JPH0377252A - Minute x-ray source - Google Patents
Minute x-ray sourceInfo
- Publication number
- JPH0377252A JPH0377252A JP1212694A JP21269489A JPH0377252A JP H0377252 A JPH0377252 A JP H0377252A JP 1212694 A JP1212694 A JP 1212694A JP 21269489 A JP21269489 A JP 21269489A JP H0377252 A JPH0377252 A JP H0377252A
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- Prior art keywords
- ray
- layer
- diffusion layer
- heat diffusion
- micro
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Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、投影型X線顕wi鏡のための微小X線源に関
するものであり、特にX線発生部の大きさが小さいにも
関わらず輝度の高い微小xls源に関するものである。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a micro X-ray source for a projection type X-ray microscope, and in particular, despite the small size of the X-ray generating part, First, it concerns a small XLS source with high brightness.
従来、試料の拡大透過X線像を得る装置として、投影型
X線顕微鏡が知られている。この装置は、第2図の概略
全体構成図に示すように、微小XwA源2を備えており
、この線源2の下には、それに接して試料支持メツシュ
又は支持膜4上に載せた測定試料3が配置され、線源2
から下方半径方向に放射され試料3を透過した発散X線
7を離れた位置で受けて検出するように、フィルム、位
置敏感検出器、蛍光板等の検出器5が配置されている。Conventionally, a projection type X-ray microscope is known as a device for obtaining an enlarged transmission X-ray image of a sample. This device is equipped with a minute XwA source 2, as shown in the schematic overall configuration diagram of FIG. Sample 3 is placed and source 2
A detector 5 such as a film, a position-sensitive detector, a fluorescent screen, etc. is arranged to receive and detect the divergent X-rays 7 emitted downward and radially from the sample 3 and transmitted through the sample 3 at a remote position.
線源2、試料3、支持メツシュ又は支持膜4及び検出器
5から成る部分はカメラ部8と呼ばれ、試料3の拡大透
過X線像を検出器5上に投影するものである。A portion consisting of the radiation source 2, sample 3, support mesh or support film 4, and detector 5 is called a camera section 8, and projects an enlarged transmitted X-ray image of the sample 3 onto the detector 5.
微小X線源2は、X線マイクロアナライザ、走査型電子
顕微鏡、透過型電子顕微鏡の走査像観察装置等の対物レ
ンズ1の焦点位置にX線を発生させたい金属の箔21を
置き、対物レンズlから数10keV−100aVに加
速した電子線6を発射してこの金属箔21に当てて特性
X線を発生させるものである。金属箔21と測定試料3
との配置関係としては、金属箔21に近接して測定試料
3を配置する方法の他に、測定用の試料3上に直接特性
X線を発生させたい金属を蒸着してその膜21を形成し
、その膜21に対して上記と同様にして電子線を当てて
X線を発生させる等の方法が用いられてきた。The micro X-ray source 2 is constructed by placing a metal foil 21 on which you want to generate X-rays at the focal position of the objective lens 1 of an X-ray microanalyzer, a scanning electron microscope, a scanning image observation device of a transmission electron microscope, etc. An electron beam 6 accelerated from l to several 10 keV to 100 aV is emitted and applied to the metal foil 21 to generate characteristic X-rays. Metal foil 21 and measurement sample 3
In addition to the method of arranging the measurement sample 3 in close proximity to the metal foil 21, there is also a method of evaporating a metal that generates characteristic X-rays directly onto the measurement sample 3 to form the film 21. However, methods have been used in which the film 21 is exposed to electron beams in the same manner as described above to generate X-rays.
第3図の拡大図を用いて、従来の微小X線源2の作用を
説明する。従来の微小X線源2は単一の金属箔又は膜2
1から成り、この表面に加速した電子線6を当てると、
その表面から内部に球の頭部を切り取った形状のX線発
生部9が形成され、その周囲に熱を発生する電子散乱部
10が形成される。このようt単一の金属箔又は膜21
を用いてX線を発生させる方法においては、X線発生部
9の大きさを小さくし、その輝度を上げることが必要で
あるが、これらを両立させることは困難であった。すな
わち、輝度を上げるためには単位面積当りの電子ビーム
を多くするか、その加速電圧を上げればよい。しかしな
がら、電子ビームを多く流すと、それを当てた部分の温
度が上昇して熱的に損傷を受けやすく、動作中に金属箔
や膜が溶解して穴があいたり、変形したりしやすい。他
方、加速電圧を上げるとX線発生部9が広がってしまう
。また、電子線6を金属箔又は膜21に当てた時に発生
する反射電子が対物レンズ、絞り、構造材籾等に当たり
、X線や二次電子を発生させ、信号のバックグラウンド
や雑音要因となる。The operation of the conventional minute X-ray source 2 will be explained using the enlarged view of FIG. The conventional micro X-ray source 2 consists of a single metal foil or membrane 2
1, and when an accelerated electron beam 6 is applied to this surface,
An X-ray generating section 9 having a shape in which the head of a sphere is cut out is formed inside from the surface thereof, and an electron scattering section 10 that generates heat is formed around the X-ray generating section 9 . Such a single metal foil or film 21
In the method of generating X-rays using the X-ray generator, it is necessary to reduce the size of the X-ray generating section 9 and increase its brightness, but it has been difficult to achieve both of these goals. That is, in order to increase the brightness, it is sufficient to increase the number of electron beams per unit area or increase the acceleration voltage. However, when a large number of electron beams are applied, the temperature of the area hit by the electron beam rises, making it susceptible to thermal damage, and metal foils and films are likely to melt during operation, creating holes or deforming them. On the other hand, if the accelerating voltage is increased, the X-ray generating section 9 will expand. In addition, reflected electrons generated when the electron beam 6 is applied to the metal foil or film 21 hit the objective lens, aperture, structural material, etc., generating X-rays and secondary electrons, which become a background signal and noise factor. .
さらに、−次電子が、対物レンズ近傍に設置されている
絞りを通過する際に発生するX線は、X線発生用金属箔
又は膜2Iを通過し、ここで発生するX線と混ざって投
影像の中心部に別の投影像を形成するため、投影像に使
用不能個所が生じる。Furthermore, the X-rays generated when the negative electrons pass through the aperture installed near the objective lens pass through the X-ray generation metal foil or film 2I, mix with the X-rays generated here, and are projected. Since another projection image is formed in the center of the image, an unusable portion is created in the projection image.
また、従来の方法では、Xi7は、電子ビーム6の進行
方向にしか取り出せない。Furthermore, in the conventional method, Xi7 can only be taken out in the direction in which the electron beam 6 travels.
すなわち、従来、微小X線源は、金属箔や蒸着薄膜とし
て単一純金属を用いるので、微小X線源として望まれる
、耐熱性に優れ、高輝度で、微小であり、反射電子、透
過電子がなく、特性X線、連続X線、バックグラウンド
、雑音の分離が良く、多方向に取り出せ、また、エネル
ギー(波長)選択が可能で、発生源の大きさや輝度、位
置を可変にでき、かつ、再現性が良い等の要件を同時に
満たすことはできず、良好な微小X線源として確立され
たものはなかった。そのため、第2図に示したような投
影型X線顕微鏡は、実用に耐えるものが作られていない
。In other words, conventionally, micro X-ray sources use a single pure metal as metal foil or vapor-deposited thin film, so they have excellent heat resistance, high brightness, and small size, which are desired as micro It has good separation of characteristic X-rays, continuous X-rays, background, and noise, can be extracted in multiple directions, can select energy (wavelength), and can vary the size, brightness, and position of the source. , good reproducibility, and other requirements at the same time, and no one has been established as a good micro X-ray source. Therefore, a projection type X-ray microscope as shown in FIG. 2 has not been manufactured to be of practical use.
したがって、本発明の目的は、上記した従来の微小X線
源の問題点を解決して、上記した微小X線源の要件を満
足する新規な微小X線源を提供することである。Therefore, an object of the present invention is to solve the problems of the conventional miniature X-ray sources described above and to provide a novel miniature X-ray source that satisfies the requirements for the miniature X-ray sources described above.
本発明の微小X線源は、電子ビーム入射側から、第1電
子散乱熱拡散層、X線発生層、及び第2電子散乱熱拡散
層からなる多重層と、この多重層に接続された直流高圧
電源とからなり、前記第1電子散乱熱拡散層を貫通して
前記X線発生層に至る微小な穴が設けられていて、この
穴にX線励起用の電子ビームを入射させるようになって
いることを特徴とするものである。The micro X-ray source of the present invention includes, from the electron beam incident side, a multilayer consisting of a first electron scattering heat diffusion layer, an X-ray generation layer, and a second electron scattering heat diffusion layer, and a direct current connected to the multilayer. a high-voltage power source, a minute hole is provided that penetrates the first electron scattering heat diffusion layer and reaches the X-ray generation layer, and an electron beam for X-ray excitation is made incident on this hole. It is characterized by the fact that
前記第1電子散乱熱拡散層の電子ビーム入射側表面に誘
電体層を設け、前記第2電子散乱熱拡散層のX線取り出
し側表面に特性X線分離連続X線吸収熱反射層を設け、
前記微小穴を前記誘電体層及び第1電子散乱熱拡散層を
貫通して設けることが最も望ましい。A dielectric layer is provided on the electron beam incident side surface of the first electron scattering heat diffusion layer, and a characteristic X-ray separation continuous X-ray absorption heat reflection layer is provided on the X-ray extraction side surface of the second electron scattering heat diffusion layer,
It is most desirable that the microholes be provided through the dielectric layer and the first electron scattering heat diffusion layer.
また、前記微小穴はピンホール又は深さの異なるV字溝
の形状をしているものでよい。Further, the microhole may be in the shape of a pinhole or a V-shaped groove having different depths.
さらに、前記直流高圧電源は前記多重層に前記電子ビー
ムの加速電圧と同程度又はそれ以上の直流電圧をかける
ものであるのが望ましい。Furthermore, it is preferable that the DC high voltage power source applies a DC voltage to the multilayer that is comparable to or higher than the accelerating voltage of the electron beam.
そして、前記直流電圧はX線発生金属の臨界励起電圧を
中心電圧としてプラス数10keVからマイナス1.0
0 e Vの範囲にあるものである。The DC voltage ranges from plus several 10 keV to minus 1.0 keV with the critical excitation voltage of the X-ray generating metal as the center voltage.
It is in the range of 0 eV.
さらに、前記直流電圧は可変であることが望ましい。Furthermore, it is desirable that the DC voltage is variable.
また、前記第1電子散乱熱拡散層、X線発生層、第2電
子散乱熱拡散層を構成する物質の原子番号を電子ビーム
入射側から順に等しいか小さくなるように選択すること
が望ましい。Further, it is preferable that the atomic numbers of the materials constituting the first electron scattering heat diffusion layer, the X-ray generation layer, and the second electron scattering heat diffusion layer are selected to be equal to or smaller in order from the electron beam incident side.
また、前記多重層の前記微小穴近傍の側面に第2電子散
乱熱拡散層と第2の特性X線分離連続X線吸収熱反射層
を設けて、前記電子ビームと平行及び直角の二方向を中
心に多方向へX線を取り出し可能にすることが望ましい
。Further, a second electron scattering heat diffusion layer and a second characteristic X-ray separation continuous X-ray absorption heat reflection layer are provided on the side surface of the multilayer near the microhole, so that two directions parallel and perpendicular to the electron beam are provided. It is desirable to be able to extract X-rays from the center in multiple directions.
上記微小X線源は、投影型X線顕微鏡、微小X線回折装
置に用いることができる。The above-mentioned micro X-ray source can be used in a projection type X-ray microscope and a micro X-ray diffraction device.
微小穴に入射した電子線はその底部のX線発生層へ当た
り、X線発生部を形成する。このようにすると、反射電
子は閉じ込められて多重層の外に出ないため、X線発生
4部は球形状になり、従来のものに一比較して球形状の
頭部に相当する部分において余分にX線を発生する。し
たがって、X線発生部の見掛けの大きさを変えないで、
X線発生部の輝度を向上させることができる。この時、
多重層には直流電圧がかかっているので、反射電子等は
多重層に引き戻されて吸収され、悪影響を与えない。The electron beam incident on the microhole hits the X-ray generation layer at the bottom, forming an X-ray generation section. In this way, the backscattered electrons are confined and do not go out of the multilayer, so the four X-ray generating parts become spherical, and compared to the conventional one, the part corresponding to the spherical head is redundant. generates X-rays. Therefore, without changing the apparent size of the X-ray generating part,
The brightness of the X-ray generating section can be improved. At this time,
Since a DC voltage is applied to the multilayer, reflected electrons and the like are drawn back into the multilayer and absorbed, and do not have any adverse effects.
次に、第1図の本発明の実施例の断面図を参照にして本
発明を説明する。Next, the present invention will be described with reference to the sectional view of an embodiment of the present invention shown in FIG.
この微小X線源2は、電子線6が入射する方向から、誘
電体層11.電子散乱熱拡散層12、X線発生層13、
電子散乱熱拡散層14、特性X線分離連続X線吸収熱反
射層15からなる多重層と、この多重層に接続された直
流高圧電源19とからなり、また、X線発生部9及びそ
の周囲の電子散乱部10近傍の多重層側面には特性X線
分離連続X線吸収熱反射層15’が設けられている。誘
電体層11及び電子散乱熱拡散層12を貫通してX線発
生層13に至るピンホール又は深さの異なるV字溝16
が設けられており、ピンホール16に対物レンズ1 (
第2図)によって絞られた電子線6が入射するようにな
っている。そして、この微小X線源2は、直流高圧電源
19によりX線発生金属の臨界励起電圧を中心電圧とし
てプラス数1OkeV〜マイナス100eVの直流高圧
が印加されている状態で使用される。This minute X-ray source 2 has a dielectric layer 11 . electron scattering heat diffusion layer 12, X-ray generation layer 13,
It consists of a multilayer consisting of an electron scattering heat diffusion layer 14, a characteristic X-ray separation continuous X-ray absorption heat reflection layer 15, and a DC high voltage power supply 19 connected to this multilayer, and also includes an A characteristic X-ray separating continuous X-ray absorbing heat reflecting layer 15' is provided on the side surface of the multilayer near the electron scattering section 10. A pinhole or V-shaped groove 16 with different depths penetrates the dielectric layer 11 and the electron scattering heat diffusion layer 12 and reaches the X-ray generation layer 13.
is provided, and the objective lens 1 (
The electron beam 6 that has been narrowed down by the lens (FIG. 2) is made incident. The minute X-ray source 2 is used in a state where a DC high voltage of plus several OkeV to minus 100 eV is applied by the DC high voltage power supply 19 with the critical excitation voltage of the X-ray generating metal as the center voltage.
これらの構成要素の役割は下記の通りである。The roles of these components are as follows.
誘電体層11は、高加速電圧時反射電子の発生を抑え、
発生する反射電子、迷電子が不特定に電子散乱拡散層1
2やX線発生層13に入り込まないように絶縁するもの
であり、また、対物レンズ1近傍にある電子ビーム絞り
からのX線を吸収して検出器5に届かないようにするも
のである。原子番号の大きいものが望ましい。The dielectric layer 11 suppresses the generation of reflected electrons at high acceleration voltage,
The generated reflected electrons and stray electrons are unspecified in the electron scattering diffusion layer 1.
2 and the X-ray generation layer 13, and also absorbs X-rays from the electron beam diaphragm near the objective lens 1 to prevent them from reaching the detector 5. One with a large atomic number is desirable.
電子散乱熱拡散層12は、入射電子が臨界励起電圧以下
のエネルギーしか持たず、エネルギーの大部分を熱とし
て放出する層で、X線発生層13の金属と同じか熱伝導
性、電気伝導性の良い高融点物質が用いられる。できる
だけ原子番号の小さい物質で、特性X線の波長が長いも
の、例えば銅が望ましい。 誘電体層11、電子散乱熱
拡散層12は、前記したように、X線発生層13に至る
ピンホール又は深さの異なるV字溝16を有することを
特徴とするもので、熱損傷を防ぐための熱拡散層を兼ね
ている。The electron scattering heat diffusion layer 12 is a layer in which incident electrons have only energy below the critical excitation voltage and releases most of the energy as heat, and has the same thermal conductivity and electrical conductivity as the metal of the X-ray generation layer 13. A substance with a high melting point is used. It is desirable to use a substance with as low an atomic number as possible and a long characteristic X-ray wavelength, such as copper. As described above, the dielectric layer 11 and the electron scattering heat diffusion layer 12 are characterized by having pinholes or V-shaped grooves 16 of different depths leading to the X-ray generation layer 13 to prevent thermal damage. It also serves as a heat diffusion layer.
X線発生1113としては高融点、高熱伝導、高電気伝
導物質で特性X線強度の高い物質であることが要求され
、金属単体、例えばタンタル、アルミニウム、チタン、
金、又はその化合物がX線発生源として良好な結果を与
える。これらの化合物を使用する時は、電子散乱熱拡散
層12は導電性物質で構威しなければならない。The X-ray generator 1113 is required to be a material with a high melting point, high thermal conductivity, high electrical conductivity, and high characteristic X-ray intensity.
Gold or its compounds give good results as an X-ray source. When using these compounds, the electron scattering heat diffusion layer 12 must be made of a conductive material.
電子散乱熱拡散層14は、X線発生物質と同様か、それ
より原子番号の小さい元素の単体からなる層である。X
線透過率が良く、熱伝導性、電気伝導性の良い高融点物
質が望ましい。The electron scattering heat diffusion layer 14 is a layer made of a single element having an atomic number similar to or smaller than that of the X-ray generating substance. X
A high melting point material with good linear transmittance, thermal conductivity, and electrical conductivity is desirable.
特性X線分離連続X線吸収熱反射層15は、軽金属元素
、又は、非晶質炭素及び高分子薄膜などの有機化合物(
1〜数層)の薄膜層よりなる。この層の主な目的は、連
続X線吸収用フィルターとしての作用であるが、X線発
生層13、電子散乱熱拡散層12.14からの熱線の反
射作用も兼ねている。この層は、使用目的に応じてその
厚さ、枚数、種類を変えることにより、波長選択特性を
変えることが可能である。The characteristic X-ray separation continuous X-ray absorption heat reflection layer 15 is made of light metal elements or organic compounds such as amorphous carbon and polymer thin films
It consists of one to several thin film layers. The main purpose of this layer is to act as a filter for continuous X-ray absorption, but it also serves to reflect heat rays from the X-ray generation layer 13 and the electron scattering heat diffusion layers 12 and 14. The wavelength selection characteristics of this layer can be changed by changing its thickness, number, and type depending on the purpose of use.
直流高圧電源19は、電子線6がX線発生層13に照射
された時の反射電子の発生を押さえること、照射電流量
とは独立に加速電圧を変えてX線発生領域9を可変とす
ること、前記の絞りを通過する際に発生するX線の低減
及び阻止を目的としている。X1m取出口18.18′
より透過電子や二次電子が検出器5方向に向かうのを引
き戻す役目もある。The DC high voltage power supply 19 suppresses the generation of reflected electrons when the X-ray generation layer 13 is irradiated with the electron beam 6, and makes the X-ray generation region 9 variable by changing the accelerating voltage independently of the amount of irradiation current. In particular, the purpose is to reduce and block X-rays generated when passing through the aperture. X1m outlet 18.18'
It also has the role of pulling back transmitted electrons and secondary electrons from heading toward the detector 5.
次に、この微小X線源用多重層の動作を説明すると、こ
の微小X線源用多重層は、X線マイクロアナライザ、走
査型電子顕微鏡、透過型電子顕微鏡の走査像観察装置等
の対物レンズ1とX線検出器5の間に組み込み、電子線
6の持つエネルギーをX線7に変換する微小X線源2を
得るためのものであり、この多重層の下に近接して試料
3を置くことにより投影型X線顕微鏡が実現する。Next, to explain the operation of this multilayer for a micro X-ray source, this multilayer for a micro 1 and an X-ray detector 5 to obtain a minute X-ray source 2 that converts the energy of an electron beam 6 into X-rays 7. By placing it there, a projection type X-ray microscope is realized.
対物レンズ1により細く絞られた数10keV〜100
eVの加速電子をピンホール又は深さの異なるV字溝1
6の底部のX線発生層13へ照射する。すると、球形状
のX線発生部9ができる。Several 10 keV to 100 narrowed down by objective lens 1
eV accelerated electrons are passed through pinholes or V-shaped grooves 1 with different depths.
The X-ray generation layer 13 at the bottom of the cell 6 is irradiated. Then, a spherical X-ray generating section 9 is formed.
従来の方法においては、第3図に関連して説明したよう
に、上部の電子が反射電子となるので、球形状の頭部を
切り取った形状のxm発生部9となるが、本発明のよう
に、多重層にピンホール又は深さの異なるV字溝16を
設けたものを用いて、電子線6を多重層の中で照射する
と、反射電子は閉じ込められて外に出ないため、X線発
生部9は球形状になり、従来のものに比較して第1図の
部分17において余分にX線を発生する。したがって、
X線発生部9の見掛けの大きさを変えないで(下から見
た大きさは従来のものと同じである。In the conventional method, as explained in relation to FIG. 3, the electrons at the top become reflected electrons, resulting in the xm generating section 9 having a spherical shape with its head cut off. When the electron beam 6 is irradiated inside the multilayer by using a multilayer with pinholes or V-grooves 16 of different depths, the reflected electrons are trapped and do not come out, so the X-ray The generating section 9 has a spherical shape and generates more X-rays at the portion 17 in FIG. 1 than the conventional one. therefore,
The apparent size of the X-ray generating section 9 remains unchanged (the size seen from below is the same as the conventional one).
)、部分17の分だけX線発生部9の輝度を向上させる
ことができる。この時、多重層12〜14には、X線発
生金属の臨界励起電圧を中心電圧として電子線6の加速
電圧と同程度又はそれ以上の直流電圧をかけておく。こ
のように動作すれば、X線発生部9.17より特性X線
と連続X線、及び、熱が、電子散乱部10より連続X線
と熱が発生する。この中の連続X線を電子散乱熱拡散層
14、特性Xm分離連続X線吸収熱反射層15でできる
だけ吸収し、熱線を特性X線分離連続X線吸収熱反射層
15.15’で反射し、第1図に示したように、電子ビ
ーム6と平行及び直角の二方向を中心に多方向へXwA
を取り出す。X線取出口18.18′の表面で二次電子
等が発生するが、これらは直流高圧電源19により多重
層に通常圧の高電圧が印加されているため、多重層に吸
収される。上記のように動作するので、投影型XWAu
@鏡のために微小点から発生するX線が供給される。), the brightness of the X-ray generating section 9 can be improved by the portion 17. At this time, a direct current voltage comparable to or higher than the accelerating voltage of the electron beam 6 is applied to the multilayers 12 to 14 with the critical excitation voltage of the X-ray generating metal as the central voltage. By operating in this manner, the X-ray generating section 9.17 generates characteristic X-rays, continuous X-rays, and heat, and the electron scattering section 10 generates continuous X-rays and heat. The continuous X-rays in this are absorbed as much as possible by the electron scattering heat diffusion layer 14 and the characteristic Xm separation continuous X-ray absorption heat reflection layer 15, and the heat rays are reflected by the characteristic X-ray separation continuous X-ray absorption heat reflection layer 15.15'. , as shown in FIG.
Take out. Secondary electrons and the like are generated on the surface of the X-ray extraction port 18, 18', but these are absorbed by the multilayer because a normal high voltage is applied to the multilayer by the DC high voltage power supply 19. Since it works as described above, the projection type XWAu
@X-rays generated from a minute point are supplied to the mirror.
なお、実験結果によると、電子散乱熱拡散層12、xl
s発生層13、電子散乱熱拡散層14を構成する物質の
原子番号は、上から下へ順に小さくなるように選択する
のが望ましい。According to the experimental results, the electron scattering heat diffusion layer 12, xl
It is desirable that the atomic numbers of the substances constituting the s-generating layer 13 and the electron scattering heat diffusion layer 14 are selected so that they decrease in order from top to bottom.
また、X線発生層13に用いる単体金属や化合物、利用
する特性X線の種類により、多重層の物質には多数の組
み合わせがあるが、X線発生層13に用いる物質として
、大別して軽元素で反射電子の少ない場合と重元素で反
射電子の多い場合、さらには、大気中で用いる場合と真
空中で用いる場合の4つが考えられる。しかしながら、
これらのいずれの場合においても、各層の材質、厚さの
調整、ピンホール、V字溝の深さの選択、及び、直流高
圧電源の電圧調整により、第1図に示した構成を変化さ
せないで対応可能である。In addition, there are many combinations of multilayer materials depending on the single metal or compound used for the X-ray generation layer 13 and the type of characteristic X-rays used. There are four possible cases: a case where there are few reflected electrons due to a heavy element, a case where there are many reflected electrons due to a heavy element, a case where the device is used in the atmosphere, and a case where the device is used in a vacuum. however,
In any of these cases, the configuration shown in Figure 1 can be maintained without changing by adjusting the material and thickness of each layer, selecting the depth of pinholes and V-grooves, and adjusting the voltage of the DC high-voltage power supply. It is possible.
ところで、誘電体層11と特性X線分離連続X線吸収熱
反射1115はその役割上、必ずしも層12〜14から
なる多重層表面に一体に設ける必要はないことを付は加
えておく。By the way, it should be added that the dielectric layer 11 and the characteristic X-ray separation continuous X-ray absorption heat reflection 1115 do not necessarily need to be provided integrally on the surface of the multilayer consisting of the layers 12 to 14 due to their roles.
なお、本発明の微小X線源は、微小X線回折装置用にも
使用できる。Note that the minute X-ray source of the present invention can also be used for a minute X-ray diffraction device.
本発明の微小X線源においては、多重層にピンホール又
は深さの異なるV字溝16を設けたので、電子線6をこ
のピンホール等を通して多重層の中で照射すると、反射
電子はその中に閉じ込められて外に出ないため、X線発
生部9は球形になり、従来のものにおいて反射電子エネ
ルギーとして失われていたエネルギーを新たに加わった
部分17でX線エネルギーに変換でき、重元素をX線発
生層13の材料とする場合、発生xi強度を20〜40
%向上させることができた。In the micro X-ray source of the present invention, pinholes or V-shaped grooves 16 with different depths are provided in the multilayer, so when the electron beam 6 is irradiated in the multilayer through the pinhole, the reflected electrons are emitted from the multilayer. Since it is trapped inside and does not escape, the X-ray generating section 9 has a spherical shape, and the newly added section 17 can convert the energy that was lost as reflected electron energy in the conventional one into X-ray energy, making it possible to generate heavy When the element is used as the material of the X-ray generation layer 13, the generation xi intensity is 20 to 40.
% could be improved.
また、直流高圧電[19を取り付けて多重層に正電圧を
かけたので、反射電子を多重層に吸収することができ、
X線取出口18.18′付近で発生する二次電子も吸収
できた。また、上記電圧により、入射電子線6の加速電
圧を、電子銃のフィラメントとアノード間にかかる電圧
以外の個所で、その電流量と独立に調整可能となり、X
線発生領域9の大きさ、輝度、位置制御が可能となった
。In addition, since a DC high-voltage electric current [19] was attached and a positive voltage was applied to the multilayer, reflected electrons could be absorbed by the multilayer.
Secondary electrons generated near the X-ray extraction ports 18 and 18' were also absorbed. In addition, the voltage mentioned above makes it possible to adjust the accelerating voltage of the incident electron beam 6 independently of the current amount at a point other than the voltage applied between the filament of the electron gun and the anode.
The size, brightness, and position of the line generation area 9 can now be controlled.
さらに、誘電体層11を多重層の表面に設けたので、外
乱要因の反射電子、絞り及びその周辺からのX線の中で
検出器5に到達するものを最小に押さえることができた
。Furthermore, since the dielectric layer 11 is provided on the surface of the multilayer, it is possible to minimize the amount of disturbance factors such as reflected electrons and X-rays from the aperture and its surroundings that reach the detector 5.
また、電子散乱熱拡散層12.14を設けたので、本発
明の微小X線源は耐熱性が向上し、耐久性も増した。Further, since the electron scattering heat diffusion layers 12 and 14 were provided, the micro X-ray source of the present invention has improved heat resistance and increased durability.
また、X線取出口側に特性X線分離連続X線吸収熱反射
層15.15′を設けたので、検出器に達する連続X線
の量が少なくなり、P/B比の良い特性X線が得られ、
投影像のコントラドが向上し、熱雑音が消えた。In addition, since the characteristic X-ray separation continuous X-ray absorption heat reflection layer 15.15' is provided on the X-ray extraction port side, the amount of continuous X-rays reaching the detector is reduced, and characteristic X-rays with a good P/B ratio are is obtained,
The contrado of the projected image has improved and thermal noise has disappeared.
さらに、X線取出口18.18′から電子ビーム6と平
行及び直角の二方向を中心に多方向へX線を取り出すこ
とが可能になった。Furthermore, it has become possible to extract X-rays from the X-ray extraction ports 18, 18' in multiple directions, centering on two directions parallel and perpendicular to the electron beam 6.
第1図は本発明の実施例の微小X線源の拡大断面図、第
2図は投影型XWA顕微鏡の概略全体構成図、第3図は
従来法の微小X線源の拡大断面図である。
1:対物レンズ、2:微小X線源、3:測定試料、4:
試料支持メツシュ又は支持膜、5:検出器、6:電子線
、7二発生X線、8;カメラ部、9X線発生部、10:
電子散乱部、11:誘電体層、12:電子散乱熱拡散層
、13:X線発生層、14:電子散乱熱拡散層、15.
15′ :特性X線分離連続X線吸収熱反射層、16:
ピンホール又は深さの異なる7字溝、17二余分にX線
を発生する部分、18.18’:X線取出口、19:直
流高圧電源、21:金属の箔
出 願 人 日本電子株式会社FIG. 1 is an enlarged sectional view of a micro X-ray source according to an embodiment of the present invention, FIG. 2 is a schematic overall configuration diagram of a projection type XWA microscope, and FIG. 3 is an enlarged sectional view of a conventional micro X-ray source. . 1: Objective lens, 2: Micro X-ray source, 3: Measurement sample, 4:
sample support mesh or support membrane, 5: detector, 6: electron beam, 7 generated X-rays, 8; camera section, 9 X-ray generation section, 10:
Electron scattering section, 11: dielectric layer, 12: electron scattering heat diffusion layer, 13: X-ray generation layer, 14: electron scattering heat diffusion layer, 15.
15': Characteristic X-ray separation continuous X-ray absorption heat reflection layer, 16:
Pinhole or 7-shaped groove with different depths, 172 parts that generate extra X-rays, 18.18': X-ray extraction port, 19: DC high voltage power supply, 21: Metal foil Applicant: JEOL Ltd. company
Claims (10)
X線発生層、及び第2電子散乱熱拡散層からなる多重層
と、この多重層に接続された直流高圧電源とからなり、
前記第1電子散乱熱拡散層を貫通して前記X線発生層に
至る微小な穴が設けられていて、この穴にX線励起用の
電子ビームを入射させるようになっていることを特徴と
する微小X線源。(1) From the electron beam incident side, a first electron scattering heat diffusion layer;
Consisting of a multilayer consisting of an X-ray generation layer and a second electron scattering heat diffusion layer, and a DC high voltage power supply connected to this multilayer,
A fine hole is provided that penetrates the first electron scattering heat diffusion layer and reaches the X-ray generation layer, and an electron beam for X-ray excitation is made to enter the hole. A small X-ray source.
面に誘電体層を設け、前記第2電子散乱熱拡散層のX線
取り出し側表面に特性X線分離連続X線吸収熱反射層を
設け、前記微小穴を前記誘電体層及び第1電子散乱熱拡
散層を貫通して設けたことを特徴とする請求項1記載の
微小X線源。(2) A dielectric layer is provided on the electron beam incident side surface of the first electron scattering heat diffusion layer, and a characteristic X-ray separation continuous X-ray absorption heat reflection layer is provided on the X-ray extraction side surface of the second electron scattering heat diffusion layer. 2. The micro X-ray source according to claim 1, wherein the micro hole is provided to penetrate the dielectric layer and the first electron scattering heat diffusion layer.
の形状をしていることを特徴とする請求項1又は2記載
の微小X線源。(3) The micro X-ray source according to claim 1 or 2, wherein the micro hole is in the shape of a pinhole or a V-shaped groove with different depths.
の加速電圧と同程度又はそれ以上の直流電圧をかけるも
のであることを特徴とする請求項1から3いずれかに記
載の微小X線源。(4) The micro X-ray according to any one of claims 1 to 3, wherein the DC high voltage power supply applies a DC voltage to the multilayer that is comparable to or higher than the accelerating voltage of the electron beam. source.
心電圧としてプラス数10keVからマイナス100e
Vの範囲にあることを特徴とする請求項4記載の微小X
線源。(5) The DC voltage ranges from plus several 10 keV to minus 100 e with the critical excitation voltage of the X-ray generating metal as the center voltage.
The minute X according to claim 4, characterized in that it is in the range of V.
source.
項4又は5記載の微小X線源。(6) The minute X-ray source according to claim 4 or 5, wherein the DC voltage is variable.
子散乱熱拡散層を構成する物質の原子番号を電子ビーム
入射側から順に等しいか小さくなるように選択したこと
を特徴とする請求項1から6いずれかに記載の微小X線
源。(7) The atomic numbers of the substances constituting the first electron scattering heat diffusion layer, the X-ray generation layer, and the second electron scattering heat diffusion layer are selected to be equal to or smaller in order from the electron beam incident side. The minute X-ray source according to any one of claims 1 to 6.
乱熱拡散層と第2の特性X線分離連続X線吸収熱反射層
を設けて、前記電子ビームと平行及び直角の二方向を中
心に多方向へX線を取り出し可能にしたことを特徴とす
る請求項1から7いずれかに記載の微小X線源。(8) A second electron scattering heat diffusion layer and a second characteristic X-ray separation continuous X-ray absorption heat reflection layer are provided on the side surface of the multilayer near the microhole, and two directions, parallel and perpendicular to the electron beam, are provided. 8. The micro X-ray source according to claim 1, wherein X-rays can be extracted in multiple directions around the center.
いた投影型X線顕微鏡。(9) A projection X-ray microscope using the minute X-ray source according to any one of claims 1 to 8.
用いた微小X線回折装置。(10) A micro X-ray diffraction apparatus using the micro X-ray source according to any one of claims 1 to 8.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1212694A JPH0377252A (en) | 1989-08-18 | 1989-08-18 | Minute x-ray source |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1212694A JPH0377252A (en) | 1989-08-18 | 1989-08-18 | Minute x-ray source |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0377252A true JPH0377252A (en) | 1991-04-02 |
Family
ID=16626884
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1212694A Pending JPH0377252A (en) | 1989-08-18 | 1989-08-18 | Minute x-ray source |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0377252A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02101112A (en) * | 1988-10-07 | 1990-04-12 | Nippon Steel Corp | Method and apparatus for heat-treating working material |
-
1989
- 1989-08-18 JP JP1212694A patent/JPH0377252A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02101112A (en) * | 1988-10-07 | 1990-04-12 | Nippon Steel Corp | Method and apparatus for heat-treating working material |
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