doping layer 4 of m is formed to form a pn junction.
(Figure c).

次に、このn形シリコン基板1を真空容器51から取り出
しマスク8を用いて、第4図の場合と同様に例えばアル
ミニウム層を真空蒸着法でほう素被膜2上および基板1
の裏面に形成し、電極31,32を得る(d図)。なお、各反
応ガスを真空容器51に導入する前には真空排気系57によ
り真空度を1×10-6Torrに保持したのちに各工程を行っ
た。
Next, the n-type silicon substrate 1 is taken out of the vacuum chamber 51 and the mask 8 is used to form, for example, an aluminum layer on the boron film 2 and the substrate 1 by vacuum vapor deposition as in the case of FIG.
Then, the electrodes 31 and 32 are obtained by forming the electrodes on the back surface (FIG. 3D). Before introducing each reaction gas into the vacuum vessel 51, each step was performed after the vacuum degree was kept at 1 × 10 −6 Torr by the vacuum exhaust system 57.

このようにして製造された素子の構造自体は第4図の工
程で製造された第3図の素子と同様であるが、表面保護
膜として酸化膜の代わりに非晶質シリコン膜を用い、非
晶質シリコン膜の窓あけ工程をホトエッチングの代わり
に金属マスクを用いてのドライエッチングで行う点が異
なっている。プラズマCVD法による非晶質シリコン膜
の比抵抗は1〜3×1010Ωcmで、熱酸化膜やCVD酸化
膜の1014〜1015Ωcmにくらべて低いため、放射線照射時
に生じる電荷が表面保護膜中に蓄積されにくく、耐放射
線性の強い素子が得られる。特に中性子線検出に用いる
場合は、混在するr線が多いためその効果が大きい。
The structure of the device thus manufactured is the same as that of the device of FIG. 3 manufactured in the process of FIG. 4, except that an amorphous silicon film is used instead of the oxide film as the surface protection film. The difference is that the window opening process of the crystalline silicon film is performed by dry etching using a metal mask instead of photoetching. The resistivity of an amorphous silicon film formed by plasma CVD is 1 to 3 × 10 10 Ωcm, which is lower than 10 14 to 10 15 Ωcm of a thermal oxide film or a CVD oxide film. It is possible to obtain an element that is hard to be accumulated in the film and has high radiation resistance. Especially when it is used for neutron ray detection, its effect is great because many r rays are mixed.

〔発明の効果〕〔The invention's effect〕

本発明によれば、プラズマCVD法により形成できる非
晶質シリコン膜を表面保護膜として用い、その膜にプラ
ズマエッチングにより開けられた窓部に、プラズマCV
D法により同位元素を含むほう素被膜の形成とドーピン
グを同時に行ってN形シリコン基板中にPN接合を形成
することにより、同一装置内で連続してプラズマ反応を
利用して大気中に素子基板をさらすことなく各工程を行
うことができる。従って清浄なシリコン基板面にほう素
被膜が膜厚の再現性および密着性よく形成でき、またマ
スクを用いてのドライエッチングによりホトエッチング
工程が不要となり、酸化膜生成工程の不要となるのと相
まって製造設備の節減,製造工程の大幅な簡略化がで
き、中性子線検出可能の耐放射線性の強い半導体放射線
素子の製造コストの低減が可能となった。
According to the present invention, an amorphous silicon film that can be formed by the plasma CVD method is used as a surface protection film, and a plasma CV is formed in a window opened in the film by plasma etching.
By forming a boron film containing an isotope and doping at the same time by the D method to form a PN junction in the N-type silicon substrate, the plasma reaction is continuously utilized in the same device to expose the element substrate to the atmosphere. Each step can be performed without exposing. Therefore, the boron film can be formed on the surface of a clean silicon substrate with good reproducibility of the film thickness and good adhesion, and the photo-etching process is not required due to the dry etching using the mask, which is not necessary for the oxide film forming process. This has made it possible to reduce manufacturing equipment, greatly simplify the manufacturing process, and reduce the manufacturing cost of semiconductor radiation devices that can detect neutron rays and have strong radiation resistance.

【図面の簡単な説明】[Brief description of drawings]

第1図(a)〜(d)は本発明の一実施例の製造工程を順次示
す断面図、第2図は半導体放射線検出素子の断面図、第
3図は中性子線検出可能の半導体放射線検出素子の断面
図、第4図(a)〜(e)は第3図の素子の従来の製造工程の
順次示す断面図、第5図は本発明の一実施例に用いるプ
ラズマ反応装置の構成図である。 1:n形シリコン基板、2:ほう素被膜、4:p形ドー
ピング層、5:非晶質シリコン膜、6:マスク。
1 (a) to 1 (d) are sectional views sequentially showing a manufacturing process of an embodiment of the present invention, FIG. 2 is a sectional view of a semiconductor radiation detecting element, and FIG. 3 is a semiconductor radiation detection capable of detecting neutron rays. Sectional views of the element, FIGS. 4 (a) to 4 (e) are sectional views sequentially showing the conventional manufacturing process of the element of FIG. 3, and FIG. 5 is a configuration diagram of a plasma reactor used in one embodiment of the present invention. Is. 1: n-type silicon substrate, 2: boron film, 4: p-type doping layer, 5: amorphous silicon film, 6: mask.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】n形半導体基板の一面の所定の領域にほう
素膜を被着し、該半導体基板のほう素被膜と接触するp
形領域を設けて半導体基板本来の部分との間にpn接合
を形成するに際し、n形半導体基板の一面にシリコン化
合物ガスを用いてのプラズマCVD法により非晶質シリ
コン膜を被着したのち、エッチング用ガスを用いてのプ
ラズマエッチングにより該非晶質シリコン膜をマスクを
介して選択的に除去し、次いでほう素化合物ガスを用い
てのプラズマCVD法により基板面の前記非晶質シリコ
ン膜除去部にほう素膜を被着すると共にほう素原子を基
板内に浸入させてp層を形成することを特徴とする半導
体放射線検出素子の製造方法。
1. A boron film is deposited on a predetermined region on one surface of an n-type semiconductor substrate, and p is brought into contact with the boron film of the semiconductor substrate.
In forming a pn junction with the original portion of the semiconductor substrate by providing the shaped region, an amorphous silicon film is deposited on one surface of the n-type semiconductor substrate by a plasma CVD method using a silicon compound gas. The amorphous silicon film is selectively removed through a mask by plasma etching using an etching gas, and then the amorphous silicon film removal portion on the substrate surface is formed by a plasma CVD method using a boron compound gas. A method for manufacturing a semiconductor radiation detecting element, comprising depositing a boron film on the substrate and infiltrating boron atoms into the substrate to form a p-layer.
JP62310514A 1987-12-08 1987-12-08 Method for manufacturing semiconductor radiation detecting element Expired - Lifetime JPH069254B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62310514A JPH069254B2 (en) 1987-12-08 1987-12-08 Method for manufacturing semiconductor radiation detecting element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62310514A JPH069254B2 (en) 1987-12-08 1987-12-08 Method for manufacturing semiconductor radiation detecting element

Publications (2)

Publication Number Publication Date
JPH01151242A JPH01151242A (en) 1989-06-14
JPH069254B2 true JPH069254B2 (en) 1994-02-02

Family

ID=18006145

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62310514A Expired - Lifetime JPH069254B2 (en) 1987-12-08 1987-12-08 Method for manufacturing semiconductor radiation detecting element

Country Status (1)

Country Link
JP (1) JPH069254B2 (en)

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* Cited by examiner, † Cited by third party
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CN100405083C (en) * 2004-11-11 2008-07-23 中国科学院近代物理研究所 Nuclear radiation detector and its manufacturing process
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