JP3138193U - Ultra-high vacuum flange with optical window - Google Patents
Ultra-high vacuum flange with optical window Download PDFInfo
- Publication number
- JP3138193U JP3138193U JP2007005794U JP2007005794U JP3138193U JP 3138193 U JP3138193 U JP 3138193U JP 2007005794 U JP2007005794 U JP 2007005794U JP 2007005794 U JP2007005794 U JP 2007005794U JP 3138193 U JP3138193 U JP 3138193U
- Authority
- JP
- Japan
- Prior art keywords
- ultra
- optical window
- window
- vacuum
- flange
- 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 - Fee Related
Links
Images
Landscapes
- Lasers (AREA)
Abstract
【課題】超高純度の材料でかつ厚さの薄い窓材を用いる真空紫外光を高効率で超高真空チェンバーに入射するための薄型光学窓付フランジを提供する。
【解決手段】超高真空チェンバーに真空紫外光を高い効率で入射するために薄い超高純度結晶を含む各種の光学窓3を超高真空両面フランジ1に取りつけ、かつ1気圧の定常圧力差ならびに1気圧の突然の圧力変化にも耐えうる構造として、剛性の大きい金属あるいは同等な特性を持つ材料で出来た支持格子7で両面からこの結晶を支えて、圧力変化に対する変形を減少させる。用いる素材は200℃までの加熱ならびに冷却に対して安定な材料とする。
【選択図】図1The present invention provides a flange with a thin optical window for allowing vacuum ultraviolet light using an ultra-high purity material and a thin window material to be incident on an ultra-high vacuum chamber with high efficiency.
Various optical windows containing thin ultra-high purity crystals are attached to an ultra-high vacuum double-sided flange to allow vacuum ultraviolet light to enter the ultra-high vacuum chamber with high efficiency, and a steady pressure difference of 1 atm. As a structure that can withstand sudden pressure changes of 1 atm, the crystal is supported from both sides by a support grid 7 made of a rigid metal or a material having equivalent characteristics, and deformation due to pressure changes is reduced. The material used is a material that is stable to heating and cooling up to 200 ° C.
[Selection] Figure 1
Description
本考案は超高真空チェンバーに真空紫外光を高い効率で入射するための薄型光学窓付フランジに関する。 The present invention relates to a thin flange with an optical window for making vacuum ultraviolet light incident on an ultra-high vacuum chamber with high efficiency.
従来、真空紫外光用の超高真空窓としてはLiF、CaF2、MgF2、BaF2、SrF2、サファイア等が用いられてきた。これらの窓は超高真空と大気との間に置かれることがあるために1気圧の定常圧力差に耐えられる必要がある。またこの窓を介して超高真空チェンバーにつながれる機器も真空排気されている場合も多く、その場合には一方側の真空リーク等によりこの窓に突然1気圧差がかかり窓が破損したり、真空がリークしたりする可能性がある。そのために数十mm径の透過域を持たせる場合は通常は4mm程度の厚さの窓材が用いられることが多かった。Conventionally, LiF, CaF 2 , MgF 2 , BaF 2 , SrF 2 , sapphire, and the like have been used as ultra-high vacuum windows for vacuum ultraviolet light. These windows need to be able to withstand a steady pressure difference of 1 atm because they can be placed between ultra-high vacuum and the atmosphere. In addition, there are many cases where the equipment connected to the ultra-high vacuum chamber through this window is also evacuated. In that case, the window is suddenly damaged by 1 atm due to a vacuum leak on one side, and the window is damaged. There is a possibility that the vacuum leaks. For this reason, when a transmission region having a diameter of several tens of mm is provided, a window material having a thickness of about 4 mm is often used.
近年超高エネルギー分解能のAr、Kr、Xeの定常真空紫外光源を利用するニーズが高まってきたが、これらの光を最大強度で真空内に導くには上記のような光学窓付きフランジが必要である。同様に今後利用できる真空紫外レーザーの波長がこれら光学窓の透過端波長(LiFの場合は約1050A)に近づくにつれて、その波長域でもできるだけ透過率の高い真空光学窓が必要とされるようになって来た。しかしながらこれら結晶の透過端に近い波長域では、窓の厚さが増加するとともに、利用できる透過光強度が激減する。 In recent years, the need to use Ar, Kr, and Xe steady-state vacuum ultraviolet light sources with ultra-high energy resolution has increased, but in order to guide these lights into the vacuum with maximum intensity, the above-mentioned flange with an optical window is required. is there. Similarly, as the wavelength of a vacuum ultraviolet laser that can be used in the future approaches the transmission edge wavelength of these optical windows (about 1050 A in the case of LiF), a vacuum optical window having a transmittance as high as possible in that wavelength region is required. I came. However, in the wavelength region near the transmission edge of these crystals, the thickness of the window increases and the available transmitted light intensity decreases drastically.
本考案は、高い光透過率を実現するため、薄い光学結晶を超高真空フランジに取り付けかつ上記の環境に耐えられる強度を持たせる構造を考案したものである。そのためには剛性の高い格子状の金属または同等な材質の格子で両側から結晶を支える構造をとる。この金属支持格子は結晶に密着し、結晶が圧力によって、あるいは加熱によって、ひずんで破損したり真空リークを生じることを抑制するものである。金属支持格子は試料に接着する面は平面とするが、その一番外周で光学窓に接し始める部分には一定の曲率を付ける事で光学窓となめらかに接触する構造とし、薄い単結晶光学窓の場合であっても、そのへきかいを予防する構造とする。また収束する光を入射させることが多いので、それらが格子の側壁で反射し、予期しない方向に広がり迷光となるのを避けるため、光の後方側の格子の幅が、光の入射側の格子の幅よりも小さいものとする。中心部はレーザー光を通すために直径5mm以上の丸穴とし、それより外の領域は透過率が50%以上できるだけ高い透過率を与える構造とする。なお結晶前方の格子の影と結晶後方の格子とができるだけ重なるようにすることが望ましい。 The present invention devised a structure in which a thin optical crystal is attached to an ultra-high vacuum flange and has a strength capable of withstanding the above environment in order to achieve high light transmittance. For this purpose, a structure is adopted in which the crystal is supported from both sides by a highly rigid lattice-like metal or a lattice of an equivalent material. The metal support lattice is in close contact with the crystal, and suppresses the crystal from being distorted or vacuum leaked by pressure or heating. The surface of the metal support grid that adheres to the sample is flat, but the part that begins to contact the optical window at the outermost periphery of the metal support grid has a structure that makes a smooth contact with the optical window by providing a certain curvature. Even in this case, the structure is to prevent the pain. In addition, since convergent light is often incident, the width of the grating on the rear side of the light is set so that the light is reflected on the side walls of the grating and spreads in an unexpected direction to become stray light. It is assumed to be smaller than the width of. The central portion is a round hole having a diameter of 5 mm or more so as to allow laser light to pass through, and the region outside the center portion has a structure that provides a transmittance as high as possible by 50% or more. It is desirable that the shadow of the lattice in front of the crystal and the lattice in the rear of the crystal overlap as much as possible.
上述の様に、本考案の超高真空用薄型光学窓付フランジでは結晶の厚みを2mm以下1mmさらには0.5mm程度にすることが可能であり、透過端付近での結晶の光透過率を80%以上に設定し、格子の影を考えた場合でも入射光に対する透過率をできるだけ高く設定するのに役立つ。 As described above, in the ultra-high vacuum thin flanged optical window flange according to the present invention, the crystal thickness can be set to 2 mm or less, 1 mm or 0.5 mm, and the light transmittance of the crystal near the transmission end can be increased. It is useful to set the transmittance for incident light as high as possible even when considering that the shadow of the grating is set to 80% or more.
金属支持格子はステンレス、ステンレスに銅を貼り付けた複合材、Cr銅あるいはBe銅等、剛性の大きい材料で、必要に応じて熱伝導度の高い材料を使用する。格子への加工はテーパー付きドリルによる加工、化学エッチングあるいは電解研磨等で行う。金属支持格子はフランジに機械的に固定する。 The metal support lattice is a material having high rigidity such as stainless steel, a composite material in which copper is bonded to stainless steel, Cr copper, or Be copper, and a material having high thermal conductivity is used as necessary. The lattice is processed by a tapered drill, chemical etching, electrolytic polishing, or the like. The metal support grid is mechanically fixed to the flange.
以下添付図面に従って一実施例を説明する。図1は超高真空用薄型光学窓付フランジの断面構造。図2は光透過部分と金属支持格子の相互関係を拡大して示す。薄型光学窓材3は金属支持格子4、7で両面から支持されている。金属支持格子4、7には光透過の領域が多数くりぬかれている。光透過薄型光学窓材3は左方のCFフランジに超高真空シールされている。また3は右方の2とはバイトンOリング6によって抑えられている。フランジ1は超高真空両面フランジであり右の装置と直接接続される。光は図2の右方から入射する。 An embodiment will be described below with reference to the accompanying drawings. Fig. 1 shows a cross-sectional structure of a flange with an ultra-high vacuum thin optical window. FIG. 2 shows an enlarged view of the mutual relationship between the light transmitting portion and the metal support grating. The thin
1 超高真空両面フランジ本体
2 薄型光学窓をバイトンOリングでおさえる金属部材
3 薄型光学窓材
4 金属支持格子
5 金属支持格子おさえ
6 バイトンOリング
7 金属支持格子
8 金属支持格子おさえ
9 接続ねじDESCRIPTION OF SYMBOLS 1 Ultra high vacuum double-
Claims (6)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2007005794U JP3138193U (en) | 2007-06-30 | 2007-06-30 | Ultra-high vacuum flange with optical window |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2007005794U JP3138193U (en) | 2007-06-30 | 2007-06-30 | Ultra-high vacuum flange with optical window |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JP3138193U true JP3138193U (en) | 2007-12-27 |
Family
ID=43288507
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2007005794U Expired - Fee Related JP3138193U (en) | 2007-06-30 | 2007-06-30 | Ultra-high vacuum flange with optical window |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3138193U (en) |
-
2007
- 2007-06-30 JP JP2007005794U patent/JP3138193U/en not_active Expired - Fee Related
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US11053592B2 (en) | Substrate temperature monitoring | |
| JP4511559B2 (en) | Exhaustable flat panel solar collector | |
| EP3195360B1 (en) | Image sensor bending by induced substrate swelling | |
| KR102466067B1 (en) | Image sensor bending using tension | |
| US9775226B1 (en) | Method and system for generating a light-sustained plasma in a flanged transmission element | |
| US20050042117A1 (en) | Optical interference display panel and manufacturing method thereof | |
| US20110005923A1 (en) | Sputtering system, rotatable cylindrical target assembly, backing tube, target element and cooling shield | |
| KR101923837B1 (en) | Anode, and x-ray generating tube, x-ray generating apparatus, and radiography system using the same | |
| TWI630637B (en) | Plasma cell with floating flange | |
| JP2011107264A (en) | Uv ray irradiation device | |
| JP4878782B2 (en) | Plasma processing apparatus and plasma processing method | |
| WO2007149214A2 (en) | Vacuum cell for optical components | |
| JP3138193U (en) | Ultra-high vacuum flange with optical window | |
| JP4490257B2 (en) | Sputtered cathode for coating process | |
| US20110005925A1 (en) | Target backing tube, cylindrical target assembly and sputtering system | |
| US20150097107A1 (en) | Apparatus for generating extreme ultraviolet light using plasma | |
| CN107112709B (en) | Laser amplification device | |
| JP2007067123A (en) | Laser pulse compressor | |
| CN102496838A (en) | Installation apparatus of high power unstable cavity laser output terminal cavity mirror | |
| CN219509533U (en) | An optical observation window for vacuum environment | |
| CN222506590U (en) | A low-radiation infrared field mirror | |
| CN110018511B (en) | Movable X-ray detection system | |
| JP2008081763A (en) | Target assembly unit and sputtering apparatus | |
| CN121447235A (en) | A vacuum window and its manufacturing method | |
| CN103513489A (en) | Laser bearing and light beam conversion device |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A521 | Request for written amendment filed |
Free format text: JAPANESE INTERMEDIATE CODE: A523 Effective date: 20070911 |
|
| R150 | Certificate of patent or registration of utility model |
Free format text: JAPANESE INTERMEDIATE CODE: R150 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20101205 Year of fee payment: 3 |
|
| LAPS | Cancellation because of no payment of annual fees |