TWI249023B - Reference leak - Google Patents

Reference leak Download PDF

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TWI249023B
TWI249023B TW94100491A TW94100491A TWI249023B TW I249023 B TWI249023 B TW I249023B TW 94100491 A TW94100491 A TW 94100491A TW 94100491 A TW94100491 A TW 94100491A TW I249023 B TWI249023 B TW I249023B
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Taiwan
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hole
leak
standard
gas
standard leak
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TW94100491A
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Chinese (zh)
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TW200624777A (en
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Jie Tang
Liang Liu
Peng Liu
Zhao-Fu Hu
Bing-Chu Du
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Hon Hai Prec Ind Co Ltd
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Abstract

This invention relates to a reference leak. The reference leak includes a thin film which a tested gas could not penetrate through, and predetermined amounts of through holes formed there through. The through holes have predetermined sizes which are in nano magnitude. Because the shapes of the through holes are standard, the sizes and the amounts of the through holes are predetermined, so a leak rate of the reference leak of present invention could be calculated directly by a vacuum science classical theory, and it could attain a wider leak rate range than the prior art; even it could achieve an ultra-small leak rate.

Description

1249023 九、發明說明: 【發明所屬之技術領域】 本發明涉及一種標準漏孔,尤其係一種通導型標準漏孔。 【先前技術】 標準漏孔係於規定條件下(入口壓力為l〇〇kPa±5%,溫度為23±7t), 漏率係已知的一種校準用漏孔。標準漏孔係真空科學技術及其應用領域一 種常用之必不可少的計量器具,特別係標準氦漏孔,係目前已得到廣泛應 用之氦質譜檢漏儀中必備之相對計量標準,使用標準漏孔定期對氦質譜檢1249023 IX. Description of the Invention: [Technical Field] The present invention relates to a standard leak, and in particular to a through-type standard leak. [Prior Art] The standard leak is under a predetermined condition (inlet pressure is l〇〇kPa±5%, temperature is 23±7t), and the leak rate is a known leak for calibration. Standard leaky vacuum science and its application field A commonly used measuring instrument, especially the standard leaking hole, is the necessary relative measurement standard in the mass spectrometer leak detector which has been widely used at present. Hole periodic 氦 mass spectrometry

漏儀之最主要參數一檢漏靈敏度進行校準,從而準確給出被測系統漏氣速 率之數量級大小。 標準漏孔具有恒定漏率,其亦稱定流量發生器,通常可分為兩大類, 第一類為通導型標準漏孔,如鉑絲-玻璃非匹配標準漏孔、金屬壓扁型標準 漏孔;第二類為滲透型標準漏孔,如石英薄膜標準漏孔。國家技術監督局 專門為此制定了 JJG793-92標準漏孔之國家計量鐾定規程。 、參見劉秀林在文獻《航空計測技術》Vol· 21,No· 5, 43-45(2001) ‘‘標 準漏孔及其鮮”-文,目觸使用之麟—賴非匹配鮮狐,漏率範 圍-般為1〇·6〜1〇_8托·升/秒,其係一種將直徑在〇· 1〜〇· 15mm的翻絲與11#硬質 玻璃做非匹配封結後,個兩種材料膨脹係數的不同而得到之漏孔。因為 於製化過程巾難以人為地控制鮮漏孔之尺寸大小、數目,漏率大小受控 性差/其醉必須借助其他設備對其進行標定才能確定,不能自定標;^ 度會導致材料熱脹冷縮,因此其易受溫度變化之影響,漏率之穩定性了 且漏率範圍較窄,難以實現更小漏率之測量。 , 金屬壓扁型標準漏孔,漏率範圍一般為1〇n ,直經之絲銅管或可伐㈣轉鍾錢産生難,從而二 於製造過程中標準漏孔之尺寸大小難以料控制,漏率 必須借助其他設備對其進行標^才能確定,不能自定標二 漏革靶圍較乍,難以實現更微小漏率之檢測。 多之範圍—般植MG—^.升/秒,制前使用較 準漏孔’其歸石英麵管吹製成各種直徑及厚度之薄膜球 7The most important parameter of the leak detector, the leak detection sensitivity, is calibrated to accurately give the magnitude of the leak rate of the system under test. Standard leaks have a constant leak rate. They are also called constant flow generators. They can usually be divided into two categories. The first type is a standard lead-type leak, such as platinum wire-glass non-matching standard leaks, metal flattening standards. Leakage; the second type is an infiltration type standard leak, such as a standard leak of quartz film. The National Technical Supervision Bureau has specially formulated the national measurement and determination procedures for JJG793-92 standard leaks. See Liu Xiulin in the literature "Aviation Measurement Technology" Vol. 21, No. 5, 43-45 (2001) ''Standard Leakage and Its Freshness' - Wen, the use of the Lin - Lai non-match fresh fox, leak The rate range is generally 1〇·6~1〇_8 托·liter/second, which is a type of twisted wire with a diameter of 〇·1~〇·15mm and 11# hard glass for non-matching. The leakage coefficient obtained by different expansion coefficients of the material is difficult to artificially control the size and number of the fresh leak holes in the manufacturing process towel, and the leak rate is poorly controlled/the drunk must be calibrated by other equipment to determine , can not self-calibration; ^ degree will cause the material to expand and contract, so it is susceptible to temperature changes, the stability of the leak rate and the narrow range of leakage rate, it is difficult to achieve a smaller leakage rate measurement. Flat type standard leak, the leakage rate is generally 1〇n, the straight copper wire or the kovar (four) turn clock money is difficult to produce, so the size of the standard leak hole in the manufacturing process is difficult to control, the leak rate must be It can be determined by other equipments, and it can not be self-calibrated. Difficult to achieve a finer detection of the leak rate of the multi-range -. MG- ^ implanted as liters / sec., Prepared using the calibrated leak 'normalized face of the quartz tube blow molding of various diameters and thickness of the film ball 7

1249023 泡’利用石英只能使統雜通過,而其錢 漏孔》由於薄膜球泡由吹製而成的,因此薄膜球泡之之標準 ,數目難以控制’通孔之尺寸難以獲取,從而在製造 解=之通 ^ :其漏,借助其他設備對其進行標定才能確可: 漏率範圍較窄,難以實現更微小漏率之檢 目疋禚,且 適用於氦氣,限制了其應用範圍。1 ’亚且’石央賴標準漏孔只 如上所述’目前所使用之標準漏孔如麵絲_玻 扁型標準祕、石鶴麟賴Μ,由於其辭必須借 進仃標定(可參見萬昭志、葉盛等人在文獻《真 ^1249023 Bubble 'use of quartz can only make the system pass, and its money leaks" because the film bulb is blown, so the standard of the film bulb is difficult to control the 'through hole size is difficult to obtain, so Manufacture solution = pass: It leaks, it can be calibrated by other equipment: The leak rate range is narrow, it is difficult to achieve a smaller leak rate inspection, and it is suitable for helium, which limits its application range. . 1 'Ya' 'Shiyang Lai standard leaks only as mentioned above' The standard leaks currently used such as the surface wire _ glass flat standard secret, Shi Helin Lai, because the words must be borrowed from the 仃 calibration (see Wan Zhaozhi , Ye Sheng and others in the literature "真 ^

No. 2, 39-41(2002) t W t W " 能自定標;漏率範圍較窄,難以實現更小漏率之檢測。 有黎於^ ’有必要提供-種標準漏孔,其能自定標、可 率之檢測等優點。 _ 【發明内容】 為解決現有技術中標準漏孔漏率必須借助其他設備對其進行標定、難 以實現更小漏率之檢測等不足,本發明之目的在於提供一種能自曰 可實現更小漏率之檢測標準漏孔。 ^ ' 為實現本發明之目的,本發明提供之一種標準漏孔,其包括一被測氣 體不能滲透之薄膜及形成於該薄膜内之預定數目之通孔,上述通孔具有^ 定尺寸孔徑。 、 優選的,所述通孔孔徑大小範圍為奈米級。 更優選的,所述通孔孔徑大小範圍為l0nm〜500nm。 優選的,所述標準漏孔之漏率滿足公式·· QlKPrρ2) χΥ, 式中,Q為標準漏孔之漏率,n(ngl)為通孔數目,?1為標準漏孔之被 測氣體流入端壓強,P2為標準漏孔之被測氣體流出端壓強, Y表禾單一通孔之氣導,其滿足公式:Y=12· 1xV^7x(D3/L) (l> 20D), 广 成中,Μ為被測氣體之分子量,D為通孔直徑,L為通孔長度。 所述標準漏孔之單一通孔漏率範圍大小為1(Γι5〜1(Γ8托·升/秒。 1249023 所述薄膜之材料包括金屬材料、陶瓷及玻璃。 所述標準漏孔可用於氦氣、空氣、氧氣及氮氣之計量。 所述通孔之形狀包括圓柱形及多邊形。 相對于先前技術’本發賴提供之標準漏孔,因域通孔之數目及尺 寸可藉由對奈米加工技術做之㈣獲得,·然後,藉由公式:Q=nx(p|_⑸X YJ式中,Q 4標準漏孔之漏率,咖以)為通孔數§,R為標準漏孔之被測 氣體肌入端壓強,p2為標準漏孔之被測氣·i出端壓^ (Dj/L) (Μ為通孔中被測氣體之分子量’ D為通孔直徑,L為通孔長度)可 計算出標準漏孔之漏率值,當滿足以1/3)1)且G2qd (式中,鸿氣體分 子自由程)兩鶴件之情盯,計算精度紐5%。討實現自定標,且漏 率範圍較寬,可實現超微小漏率之檢測。 【實施方式】 下面結合附圖將對本發明作進一步之詳細說明。 、,見第六圖,本發騎提供之鮮漏孔丨⑻,其包括—防止被測氣體渗 透之薄膜30,及形成於薄膜3〇内之預定數目之通孔3G1 ;通孔3Q1具有預定 尺寸孔徑,該孔徑大小範_選為奈米級(即小於丨_);通孔之孔徑大小範 圍更優選為IGnm〜5_m。鮮漏孔100可胁氦質譜檢漏儀之準較標、微 型真空泵抽速之測量、氣时面科學研究巾,提供微小流量之等領域。 對於薄膜30,其材質可為金屬材料、玻璃、陶瓷等;其材質之選擇決 定最終所形成之標準漏孔1〇〇之適用氣體種類。若選擇金屬材料,則可應用' 於氦氣之醇·,因為氦氣不能滲透金屬材料:若選擇玻璃或陶究了則 可應用於空氣、氧氣、氬氣之漏率測量,因為空氣、氧氣、氬氣等不能渗 透玻璃及陶瓷。 / 參見第一圖至第五圖,本發明所提供之標準漏孔,可藉由以預定尺寸 及數目之奈米線為模板之圖形轉移技術實現,其包括以下步驟: 第一,提供一潔淨之矽基底1,其晶向可為<U1>、<1〇〇>、<u〇>、或 其他晶向;本實施例中優選為<111〉晶向,即Si<iii> ; 第二,於上述矽基底1上形成一催化劑薄膜,催化劑薄膜之材料可為 金、鐵、鈷、銀等’本實施例中採用金薄膜2作為催化劑;金薄膜2之厚度 1249023 範圍為0. 2nm〜10nm ,優選為lnm ;其中,金薄膜2之形成方法包括蒸鍍、濺 射或電鍍等,然後,採用光刻工藝或電子束刻触技術在上述金薄膜2上形成 預定數目及尺寸大小之圖案結構21,且圖案結構21之尺寸小於1μπι,以使單 一圖案結構21上只生長一根奈米線;也可以在矽基底丨上藉由印刷技術直接 形成具有預定尺寸且排列規則之圖案結構21之金薄膜2 ;其中,圖案結構21 之具體形狀可為微小方塊及其變形結構; 第二,將上述形成有金薄獏2之矽基底置於CVD反應腔體(圖中未示 出)’亚向CVD反應腔體内提供氣相之含石夕物質,本實施例中採用四氣化石夕 (SiQ4)氣體;控制四氣化矽氣體之濃度,將CV])反應腔體内之溫度控制在 700 C〜900°C,在上述金薄膜2之催化作用下,在具有圖案結構之位置將生 長出-維奈米結構’如奈米線、奈米棒;本實關中,树基幻生長出石夕 奈米線1卜其為陳縣構;料米線山歸<ηι〉方向剩,即垂直於石夕 土氐八中石夕示米線11之孔後大小範圍優選為lOnm〜500nm,石夕奈米線11 之長度乾Ml_n〜1G_ ;具體之轉米線u之孔徑及長度可藉由控制金 薄獻中之圖案結觀的尺寸、_維奈米結構之生長溫度、生長氣氛濃度及 生長日守間來雜’在圖案結構21之尺寸不大於丨_之條件下,可藉由控制_ 條件使得轉米線u之數目等於圖案結構21之數目m線Η之直徑、 長度受金薄膜2之厚度、生長溫度、生錢氛濃度以及生長時間等條件控 ,。另’可根據後續n要,可將料米線n氧化成二氧化科米線。 為保證以Κη觀城計算_之結果縣拙町,要求本步财之石夕奈 米線11長度不小於20倍其直徑大小。 第四,於生長神奈米線u之⑦基底丨上沈積—第二膜層,第二膜層之 貝1為金屬材料、玻璃、吨;其材質之選擇決定最終所形成之標準漏 ^適用氣體種類,如果選擇金屬材料,則可應用於氮氣之漏率測量,因 ,透金屬;如果選抛璃或喊,則可應用於空氣、氧氣、复 :::二:里,因為空軋、氧氣、氬氣等不能滲透玻璃及陶瓷;本實施例 :t ίΐί層3,如鎳,等,其沈積之厚度可根據需要,在矽奈米 雷化2二圍ί调即’亚且’在沈積完金屬膜層3之後,還可採用機械或 電化學拋先寺功使金屬_3上表科齊、去除露頭之料鱗u端部、 10 1249023 於石夕奈米線11直徑之20 根據預定漏糊節所f之錢料度,保持直不小 倍; ’、 η及=底H反麟子雜(Reatlve lQn EtGhlng,_去_奈米線 二夕基底1材料而不損傷金屬膜層3 ’從而在金屬膜層3形成尺寸财奈米 子刻二t=31(其中,通孔31垂直於發基底1平面);由於採用反應離 金屬膜岸3大奈米線U及石夕基底1材料,而不損傷石夕奈米線11周圍之 石夕夺石夕示未線完全侧掉;因此’獲得之通孔31之孔徑大小與 31I 致’通孔&之長度與最終金屬膜層3之厚度-致,通孔No. 2, 39-41 (2002) t W t W "Self-calibration; the leak rate range is narrow, making it difficult to detect smaller leak rates. There are Li Yu ^ ‘It is necessary to provide a standard leak, which can self-calibration, rate detection and so on. _ SUMMARY OF THE INVENTION In order to solve the problem that the standard leak leak rate in the prior art must be calibrated by other equipment, and it is difficult to detect a smaller leak rate, the object of the present invention is to provide a self-sufficient and small leak. The rate of detection of standard leaks. For the purpose of the present invention, the present invention provides a standard leak which includes a film impermeable to a gas to be measured and a predetermined number of through holes formed in the film, the through holes having a pore size. Preferably, the through hole aperture size ranges from nanometer. More preferably, the through hole has a pore size ranging from 10 nm to 500 nm. Preferably, the leak rate of the standard leak hole satisfies the formula ···································· 1 is the pressure of the inflow end of the measured gas of the standard leak hole, P2 is the pressure of the outflow end of the measured gas of the standard leak hole, and the air conductance of the single pass hole of Y and the formula, which satisfies the formula: Y=12·1xV^7x (D3/ L) (l > 20D), in Guangcheng, Μ is the molecular weight of the gas to be measured, D is the diameter of the through hole, and L is the length of the through hole. The standard through-hole leakage rate of the standard leak is 1 (Γι5~1 (Γ8 Torr·sec. sec. 1249023) The material of the film includes metal material, ceramic and glass. The standard leak hole can be used for helium gas. Metering of air, oxygen and nitrogen. The shape of the through hole includes a cylindrical shape and a polygonal shape. Compared with the standard leakage provided by the prior art, the number and size of the through hole can be processed by the nanometer. The technology does (4) obtain, and then, by the formula: Q = nx (p | _ (5) X YJ, Q 4 standard leak leakage rate, coffee) is the number of through holes §, R is the standard leak measured Gas pressure at the end of the muscle, p2 is the measured gas of the standard leak hole · i terminal pressure ^ (Dj / L) (Μ is the molecular weight of the gas in the through hole ' D is the diameter of the through hole, L is the length of the through hole) The leak rate of the standard leak can be calculated. When the two cranes are in the range of 1/3)1) and G2qd (in the formula, the gas gas free path), the calculation accuracy is 5%. To achieve self-calibration, and a wide range of leak rates, the detection of ultra-small leak rate can be achieved. [Embodiment] The present invention will be further described in detail below with reference to the accompanying drawings. See the sixth figure, the fresh leak hole 丨 (8) provided by the present ride includes a film 30 for preventing penetration of the gas to be measured, and a predetermined number of through holes 3G1 formed in the film 3〇; the through hole 3Q1 has a predetermined The size of the pore size is selected to be nanometer (i.e., smaller than 丨_); the pore size of the through hole is more preferably IGnm 〜5_m. The fresh leak hole 100 can be used to measure the quasi-standard of the mass spectrometer leak detector, the measurement of the micro vacuum pumping speed, the scientific research of the gas-time surface, and the provision of small flow. For the film 30, the material may be a metal material, glass, ceramics or the like; the choice of the material determines the type of gas suitable for the standard leak hole 1 最终 which is finally formed. If you choose metal materials, you can use 'air alcohol' because helium cannot penetrate metal materials: if you choose glass or ceramics, it can be used for air, oxygen, argon leak rate measurement, because air, oxygen , argon gas, etc. can not penetrate glass and ceramics. / Referring to the first to fifth figures, the standard leak provided by the present invention can be realized by a pattern transfer technique using a predetermined size and number of nanowires as a template, which comprises the following steps: First, providing a clean The substrate 1 may have a crystal orientation of <U1>, <1〇〇>, <u〇>, or other crystal orientation; in this embodiment, it is preferably <111> crystal orientation, i.e., Si<; iii >; Second, a catalyst film is formed on the ruthenium substrate 1 , and the material of the catalyst film may be gold, iron, cobalt, silver, etc. 'In this embodiment, the gold film 2 is used as a catalyst; the thickness of the gold film 2 is 1249023 The range of 0. 2 nm to 10 nm, preferably 1 nm; wherein the gold film 2 is formed by evaporation, sputtering or electroplating, etc., and then formed on the gold film 2 by photolithography or electron beam etching. a pattern structure 21 of a number and size, and the size of the pattern structure 21 is less than 1 μm so that only one nanowire is grown on the single pattern structure 21; or a predetermined size can be directly formed on the base substrate by a printing technique and Arranged pattern structure 21 The film 2; wherein, the specific shape of the pattern structure 21 may be a minute square and a deformed structure thereof; secondly, the substrate having the gold thin tantalum 2 formed thereon is placed in a CVD reaction chamber (not shown) The CVD reaction chamber provides the gas-containing material in the gas phase. In this embodiment, the gas of SiQ4 is used; the concentration of the gas of the gasification of the gas is controlled, and the temperature in the reaction chamber of the CV] is controlled at 700. C ~ 900 ° C, under the catalysis of the above gold film 2, in the position of the pattern structure will grow -Vanami structure 'such as nanowires, nanorods; in this reality, the tree base magic grows out of Shi Xi The rice line 1 is the structure of Chenxian County; the rice noodle is returned to the direction of ηι>, that is, the size of the hole perpendicular to the stone in the Xixi 氐 中 中 夕 示 示 示 示 优选 优选 优选 优选 优选 优选 优选 优选 优选 优选 优选 优选 优选 , 夕 夕The length of the nanowire 11 is dry Ml_n~1G_; the diameter and length of the specific rice noodle u can be controlled by controlling the size of the pattern in the thin gold sheet, the growth temperature of the venetian structure, the concentration of the growth atmosphere, and the growth day In the case where the size of the pattern structure 21 is not greater than 丨_, it can be controlled by _ Conditions are such that the number of revolutions equal to the number u noodle of 21 m wire diameter Η pattern structure, the thickness of the gold film by a length of 2, the growth temperature, and the concentration of the growth atmosphere with money, time-controlled conditions. Alternatively, the rice noodle n can be oxidized to the dioxide Komi line according to the subsequent n. In order to ensure that the results of the calculation of the city 拙 拙 拙 拙 , , , , , , , , , , , 要求 要求 要求 要求 要求 11 11 11 11 11 11 11 11 Fourth, the second film layer is deposited on the substrate 丨 of the growth god nano line u, and the second film layer is made of metal material, glass, and ton; the choice of material determines the final standard leakage gas. Type, if metal material is selected, it can be applied to the leakage rate measurement of nitrogen, because it is transparent to metal; if it is selected to be thrown or shouted, it can be applied to air, oxygen, and complex:::2, because of empty rolling, oxygen , argon gas, etc. can not penetrate glass and ceramics; this embodiment: t ίΐί layer 3, such as nickel, etc., the thickness of its deposition can be adjusted according to the needs of the 矽 nanometer 2 二 二 ί ί ί ' ' ' ' ' ' ' After the completion of the metal film layer 3, mechanical or electrochemical polishing of the first temple can be used to make the metal _3 on the surface of the table, remove the outcrop material scale u end, 10 1249023 on the Shi Xi Nai line 11 diameter 20 according to the schedule The material of the leaky paste is kept at a small time; ', η and = bottom H anti-linking (Reatlve lQn EtGhlng, _ go_nano line Erxi base 1 material without damaging the metal film layer 3 'Therefore, the size of the metal film layer 3 is formed by the second half of the tN=2 (where the through hole 31 is perpendicular to the base 1) Plane); due to the use of the reaction from the metal film shore 3 large nanowire U and Shi Xi base 1 material, without damaging the stone Xi Nian line 11 around the stone eve stone show that the line is completely off; therefore The aperture size of the through hole 31 and the length of the through hole & and the thickness of the final metal film layer 3, the through hole

干),線U之數目相等;進而獲得一粧拠·如第五圓所V i、、rt 預定尺寸孔徑及數目。當然,亦可以_濕法職(如, 錢^寺腐錄)或等離子體刻鱗卫藝去时奈米線u及德底i材料, 而不知'傷金屬膜層3 ;或根據不同的奈米線材料及第二膜層之材質選擇適當 之去除工藝。 、 田 -上述標準漏孔之製作工藝中,若採用其他晶向之石夕基底,則生長出之 夕不米線與$基底平面成—定之角度;相應的,製成之標準漏孔之通孔也 與基底成-定之角度;其通孔之孔徑大小、數目仍由雜米線之直徑大小、 數目決定。 、下面將具體說明本發明所提供之標準漏孔漏率之計算。如上所形成之 標準漏孔10,因為其通孔31之形狀標準(為圓柱形),尺寸及數目都^知, 且孔徑大小達奈米級;因此可用真空科學之經典理論計算直接得出其漏率 值。例如壓強為大氣壓強之I氣,其平均自由程λ>5()ηιη ;壓強為i托之氮 氣,其平均自由程λ>38ηιπ。在滿足A>(1/3)D之條件下,本發明所提供之 標準漏孔之氣流導可用克努曾(Knusen)公式計算。對於直徑為D,長度為匕, 且L-20D之單一通孔,在2(rc條件下,按Knusen公式,氦氣之流導(穩定狀 態下,單位壓力差下通孔之氣流通量)滿足: Y=12· 1xV29m7x(D3/L)……(1) 公式(1)中,Y為單個通孔氦氣之流導,單位為升/秒江“); Μ為通孔中氦氣之分子量,Μ二4 ; D為通孔之直徑,單位為厘米(cm); 11 1249023 L為通孔之長度,單位為厘米(cm)。 對於任意溫度條件下,公式⑴之修正為:㈣· lxV^xV77^x (D3/L)……⑵ 公式(2)中,T為絕對溫度值,單位為開爾文(κ)。 而且,單位時間内通過標準漏孔之氦氣流量,即標準漏孔之漏率滿足: Qi=nx(Prρ2) χγ ……(3) 公式(3)中,Qi為標準漏孔之漏率,單位為托·升; η為標準漏孔中通孔之數目,且為签數(η—ι);Dry), the number of lines U is equal; and thus a makeup 拠, such as the fifth circle V i, rt, the predetermined size aperture and number. Of course, you can also _ wet legal duties (such as, Qian ^ Temple Corruption) or plasma engraved guardian to go when the nanowire u and Dedi i materials, but do not know 'injury metal film layer 3; or according to different nai The material of the rice noodle material and the second film layer are selected to be appropriately removed. In the production process of the above-mentioned standard leak hole, if other stone-like bases are used, the growth of the non-rice line and the base plane are at an appropriate angle; correspondingly, the standard leak hole is made. The hole is also at an angle to the substrate; the size and number of the apertures of the through hole are still determined by the size and number of the diameter of the rice noodle. The calculation of the standard leak leak rate provided by the present invention will be specifically described below. The standard leak hole 10 formed as above has a standard size (cylindrical shape) of the through hole 31, the size and the number are known, and the pore size is up to the nanometer level; therefore, it can be directly obtained by the classical theoretical calculation of vacuum science. Leakage rate value. For example, the pressure is atmospheric pressure, and the mean free path λ > 5 () ηιη; the pressure is i to the nitrogen gas, and the mean free path λ > 38 ηιπ. Under the condition that A > (1/3) D is satisfied, the gas flow guide of the standard leak provided by the present invention can be calculated by the Knusen formula. For a single through hole of diameter D, length 匕, and L-20D, in 2 (rc condition, according to the Knusen formula, the flow of helium (in steady state, the flow flux of the through hole under unit pressure difference) Satisfaction: Y=12· 1xV29m7x(D3/L)......(1) In formula (1), Y is the conductance of a single through-hole helium gas, the unit is liter/second river “); Μ is the helium in the through hole Molecular weight, Μ 2 4 ; D is the diameter of the through hole, the unit is centimeter (cm); 11 1249023 L is the length of the through hole, the unit is centimeter (cm). For any temperature condition, the correction of formula (1) is: (4) · lxV^xV77^x (D3/L) (2) In equation (2), T is the absolute temperature value in Kelvin (κ). Moreover, the helium flow through the standard leak per unit time, ie the standard leak The leak rate of the hole satisfies: Qi=nx(Prρ2) χγ (3) In equation (3), Qi is the leakage rate of the standard leak, the unit is Torr· η; η is the number of through holes in the standard leak, And the number of tickets (η-ι);

Pi為標準漏孔之被測氣體流入端壓強,單位為托(T〇rr); P2為彳示準漏孔之被測氣體流出端塵強,單位為托。 因此,當通孔直徑D為lOOnm,長度L為5/zm,PF760TOIT,PH),通孔 數n=l,溫度為2(TC時,由公式(1)及公式(3)可知,單一通孔之氦氣流導 Y 12. lxV29/4x((l〇 )/(5x10 4))=6. 51xl(TuL/s,標準漏孔之漏率q=(76〇-〇) x6· 51x10 u=4.95xl(T8Torr.L/s ; fPelTorr,本發明所提供之標準漏孔可 實現1(T15Toit.L/s的漏率。 s通孔之數目η為1000時,則由公式(3)可知,標準漏孔之漏率相應為 η=1時之1〇〇〇倍。 另一實施例中,在矽基底上沈積一金屬薄膜,採用聚焦離子束直寫技 術在上述金屬薄膜上刻出圓柱形通孔,通孔之孔徑一般在1〇nm以上;然後 抓用必要之刻蝕技術去除通孔附近之矽基底,即可獲得一標準漏孔。 本發明所提供之標準漏孔,藉由變更第二膜層之材質,將適用於氦氣 之i屬材料更換為二氧化碎,可獲得適用於空氣、氧氣、氬氣之標準漏孔, 在其漏率之計算時,相應地改變公式(1)及公式(幻中从值即可。 另外,以上所述之標準漏孔之通孔之形狀為圓柱形,其也可以為其他 形狀,只要其不偏離本發明之效果。如通孔之形狀可為多邊形,但對於流 導汁异公式(〇及(2),需要考慮相應之形狀修正係數。 另外,本領域技術人員還可在本發明精神内做其他變化,如採用其他 材料或其他方法製作標準漏孔等設計,只要其製作之標準漏孔具有預^尺 寸及數目;即可實現自定標。 12 1249023 綜上所述,本發明確已符合發明專利要件,爰依法提出專利申請。惟, 以上所述者僅為本發明之較诖實施例,舉凡熟悉本案技藝之人士,於援依 本案發明mm作之等效修飾或變化m含於町之申請專 【圖式簡單說明】 第一圖係相關本發明實施例之矽基底之示意圖。 第一圖係石夕基底上形成一催化劑薄膜之示意圖。 第三圖係矽基底上生長有一維奈米結構之示意圖。Pi is the pressure at the inflow end of the measured gas in the standard leak hole, and the unit is the support (T〇rr); P2 is the dust intensity of the measured gas outflow end of the quasi-leakage hole, and the unit is the support. Therefore, when the through hole diameter D is 100 nm, the length L is 5/zm, PF760TOIT, PH), the number of through holes is n=l, and the temperature is 2 (TC, it is known from the formula (1) and the formula (3) that the single pass The airflow of the hole is guided by Y 12. lxV29/4x((l〇)/(5x10 4))=6. 51xl (TuL/s, the leakage rate of the standard leak hole q=(76〇-〇) x6· 51x10 u= 4.95xl (T8Torr.L / s; fPelTorr, the standard leak provided by the present invention can achieve 1 (T15 Toit. L / s leak rate. When the number of s through holes η is 1000, then from equation (3), The leak rate of the standard leak hole is correspondingly 1 times that of η = 1. In another embodiment, a metal film is deposited on the ruthenium substrate, and a cylindrical shape is carved on the metal film by a focused ion beam direct writing technique. The aperture of the through hole and the through hole is generally above 1 〇 nm; then a standard leak is obtained by removing the ruthenium substrate near the through hole by using the necessary etching technique. The standard leak provided by the present invention is changed by The material of the second film layer is changed to the oxidized slag of the i-type material suitable for helium, and the standard leak hole suitable for air, oxygen and argon can be obtained. When the leak rate is calculated, the formula is changed accordingly. 1) and the formula (the imaginary value is sufficient. In addition, the shape of the through hole of the standard leak hole described above is cylindrical, and it may be other shapes as long as it does not deviate from the effect of the present invention. The shape may be a polygon, but for the flow-through juice formula (〇 and (2), the corresponding shape correction factor needs to be considered. In addition, other variations may be made by those skilled in the art within the spirit of the invention, such as using other materials or other The method is to make a standard leak hole design, etc., as long as the standard leak hole produced has the pre-size and number; the self-calibration can be realized. 12 1249023 In summary, the invention has indeed met the requirements of the invention patent, and the patent application is filed according to law. However, the above is only a comparative example of the present invention. For those who are familiar with the art of the present invention, the equivalent modification or variation of the invention in the case of the aid of the present invention is included in the application of the town [simplified description] The first figure is a schematic diagram of a crucible substrate according to an embodiment of the present invention. The first figure is a schematic diagram of forming a catalyst film on the substrate of the Shixi. The third figure is a structure of a vitamin nanostructure grown on the substrate. FIG.

第—四圖係於生長有一維奈米結構之矽基底上形成第二膜層之示意 第五圖係去除一維奈米結構及矽基底材料之結構示意圖。 。Θ 第六圖係相關本發明之標準漏孔之剖面示意圖。 【主要元件符號說明】 矽基底 1 標準漏孔 標準漏孔 100 矽奈米線 金薄膜 2 圖案結構 金屬膜層 3 薄膜 通孔 31 通孔 10 11 21 30 301The fourth figure is a schematic diagram of forming a second film layer on a substrate on which a one-dimensional nanostructure is grown. The fifth figure is a schematic view showing the structure of removing the one-dimensional nanostructure and the base material. .第六 The sixth figure is a schematic cross-sectional view of a standard leak according to the present invention. [Main component symbol description] 矽 base 1 standard leak hole standard leak hole 100 矽 nano line gold film 2 pattern structure metal film layer 3 film through hole 31 through hole 10 11 21 30 301

1313

Claims (1)

1249023 十、申請專利範圍: 1· 一種標準漏孔,其包括: 一被測氣體不可滲透之薄膜;及 形成於該薄膜内預定數目之通孔,通孔具有預定尺寸孔徑。 2·如申請專利範圍第丨項所述之標準漏孔,其改良在於所述薄膜之材質包 括金屬材料、玻璃及陶瓷。 3·如申請專纖圍第丨項所述之鮮漏孔,其改良在於所述通孔形狀包括 圓柱形及多邊形。 4·如申請專概U第1項所述之標準漏孔,其改良在於所述通孔之孔徑大 小為奈米級。 5·如申請專繼m第4項所述之鮮漏孔,其改良在於所述通孔之孔徑大 小範圍為10nm〜500nm。 6.如申請專利範圍帛1項所述之標準漏孔,其&良在於所述標賴孔之單 一通孔之漏率範圍大小為1〇_15〜10·8托·升/秒。 7·如申請專利範圍第1項所述之標準漏孔,其改良在於所述通孔之長度不 小於20倍通孔之孔徑大小。 8.如申請專利範圍第7項所述之標準漏孔,其改良在於所述標準漏孔之漏 率滿足公式: Q=nx(PrP2) χΥ, 其中,Q為標準漏孔的漏率,η(η^1)為標準漏孔中通孔的數目,?1為 漏孔的被測氣體流入端壓強,ρ2為漏孔的被測氣體流出端壓強, Υ為早'一通孔的氣導’其滿足公式: Υ=12· \χ4Ϊ9ΙΜ x(D3/L), 其中,Μ為被測氣體之分子量,D為通孔直徑,l為通孔長度。 141249023 X. Patent application scope: 1. A standard leak hole comprising: a film impermeable to a gas to be measured; and a predetermined number of through holes formed in the film, the through holes having a predetermined size aperture. 2. The standard leak as described in the scope of claim 2 is improved in that the material of the film comprises a metal material, glass and ceramic. 3. The improvement of the fresh leak as described in the section of the special fiber is that the shape of the through hole includes a cylindrical shape and a polygonal shape. 4. The standard leak as described in the application of the first item U, the improvement is that the diameter of the through hole is nanometer. 5. The method of applying the special fresh hole according to item 4 of the item m is improved in that the diameter of the through hole is in the range of 10 nm to 500 nm. 6. The standard leak according to claim 1, wherein the leak rate of the single through hole of the standard hole is 1 〇 15 to 10 · 8 Torr / sec. 7. The standard leak as described in claim 1 is improved in that the length of the through hole is not less than 20 times the aperture size of the through hole. 8. The standard leak as described in claim 7 is improved in that the leakage rate of the standard leak is such that: Q = nx (PrP2) χΥ, where Q is the leak rate of the standard leak, η (η^1) is the number of through holes in the standard leak hole? 1 is the pressure at the inflow end of the measured gas of the leak hole, ρ2 is the pressure at the outflow end of the gas to be measured of the leak hole, and Υ is the air conductance of the earlier 'one through hole' which satisfies the formula: Υ=12· \χ4Ϊ9ΙΜ x(D3/L) Where Μ is the molecular weight of the gas to be measured, D is the diameter of the through hole, and l is the length of the through hole. 14
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