TWI247099B - Stable high temperature sensor/heater system and method with tungsten on AlN - Google Patents

Stable high temperature sensor/heater system and method with tungsten on AlN Download PDF

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TWI247099B
TWI247099B TW93114815A TW93114815A TWI247099B TW I247099 B TWI247099 B TW I247099B TW 93114815 A TW93114815 A TW 93114815A TW 93114815 A TW93114815 A TW 93114815A TW I247099 B TWI247099 B TW I247099B
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layer
substrate
temperature
sensor
response
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TW93114815A
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TW200510702A (en
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James D Parsons
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Heetronix
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Abstract

A sensor system has an AlN substrate (4), a W layer (2) on the substrate, a signal source (70) adapted to apply an electrical actuating signal to the W layer, and a sensor (72) adapted to sense the response of the W layer. The W layer can comprise a thin film, with various types of optional protective layers (12) over the film. Applications include sensing temperature, fluid flow rates, fluid levels, pressure and chemical environments. For a planar heater, the W layer comprises a plurality of conductive strands (34) distributed on the substrate, with the strands generally parallel and serpentine shaped for a rectangular substrate (32), and extending along respective lines of longitude (40) that merge at opposite poles (44) of the substrate for a circular substrate (42).

Description

1247099 九、發明說明: 【發明所屬之技術領域】 本發明係關於適合高溫應用之感測系統,且更特定言之 係關於在一 A1N基板上使用鎢作為一感測及/或加熱元件。 【先前技術】 在多種類型感測及平面加熱系統(諸如感測溫度、流體流 動速率及水平、壓力及氣體環境之系統,自測平面加熱器 及高速均句加熱器)之能力中不斷尋找改良。已找到待增強 之特徵包括較快反應時間、較強靈敏性、較高溫度能力及 低偏移。 ?溫度量測 諸如感測器之所使用之設備通常分為6類 (ICs) ; (2)高溫計;(3)電阻溫度偵測器(rti 節器;(5)熱電偶(TCs); (6)電動機械及體積 :(1)積體電路1247099 IX. DESCRIPTION OF THE INVENTION: FIELD OF THE INVENTION The present invention relates to sensing systems suitable for high temperature applications, and more particularly to the use of tungsten as a sensing and/or heating element on an A1N substrate. [Prior Art] Continuously looking for improvements in the capabilities of various types of sensing and planar heating systems such as sensing temperature, fluid flow rate and level, pressure and gas environment systems, self-testing planar heaters and high speed uniform heaters . Features that have been identified to be enhanced include faster response times, greater sensitivity, higher temperature capabilities, and lower offset. Temperature measurement devices such as sensors are generally classified into six categories (ICs); (2) pyrometers; (3) resistance temperature detectors (rti nodes; (5) thermocouples (TCs); (6) Electric machinery and volume: (1) integrated circuit

至該TC接合之電輸入(如電流), 但是確實需要電輸入來維 93277.doc 1247099 持參考接合。EMVs包括諸如金屬卷板及金屬條之裝置、測 定體積的管子及其中使用金屬/流體之膨脹/收縮來量測溫 度之球狀溫度計。 流動速率及流體水平 藉由所知為質量流動控制器之設備中之溫度感測器(通 常為RTDs)來完成氣體之精確流動速率監測及控制。在該等 "又備中’在主流動路徑周圍饋入一部分總氣流。當氣體穿 過替代路徑時,該氣體被加熱。在常壓下,每一氣體有已 去且唯之熱谷量。因此,可使用沿該替代流動路徑串聯 之2至4個/JEL度感測裔之間溫度的差別來量測及控制通過該 設備之氣體流動速率。應用包括所有需要精確控制之方 法,例如,半導體晶片製造。 對單流動感測為或一流體水平感測器而言,周圍環境 之熱容量由其組合物、狀態(氣態或液態)、密度及流經該傳 感器時之速率狀。-位槽中已知位置之自加熱溫度 感測器指示是將該槽注入至該感測器位置下方或上方亦或 指示穿過其之氣體/流體之流動速率。 壓力感測器 與本發明相關之最常用之壓力感測器為熱電偶⑽氣壓 計。使用TC氣壓計量測真空系統中之大氣壓狀讀托之 間的壓力。然@’其對來自壓力變化之表面溫度變化之靈 敏性及其高溫能力受到限制。 平面加熱器 平面加熱器能在一 基板之除邊緣處 之外的全部區域上提 93277.doc -6 - 1247099The electrical input (such as current) to the TC junction, but does require electrical input to maintain the reference junction. EMVs include devices such as metal coils and metal strips, tubes of measured volume, and spherical thermometers that use metal/fluid expansion/contraction to measure temperature. Flow Rate and Fluid Level The precise flow rate monitoring and control of the gas is accomplished by temperature sensors (usually RTDs) in devices known as mass flow controllers. In the "replacement', a portion of the total airflow is fed around the main flow path. The gas is heated as it passes through the alternate path. Under normal pressure, each gas has a depleted and only hot valley. Thus, the difference in temperature between 2 to 4/JEL degrees of sensing in series along the alternate flow path can be used to measure and control the gas flow rate through the device. Applications include all methods that require precise control, such as semiconductor wafer fabrication. For a single flow sensing or a fluid level sensor, the thermal capacity of the surrounding environment is characterized by its composition, state (gaseous or liquid), density, and rate of flow through the sensor. The self-heating temperature sensor at a known location in the bit slot indicates that the tank is injected below or above the sensor location or indicates the flow rate of gas/fluid passing therethrough. Pressure Sensor The most common pressure sensor associated with the present invention is a thermocouple (10) barometer. The pressure between the atmospheric pressure readings in the vacuum system was measured using TC air pressure. However, @' is limited in its sensitivity to surface temperature changes from pressure changes and its high temperature capability. Planar heaters Planar heaters can be applied to all areas except the edge of a substrate. 93277.doc -6 - 1247099

Thermocouples on Ceramics” 第 62頁:在 A1N晶粒上沈積相 對PtRh薄膜之Pt以用作薄膜熱電偶(TCs)。討論了相對於溫 度(至1500°C)之TC結合之偏移。 ISHM ’91 年學報 Υ·Η. Chiao 等人之 ’’Interfacial Bonding in Brazed and Cofired Aluminum Nitride” 第 460 — 480 頁:討論 了用於在AIN與包括W之幾種金屬之間連接介面之反應及 將其與連接方法(蒸或共燒(cofiring))對比。揭示了 一多層 A1N/W結構,其中由於聯鎖顆粒邊界而形成介面連接。儘 管未在本文中揭示,但是已使用該種結構作為一加熱器, 但其不具有任何感測實際溫度之機構。 專利案第6,084,221號:討論了用於平面加熱器應用之 A1N上之銀及銀合金。 專利案第6,103,146號:將由促進人11、人卜?卜?(1及1〇1混 合物及合金之應用的傳導膏組合物組成之厚膜、可筛網印 刷電路直接施加於A1N基板表面。 專利案第6,242,719號:將厚膜描述為係藉由化學氣相沈 積而在A1N上沈積。 2001年5月29日以本發明發明者之名發佈之專利案第 6,239,432號:藉由一包括\¥、界(:、\¥2€之傳導裝配層將一 SiC之IR吸收本體電連接並機械連接至一 A1N基板。 【發明内容】 本發明尋找提供一種可達到比先前感測系統較快反應時 間、較強靈敏性、較高溫度能力及較低偏移之新型感測系 統及方法。 93277.doc -8- 1247099 s在:較佳實施例中,在一 A1N基板之上提供一鎢薄膜層, 同t提供一對該鎢層施加一電致動訊號之訊號源及一感測 該鎢層對該致動訊號之回應的感測器。可在該鎢層上提供 不同抗氧化保護層,該等保護層包括金、、Au_pt 。金(在该合金上具有視情況之鎢或B2〇rSiQ2層)或p《在 - 孩Pt上具有視情況之32〇3_81卩2層)。亦可在該保護層上提供 — A1N 蓋。 ’、 在一較佳之實施例中之該鎢層包含分佈於一平面A1N基 板上之複數個傳導線。對諸如矩形之基板形狀而言,料籲 線較佳蜿蜒成型並平行。對一圓形基板而言,該等線較佳 /口各自之經線延伸並在該基板之相反極點處合併。 、‘ A1N基板上之鶴為較佳時,本發明可歸納為一 aw基 板及該基板上之一傳導層之使用,該傳導層在一預定溫度 操作範圍内具有在基板的1〇〇+/-〇 〇7之内的膨脹係數,且 其大體上不和該基板反應且大體上展示與該基板無固體溶 解性或相互擴散性。亦可將其歸納為一絕緣基板及該絕緣 _ 基板上一鎢傳導層之使用,該傳導層在一預定溫度操作範 圍内具有在該基板之1.00+/_0 07之内的膨脹係數,且其大 體上不與该基板反應且大體上展示與該基板無固體溶解性 或相互擴散性。 用於所述材料系統之應用包括:可自測其自身溫度之平 面加熱器、僅使用一單個W/A1N元件或使用一對在該流體 流動路桎中間隔之該等元件(加熱一元件,另一元件不加熱 且兩者都在其各自位置感測該流體溫度)之流體流動速率 93277.doc -9 - 1247099 感測器、可感測其是否浸入一預定流體中之流體水平感測 15 '其中該感測器之電壓/電流關係與環境氣體壓力有關之 壓力感測器及用於其中該鎢層受環境變更支配而改變其回 應特徵之環境的化學感測器。 自以下詳細敍述及該等附圖熟悉此項技術者將明瞭本發 明之該等及其它特徵及優勢。 【實施方式】 本發明提供一種用於感測溫度、流體流動速率、壓力及 化學環境條件之新穎系統及方法,且其可用作能感測其自 身溫度之加熱器,並比先前之感測器具有較高溫度能力、 較強靈敏性、較快反應時間及/或較低偏移。在該較佳實施 例中’其基於在一A1N基板上形成之一鎢(w)薄膜(通常將一 薄膜之定義為具有約為100一 10,000埃之厚度)感測器層之 上。因為A1N在330°Κ時具有約為4·4χ1(Γ6/°Κ之熱膨脹係數 並在1273〇Κ時具有約為5.3χ10-6ΛΚ之熱膨脹係數,而同時 鎮之熱知胺係數在330°Κ時約為4·6χ1(Γ6/°Κ且在1273CK時 約為5·1χ1〇-6/〇Κ,所以該等材料之組合尤其有利。因此該 等兩個材料之熱膨脹係數彼此非常接近,其允許在一廣泛 溫度範圍内的高度結構穩定性。Α1Ν基板具有絕緣性,同時 鎢通常為導電性且具有以所知方式隨溫度而改變之電阻係 數。1982年重版之American Institute of Physics Handbook, 第二版中第9-41頁中討論了鎢之溫度一電阻係數特徵,其 内容以引用方式倂入本文。 當W/A1N為一較佳材料組合時,該材料系統可歸納為在 93277.doc -10- 1247099 基板上具有傳導層的AIN基板或在基板上具有鎢層的絕緣 基板,在任一情形下之傳導層在一預定溫度操作範圍内具 有在基板之1.00+/-0.07之内的膨脹係數,且大體上不與該 基板反應且大體上與該基板不具有固體溶解性或相互擴散 性。 A1N具有一約比陶瓷A12〇3之熱傳導率高十倍之約為 1+7-2.4 W/cfK的熱傳導率,當其自身被厂相鄰鎢層加熱 日守,孩雨傳導率使其作為一加熱器很有效率。A1N亦展示一 所需之對與諸如鎢之金屬產生化學發應的高抗性。其在約 25〇〇它時昇華並依賴於其環境而具有約為自ll5(rc至 180(TC之上部連續使用溫度,並使其在高溫範圍内適用。 鎢具有約為341(TC之溶化溫度且已知在18〇(rc以下不與 A1N起化學反應,其亦有利於與Am之組合物中的高溫 作。 '、 在惰性環境中於約1880°c之溫度下鎢與A1N之間的完全 不存在或不可測之慢速化學反應、㈣溶解性及相互擴散 性確保鹤電路之截面不因與A1N基板起化學反應而減少,其 亦確保該A1N基板表面不變得具有傳導 詩:著^電路之方法之裂縫的A1N基板表面 -乍度範圍内之非常匹配的溫度膨脹係數確保了在熱循 環中鎢電路不在該A1N基板剝離。 … 如以下將進一步詳細描述,可在該鎢電路層上提供由 或Au-Pt合金組成之額外電路層以執行三個功能:⑴ 保4 5亥鎢電路不被氧化;(2)將A1N基板上之電路與該等蓋 93277.doc 1247099 «在起㈣成—具有在頂部及底部暴露之電絕緣層 \㈣多層電路;(3)為電路路徑提供額外截面面積。 /亥等額外屯路層及鎢(或wc,當碳與鎢反應以為另一層 =接合劑時)之間的兼容性f求包括:⑴至最大操作溫度 間具有少量或無化學反應;⑺其在有限相互擴散及有 限固體溶解性下接人,蕤士卢士孤 卜接口猎此在相對之面對介面處或其附近 ”持月,、、、貞區別,(3)限制其間之最大固體溶解性以使盆在最 大操作溫度時不形成—同形或僞同形相位圖;⑷其彼此不 形成化合物’·及(5)其溶化溫度超出該最大操作溫度。需求i ;4確保該等額外電路層不料(或—破壞其介面並確保 忒組合電路電阻不在可操作情況下偏移。 亦如以下之進—步詳細描述,—些實施例包括领石夕酸鹽 混合物(B203 + Sl〇2)之封裝。以不反應之形式施加該臀酸 孤此口物且接著藉由將該結構加熱至至少丨〇⑻。C來使其反 應。該反應後之混合物為一黏合至可氧化之表面並覆蓋不 可氧化之層的玻璃。其不消&gt;耗其接觸之電路層且保持為一 電絕緣體。 可藉由在一 A1N基板或蓋之邊緣上及周圍施加或沈積之 額外電路材料或藉由在該基板或蓋令之通路内施加或沈積 之額外電路材料自該電路層自身之延伸區域部分形成向該 嫣電路層施加電訊號之電極。 可為導線或帶附著而在該鎢電極之頂部上提供額外電極 層。該等額外層可包括碳、鉑或金。碳提供一在加熱至約 700t以上時將W接合至W或將W接合至M〇的熱活性接合 93277.doc -12- 1247099 材料,在該接合材料處藉由與W及Mo反應來消耗碳以形成 在高於1 800°C溫度時仍保持完整之碳化金屬接合介面。鉑 提供一於其上可焊接Pt或Au之基座,該接合將在等於在焊 接過程中形成之Pt或Au-Pt合金之熔點的溫度下保持完 整。金提供一於其上接合Au或焊接Pt之基座,該接合將在 等於在焊接過程形成之Au或Au-Pt合金之熔點的溫度下保 持完整。 該額外電極層亦可包括分層之Pt及Au或Au-Pt合金。其提 供一於其上接合Au或焊接Pt之基座。 參與蒸、接合或焊接處理之該等電極材料的厚度應至少 為該引線之直徑或該引導帶厚度的0.05倍。可藉由A1N暴 露、封裝或覆蓋該等電極。 處理事項 與W接觸之A1N基板或蓋表面:藉由靜電力及藉由貫穿 A1N表面之裂縫將W膜固持在A1N表面。儘管難於確定數 量,但是觀察所得結果指示在所有陶瓷A1N表面(平均粗糙 度2 2微英吋(0.05 Mms))上獲得良好W黏著。然而,W之最 大厚度直接與A1N平均表面粗糙度成比例。A1N表面上之W 之最大厚度約為該平均表面粗糙度的100倍。 在A1N基板及蓋上之施加及其上之’’形成&quot;:可使用若干氣 相沈積技術(諸如RF/DC濺鍍、RF/DC共同濺鍍、電子束蒸 發及化學氣相沈積(CVD))以正確結合來將W施加至A1N基 板。由於藉由物理接合而不是化學接合來產生黏著,所以 在W沈積中A1N表面溫度並不重要。 93277.doc -13- 1247099 當沈積時,除非藉由CVD沈積否則W膜將不具有理論密 度。可藉由熱退火增加膜密度並減少顆粒邊界區域。當密 度或顆粒邊界區域對保護該W/A1N介面使之免受額外電路 層金屬而言係重要時,應在施加額外電路層金屬之前將w 退火。退火溫度範圍為800°C至1400°C,密度及顆粒生長視 溫度所處時間而定。退火氣氛應為真空或惰性(Ajt,N2)。Thermocouples on Ceramics” Page 62: Pt is deposited on A1N grains relative to PtRh films for use as thin film thermocouples (TCs). The offset of TC binding relative to temperature (to 1500 ° C) is discussed. ISHM '91 Journal of Υ·Η. Chiao et al.''Interfacial Bonding in Brazed and Cofired Aluminum Nitride pp. 460-480: discusses the reaction for connecting interfaces between AIN and several metals including W and Connection method (steaming or cofiring) comparison. A multilayer A1N/W structure is disclosed in which interface connections are formed due to interlocking grain boundaries. Although not disclosed herein, such a structure has been used as a heater, but it does not have any mechanism for sensing the actual temperature. Patent No. 6,084,221: discusses silver and silver alloys on A1N for planar heater applications. Patent Case No. 6, 103, 146: Will it be promoted by people 11, and people? Bu? A thick film, screenable printed circuit consisting of a conductive paste composition of a mixture of 1 and 1 〇1 and an alloy is applied directly to the surface of an A1N substrate. Patent No. 6,242,719: The thick film is described as being by chemical vapor phase Deposition and deposition on A1N. Patent No. 6,239,432 issued on May 29, 2001 in the name of the inventor of the present invention: a SiC comprising a conductive assembly layer including \¥, boundary (:, \¥2€) The IR absorbing body is electrically connected and mechanically connected to an A1N substrate. SUMMARY OF THE INVENTION The present invention seeks to provide a faster response time, greater sensitivity, higher temperature capability, and lower offset than previous sensing systems. A novel sensing system and method. 93277.doc -8- 1247099 s In the preferred embodiment, a tungsten thin film layer is provided over an A1N substrate, and a pair of tungsten layers are applied to apply an electrical actuation signal. a signal source and a sensor that senses the response of the tungsten layer to the actuation signal. A different oxidation protection layer may be provided on the tungsten layer, the protective layer comprising gold, Au_pt, gold (on the alloy Depending on the case of tungsten or B2〇rSiQ2 layer) or p - a layer of 32 〇 3_81 卩 2 on the Pt.). An A1N cover may also be provided on the protective layer. ' In a preferred embodiment, the tungsten layer is distributed on a planar A1N substrate. a plurality of conductive lines. For a shape of a substrate such as a rectangle, the material lines are preferably formed and parallel. For a circular substrate, the lines are preferably/exposed to each other and extend over the substrate. The opposite pole is merged. When the 'A1N substrate crane is preferred, the invention can be summarized as an aw substrate and a conductive layer on the substrate, the conductive layer having a substrate on a predetermined temperature operating range. a coefficient of expansion within 1 〇〇 〇〇 〇〇 7 and which does not substantially react with the substrate and generally exhibits no solid solubility or interdiffusion with the substrate. It can also be summarized as an insulating substrate and The use of a tungsten-conducting layer on the substrate, the conductive layer having an expansion coefficient within 1.00+/_0 07 of the substrate within a predetermined temperature operating range, and which substantially does not react with the substrate and substantially Demonstrate no solid solubility with the substrate Interdiffusion. Applications for the material system include: a planar heater that can self-measure its own temperature, use only a single W/A1N component, or use a pair of such components spaced in the fluid flow path ( Fluid flow rate for heating one element, the other element is not heated and both sense the temperature of the fluid at its respective position 93277.doc -9 - 1247099 Sensor, fluid that can sense whether it is immersed in a predetermined fluid Level sensing 15' is a pressure sensor in which the voltage/current relationship of the sensor is related to ambient gas pressure and a chemical sensor for an environment in which the tungsten layer is subject to environmental changes to change its response characteristics. These and other features and advantages of the present invention will become apparent from the <RTIgt; [Embodiment] The present invention provides a novel system and method for sensing temperature, fluid flow rate, pressure, and chemical environmental conditions, and which can be used as a heater capable of sensing its own temperature and is more sensitive than previous sensing The device has higher temperature capability, greater sensitivity, faster response time, and/or lower offset. In the preferred embodiment, it is based on the formation of a tungsten (w) film (typically a film defined as having a thickness of about 100 to 10,000 angstroms) on an A1N substrate. Since A1N has a thermal expansion coefficient of about 4·4χ1 (Γ6/°Κ at 330°Κ and a thermal expansion coefficient of about 5.3χ10-6ΛΚ at 1273〇Κ, while the thermal amine coefficient of the town is at 330°Κ The time is about 4·6χ1 (Γ6/°Κ and about 5·1χ1〇-6/〇Κ at 1273CK, so the combination of these materials is particularly advantageous. Therefore, the thermal expansion coefficients of the two materials are very close to each other, Allows for a high degree of structural stability over a wide temperature range. The substrate is insulating, while tungsten is generally electrically conductive and has a resistivity that varies with temperature in a known manner. The American Institute of Physics Handbook, reprinted in 1982 The temperature-resistance characteristics of tungsten are discussed in pages 2–41 of the second edition, the contents of which are incorporated herein by reference. When W/A1N is a preferred material combination, the material system can be summarized as 93277.doc -10- 1247099 An AIN substrate having a conductive layer on a substrate or an insulating substrate having a tungsten layer on the substrate, in either case the conductive layer has an expansion within 1.00 +/- 0.07 of the substrate within a predetermined temperature operating range Coefficient, and generally Does not react with the substrate and has substantially no solid solubility or interdiffusion with the substrate. A1N has a thermal conductivity of about 1+7-2.4 W/cfK which is about ten times higher than the thermal conductivity of ceramic A12〇3. When it is heated by the adjacent tungsten layer of the factory, the child's rain conductivity makes it very efficient as a heater. A1N also exhibits a high resistance to chemical reactions with metals such as tungsten. It sublimes at about 25 〇〇 and depends on its environment and has a temperature of approximately ll5 (rc to 180 (continuous use temperature above the TC and makes it suitable for use in the high temperature range. Tungsten has a solubility of about 341 (TC) The temperature is also known to be 18 〇 (the following rc does not chemically react with A1N, which is also advantageous for high temperatures in the composition with Am. ', between tungsten and A1N at a temperature of about 1880 ° C in an inert atmosphere The slow chemical reaction, (4) solubility and interdiffusion, which are completely absent or unmeasurable, ensure that the cross section of the crane circuit is not reduced by chemical reaction with the A1N substrate, which also ensures that the surface of the A1N substrate does not become conductive: The surface of the A1N substrate with the crack of the ^ circuit method - the temperature range The very well-matched temperature expansion coefficient within the thermocouple ensures that the tungsten circuit does not peel off the A1N substrate during thermal cycling. As will be described in further detail below, an additional circuit layer composed of or an Au-Pt alloy can be provided on the tungsten circuit layer. Perform three functions: (1) protect the 4 5H tungsten circuit from oxidation; (2) place the circuit on the A1N substrate with the cover 93277.doc 1247099 «In the beginning (four) - have the electrical insulation layer exposed at the top and bottom\ (4) Multi-layer circuits; (3) Provide additional cross-sectional area for circuit paths. Compatibility between additional ruthenium layers such as hai and tungsten (or wc, when carbon reacts with tungsten to form another layer = cement) f includes: (1) little or no chemical reaction between the maximum operating temperatures; (7) In the case of limited interdiffusion and limited solid solubility, the gentleman is connected to the interface at or near the opposite interface, holding the difference between the moon, the, and the ,, and (3) limiting the maximum solid solubility between them. So that the basin does not form a homomorphic or pseudo-homomorphic phase diagram at the maximum operating temperature; (4) it does not form a compound with each other' and (5) its melting temperature exceeds the maximum operating temperature. Demand i; 4 ensures these additional circuit layers Unexpectedly (or - destroying its interface and ensuring that the combined circuit resistance is not offset in the case of operation. Also as described in the following paragraphs - some examples include a mixture of lead salts (B203 + Sl〇2) Encapsulating. The glutamic acid is applied in a non-reactive form and then reacted by heating the structure to at least 丨〇(8). C. The mixture after the reaction is bonded to an oxidizable surface and covered. Non-oxidizable a layer of glass. It does not have to be in contact with the circuit layer and remains as an electrical insulator. Additional circuit material can be applied or deposited on and around the edge of an A1N substrate or cover or by the substrate or cover An additional circuit material applied or deposited in the via is formed from an extended portion of the circuit layer itself to form an electrode for applying an electrical signal to the germanium circuit layer. Additional electrode layers may be provided on top of the tungsten electrode for wire or tape attachment The additional layers may comprise carbon, platinum or gold. The carbon provides a thermally active bond 93277.doc -12-1247099 material that joins W to W or joins W to M〇 when heated to above about 700 t. The bonding material consumes carbon by reacting with W and Mo to form a carbonized metal bonding interface that remains intact at temperatures above 1 800 ° C. Platinum provides a pedestal on which Pt or Au can be soldered, the bonding It will remain intact at a temperature equal to the melting point of the Pt or Au-Pt alloy formed during the soldering process. Gold provides a pedestal on which the Au or solder Pt is bonded, which will be equal to the Au formed during the soldering process or Au-Pt alloy The temperature remains constant at the temperature of the melting point. The additional electrode layer may also comprise a layered Pt and Au or Au-Pt alloy. It provides a pedestal on which the Au or solder Pt is bonded. Participation in steaming, bonding or soldering processes The thickness of the electrode material should be at least 0.05 times the diameter of the lead or the thickness of the guiding tape. The electrodes can be exposed, encapsulated or covered by A1N. The A1N substrate or cover surface that is in contact with W: by electrostatic force And holding the W film on the surface of the A1N by cracks penetrating the surface of the A1N. Although it is difficult to determine the amount, the observation results indicate that good W adhesion is obtained on all ceramic A1N surfaces (average roughness of 2 2 μm (0.05 Mms)). However, the maximum thickness of W is directly proportional to the average surface roughness of A1N. The maximum thickness of W on the surface of A1N is about 100 times the average surface roughness. Application on the A1N substrate and cover and its 'formation': several vapor deposition techniques (such as RF/DC sputtering, RF/DC common sputtering, electron beam evaporation, and chemical vapor deposition (CVD) can be used. )) Apply W to the A1N substrate with the correct combination. Since adhesion is produced by physical bonding rather than chemical bonding, the A1N surface temperature is not important in W deposition. 93277.doc -13- 1247099 When deposited, the W film will not have a theoretical density unless deposited by CVD. The film density can be increased by thermal annealing and the particle boundary region can be reduced. When the density or grain boundary region is important to protect the W/A1N interface from additional circuit layer metals, w should be annealed prior to application of additional circuit layer metal. The annealing temperature ranges from 800 ° C to 1400 ° C, and the density and particle growth depend on the time of the temperature. The annealing atmosphere should be vacuum or inert (Ajt, N2).

當需要藉由”形成”來促進較上層之接合時,可將鎢膜部 分或全部轉化成WC。在該處理中,如藉由濺鍍、物理氣相 沈積或CVD或石墨之物理施加(例如篩網印刷)來沈積或退 火w薄膜一樣施加碳。藉由熱感生擴散將…膜轉變成 (’’形成&quot;)。形成溫度範圍為80〇^:至14〇〇。(::,更佳具有較高 之溫度。該”形成”氣氛應為真空或惰性(Ar、N2)。對本發Z 之目的而σ ,該等申睛專利範圍中提及之,,W&quot;亦包括 WC ’儘官已發現wc^bw具有較低熱膨脹係數且因此除了 在適當位置接合一重疊層之外並不如〜一般適用。When it is desired to "form" to promote bonding of the upper layer, the tungsten film may be partially or completely converted into WC. In this treatment, carbon is applied as in the case of depositing or annealing a film by sputtering, physical vapor deposition or physical application of CVD or graphite (e.g., screen printing). The film is transformed into (''formed&) by thermal induced diffusion. The formation temperature range is from 80 〇^: to 14 〇〇. (::, preferably has a higher temperature. The "forming" atmosphere should be vacuum or inert (Ar, N2). For the purpose of the present Z, σ, as mentioned in the scope of these patents, W&quot; Also included is the WC's officially found that wc^bw has a lower coefficient of thermal expansion and therefore is not as suitable as the general application except for joining an overlapping layer in place.

若待藉由額外電路層金屬層來覆蓋W,則沈積w之最小 較佳厚度等於A1N基板表面之平均粗糙度。若w僅為包含該 電路徑之膜’則由以下兩需求之較強者判定其最小;T 度··⑴W之後處理厚度應至少為該剔表面之平均粗縫度 二……或⑺其厚度乘以其寬度(截面面積)應足夠提供該If W is to be covered by an additional circuit layer metal layer, the minimum preferred thickness of the deposition w is equal to the average roughness of the A1N substrate surface. If w is only the film containing the electrical path, then the minimum of the following two requirements is determined to be the minimum; after T degrees · (1) W, the thickness of the treatment should be at least the average roughness of the surface of the picking surface two ... or (7) its thickness multiplied The width (sectional area) should be sufficient to provide the

…所而之电流處理能力。當沒有關於最小W 厚度之基本限制時,低質量輻射加熱器或電路應用通常不 需要大於1 〇微米之厚度。 額外電路層CACL)金屬··該如經施加/沈 積之ACLs可由一 93277.doc -14- 1247099 個或多個層組成,順序地施加/沈積每一層。可藉由著色、 篩網印刷、電鍍或氣相沈積(技術視材料而定)來施加ALC 之每一層。 經處理之ACL可為一由元件或合金或兩者之分級組合物 組成之單或多層膜。經處理之ACL可為如經施加/沈積的或 可將其熱處理以重新分配膜組合物。儘管在熱處理中可在 該ACL之一個或多個(但非所有)層中發生溶化,但是該所得 合金在相同處理溫度下必須為固體。舉例而言,可藉由將 一 Au/Pt多層結構加熱至一超出Au之溶化溫度但低於該所 需合金之溶化溫度的溫度來形成Au-Pt合Au。在該情況中僅 有Au溶化,因此其被Pt很快消耗以形成一具有較高溶化溫 度之合金。 根據該(等)經施加/沈積之ACL金屬之厚度應可使ACL之 後處理厚度等於或大於A1N表面平均粗糙度。該如經施加/ 沈積之ACL之最小較佳厚度為5xl0_6 cm。可藉由W+ACL 截面面積足夠提供感測器或加熱器所需之電流處理能力之 需要來判定ACL之最小厚度。藉由其給予與A1N相關之電路 之線及藉由W和ACL之間膨脹係數差異來限制ACL之最小 厚度。迄今所執行之試驗調查顯示該上部厚度限制比W厚 度大6 0倍。 碳反應接合:碳提供一熱活性接合材料,當加熱超過約 700°C時其將W/Mo線/帶接合至W電極,其中藉由與W及Mo 發應消耗碳以在W與W或W與Mo之間形成一 WC或Mo-碳化 物接合介面,在超出1800°C之溫度下該接合仍保持完整。 93277.doc -15- 1247099 參。反應接合處理之電極材料之厚度應足夠消耗所有碳。 該接合處理需要c、w^。相互擴散以使得完成接合進行 =速率直接與溫度成比例。參與銅焊、接合或谭接處理之 电桎材料之厚度應為該電線之直徑之〇 · 〇 5倍或為該帶或壓 “之厚度的0.05倍。根據試驗調查料,其為功能接合 =取小f度需求。然而,在該比率下很難達到強接合(低良 推薦該電極厚度至少為該電線直徑枝丨倍或至少為帶 厚度之G.1倍,此係由於良率較高並改良了該接合之粗链...the current processing capability. Low quality radiant heaters or circuit applications typically do not require thicknesses greater than 1 〇 microns when there is no fundamental limit on minimum W thickness. Additional Circuit Layer CACL) Metal The ACLs as applied/deposited may consist of a layer of 93277.doc -14-1247099 or layers, which are applied/deposited sequentially. Each layer of ALC can be applied by coloring, screen printing, electroplating, or vapor deposition (technical depending on the material). The treated ACL can be a single or multilayer film comprised of a graded composition of elements or alloys or both. The treated ACL can be as applied/deposited or it can be heat treated to redistribute the film composition. Although melting may occur in one or more (but not all) layers of the ACL during heat treatment, the resulting alloy must be solid at the same processing temperature. For example, Au-Pt-bonded Au can be formed by heating an Au/Pt multilayer structure to a temperature that exceeds the melting temperature of Au but below the melting temperature of the desired alloy. In this case only Au is dissolved, so it is quickly consumed by Pt to form an alloy having a higher melting temperature. The thickness of the ACL metal to be applied/deposited should be such that the post-treatment thickness of the ACL is equal to or greater than the average roughness of the A1N surface. The minimum preferred thickness of the applied/deposited ACL is 5 x 10 6 cm. The minimum thickness of the ACL can be determined by the W+ACL cross-sectional area sufficient to provide the current handling capability required by the sensor or heater. The minimum thickness of the ACL is limited by the line to which the circuit associated with A1N is applied and by the difference in expansion coefficients between W and ACL. Tests conducted so far have shown that the upper thickness limit is 60 times greater than the W thickness. Carbon reactive bonding: carbon provides a thermally active bonding material that bonds the W/Mo wire/band to the W electrode when heated above about 700 ° C, wherein carbon is consumed by W and Mo to be in W and W or A WC or Mo-carbide bonding interface is formed between W and Mo, and the bonding remains intact at temperatures exceeding 1800 °C. 93277.doc -15- 1247099 Participation. The thickness of the electrode material for the reactive bonding treatment should be sufficient to consume all of the carbon. This bonding process requires c, w^. Interdiffusion so that the bonding is completed = the rate is directly proportional to the temperature. The thickness of the electrode material involved in brazing, joining or tanning shall be 5 times the diameter of the wire or 0.05 times the thickness of the tape or pressure. According to the experimental investigation, it is a functional joint = Take a small f-degree requirement. However, it is difficult to achieve strong bonding at this ratio (low-recommended, the electrode thickness is at least G.1 times the wire diameter or at least the strip thickness, which is due to higher yield. And improved the thick chain of the joint

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Au與Pt合金接合:—pt電極層提供—於其上焊接或焊 接/接合/銅焊如線/帶之基座;在等於pt或接合過程中形成 之Au Pt 口金之熔點之溫度時該線/帶及該電極間形成之接 合將仍保持Μ。—Au電極層、分層之pmAu電極層及 Au_Pt合金電極層各自提供一於其上焊接/接合Μ線/帶或焊 接/銅焊Pt線/帶之基座;在等於Au或接合過程中形成之 Au Pt a至之溶點之溫度時該線/帶及該電極間形成之接合 將仍保持完整。參與銅焊、接合或焊接處理之該等電極材 料之厚度與於碳反應接合相似。 應藉由接合、銅焊或焊接將該等引導線/帶附著於該等電 極墊。引導線材料之膨脹係數應在後處理電極層之組合物 膨脹係數的兩倍以内。可壓扁該等導線被接合/焊接/銅焊至 黾極之邛刀在5亥種情況中垂直其扁平表面之導線直徑為 在判定電極層之最小厚度中使用的合適直徑。 圖1說明根據本發明之一感測器,其中較佳地在A1N基板4 93277.doc -16- 1247099 將該等鎢電路進一步接合至該基板的封裝14。 該硼矽酸鹽混合物由45重量%之82〇3 + 55重量%iSi02組 成。將其在1000 °C下在空氣申反應5分鐘。 在圖5所示之實施例中,在圖4中未反應之B2〇3 + Si〇2頂部 上放置一 A1N盍16且熱反應該所得結構以在合適額外保護 處接合該A1N蓋16。封装14及蓋16均將該等電極墊6暴露以 接收用來向該鎢電路施加一電訊號之導線或帶。在1〇〇〇它 下在空氣中反應該硼矽酸鹽5分鐘以在合適處接合該蓋。 在圖6所示之實施例中,施加au與Pt層18與2〇以作為圖i 中所示之完成結構上之該鎢層上的薄膜;pt或可為頂 部層。其結果為一在該A1N基板4上之三層電路。接著熱反 應該組合體以形成一兩層電路,其具有一相似於圖3所示之 組態’其具有包含鶴之較低層及包含一具有由Au與pt層之 相關厚度判定之Au_Pt合金電路之頂部層。 在一示範中,在該A1N基板上濺鍍沈積一 1〇〇〇埃鶴層,接 著係100埃Au及1000埃Pt濺鍍沈積層。根據圖!中所述在電 極準備期間完成形成該Au-Pt合金之熱反應。 圖7及8中說明另一具有一 ACL及一保護A1N蓋之實施 例。先參看圖7,如圖6,提供一基板組合體,其具有在基 板4之鎢層2上之Ail及Pt層18及20(不需以該順序)。提供一 A1N蓋22,其具有由鎮層2’、Au及Pt(或Pt及Au)層1 8,及20, 組成之相似三層導體結構,所有層都具有與基板4上之層相 同之幾何。將蓋22定位於基板4上並與該等不同層對準。接 著熱反應該組合體以形成如圖8所示之三層電路,該三層電 93277.doc -19- 1247099 路具有分別S品近基板4及蓋24之鶴® 2 # &lt;螞層2及2亚將一 Au_pt合金 電路層24夾在其中。在一示筋巾 * 牡不乾中,在10⑻埃濺鍍沈積之鎢 層上濺鍍沈積100埃厚之Au層及1〇〇〇埃厚之声。 圖9說明自熱反應圖6所示結構所得之結構,曰其在該鶴電 路層2上具有-Au-Pt合金電路層26。以與圖4之封裝14相似 之方式在3結構上形成一删秒酸鹽封裝2 8。 圖1〇說明-實施例,其十藉由A1N蓋30進一步保護圖9之 結構。該蓋位於合適位置處,在⑽代下在空氣中反應該 哪矽酸鹽5分鐘以接合在該蓋上。 本發明可有利地用於一平面加熱器。圖u說明一形成於 一矩形(包括正方形)A1N基板上之加熱器,該基板在沒有 ACLs的情況下作為一可如上所述製造之鎢加熱元件之基 座。形成該鎢層使其較佳為一系列大體上平行、蜿蜒成二 之線34,該等線平行且藉由端子條%在該基板之相對末端 處連接,且較佳地在該陣列之相對角處提供電極%。 該蜿蜒.形狀在全部A1N基板區域(除了其邊緣)上提供均 勻加熱並導致在快速熱傾斜中更均勻地 一以™秒之速率極快上升而= 板。右该電路線筆直,則初次加熱在每一線之中心及在其 終端之180。轉向處最快速發生,纟由於當熱量極快傾斜時 之熱梯度平行而將該基板置於被破壞之危險中。 對一薄(厚度為0.01英吋至〇〇14英吋⑺〇25釐米至〇 〇% 釐米))、低質量A1N基板而言,線34之寬度應不超出英吋 (0.25屋米)且該等線之間的間隔應均勻且不超出〇·们英吋 93277.doc -20- 1247099 (0.18釐米)以確保越過線之間之間隔的熱梯度將不會導致 基板破壞。 垂直於該線傳導路徑之一蜿蜒之線的峰與穀之間的距離 應不超出該線自身之寬度。應彎曲該等線而不形成尖銳之 角。平行於該線傳導路徑之該等線峰與穀之間的距離應不 大於1英吋(2.5 cm)以預防在快速加熱中基板破裂,較短之 距離可在快速加熱中在該基板表面上提供更均勻加熱。 該等線之組合電阻為一單線之電阻除以該圖案中線之總 數量再加上一電極條之電阻。平行傳導線允許以合適電壓 及薄膜線(100 — 1〇,〇〇〇埃厚)快速加熱至高溫。 與圖11中提供之端子條36—起,該等鎢線不僅幾何平行 且電平行。可在每一線之相對末端處用單獨電極替換該等 端子條36,但其非所需。將電極38置於該基板之相對角處 以保持越過不同線而下降至低位準之電壓中的任何變化。 在圖12所述之一替代實施例中,在每一電極條%上提供 多個導線端子4G並使其正好彼此相對,且與其服務之線相 關(每一電極服務不多於兩條線)。 圖13說明一用於一圓形基板42之較佳鎢線圖案,其確保 在高溫下處於相對處之電極44之間的電場強度不超出該 A1N基板之介電分解強度;超出該介電分解強度可導致該基 板破裂或損壞。該基板之介電強度隨著溫度增加而減少且 其預汁在1300C日守為約2000伏/英对(787伏/釐米)。 鎢線46被彎曲且其大體上沿著各自之經線延伸,該等經 線在包含電極44之相反極處合併。該等線關於穿過極電極 93277.doc -21 - 1247099 之中心線48對稱。為確保功率沿著每一線之長度均勻耗 散,儘官當該等線自電極可發出可交叠,但是垂直於其傳 導路徑之線寬度應保持不變。 由於自中心線48具有不同距離之線有不同長度,所以與 其它線相關之每-線之寬度應朝向該中心線遞減以使每一 線每單位長度之功率耗散接近其它線每單位長度之功率耗 散。其確保將該A1N基板均勻加熱且該基板不會由於熱梯度 而損壞。為確保垂直於該線路徑之線之間的熱梯度不會導 致一薄、低質量A1N基板損壞,該等線之中點間的最大間隔 應不超出0.07英时(0._米)。線之間的間隔距離不必相同 :應關於中心線48對稱。對高於戰之加熱器溫度而 吕,線中點之間的間隔應小於〇 〇7英吋(〇18釐米)。 圖14及15說明本發明對一溫度感測^、一單端加熱器或 一可感測自身溫度之加熱器的應用。 在圖14中,如圖卜一電壓源5〇施加一電壓使其越過一沈 積於A1N基板4之上之鎢傳導膜2。一安培計52監測通過該鎢 膜之電流。t用於感測周圍環境之溫度時,㈣低電壓以 施加一不會顯著加熱該鎢膜之致動訊號。根據鎢電阻之已 知溫度係數,從而藉由其周圍環境之溫度判定該膜之電 阻。可藉由經施加電壓除以所測電流來判定該膜之電阻從 而判定周圍環境之溫度。由該安培計52感測之該鎢膜對一 已知經施加電壓的回應隨著周圍溫度而改變。可在該鎢膜 中持績且不導致該膜顯著加熱之電流位準係由若干因素判 疋如周圍溫度、膜厚度、表面面積與形狀及環境之熱容 93277.doc -22- 1247099 量。通常,一旦達到加熱臨限值,則該膜將經受隨電流水 平之持續增加而迅速增加之加熱。當周圍環境溫度 該加熱臨限值增加。 當用作一開端加熱器時,施加一較高電壓位準。可將該 系統預隸準至至少接近—可自給定施加電壓位準所得^ 加熱量且不需要安培計52。 為作為一可感測自身溫度之加熱器來操作,將安培計μ 添加回該電路以感測通過該鶴層之電流。可藉由使用電塵 與電流位準及判定自其中操作該單元之m電阻曲線 之溫度的該膜之已知幾何來精確判定該膜之溫度。 圖15之系統類似於圖14之系統,但並非施加電壓使其越 過該鎢膜之並感測所得電流,而是使用電流源54驅動二穿 過該膜2之致動電流並使用伏特計%感測越過該膜之所得 電壓。可以與圖14相同之方式再次判定該膜乏溫度。 量測如圖1所示之一結構之溫度一電阻特徵並與圖“所 示之鎢之已知理論電阻—溫度曲線58對比。可藉由空心圓 6〇指示在流動Ar環境中所得之量測結果並追蹤非常接近 14〇〇°C之量測臨限值之理論曲線。在空氣中所得之量測追 蹤約為26(TC之溫度的理論曲線,超過該溫度其由辟該鎢之 氧化而開始脫離該理論曲線。藉由實心圓62指示在空氣環 境中所得之量測。 在一水冷溶凝石英管中執行圖16之沿試驗。在一 AW片 上放置原型感測斋,其位於一 RF加熱石墨感受器上。自兩 個感測器電極中的每一個延伸之導線穿過一 〇型環密封延 93277.doc -23- 1247099 伸至用於對感測裔提供不變電流輸入之精確電壓及電流 源亚延伸至一用於量測該感測器之輸出電壓的萬用表。據 佗其為第一次測出一鎢薄膜之靈敏性。可使用圖1 6中陳述 之貝料來校準一已知截面及長度之鎢薄膜來用作溫度感測 器。 在一線球接合器之加熱器夾盤上執行空氣中之測試,其 中原型感測器夾在該加熱器夾盤表面上。該等感測器之頂 部及側面使用矽質棉絕緣。使用自顯微操控器延伸並壓縮 地連接至感測器電極之金探針來製造至感測器電極之電接 觸。使用施加電流與所量測之感測器輸出電壓及一來自波 形示蹤器之施加電壓€從該波形示蹤器讀取之電壓越過該 等感測器且電流穿過該等感測器)進行雙線電量測。 亦測試圖11所示之類型的平面電熱器。其尺寸為4 25 in. χ4·25 ΐη·χ0·014 in•厚(10·8 cmxl〇.8 cmx0.036 cm)。在約 500 C %獲得最大加熱速率且最大溫度約為15〇〇它,其兩者 均被有用功率限制。在圖17之面積功率密度相對溫度之曲 線中表現該所偵測之每單元A1N基板面積之功率,同時在圖 18之體積功率密度相對溫度之曲線中表現該所得之每單元 A1N基板體積之功率。 亦可藉由里測一自加熱感測器溫度中之變化來使用本發 明’該❹】器位於沿該流動路徑4 ’且既可浸入該流體中 亦可接觸該流動路徑壁。在圖19之說明中,藉由量測—本 文所述類型之位於沿流動路徑處且既可浸入該流中亦可接 觸該流動路徑壁68之自加熱感測器66來感測一氣體或流體 93277.doc -24- 1247099 (由蔚頭64指示)之流動速率。在本文所述之本實施例及其後 之實^例中,說明了致動訊號係由一可調整電流源70提 七、其中伏特計72感測該感測器之電壓回應,其依次對應 該感測器電阻從而對應該流體溫度。然而,可提供一電壓 來作為致動訊號並感測所得電流。藉由對比所感測之溫度 /、在V 動速率日守之溫度並考慮該流體之熱容量則可判定 該流動速率。 在圖20所忒明之差示流動速率感測器中,本文所述類型 之兩個或兩個以上感測器74, 76沿流體流動路徑64串聯。 藉由量測感測器之間的溫度差異來感測流動速率。在零流 動時,藉由自電流源70,至代表已知溫度之電阻的已知電流 (或已知電壓)來電阻地自加熱上游感測器74。藉由一小許多 之非自加熱電流或電壓偏壓(流)下游感測器76。可自一普通 電流源或相等地自如所示之一對獨立電流源7〇,提供致動電 流。該流體流動自上游自加熱感測器74移除熱量並將其中 一些熱量釋放至下游感測器76。越過各個該等感測器之電 壓中之變化通過該氣體或流體之熱容量與流動速率相關。 可在一平行該主流流動路徑之管道中使用該類型之差示流 動速率感測以判定通過該路徑之流動速率。 圖21說明本發明對一流體水平感測器之應用,其中將根 據本發明之感测το件66安置在一流體容器78内或與該容器 之外壁接觸之固定位置處。一在該容器中之流體8〇上升及 下降導致感測器66替代地浸入該流體或自該流體8〇清除。 該感測器緊罪之環境之熱容量視該流體水平是否已上升至 93277.doc -25- 1247099 足夠沈浸該感測器而定。當該感測器在一容器之已知水平 處且其用作一如上所述之自加熱溫度感測器時,可藉由感 測可多快速地自該感測器撤走熱量來判定該感測器是否浸 入在流體中。當以一流體感測器形式描述本應用時,其亦 可用於偵測至少在一最小密度水平上在一密封容器中是否 存在氣體。 當將本發明應用至上述流動速率或流體水平感測應用 時,本發明之主要優勢在於更快之回應時間(與高基板熱傳 導性相關)、較強靈敏性(亦與高基板熱傳導性相關)及相對 較低或無偏移(與W感測電路及A1N基板之間的小膨脹係數 錯配有關)。 在圖22中,使用本發明之該感測器66來感測密封容器。 中之氣體壓力。可藉由判定所需之維持越過該感測器之特 定電壓之電流或所需之維持越過該感測器之特定電流之電 壓來感測该容器中之壓力。該資料可與該容器中具有已知 熱容量之氣體的壓力/密度相關,該容器可為一真空室。調 整圖22中所示之電流源70以維持一如被伏特計72所感測之 越過感測1§之特定電壓位準。藉由電流源所提供之壓力計 84來說明電流位準向容器中壓力位準之轉化。本發明啓用 一比目前確實可用之熱電偶更靈敏之電壓、電流感測且因 此啓用一更靈敏之壓力感測且亦能在比可用熱電偶更高之 溫度下操作。 圖23說明了使用本發明來偵測其環境之化學組合物。如 圖1 ’该感測|§使電路材料暴露在環境中以使得藉由待感測 93277.doc -26 - 1247099 或BeO)中。該基板係加熱器且自電阻加熱電路金屬接收熱 量。 嫣、線型:該類型電阻加熱鎢線在燈泡中及鹵素鎢燈中使 用。 自&quot;亥等概述中可看出本發明在用於溫度感測及加熱之操 作Μ度|&amp;圍、精確度及回應時間中得到顯著改良。改良亦 存在於ί展境範圍、靈敏性、低偏移、較強熱抗震動性及加 熱效率中。 S展不並描述本發明之若干說明性實施例時,熟悉此項 技術者將想起諸多變更及替代實施例。該等變更及替代係 預期的且其不背離如所附申請專利範圍所定義之本發明之 精神及範疇。 【圖式簡單說明】 圖1係根據本發明之一實施例之感測器/加熱器的透視 圖,其中在一 Α1Ν基板上有一薄膜鎢層; 圖2係另一實施例之剖視圖,其中藉由一 wc層將Α1Ν基板 及蓋接合在一起; 圖3係另一實施例之透視圖,其中在圖丨之該鎢層上具有 一保護層; 圖4係另一實施例之透視剖視圖,其中在圖1之該結構上 有一保護封裝; 圖5係另一實施例之透視剖視圖,其中在圖*之該結構上 具有一 Α1Ν蓋; 圖6係另一實施例之一前軀體之透視圖,其中 93277.doc -28- 1247099 為圖i所示之結構提供一保護蓋; 圖7係另一貫她例之透視剖視圖,其中如圖6中所述之_ 對該等結構共同裝配; 圖8係一藉由熱回應圖12之結構形成之結構的透視剖視 圖; 圖9係另一貫她例之透視剖視圖,其中在熱回應圖6之結 構後在該結構上形成一保護封裝; 圖10係具有一 A1N蓋之圖9所示之結構的透視剖視圖; 圖11與12係說明根據本發明之一實施例之一矩形平面加 熱器之平面圖,其具有兩個不同電極組態; 圖13係說明一圓形平面加熱器實施例之平面圖。 圖14與15係說明本發明之兩種加熱器/溫度感測器實施 例之簡化示意圖,其分別具有電壓及電流驅動; 圖16係對比圖1所示之結構之理論及所量測之靈敏性對 溫度特徵之圖表; 圖17與18分別係用於圖丨丨所述實施例之用作溫度之功能 之每單位基板面積能量及每單位基板體積能量的曲線圖; 圖19、20、21、22與23係說明本發明分別對一單元件流 動速率感測器、雙元件流動速率感測器、流體位準感測器、 壓力感測器及環境感測器之施加的簡化示意圖;及 圖24、25及26分別係概述用於不同操作環境之本發明之 各種實施例之溫度範圍、使用本發明之各種實施例之溫度 感測器與先前技術溫度感測器對比之特徵及使用本發明2 各種實施例之加熱器與先前技術加熱器對比之特徵的表 93277.doc -29- 1247099 格。 【主要元件符號說明】 2 W層 2' W層 4 A1N基板 6 電極 8 A1N蓋 10 WC層 12 Au薄膜 14 封裝 16 A1N蓋 18 Au(或Pt)層 18, Au(或Pt)層 20 Pt(或Au)層 20! Pt(或Au)層 22 A1N蓋 24 Au-Pt電路層/A1N蓋 26 Au-Pt合金電路層 28 封裝 30 A1N蓋 32 A1N基板 34 導線 36 端子條/電極條 38 電極 93277.doc - 30 - 導線端子/經線 圓形基板 電極 W線 中心線 電壓源 安培計 電流源 伏特計 W之已知理論電阻一溫度曲線 空心圓 實心圓 箭頭(指示一氣體或流體) 感測器 流動路徑壁 電流源 電流源 伏特計 上游感測器/自加熱感測器 下游感測器 流體容器 流體 密封容器 壓力計 氣體槽 -31 -Au and Pt alloy bonding: - pt electrode layer provides - soldering or soldering / bonding / brazing such as wire / tape pedestal; at a temperature equal to the temperature of the melting point of Au Pt gold formed during pt or bonding The bond formed between the tape and the electrode will remain Μ. The Au electrode layer, the layered pmAu electrode layer and the Au_Pt alloy electrode layer each provide a pedestal on which the bonding/bonding //belt or the solder/brazed Pt wire/tape is formed; formed at equal to Au or during bonding The bond formed between the wire/tape and the electrode will remain intact as the temperature of the Au Pt a to the melting point. The thickness of the electrode materials involved in brazing, bonding or soldering processes is similar to that of carbon bonding. The lead wires/tapes should be attached to the electrode pads by bonding, brazing or soldering. The expansion coefficient of the guide wire material should be within twice the expansion coefficient of the composition of the post-treatment electrode layer. The diameter of the wire which can be flattened/welded/brazed to the bungee of the wire which is perpendicular to its flat surface in the case of 5 liters is the appropriate diameter used in determining the minimum thickness of the electrode layer. 1 illustrates a sensor in accordance with the present invention, wherein the tungsten circuits are further bonded to the package 14 of the substrate, preferably on an A1N substrate 4 93277.doc -16-1247099. The borosilicate mixture consisted of 45% by weight of 82 〇 3 + 55 wt% iSiO 2 . It was reacted at 1000 ° C for 5 minutes in air. In the embodiment shown in Figure 5, an A1N盍16 is placed on top of the unreacted B2〇3 + Si〇2 in Figure 4 and the resulting structure is thermally reacted to join the A1N cover 16 at a suitable additional protection. Both the package 14 and the cover 16 expose the electrode pads 6 to receive wires or strips for applying an electrical signal to the tungsten circuit. The borosilicate was reacted in air at 1 Torr for 5 minutes to join the lid where appropriate. In the embodiment illustrated in Figure 6, au and Pt layers 18 and 2 are applied as a film on the tungsten layer of the finished structure shown in Figure i; pt or may be a top layer. The result is a three-layer circuit on the A1N substrate 4. The assembly is then thermally reacted to form a two-layer circuit having a configuration similar to that shown in Figure 3, which has a lower layer comprising a crane and an Au_Pt alloy having a thickness determined by the Au and pt layers. The top layer of the circuit. In one example, a 1 Å enamel layer is sputter deposited on the A1N substrate, followed by a 100 angstrom Au and a 1000 angstrom Pt sputter deposition layer. According to the map! The thermal reaction to form the Au-Pt alloy is completed during electrode preparation as described. Another embodiment having an ACL and a protective A1N cover is illustrated in Figures 7 and 8. Referring first to Figure 7, as shown in Figure 6, a substrate assembly is provided having Ail and Pt layers 18 and 20 on the tungsten layer 2 of the substrate 4 (not in this order). An A1N cover 22 is provided having a similar three-layer conductor structure consisting of a town layer 2', Au and Pt (or Pt and Au) layers 18, and 20, all of which have the same layer as the substrate 4 geometric. The cover 22 is positioned on the substrate 4 and aligned with the different layers. The composition is then thermally reacted to form a three-layer circuit as shown in FIG. 8. The three-layer electrical 93277.doc -19-1247099 road has a S-substrate 4 and a cover 24 of the crane® 2 # &lt; And 2 sub-layered an Au_pt alloy circuit layer 24 therein. In a ribbed towel, a 10 angstrom thick Au layer and a 1 angstrom thick sound were sputtered on a 10 (8) angstrom sputter deposited tungsten layer. Fig. 9 is a view showing the structure obtained by the self-heating reaction of the structure shown in Fig. 6, which has a -Au-Pt alloy circuit layer 26 on the crane circuit layer 2. A seclating acid salt package 28 is formed on the 3 structure in a manner similar to package 14 of FIG. Figure 1A illustrates an embodiment in which the structure of Figure 9 is further protected by an A1N cover 30. The lid was placed in position and the niobate was reacted in air for 5 minutes under (10) generation to engage the lid. The invention can be advantageously applied to a planar heater. Figure u illustrates a heater formed on a rectangular (including square) A1N substrate which, in the absence of ACLs, acts as a base for a tungsten heating element that can be fabricated as described above. The tungsten layer is formed such that it is preferably a series of substantially parallel, twisted lines 34 that are parallel and connected at the opposite ends of the substrate by terminal strip %, and preferably in the array The electrode % is provided at the opposite corner. The shape provides uniform heating across all A1N substrate regions (except for their edges) and results in a more uniform rise in the rapid thermal tilt at a rate of TM seconds and a plate. The circuit line is straight to the right, and is initially heated at the center of each line and at its terminal 180. The turning occurs most rapidly, and the substrate is placed in danger of being destroyed due to the parallel thermal gradients when the heat is extremely tilted. For a thin (0.01 inch to 〇〇 14 inch (7) 〇 25 cm to 〇〇 % cm), low quality A1N substrate, the width of line 34 should not exceed 吋 (0.25 m) and The spacing between the lines should be uniform and not exceed 〇 们 277 93277.doc -20-1247099 (0.18 cm) to ensure that the thermal gradient across the spacing between the lines will not cause substrate damage. The distance between the peak and the valley perpendicular to one of the line conduction paths should not exceed the width of the line itself. These lines should be bent without forming sharp corners. The distance between the peaks and the valleys parallel to the line conduction path should be no more than 1 inch (2.5 cm) to prevent the substrate from rupturing during rapid heating, and the shorter distance can be on the surface of the substrate during rapid heating. Provides more uniform heating. The combined resistance of the lines is the resistance of a single line divided by the total number of lines in the pattern plus the resistance of an electrode strip. Parallel conductive lines allow rapid heating to high temperatures with a suitable voltage and film line (100 - 1 〇, 〇〇〇 厚 thick). Together with the terminal strips 36 provided in Figure 11, the tungsten wires are not only geometrically parallel but also electrically parallel. The terminal strips 36 can be replaced with separate electrodes at the opposite ends of each line, but are not required. Electrodes 38 are placed at opposite corners of the substrate to maintain any change in voltage that drops to a lower level across different lines. In an alternative embodiment illustrated in Figure 12, a plurality of wire terminals 4G are provided on each electrode strip % and are just opposite each other and are associated with their service line (each electrode serves no more than two wires) . Figure 13 illustrates a preferred tungsten pattern for a circular substrate 42 that ensures that the electric field strength between the opposing electrodes 44 at elevated temperatures does not exceed the dielectric decomposition strength of the A1N substrate; beyond the dielectric decomposition The strength can cause the substrate to crack or be damaged. The dielectric strength of the substrate decreases with increasing temperature and its pre-slurry is about 2000 volts/inch pairs (787 volts/cm) at 1300C. The tungsten wires 46 are bent and extend generally along respective warp threads that merge at opposite ends of the electrode 44. The lines are symmetrical about a centerline 48 that passes through the electrode electrodes 93277.doc -21 - 1247099. To ensure that the power is evenly dissipated along the length of each line, the line can be overlapped from the electrodes, but the line width perpendicular to its conduction path should remain constant. Since the lines having different distances from the center line 48 have different lengths, the width of each line associated with other lines should be decremented toward the center line so that the power dissipation per unit length of each line is close to the power per unit length of other lines. dissipation. It ensures uniform heating of the A1N substrate and the substrate is not damaged by thermal gradients. To ensure that the thermal gradient between the lines perpendicular to the line path does not cause damage to a thin, low-mass A1N substrate, the maximum spacing between the points in the lines should not exceed 0.07 inches (0._m). The spacing distance between the lines does not have to be the same: it should be symmetrical about the centerline 48. For temperatures above the heater temperature, the spacing between the midpoints of the line should be less than 〇 7 inches (〇 18 cm). Figures 14 and 15 illustrate the application of the present invention to a temperature sensing device, a single ended heater or a heater that senses its own temperature. In Fig. 14, a voltage source 5 is applied with a voltage to pass over a tungsten conductive film 2 deposited on the A1N substrate 4. An ammeter 52 monitors the current through the tungsten film. When t is used to sense the temperature of the surrounding environment, (4) a low voltage is applied to apply an actuation signal that does not significantly heat the tungsten film. The resistance of the film is determined by the temperature of its surrounding environment based on the known temperature coefficient of the tungsten resistor. The temperature of the surrounding film can be determined by dividing the applied voltage by the measured current to determine the resistance of the film. The response of the tungsten film sensed by the ammeter 52 to a known applied voltage changes with ambient temperature. The current level that can be sustained in the tungsten film without causing significant heating of the film is determined by several factors such as ambient temperature, film thickness, surface area and shape, and ambient heat capacity 93,277.doc -22-1247099. Typically, once the heating threshold is reached, the film will undergo a rapid increase in heating as the current level continues to increase. When the ambient temperature increases, the heating threshold increases. When used as an open heater, a higher voltage level is applied. The system can be pre-registered to at least close to - the amount of heating that can be obtained from a given voltage level and without the need for an ammeter 52. To operate as a heater that senses its own temperature, an ammeter μ is added back to the circuit to sense the current through the crane layer. The temperature of the film can be accurately determined by using the electrical dust and current levels and determining the known geometry of the film from which the temperature of the m resistance curve of the cell is operated. The system of Figure 15 is similar to the system of Figure 14, but instead of applying a voltage across the tungsten film and sensing the resulting current, the current source 54 is used to drive the two actuation currents through the membrane 2 and use a voltmeter. The resulting voltage across the membrane was measured. The film depletion temperature can be determined again in the same manner as in Fig. 14. The temperature-resistance characteristic of one of the structures shown in Figure 1 is measured and compared to the known theoretical resistance-temperature curve 58 of tungsten shown in the figure. The amount obtained in the flowing Ar environment can be indicated by a hollow circle 6〇. The results are measured and tracked very close to the theoretical curve of the measured limit of 14 ° C. The measured trace in air is about 26 (the theoretical curve of the temperature of TC, beyond which the oxidation of the tungsten is Starting from the theoretical curve, the measurement obtained in the air environment is indicated by a solid circle 62. The edge test of Fig. 16 is performed in a water-cooled condensed quartz tube. Prototype sensing is placed on an AW sheet, which is located at RF heating on the graphite susceptor. The wire extending from each of the two sensor electrodes extends through a 〇-ring seal extension 93277.doc -23-1247099 to provide precise current input to the sensing person The voltage and current source sub-extends to a multimeter for measuring the output voltage of the sensor. It is the first time to measure the sensitivity of a tungsten film. It can be calibrated using the material shown in Figure 16. a tungsten film of known cross section and length As a temperature sensor. Perform a test in the air on the heater chuck of the ball ball adapter, where the prototype sensor is clamped on the surface of the heater chuck. The top and sides of the sensors are made of tannin. Cotton insulation. The electrical contact to the sensor electrode is made using a gold probe that extends from the micromanipulator and is compressively connected to the sensor electrode. The applied current is measured with the measured sensor output voltage and The applied voltage of the waveform tracer, the voltage read from the waveform tracer across the sensors and the current passing through the sensors, performs a two-wire power measurement. The type shown in Figure 11 is also tested. Planar electric heater. Its size is 4 25 in. χ4·25 ΐη·χ0·014 in•thickness (10·8 cmxl〇.8 cmx0.036 cm). The maximum heating rate is obtained at about 500 C % and the maximum temperature is about 15 〇〇, both of which are limited by the useful power. The area power density versus temperature curve of Figure 17 shows the power of the detected A1N substrate area per cell, while the volume power density versus temperature in Figure 18 The resulting A1N basis per unit in the curve The power of the volume can also be used by measuring the change in the temperature of the self-heating sensor. The device is located along the flow path 4' and can be immersed in the fluid or in contact with the wall of the flow path. In the illustration of Fig. 19, a gas is sensed by self-heating sensor 66 of the type described herein located along the flow path and immersing in the flow or contacting the flow path wall 68. Or the flow rate of fluid 93277.doc -24-1247099 (indicated by the head 64). In the present embodiment described herein and the following examples, the actuation signal is illustrated by an adjustable current source 70. Seventh, wherein the voltmeter 72 senses the voltage response of the sensor, which in turn corresponds to the sensor resistance and thus corresponds to the fluid temperature. However, a voltage can be provided as the actuation signal and the resulting current is sensed. The flow rate can be determined by comparing the sensed temperature / temperature at the V-speed and considering the heat capacity of the fluid. In the differential flow rate sensor illustrated in Figure 20, two or more sensors 74, 76 of the type described herein are connected in series along the fluid flow path 64. The flow rate is sensed by measuring the temperature difference between the sensors. At zero flow, the upstream sensor 74 is electrically self-heated by a known current (or known voltage) from current source 70 to a resistor representing a known temperature. The downstream sensor 76 is biased (flowed) by a small amount of non-heating current or voltage. The independent current source 7〇 can be supplied from an ordinary current source or equally as shown to provide an actuating current. The fluid flow removes heat from the upstream self-heating sensor 74 and releases some of the heat to the downstream sensor 76. The change in voltage across each of the sensors is related to the flow rate through the heat capacity of the gas or fluid. This type of differential flow rate sensing can be used in a conduit parallel to the main flow path to determine the flow rate through the path. Figure 21 illustrates the application of the present invention to a fluid level sensor in which a sensing member 66 is disposed in a fluid container 78 or at a fixed location in contact with the outer wall of the container. A rise and fall of the fluid 8 in the container causes the sensor 66 to be immersed in or removed from the fluid. The heat capacity of the sensor's tight environment depends on whether the fluid level has risen to 93277.doc -25-1247099 depending on the sensor. When the sensor is at a known level of the container and it is used as a self-heating temperature sensor as described above, the heat can be determined by sensing how quickly the sensor can remove heat from the sensor. Whether the sensor is immersed in the fluid. When the application is described in the form of a fluid sensor, it can also be used to detect the presence or absence of gas in a sealed container at least at a minimum density level. When applying the present invention to the above flow rate or fluid level sensing applications, the main advantages of the present invention are faster response times (related to high substrate thermal conductivity) and greater sensitivity (also associated with high substrate thermal conductivity). And relatively low or no offset (related to the small expansion coefficient mismatch between the W sensing circuit and the A1N substrate). In Figure 22, the sensor 66 of the present invention is used to sense a sealed container. Gas pressure in the middle. The pressure in the vessel can be sensed by determining the desired current to maintain a particular voltage across the sensor or the voltage required to maintain a particular current across the sensor. This data may be related to the pressure/density of the gas having a known heat capacity in the vessel, which may be a vacuum chamber. The current source 70 shown in Figure 22 is adjusted to maintain a particular voltage level as sensed by the voltmeter 72 across the sense 1 §. The conversion of the current level to the pressure level in the vessel is illustrated by a pressure gauge 84 provided by the current source. The present invention enables voltage and current sensing that is more sensitive than currently available thermocouples and thus enables a more sensitive pressure sensing and can operate at higher temperatures than available thermocouples. Figure 23 illustrates a chemical composition for use in the present invention to detect its environment. As shown in Figure 1 'this sensing|§ exposes the circuit material to the environment so that it is to be sensed by 93277.doc -26 - 1247099 or BeO). The substrate is a heater and receives heat from the resistance heating circuit metal.嫣, line type: This type of resistance heating tungsten wire is used in the bulb and halogen tungsten lamp. It can be seen from the overview of &quot;Hai et al. that the present invention is significantly improved in the operating temperature, &amp; circumference, accuracy and response time for temperature sensing and heating. Improvements also exist in zh's range, sensitivity, low offset, strong thermal shock resistance and heating efficiency. A number of variations and alternative embodiments will be apparent to those skilled in the art when a number of illustrative embodiments of the invention are described. Such changes and substitutions are intended to be and are not intended to be in the spirit and scope of the invention as defined by the appended claims. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a perspective view of a sensor/heater according to an embodiment of the present invention, wherein a thin film tungsten layer is provided on a substrate of one turn; FIG. 2 is a cross-sectional view of another embodiment, wherein Figure 1 is a perspective view of another embodiment having a protective layer on the tungsten layer of the Figure; Figure 4 is a perspective cross-sectional view of another embodiment, wherein Figure 4 is a perspective view of another embodiment of the present invention; Figure 1 is a perspective cross-sectional view of another embodiment, wherein the structure of Figure 4 has a top cover; Figure 6 is a perspective view of a front body of another embodiment, 93277.doc -28- 1247099 provides a protective cover for the structure shown in Figure i; Figure 7 is a perspective cross-sectional view of another example, wherein the structures are assembled as shown in Figure 6; Figure 8 is A perspective cross-sectional view of the structure formed by the heat response to the structure of Fig. 12; Fig. 9 is a perspective cross-sectional view of another example in which a protective package is formed on the structure after the structure of the heat is restored; Fig. 10 has a The structure of the A1N cover shown in Figure 9 Cross-sectional view; FIG. 11 is a plan view illustrating a rectangular plane 12 based heater of one embodiment in accordance with one embodiment of the present invention, having two different electrodes configuration; FIG. 13 lines of a plan view illustrating a circular planar heater embodiment. Figures 14 and 15 are simplified schematic views of two heater/temperature sensor embodiments of the present invention, each having voltage and current drive; Figure 16 is a comparison of the theory and measurement of the structure shown in Figure 1 Graphs of temperature versus temperature characteristics; Figures 17 and 18 are graphs of energy per unit substrate area and energy per unit substrate volume for the function of temperature used in the embodiment of the Figure; Figure 19, 20, 21 22 and 23 illustrate simplified views of the application of the present invention to a single element flow rate sensor, a dual element flow rate sensor, a fluid level sensor, a pressure sensor, and an environmental sensor, respectively; 24, 25 and 26 respectively summarize the temperature range of various embodiments of the present invention for different operating environments, the characteristics of the temperature sensor using various embodiments of the present invention, and the prior art temperature sensor, and the use thereof. Invention 2 Table 93277.doc -29- 1247099 of the characteristics of the heaters of the various embodiments compared to prior art heaters. [Main component symbol description] 2 W layer 2' W layer 4 A1N substrate 6 Electrode 8 A1N cover 10 WC layer 12 Au film 14 Package 16 A1N cover 18 Au (or Pt) layer 18, Au (or Pt) layer 20 Pt ( Or Au) layer 20! Pt (or Au) layer 22 A1N cover 24 Au-Pt circuit layer / A1N cover 26 Au-Pt alloy circuit layer 28 package 30 A1N cover 32 A1N substrate 34 wire 36 terminal strip / electrode strip 38 electrode 93277 .doc - 30 - Wire Terminal / Warp Round Substrate Electrode W Line Center Line Voltage Source Amperage Current Source Voltmeter W Known Theoretical Resistance - Temperature Curve Hollow Round Solid Circle Arrow (Indicating a Gas or Fluid) Sensor Flow Path wall current source current source voltmeter upstream sensor / self-heating sensor downstream sensor fluid container fluid sealed container pressure gauge gas tank -31 -

Claims (1)

1247|)淑114815號專利申請案 ’‘ 中文申請專利範圍替換本(94年7月) 十、申請專利範圍: 1. 一種感測器系統,其包含: 一 A1N基板(4), 一在該基板上之W層(2), 一經調適以向該W層施加一電致動訊號之訊號源 (7〇),及 、、二调適以感測該W層對該致動訊號之回應的感測器 (72)。 2·如請求項1之系統,該|層包含一薄膜。 3·如睛求項1之系統,其進一步包含一在該…層上之抗氧化 保護層(12)。 4·如凊求項1之系統,其建構為一溫度感測器,其中該致動 七號向4 w層施加一非加熱電訊號,且該感測器感測該w 層對違致動訊號之回應,作為該感測器附近溫度之指示。 5.如凊求項1之系統,其中該訊號源施加一訊號以加熱該w 層。 6·如凊求項5之系統,其中該感測器感測該w層指示其溫度 之回應。 士月求員6之系統,其進一步包含一在表層上具有一額外 W層(2)之額外A1N基板,連接該訊號源以對該額外w 層鈀加大體上非加熱電訊號,且連接一感測器(72)以感 測一該額外W層指示其溫度之的回應, 该頟外基板及W層安置在一流體流動路徑(64)中之該 基板及傳導層之下游,其中該W及額外W層之間的溫度之 93277-940708.doc 1247099 差別對應該流體流動速率。 8 ·如明求項1之糸統’該基板及W層安置在一流體流動路徑 (6 4)中’可控制該訊號源以施加一加熱該w層之致動訊 號’其中由該感測器所感測之回應對應一沿該路徑之流 體流動速率。 9·如請求項1之系統,其中將該基板及w層交替地浸入一預 定流體(80)中並自該流體清除,由該感測器所感測之回應 指示該基板及W層是否在該流體中。 1 〇·如請求項1之系統,其中該基板及W層安置在一可變壓力 環境(82)中,該感測器感測該w層之回應,作為在該環境 中之壓力的指示。 U·如睛求項1之系統,其中該基板及…層安置在一環境(86) 中’在該環境中該W層受改變該W層對一給定致動訊號之 回應的該環境之變更支配,其中該致動訊號與該回應之 間的關係指示該環境之化學本質。 12. 一種電路元件,其包含: A1N基板(32),及 一在該基板上之W薄膜層(34)。 13. 如睛求項12之電路元件,其中該W層包含分佈於該基板上 之禝數個導線(34),其中該基板為矩形且該等線大體上平 行並碗蜓成型。 4·如叫求項13之電路元件,其中該|層包含分佈在該基板上 之複數個導線’其中該基板為圓形(42)且該等線沿各自之 二、束(4〇)延伸,該等經線在該基板之相對極點(44)處合 93277-M0708.doc 1247099 15. 併。 一種感測方法,其包含以下步驟: 16. 17. 18. 感測該W層對該致動訊號之回應。 如請求項15之方法’其中對該W層施加一非加熱致動 唬亚感測其回應,以作為其附近溫度之指示。 如請求Jf 1 4 、^之方法,其中該致動訊號加熱該 如睛求項1 7 、/之方法,其中感測該W層之溫度。1247|)Shu 114815 Patent Application '' Chinese Patent Application Substitution (June 1994) X. Patent Application Range: 1. A sensor system comprising: an A1N substrate (4), one at The W layer (2) on the substrate is adapted to apply an electrical actuation signal source (7〇) to the W layer, and the second is adapted to sense the response of the W layer to the actuation signal. Sensor (72). 2. The system of claim 1 wherein the layer comprises a film. 3. The system of claim 1, further comprising an anti-oxidation protective layer (12) on the layer. 4. The system of claim 1, which is constructed as a temperature sensor, wherein the actuation No. 7 applies a non-heating electrical signal to the 4 w layer, and the sensor senses the w layer to actuate the violation The response of the signal is an indication of the temperature near the sensor. 5. The system of claim 1, wherein the signal source applies a signal to heat the w layer. 6. The system of claim 5, wherein the sensor senses a response of the w layer indicating its temperature. The system of claim 6 further comprising an additional A1N substrate having an additional W layer (2) on the surface, connecting the signal source to add substantially unheated electrical signals to the additional w layer of palladium, and connecting one The sensor (72) senses a response of the additional W layer indicating its temperature, the outer substrate and the W layer being disposed downstream of the substrate and the conductive layer in a fluid flow path (64), wherein the W The temperature between the additional W layers is 93277-940708.doc 1247099 The difference corresponds to the fluid flow rate. 8 · The system of claim 1 wherein the substrate and the W layer are disposed in a fluid flow path (6 4) to control the signal source to apply an actuation signal for heating the w layer, wherein the sensing is performed by the sensing The response sensed by the device corresponds to a fluid flow rate along the path. 9. The system of claim 1, wherein the substrate and the w layer are alternately immersed in and removed from a predetermined fluid (80), and the response sensed by the sensor indicates whether the substrate and the W layer are in the In the fluid. The system of claim 1, wherein the substrate and the W layer are disposed in a variable pressure environment (82) that senses the response of the w layer as an indication of the pressure in the environment. U. The system of claim 1, wherein the substrate and layer are disposed in an environment (86) in which the W layer is subjected to an environment in which the W layer responds to a given actuation signal. The change governs, wherein the relationship between the actuation signal and the response indicates the chemical nature of the environment. 12. A circuit component comprising: an A1N substrate (32), and a W film layer (34) on the substrate. 13. The circuit component of claim 12, wherein the W layer comprises a plurality of wires (34) distributed over the substrate, wherein the substrate is rectangular and the wires are substantially parallel and formed into a bowl. 4. The circuit component of claim 13, wherein the layer comprises a plurality of wires distributed on the substrate, wherein the substrate is circular (42) and the wires extend along respective two, bundles (4 turns) The warp threads are joined at the opposite pole (44) of the substrate 93277-M0708.doc 1247099 15. A sensing method includes the following steps: 16. 17. 18. Sensing the W layer's response to the actuation signal. The method of claim 15 wherein a non-heating actuation is applied to the W layer to sense its response as an indication of the temperature in its vicinity. A method of requesting Jf 1 4 , ^, wherein the actuating signal heats the method of claim 7, wherein the temperature of the W layer is sensed. 93277-940708.doc -3 -93277-940708.doc -3 - I247Q99 f 〇93114815號專利申請案 中文圖式替換頁(94年7月) 93277I247Q99 f 〇93114815 Patent Application Chinese Graphic Replacement Page (July 94) 93277
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