JPS5966031A - High brightness surface ionization type ion source and its manufacturing method - Google Patents

High brightness surface ionization type ion source and its manufacturing method

Info

Publication number
JPS5966031A
JPS5966031A JP57175390A JP17539082A JPS5966031A JP S5966031 A JPS5966031 A JP S5966031A JP 57175390 A JP57175390 A JP 57175390A JP 17539082 A JP17539082 A JP 17539082A JP S5966031 A JPS5966031 A JP S5966031A
Authority
JP
Japan
Prior art keywords
ion
tungsten
ion source
melting point
manufacturing
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.)
Granted
Application number
JP57175390A
Other languages
Japanese (ja)
Other versions
JPH0145699B2 (en
Inventor
Osamu Tsukagoshi
修 塚越
Kiyoshi Komatsu
小松 清
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.)
Ulvac Inc
Original Assignee
Ulvac Inc
Nihon Shinku Gijutsu KK
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 Ulvac Inc, Nihon Shinku Gijutsu KK filed Critical Ulvac Inc
Priority to JP57175390A priority Critical patent/JPS5966031A/en
Publication of JPS5966031A publication Critical patent/JPS5966031A/en
Publication of JPH0145699B2 publication Critical patent/JPH0145699B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J27/00Ion beam tubes
    • H01J27/02Ion sources; Ion guns
    • H01J27/022Details

Abstract

PURPOSE:To reduce the emission area of ion source substance thus to improve ion emission per unit area by covering the surface of ion generating section composed of porous W except the central portion with an ion inpermeable film having high melting point such as W. CONSTITUTION:A porous W5 cut into a conical shape is electron beam welded onto the tubular member 6 of Ta to form a conical ion generating section the surface of which is spattered with W7. Thereafter the leading edge is cut to have the diameter of 0.3-0.5mm. phi to remove collapsed portion from the cutting face through electrolytic grinding. Since the evaporated ion source substance will emit only through said cutting face 8 having small diameter, ion beam of high brightness can be produced.

Description

【発明の詳細な説明】 この発明は高輝度表面電離型イオン源およびその製造法
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high brightness surface ionization type ion source and a method for manufacturing the same.

試料面に一次イオン・ビームを照射するとき試料表面か
ら放出される二次イオンを質1・分析して試料表面の元
素分布や状態を測定する二次イオン質量分析法(SIM
S)に用いられる装置の一例としてイオンマイクロプロ
ーブ質量分析計(I MMA )が知られており、この
型の装置は主として元素の定舖分析或いは線、面や深さ
方向の元素の分布を解析するのに用いられる。そして−
次イオン電流を向上させビームスポットの大きさを小さ
くすることによって、空間的な分解能即ち試料中の元素
を検出するときの1眸偉力、検出限界を高め、また例え
ば半導体基板のキャリヤ以外の不純物やICチップ等の
極微量不純物の空間的分布の分析ができるようになるこ
とが望められておシ、従って微量元素の分析には装置の
高真空化と共に電流、密度の高いイオン源が要求される
Secondary ion mass spectrometry (SIM) is a method that measures the elemental distribution and state of the sample surface by analyzing the secondary ions emitted from the sample surface when the sample surface is irradiated with a primary ion beam.
The ion microprobe mass spectrometer (IMMA) is known as an example of a device used for S. used to do. And-
By improving the secondary ion current and reducing the size of the beam spot, we can increase the spatial resolution, that is, the ability to detect elements in a sample, and the detection limit. It is hoped that it will be possible to analyze the spatial distribution of extremely small amounts of impurities in IC chips, etc. Therefore, the analysis of trace elements requires a high-vacuum device as well as an ion source with high current and density. .

とζろでプローブイオンを細いビームにして試料表面の
局所分析を行なうIMMAやHVCitlいられる表面
市)離型イメン源を月1いて試料表面のビーノ、ス、J
Fノット犬き寧をある小さな値(例えげ招Iltm96
)に制限しようとする場合、一般にはイオン源より31
−生1.たイオンビームを収束系に通すことで微小ス・
Iセラト寸法をイ:することが考えられるが、試料表面
へσ)到達ビーノ・電流値が小さくなり、表面分析だ7
 V(ij不利となる。1・(料表ff+’+に到達す
るビーム電流飴(ヤ太値)は、 Ipmax = ’rπ2−B−d′8/ 16 Cs
 ””で表わされ、ここでBは輝度、dはビーノ、スポ
ット・の大きさ、CFIけ球面収差係数であり、従って
ビーフ2電流値(ハ)イオン源の輝度に比例することが
わかZ)。
IMMA and HVCitl are used to perform local analysis of the sample surface by using probe ions as a narrow beam using a laser beam.
A small value (e.g. invitation Iltm96)
), generally 31
- Raw 1. By passing the ion beam through a focusing system, a minute amount of radiation is generated.
It is conceivable to change the I Cerato dimensions to A:, but the current value reaching the sample surface will be smaller, and the surface analysis will be difficult.7
V(ij will be disadvantageous.1・(The beam current value (thick value) that reaches ff+'+ is Ipmax = 'rπ2-B-d'8/ 16 Cs
``'', where B is the brightness, d is the size of the spot, and CFI is the spherical aberration coefficient. Therefore, it can be seen that the beef 2 current value (c) is proportional to the brightness of the ion source. ).

以上のような観、点からこの棹の分析VCおいて、試*
′1表面にできるだけ小さな径でしかもできるだけ強い
一次イオンビームスポットを形成するために1−]イオ
ン源の輝度をできるだけ高くすZ、必要があり、高輝度
のイオン源が要求される。しかしながら、従来提案され
てきた表面↑Ff、 I’lfl型イオン源では、第1
図に示すようにイオン発生部を構成しているポーラスタ
ングステン1は加工上の観、点からその有効径を2隨り
稈度にするのが限度であり、それ以下にすることは実m
′的に困611[であつブこ。なお第1図において2は
カソード、3−ヒーター、4け電接を示す。捷だ、]ゼ
ポーラスタングステンの周辺fi+−からもイオン種の
蒸気が起こるブ(め、大輝度のビームを引き出そうとす
ると、無駄なイオン種の放出が伴ない、その結果イオン
源の汚染や1(f。
From the above viewpoints and points, in the analysis of this VC, the test *
In order to form a primary ion beam spot as small as possible and as strong as possible on the surface, it is necessary to make the brightness of the ion source as high as possible, and a high brightness ion source is required. However, in the conventionally proposed surface ↑Ff, I'lfl type ion source, the first
As shown in the figure, the limit for the effective diameter of the porous tungsten 1 that constitutes the ion generating part is 2 culms from the viewpoint of processing, and it is practically impossible to make it smaller than that.
``It's difficult 611. In FIG. 1, 2 represents a cathode, 3 represents a heater, and 4 represents an electrical connection. Ion species vapor is also generated from the surrounding fi+- of Zeporus tungsten.If you try to extract a beam of high brightness, you will emit wasted ion species, resulting in contamination of the ion source and (f.

気的なP縁不良(イオン11+1が金属である14^合
)等巾じることになる。
This results in a wide range of problems, such as a mechanical P edge defect (14^ where ions 11+1 are metal), etc.

そこで、この発明0:1、イオン1−111物質の放出
面■11を小さくして単位面積尚りのイオン放出晴を向
上するようにしブζ高輝度表面電hlE2X’Jイオン
源を提供することを目r白とする。
Therefore, it is an object of the present invention to provide a high brightness surface electron hlE2X'J ion source by reducing the emission surface (11) of the ion 1-111 substance to improve the ion emission per unit area. is the white of the eye.

従ってとの発明によるイオン源においてはポーラスタン
グステンから成るイオンさv、:生部の表面はその中心
部分を除いてタングステン等の融点の高いイオン不透過
性膜で被覆される。好ま1−くけ、イオン発生部は円錐
形を成し、その先端部だけからイメン百1′1勿質が放
出されるように$pt成される。
Therefore, in the ion source according to the invention, the surface of the ion source made of porous tungsten is coated with an ion-impermeable film having a high melting point, such as tungsten, except for the central part. Preferably, the ion generating section has a conical shape, and is constructed so that the ion generating portion is emitted only from its tip.

寸たこの発す]の別の目的は−fr:、 Fのイオン源
の簡+1!+々製造方法を提供することにある。
Another purpose of the octopus emitted] is -fr:, the simple +1 of the F ion source! The object of the present invention is to provide a manufacturing method.

すなわちこの発明の製造方法は、ポーラスタングステン
からbV、るイオン発生部をその中央部分を除いてタン
グステン宿の融点の高くしかもイオン2J’Gシ(を曲
さない物質でスパッター蒸着することを特徴としている
That is, the manufacturing method of the present invention is characterized in that the ion generating part made of porous tungsten is sputter-deposited, except for the central part, with a substance that has a high melting point of tungsten and does not bend the ions (2J'G). There is.

寸ブここの発明の別のJP、’?徴によれば、イオン源
のjJtJ ′、’r’i 法t、I 、rlF−ラス
タングステンから成るイオン発生部を円錐形状に3Fイ
成し、その表面にタングステン宿1の融点の高く[、か
も発生イオン蒸気を]ltlさない’l?7+ ’(?
iでy!c5I!lfシ、そしで円り1o形状のイオン
発生部の先j’41を切削すZ、ことから成る。
Another JP of this invention, '? According to the characteristics, the ion generating part of the ion source made of tungsten is formed into a 3F conical shape, and the ion generating part of the ion source is made of tungsten having a high melting point [, Doesn't it generate ionic vapor? 7+'(?
i and y! c5I! lf, and Z to cut the tip j'41 of the circular 1o-shaped ion generating part.

仁のように、この発明の製造法によれ&J″、従来−C
&1有効径2tnTAt73稈11’)−が限界であっ
たものが[]、5〜r1.5 nrrxl iたはそれ
以下のイオン放出[]をもつイオン源を節J14雀つ容
易に得ることができ、またとう17てイ(1られだこの
発明によるイオン源は、−次イオンビームスポットの大
きさを小さくできるだけでなく、イオン発生部で発生さ
れたイオン蒸気が周囲に拡散せずに中央1(1(のイオ
ン放出口のみから放出されるので単位面粘当りのイオン
放出14iすなわち輝度が著しく向上され得る。すなわ
ち小さな一次イオンビームスポットを得る場合同一径の
スポットのビーム軍、流を16〜50倍に増強でき、高
感度の分析が可能となる。また発生イオンを有効に細い
イオンビーム、として放出できるので余分のイオンによ
る系の汚染を避けることができる〇 以下この発明を添附図面の第2+3+4図を参照して説
明する。
According to the manufacturing method of this invention, conventional-C
&1 effective diameter 2tnTAt73culm11') - was the limit [], but it is now possible to easily obtain an ion source with ion emission [] of 5 to r1.5 nrrxl i or less. Moreover, the ion source according to the present invention not only can reduce the size of the -order ion beam spot, but also allows the ion vapor generated in the ion generation section to be distributed in the center 1 (1) without being diffused to the surroundings. Since the ions are emitted only from the ion emitting port of 1, the ion emitted per unit surface viscosity (14i), that is, the brightness can be significantly improved.In other words, when obtaining a small primary ion beam spot, the beam force and current of the spot of the same diameter is 16 to 50. This invention can be doubled, making highly sensitive analysis possible. Also, since the generated ions can be emitted effectively as a narrow ion beam, contamination of the system by extra ions can be avoided. This will be explained with reference to the figures.

第2〜4図にはこの発明の製造方法の一実ノイ11例を
示し、第2図には、円ψIL形状に切削したポーラスタ
ングステン5をタンタルの管状体6に電子ビーム溶接す
る工程を示す。こうして形成された円錐形状のイオン発
生部の表面にし1第3図に示すようにタングステン7が
厚さ10 /Im ’IA 瓜にス/ぞツタ−蒸着され
る。その後第4図に示すように先端部はり1すJl’V
られ、その径が[]、 3−0.5 mm%になるよう
にされる。切削面81tJ例えば和1解研摩Vこよって
孔のつぶれたIr41分を取り去る。従ってイオン種の
蒸発物はこの小さな径の(:す削rf+i 8だけから
放出される7’Cめ高ZIlt度のイオンビームがイ仔
られる。
2 to 4 show 11 examples of the manufacturing method of the present invention, and FIG. 2 shows a process of electron beam welding a porous tungsten 5 cut into a circular ψIL shape to a tantalum tubular body 6. . As shown in FIG. 3, tungsten 7 is vapor-deposited onto the surface of the conical ion generating portion thus formed to a thickness of 10/Im'IA. After that, as shown in Fig. 4,
and its diameter is [], 3-0.5 mm%. For example, the cut surface 81tJ is polished by polishing V to remove the Ir41 portion that has crushed the hole. Therefore, the evaporated material of the ion species is generated by an ion beam with a high ZIlt degree of 7'C which is emitted only from this small diameter (: rf+i 8).

第5図には別の実施例を示し、この例では従来形のポー
ラスタングステン9の表面に中央部10を残してタング
ステン11がス・ぞツタ−蒸着すれる。
FIG. 5 shows another embodiment, in which tungsten 11 is deposited in strips on the surface of conventional porous tungsten 9, leaving a central portion 10.

上記各実施e11で&Jイオン発生131sの破1゛f
月としてタングステンについてn己載してきjc−が1
.+Iり常12 OF1〜1300°C程度の温度に而
[えしかも発(1:′イメン蒸気をしゃ断できる導電性
物質であれば任意の物質例え11:J、’ PAo 、
 Ta A!を使用′1′ることができる。
&J ion generation 131s failure 1゛f in each of the above implementations e11
I have posted about tungsten as a moon and jc- is 1
.. +I Normal 12 OF1 - At a temperature of about 1,300°C, it is also emitted (1:' Any conductive material that can cut off the steam. Example 11: J,' PAo,
Ta A! '1' can be used.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来型のイオンilI江を示す概略図、龜・、
2〜4図はこの発明のイオン源の一実施例の製造工程を
示す断面図、第5図はこの発明の別の実施例を示す断面
図である。 図中、  5,9:イオン発生部、  7.11:タン
グステン被覆。 第1図 第2図 第3圓 第4図 第5図 手続補正書(自発) 昭和57年10月29日 特許庁長官殿 ■、事件の表示 昭和57  年特許願第175390号その製造法 3、補正をする者 事イI[との関係     特3゛「出願人柱 所 神
奈川県茅ケ崎市萩園2500番地名称  日本真空技術
株式会社 4、代理人 5、補正の対象 明細書の発明の詳細な説明の掴 6、補正の内容 明細賓第4頁第6行中の「カンード」を1イオン生成部
」と補正します。
Figure 1 is a schematic diagram showing a conventional ion IllI river.
2 to 4 are cross-sectional views showing the manufacturing process of one embodiment of the ion source of the present invention, and FIG. 5 is a cross-sectional view showing another embodiment of the present invention. In the figure, 5, 9: ion generation part, 7.11: tungsten coating. Figure 1 Figure 2 Figure 3 Circle Figure 4 Figure 5 Procedural amendment (spontaneous) October 29, 1980 Dear Commissioner of the Patent Office ■, Indication of the case 1982 Patent Application No. 175390 Process for its production 3, Relationship with the person making the amendment (Part 3): Applicant Address: 2500 Hagizono, Chigasaki City, Kanagawa Prefecture Name: Japan Vacuum Technology Co., Ltd. 4, Agent 5, Grasp the detailed description of the invention in the specification to be amended 6. Details of the correction The word ``cando'' in line 6 of page 4 will be corrected to read ``1 ion generator.''

Claims (1)

【特許請求の範囲】 1、ホーラスタングステンから成るイオン発生部の表面
をその中央部分を除いてタングステン等の融点の高いイ
オン不透過性j換丁被穎し、イオン111j !ll雪
質放出面積を小さくしたことを!1斤徴とする高輝世表
面電1illi型イオン源。 2、ホーラスタングステンから成2)イオン発生部の表
面をその中央部分を除いてタングステン等の融点の高い
イオン不透過性物質でスノセツター蒸着することを特徴
とする特許請求の94ii>、間第1項に衛j載のイオ
ンのの製造法〇 五r式−ラスタンゲステンから成るイオン発生部を円錐
形状に形成し、その表面上にタングステン等の融点の高
いイオン不透過性物質を蒸着し、そして円錐形状のイオ
ン発生部の先端を切削してイオン種の放出口を形成する
ことから成ることを特徴とする特許請求の範囲第1項に
記載のイオン源の製造法。
[Claims] 1. The surface of the ion generating part made of tungsten, except for the central part, is coated with an ion-impermeable material having a high melting point, such as tungsten, so that ions 111j! ll The snow quality release area has been reduced! High brightness surface electron 1illi type ion source with 1 loaf. 2. Made of horus tungsten 2) An ion-impermeable substance with a high melting point such as tungsten is deposited on the surface of the ion generating portion except for the central portion thereof using a snow setter. The method for producing ions described in Nihii J is to form an ion generating part made of type 5R-rustungsten into a conical shape, depositing an ion-impermeable substance with a high melting point such as tungsten on its surface, and 2. The method of manufacturing an ion source according to claim 1, further comprising cutting the tip of the conical ion generating section to form an ion species discharge port.
JP57175390A 1982-10-07 1982-10-07 High brightness surface ionization type ion source and its manufacturing method Granted JPS5966031A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57175390A JPS5966031A (en) 1982-10-07 1982-10-07 High brightness surface ionization type ion source and its manufacturing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57175390A JPS5966031A (en) 1982-10-07 1982-10-07 High brightness surface ionization type ion source and its manufacturing method

Publications (2)

Publication Number Publication Date
JPS5966031A true JPS5966031A (en) 1984-04-14
JPH0145699B2 JPH0145699B2 (en) 1989-10-04

Family

ID=15995260

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57175390A Granted JPS5966031A (en) 1982-10-07 1982-10-07 High brightness surface ionization type ion source and its manufacturing method

Country Status (1)

Country Link
JP (1) JPS5966031A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6269453A (en) * 1985-09-24 1987-03-30 Hitachi Ltd Ion source
CN107210749A (en) * 2014-10-13 2017-09-26 亚利桑那州立大学董事会代表亚利桑那州立大学法人团体利益 A Ces Ium Ion Sources for ion microprobe
US10672602B2 (en) 2014-10-13 2020-06-02 Arizona Board Of Regents On Behalf Of Arizona State University Cesium primary ion source for secondary ion mass spectrometer

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6269453A (en) * 1985-09-24 1987-03-30 Hitachi Ltd Ion source
CN107210749A (en) * 2014-10-13 2017-09-26 亚利桑那州立大学董事会代表亚利桑那州立大学法人团体利益 A Ces Ium Ion Sources for ion microprobe
EP3207636A4 (en) * 2014-10-13 2018-10-31 Arizona Board of Regents, a Body Corporate of the State of Arizona acting for and on behalf of Arizona State University Cesium primary ion source for secondary ion mass spectrometer
US10672602B2 (en) 2014-10-13 2020-06-02 Arizona Board Of Regents On Behalf Of Arizona State University Cesium primary ion source for secondary ion mass spectrometer
CN107210749B (en) * 2014-10-13 2021-03-19 亚利桑那州立大学董事会代表亚利桑那州立大学法人团体利益 Primary cesium ion source for secondary ion mass spectrometer

Also Published As

Publication number Publication date
JPH0145699B2 (en) 1989-10-04

Similar Documents

Publication Publication Date Title
Reed Electron probe microanalysis
Titze et al. Automated in‐chamber specimen coating for serial block‐face electron microscopy
Heard et al. Determination of the elemental composition of mature wheat grain using a modified secondary ion mass spectrometer (SIMS)
US11004656B2 (en) Methods and apparatus for determining, using, and indicating ion beam working properties
JPS5966031A (en) High brightness surface ionization type ion source and its manufacturing method
US5536944A (en) Thermal field emmission electron gun
US6531811B1 (en) Liquid metal ion source and method for producing the same
JP2007123207A (en) Evaluation method of electrode for battery
Jäger et al. Some observations on sample sputtering in a glow discharge
Ives et al. Depth Profile Analysis of Multilayer Ni Fe Alloy Coatings by Glow Discharge Optical Emission Spectroscopy (GDOES) and Energy Dispersive X‐ray (EDX) Linescan—a Comparative Study
JP7278894B2 (en) Sample support, adapter, ionization method and mass spectrometry method
JPS59155941A (en) Electron-beam inspection device
JP2022093834A (en) Sample support, ionization method, and mass spectrometry method
JP2004319149A (en) Electron source and electron beam device using it
Tuck Surface studies of thermionic emitters by methods unique to them
US8669525B2 (en) Sample inspection methods, systems and components
JPS60121652A (en) Sample holder for mass spectrometry
KR100303632B1 (en) Cold cathode element
EP2672504A2 (en) Combined directional electron detector
Griffith et al. Low‐energy electron microscopy (LEEM) and mirror electron microscopy (MEM) of biological specimens: Preliminary results with a novel beam separating system
JP3419653B2 (en) Gallium ion source and method for producing the same
Musselman et al. Effects of sample geometry on interelement quantitation in laser microprobe mass spectrometry
JP7471174B2 (en) Sample Support
CN220691960U (en) Open type bar-shaped anode micro-focus X-ray tube
Klemperer et al. On the Spherical Aberration of Electron Emission Systems