TW386248B - Multi-beam array electron optics - Google Patents

Multi-beam array electron optics Download PDF

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TW386248B
TW386248B TW87105749A TW87105749A TW386248B TW 386248 B TW386248 B TW 386248B TW 87105749 A TW87105749 A TW 87105749A TW 87105749 A TW87105749 A TW 87105749A TW 386248 B TW386248 B TW 386248B
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pattern generator
item
array
scope
patent application
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TW87105749A
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Chinese (zh)
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John C Wiesner
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John C Wiesner
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y10/00Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y40/00Manufacture or treatment of nanostructures
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/30Electron-beam or ion-beam tubes for localised treatment of objects
    • H01J37/3002Details
    • H01J37/3007Electron or ion-optical systems
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/30Electron-beam or ion-beam tubes for localised treatment of objects
    • H01J37/317Electron-beam or ion-beam tubes for localised treatment of objects for changing properties of the objects or for applying thin layers thereon, e.g. for ion implantation
    • H01J37/3174Particle-beam lithography, e.g. electron beam lithography
    • H01J37/3175Projection methods, i.e. transfer substantially complete pattern to substrate
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J2237/00Discharge tubes exposing object to beam, e.g. for analysis treatment, etching, imaging
    • H01J2237/06Sources
    • H01J2237/063Electron sources
    • H01J2237/06325Cold-cathode sources
    • H01J2237/06341Field emission
    • H01J2237/0635Multiple source, e.g. comb or array
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J2237/00Discharge tubes exposing object to beam, e.g. for analysis treatment, etching, imaging
    • H01J2237/30Electron or ion beam tubes for processing objects
    • H01J2237/317Processing objects on a microscale
    • H01J2237/3175Lithography
    • H01J2237/31774Multi-beam

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Nanotechnology (AREA)
  • Analytical Chemistry (AREA)
  • Physics & Mathematics (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Manufacturing & Machinery (AREA)
  • Mathematical Physics (AREA)
  • Theoretical Computer Science (AREA)
  • Electron Beam Exposure (AREA)

Abstract

A multi-beam array optics system useful as a pattern generator for electron beam lithography includes a source of electrons having an array of individual field emission elements each of which can generate an individual electron beam; a beam assemblage optics being set as assemblage for receiving the individual electron beams to accelerate and control the individual electron beams; and a target location being set on a place to that the beam assemblage optics directs the assemblage of the individual electron beams.

Description

Μ Β7 五、發明説明(1 ) 本發明係關於多束陣列充電粒子光學(透鏡)及相 關系統,而特別是關於使用一多束陣列的~圖樣產生器 (patterngenerator)。 於電子束圖樣產生之領域中眾所週知的是,要可以 增加圖樣產生系統的產量。而此等圖樣產生系統的雨個 主要應用是,藉由光_微影.(photolithography)來製 作使用在半導體製程中所用的光罩以及將圖樣直接的刻 寫在晶片上來形成半導體元件。如此必需要個別的去掃 描一電子束或是離子束圖樣到一基材上,即一光罩或是 一晶片而言,相對來講是一緩慢的過程。有人嘗試的去 改良此產量,例如在所描述的電子束圖樣產生器中,由 0.厂0.]^11〇61〇£8等人在微電子電路工程8 3 (Microcircuit Engineering 83) ,1 9 8 3 之第 99頁 及此之後的”一個觀念以一10GHz的圖素率(多重)E-束機(A Concept for a 10 GHz Pixel Rate (Multiple) E-B. earn Machine) +’’中所揭露的一個,可 以個別明暗閃爍的3 2 X 3 2的聚焦電子束U m a t r i x o f 32*32 focused electron'beamlets)的 一陣列的使 經濟部中央標隼局員工消費合作社印袋 用。任一個光束(b e a ml e t s )可以藉由所謂的蒼蠅眼稜 ,鏡而得以被個別的聚焦,此蒼蠅眼棱鏡係由一些很小的 鏡片所組合成的合成物,而任一個小鏡片係與一光束相 關。, . 這個方法的缺失是至少任一個個別的光束是易受於 2 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) A7 B7 五、發明説明(2 ) 因發生在電子光束柱中的污染所造成的各種非對稱性所 影響,例如由於小粉塵粒子落入光束柱中的鏡鏡所造成 的影響。此一污染在各個不同的光束上發生不同的影 響,造成了光束相對於彼此而被互相替代,降低了所被 刻寫之圖樣的精_.確性。 另外還有微光束柱法,在此法中,個別的微光束柱 每一個例如具有一公分的直徑,被配置在一矩形的陣列 上,去提供一多重的電子束。由於每一個皆有其個別的 的偏向器,加速器及聚焦電子束透鏡。所以需要去個別 的製作此等微光束柱,也因此造成其既複雜又昂貴。 再來是陣列陰極法,它可獲得一個或是二次元的電 子束來源的高密度整合。由於介電性的崩潰,此類元件 便爲可被輸入到此等現跡之電子的能源所侷限,也因此 對電子束圖樣產生器的利用性有所限制。 另外在此技藝中習知的還有使用藉雷射光束來當作 多束的電子來源而放光的負電子族(negativeM B7 V. Description of the invention (1) The present invention relates to a multi-beam array charging particle optics (lens) and related systems, and in particular to a pattern generator using a multi-beam array. It is well known in the field of electron beam pattern generation that the production of a pattern generation system can be increased. The main application of these pattern generation systems is to use photolithography to make photomasks used in semiconductor manufacturing processes and to write patterns directly on wafers to form semiconductor elements. Therefore, it is necessary to individually scan an electron beam or ion beam pattern onto a substrate, that is, a photomask or a wafer, which is a relatively slow process. Some people have tried to improve this output, for example, in the described electron beam pattern generator, from the factory 0.] ^ 11〇61〇 £ 8 and others in Microcircuit Engineering 83 3, 1 9 8 3 on page 99 and thereafter "A Concept for a 10 GHz Pixel Rate (Multiple) EB. Earn Machine) +" An array of 3 2 X 3 2 focused electron beams (U matrixof 32 * 32 focused electron'beamlets) that can be individually and individually blinked is used to print bags for the consumer cooperative of employees of the Central Bureau of Standards of the Ministry of Economic Affairs. bea ml ets) can be individually focused by the so-called fly eye prism, which is a composite of a few small lenses, and any small lens is related to a light beam. The lack of this method is that at least any one of the individual beams is susceptible to 2 paper standards applicable to Chinese National Standards (CNS) A4 specifications (210X297 mm) A7 B7 V. Description of the invention (2) Because it occurs in the electron beam column Pollution in The effects of various asymmetries, such as those caused by small dust particles falling into the mirror of the beam column. This pollution has different effects on different beams, causing the beams to be affected relative to each other. Substituting each other reduces the accuracy of the pattern being written. In addition, there is also a microbeam column method, in which individual microbeam columns each have a diameter of, for example, one arranged in a rectangular array. In order to provide multiple electron beams, each one has its own deflector, accelerator, and focusing electron beam lens. Therefore, it is necessary to separately make these microbeam columns, which is also complicated and expensive. Then there is the array cathode method, which can obtain a high-density integration of one or two-dimensional electron beam sources. Due to the collapse of dielectric properties, such elements are the energy source for electrons that can be input to these existing traces. The limitation also limits the usability of the electron beam pattern generator. In addition, it is also known in the art to use a laser beam as a source of multiple electrons. Group light negative electron (negative

I electron affinity)的光影陰極。Schneider 等人, 在 J . Vac. Sci. T e c h n ο 1. B 1 4 ( 6 ), 3782-3766, Nov/Dec 1996所發表的此一電子束系統。負電子族 材質,例如G a A s化合物係眾所週知(的對污染物極爲敏 感,如此會減低或是消除了電子的放射。而在一電子束 圖樣產生器之一般可見的眞空環境中,可以因此預期到 此一多束陰極之受限的壽命。 3 本纸張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) (請先閱讀背面之注意事項再填寫本頁 ' 經濟部中央梯準局員工消費合作社印架 A7 -— ___ B7 五、發明説明(3) — 在此領域中的習知工作並未解決當需於商業上可行 時之增加受充電粒子束系統的產量所發生的問題。於半 導體晶片上直接刻寫的此等商品化之主要障礙在於一方 面傳統充電粒子束的低產量,而另一方面則是此等平行 陣列光束來源的一極其受限的光束能量,即約在數百伏 特左右。(請看,例如iyiac_Doiiald.等人, Proceedings SPIE 2522 (1995) 220-229.) 此一受限的光束能量迫使由放射器到目標物的光學 路徑長度必須非常的短(大約是1mm左右)以便沒有不 當之內部光束(inter-beamlet)的扭.曲。另外,由於 低能量,此等粒子不能穿透在目標物上之傳統的厚光阻 材料(4 0 0 0 A )。也因此使此光阻不能曝光。此外對準 用之標註亦是位在此光阻之下,因而不爲此光束所視。 因此今日之商業使用的電子束微影係已受限於光罩的 製作。甚至對光罩的製作來說它也是希望能夠使用傳統 的能量光束而得以增加產量,特別是當積體電路變得愈 益複雜而需求愈益複雜之光罩的時候。 經濟部中央標準局員工消費合作社印繁 根據本發明,一種圖樣產生器及一使用一充電粒子 來源來產生圖樣的方法,此來源是一個別來源的元素之 陣列.,具體的形成在一單一的基材上,而在此來源中的 任一個來源元素放射出一個別充電的粒子束。此等充電 ,的粒子束於是通過一(光)束聚集組合透鏡(beam assemblage optics),而此(光).束聚集組合透“接 4 本紙張尺度適用中國國家標準(CNS ) A4規格(21〇乂297公麓) ~~~ ------B7 五、發明説明(4 ) 收此個別之充電的粒子束並視同其等係一單一的光束般_ 的予以控制及加速。也就是說,在此束聚集組合透鏡 中,對任一光束而言並沒有個別的偏向器或是加速器》 易言之,此等個別充電的粒子束被視爲一單一的整體光 束’而因此被加速並導引到一目標物上,例如,固定在 一適當支撐上的一半導體晶片或是一於光罩材料 (r e t i c 1 e )下的基材上’就如同在一傳統的充電粒子束 微影一般。 一般而言此束聚集組合透鏡包括至少一個偏向器其 係本質上用來均勻地偏折整個聚集的光束,一聚焦元件 (f 〇 c u s e 1 e m e n t )係一傳統的”棱鏡”,還有—加速 器元件它將整個聚集的光束視爲一個單一的光束而予以 加速,也就是,它並非獨立的加速個別的光束而是均勻 的加速所有的光束。此外,此圖樣產生器可以操作在一 向量(vector)的掃描或是光柵(raster)的掃描模式下。 在此來源中的任一個個別的元素可以藉明或暗而被 個別地定址。在某些具體實施例中此等個別之明或暗的 來源元素被取而代之的是一整群元素(例如一來源元素 的矩形次陣列)的明或暗。此等明或暗一般係由一提供 ,到任一來源元素之個別來源電位(source potential) 或是藉由一提供到任一來源元素的個別的引出電位 (extraction potential )戶斤完成。 (光)束(e a m ”)在此處被看成一可受鑑定的― 5 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) A7 B7 五、發明説明(5 ) 束充電的粒子。依據一般的使用,此揭露書使用此名詞‘ 束’,係與是否此束是暗(關閉)或是(打開)無關。是以 如此而界定了一靜態的束軸,而此束軸則是爲於此光束 中之粒子所跟隨的一中心路徑。而光束(Weamlet”) 於此處則特別被視爲在一多束系統中的聚集組合光束中 的一個別的(光)束。 多束(m u 11 i - b e a m )在此則被視爲.在一單一群組 束中的多重的充電粒子束。(”多束”使用於此並不意味 著在此要被視爲於此技藝中所習知的多重光柱的電子束 系統,在此系統中個別的電子束係任一個均在其自己個 別的光.束柱內而且任一個均有其個別的光學佈局。)。” 陣列(array ) ”該名詞使用於此被視爲(但不侷限於 此),例如一列及行陣列而不論希望它具有什麼型狀, 也就是設置成一維或是二維的,正方形、矩形、圓形或 是線形。其他的陣列幾何或許也是適當的。此陣列也不 需要放置在一平面上而可以是某些其他的具規則的表 , · > 經濟部中央標準局員工消費合作社印製 (請先閱讀背面之注意事項再填寫本頁) 面,例如一個球形或是圓柱形的表面。此個別粒子來源 元素的陣列係設置有選取器用來由來源元素中引出粒 子,藉此起始了個別的電子束之多樣性的形成。此一選 取的動作可以藉由與一其本身被當作一個別選取器陣列 的此陣列源,或是當作集體聚集而對所有的粒子來源當 ,作一單一的選取器的此陣列源的一結構整體化而達成。 此來源元素_的陣列是提供有暗(空白; 6 本紙張尺度適用中國國家標隼(CNS ) A4規格(210X297公釐) Λ7 _____._ B7 五、發明説明(6 ) blanking)及亮(非空白;unblanking)(關閉或開 啓)的結構’其中一個具體實施例係無關於任一個其他 來源元素的操作在任一個來源元素上。另外在某些具體 實施例上此獨立性並非是個別的來源元素。例如可以藉. 由一矩形陣列來描.述藉之而無關於其他列或是行的去開 啓或是關閉來源元素的一整個被選定的列或是行,或者 是去關閉來源元素的小矩形區。此空'白可藉此個別的來 源元素電位(電壓)的獨立控制或是經由被設置有個別 的選取器之處的此個別的選取電位,或是合倂此等而予 以提:供。 . 經濟.邱中央標準局員工消費合作社印製I electron affinity). This electron beam system, Schneider et al., J. Vac. Sci. T e c h n ο 1. B 1 4 (6), 3782-3766, Nov / Dec 1996. Negative electron family materials, such as GaAs compounds, are well-known (very sensitive to pollutants, which will reduce or eliminate the emission of electrons. In the generally visible empty environment of an electron beam pattern generator, you can therefore The limited life of this multi-beam cathode is expected. 3 This paper size is applicable to the Chinese National Standard (CNS) A4 (210X297 mm) (Please read the precautions on the back before filling out this page Bureau Consumers' Cooperative Printing Stand A7-___ B7 V. Description of Invention (3)-Known work in this field has not solved the problems that occur when increasing the output of the charged particle beam system when it is commercially feasible The main obstacle to such commercialization directly written on semiconductor wafers is the low yield of traditional charged particle beams on the one hand, and an extremely limited beam energy of these parallel array beam sources on the other hand, which is about Hundreds of volts. (See, for example, iyiac_Doiiald. Et al. Proceedings SPIE 2522 (1995) 220-229.) This limited beam energy forces the emitter to the eye. The optical path length of the object must be very short (about 1mm) so that there is no improper twist of the internal beam (inter-beamlet). In addition, due to the low energy, these particles cannot penetrate the traditional object of the target Thick photoresist material (4 0 0 A). It also makes this photoresist unable to be exposed. In addition, the marking for alignment is also under this photoresist, so it is not seen by this light beam. Electron beam lithography has been limited to the production of photomasks. Even for the production of photomasks, it is also hoped that it can use traditional energy beams to increase production, especially as integrated circuits become more complex and demand becomes more complex. According to the present invention, a pattern generator and a method for generating a pattern using a source of charged particles, the source is an array of elements from other sources, specifically Is formed on a single substrate, and any source element in this source emits an otherwise charged particle beam. These charged particle beams then pass through (Light) beam assemblage optics, and this (light) beam assemblage combination lens is connected to the 4 paper sizes applicable to the Chinese National Standard (CNS) A4 specification (21〇 乂 297 feet) ~~~- ----- B7 V. Description of the invention (4) The individual charged particle beam is received and controlled as if it were a single beam. That is, in this beam-gathering combination lens "There is no individual deflector or accelerator for any beam." In other words, these individually charged particle beams are treated as a single overall beam 'and are therefore accelerated and guided to a target, For example, a semiconductor wafer fixed on a suitable support or a substrate under a mask material (retic 1 e) is like a conventional charged particle beam lithography. Generally speaking, this beam-focusing combination lens includes at least one deflector, which is essentially used to deflect the entire focused beam uniformly, a focusing element (focuse 1 ement) is a traditional "prism", and-an accelerator The device accelerates the entire collected beam as a single beam, that is, it does not accelerate individual beams independently but accelerates all beams uniformly. In addition, the pattern generator can operate in a vector scan or raster scan mode. Any individual element in this source can be individually addressed by light or darkness. In some embodiments, these individual light or dark source elements are replaced by the light or dark of a whole group of elements (e.g., a rectangular sub-array of source elements). These light or dark are generally completed by a source to an individual source potential of any source element, or by an individual extraction potential provided to any source element. The (light) beam (eam) is here regarded as an identifiable ― 5 paper sizes are applicable to the Chinese National Standard (CNS) A4 specifications (210X297 mm) A7 B7 V. Description of the invention (5) Beam charged particles . According to general usage, this disclosure uses the term 'bundle', which has nothing to do with whether the beam is dark (closed) or (open). In this way, a static beam axis is defined, and this beam axis is It is a central path followed by the particles in this beam. The beam (Weamlet) is here particularly regarded as another (light) beam of the aggregated combined beam in a multi-beam system. Multiple beams (m u 11 i-be e a m) are considered here. Multiple charged particle beams in a single group beam. (The use of "multibeam" here does not mean that it is to be considered here as a multi-beam electron beam system known in the art. In this system, each of the individual electron beam systems is in its own individual. Light. Beam column and each one has its own optical layout.). The term "array" is used here (but not limited to this), such as an array of columns and rows, regardless of what shape it is intended to be, that is, set in one or two dimensions, square, rectangular , Round, or linear. Other array geometries may be appropriate. This array does not need to be placed on a plane, but can be some other regular table. ≫ Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs (please read the precautions on the back before filling this page). For example, a spherical or cylindrical surface. This array of individual particle source elements is provided with a selector for extracting particles from the source elements, thereby starting the formation of the diversity of individual electron beams. The action of this selection can be treated as a single selector with this array source as a separate selector array, or as a collective aggregation for all particle sources. A structure was integrated. The array of this source element _ is provided with dark (blank; 6 paper sizes are applicable to China National Standard (CNS) A4 specifications (210X297 mm) Λ7 _____._ B7 V. Description of the invention (6) blanking) and bright (non- 'Blank (unblanking) (closed or on) structure' One of the specific embodiments has no operation on any other source element on any source element. In addition, this independence is not an individual source element in some specific embodiments. For example, it can be described by a rectangular array. It can be used to turn on or off the entire selected column or row of the source element without referring to other columns or rows, or to close the small rectangle of the source element. Area. The empty white can be provided by the independent control of the potential (voltage) of the individual source elements, or through the individual selection potential where the individual selector is provided, or a combination of these. . Economy. Printed by Qiu Central Standard Bureau employee consumer cooperative

(請先閲讀背兩.之注意事is再填*?本頁J 線、 在另一個具體實施例中’此來源陣列不僅包括一個 獨立的暗亮(空白;blanking)結構還包括有獨立的 稜鏡(任一個來源元素有一個)用來聚焦粒子束。(稜 鏡及(透鏡)光學或是(透鏡的)光學的,於此處係協 定成不是用來當作光的鏡片或是光的反射稜鏡而是被當 成用於聚焦經充電之粒子束的電磁或是靜電結構。)此 等稜鏡係於此來源結構的製作中藉由附加的步驟所製 作。此等稜鏡被用在特定的粒子束系統的應用中。例如 爲有效的光束傳輸而將此來源透鏡與此光柱透鏡相匹 配。在一具體實施例上,獨立的偏向器係提供給獨立的 光束。再一次,此等獨立的偏向器係於此來源結構的製 作過程中藉由附加的歩驟來製作並被整合在此結構中。. 一選定的光宋偏向器;當被致動時,造成由此相關來源 7 本纸張尺度適用中國國家標準(〇1\$)六4規格(210父297公漦). Λ7 B7 五、發明説明( 經濟部中央標準局員工消費合作社印製 元素放射出的此特定電子束的方向由—般係對齊於此 粒子束系統軸的方向改變到一稍稍不同的方向上,一搬 來講此偏折係僅僅於此整個光束軸的幾度而已,但在其 他的具體實施例中卻會比較大。 1 預期於本發明的範圍中的此來源陣列所放射出的粒 . · . . . 子是電子或是離子,在一個使用電子當作充電粒子的具 體實施例中,此粒子來源被稱做一陰極或是陰極陣列藉 之強調此等獨立陰極的多重性。此來源陣列一般係被製 怍成一個一體化的結構。有很多關於此一體化的陰極陣 著述,在此等技藝中還有數種眾所周知的適當之放 射技術及結構,包括有場放射,負電子族(negative electron affinity)及被佈置成放射器陣列的熱電子 陰極。 被用來製作次微米電子放射器陣列的製程係於1 9 9 3 年4月6日發給MacDonald等人的美國專利編號5, 1 9 9 , 1 9 7 (U.S. Pat. No. 5, 199, 197)及於 1 9 9 2年6月3 0日發給J 〇 n e s的美國專利,編號5, 1 2 6, 287 (U.S. Pat. No. 5 , 1 2 6, 287)中所述, 而此兩案例則被合倂於此當作本發明的參考文獻。1 9 9 4 年9月8日發給MacDonald的美國專利,編號5, 3 63, 021(U.S. Pat. No. 5, 363,021)中所述的一體化 的二維陣列的放射結構之優點亦被倂入本案當作一參考 文獻。如於199〇年2月20日發給Jones等人的美國專 請 先 閲 背 \έ 之 注(Please read the back two. Please note the is before filling in *? J line on this page, in another specific embodiment 'this source array includes not only an independent dark (blanking) structure but also independent edges A mirror (one of any source element) is used to focus the particle beam. (稜鏡 and (lens) optics or (lensic) optics are here agreed not to be lenses or light used as light Reflective 稜鏡 is used as an electromagnetic or electrostatic structure for focusing the charged particle beam.) These 稜鏡 are made by additional steps in the production of this source structure. These 稜鏡 are used in In the application of specific particle beam systems. For example, this source lens is matched with this light beam lens for effective beam transmission. In a specific embodiment, an independent deflector is provided to an independent beam. Again, these and so on An independent deflector is produced by additional steps in the production process of this source structure and is integrated in this structure .. A selected light-song deflector; when activated, causes the relevant source 7 Paper ruler Degree applies to the Chinese National Standard (〇1 \ $) of the six 4 specifications (210 father 297 public 漦). Λ7 B7 V. Description of the invention -Generally, the direction of the axis of the particle beam system is changed to a slightly different direction. The deflection is only a few degrees of the entire beam axis, but it will be compared in other specific embodiments. 1 The particles emitted by this source array within the scope of the invention are expected to be electrons or ions. In a specific embodiment using electrons as charged particles, the source of the particles is called A cathode or cathode array is used to emphasize the multiplicity of these independent cathodes. This source array is generally made into an integrated structure. There are many writings about this integrated cathode array, and in these techniques also There are several well-known appropriate radiation technologies and structures, including field emission, negative electron affinity, and thermionic cathodes arranged in an array of emitters. The process for making sub-micron electron emitter arrays was issued on April 6, 1993 to MacDonald et al., U.S. Pat. No. 5, 199, 197 (US Pat. No. 5, 199, 197) And as described in US Pat. No. 5, 1 2 6, 287 (US Pat. No. 5, 1 2 6, 287) issued to Jones on June 30, 1992, and these two Cases are incorporated herein as a reference for the present invention. US Patent No. 5, 3 63, 021 issued to MacDonald on September 8, 1984 (US Pat. No. 5, 363, 021) The advantages of the integrated two-dimensional array radiation structure described in the above are also incorporated into this case as a reference. For example, a U.S. patent issued to Jones and others on February 20, 1990

I 4 頁1 訂 線 本纸張尺度適用中國國家標準(CNS ) Λ4規格(210X2W公敍) Λ7 五 '發明説明(8) 經濟部中央標準局員工消費合作杜印製 利編號 4,902,8 9 8 (U.S. Pat. No. 4, 902, 898 )中所述之用來製作離子放射器列的程序亦被當成 本案的參考文獻。 因此根據本發明,一多束光學系統包括一多束產生 器用來產生電子束的一聚集組合,以及(光)束聚集電 子光學(透鏡)用來視其爲一單一而整體的光束而予以 雙重的加速並導引此束聚集組合到一目標上,例如一半 導體晶片或是光罩材料基材(reticle substrate)' 上。此多束產生器包括一放射陣列(一個場放射器陰極 的陣列),以及一放射控制陣列用來控制此放射電流的 大小,這兩者皆成型在一單一的(例如,矽)基材上。 在一具體實施例中此控制陣列係相隨於此場放射器之後 的一整體化的選用器/空白閃爍器 (extractor/blanker)電極陣列(也.就是,在空間中 係沿著此被放射的光束一序列的)。於一具體實施例中 ,的此多束產生器包括一靜電偏向器陣列,藉由一適當的 數量來偏折此個別的光束,還有在某些具體實.施例中一 相隨的稜鏡陣列亦一體成型在此相同的基材上。 此(光)束的聚集組合(透鏡)光學會考慮在一很 短的完全光束路徑長度中傳輸全部光束電流的相對高準 位的必須性,藉此,後加速此光束巨集組合到一所要的 最後光束能量。此最後的光束能量於是被選擇去降低內 部光束的內部相互作用,藉此允許於此放射陣列及此目 本紙張尺度適用中國國家標準(CNS ) Λ4規格(210X297公釐) 請 先 背 面 Ί 再 填 % 訂 線 Λ7 經濟部中央標準局員工消費合作社印製 五、發明説明(9) 標之間的空間的伸長。藉被增加的長度如此便可能去利 用傳統的電子光學(透鏡)來聚焦及偏向。此光束能量 也被選定使之可以去穿透傳統厚度的光阻材料以便得以 去曝光此光阻並顯影背向散射的訊號,藉以用來決定或 許可能位在光阻之下的對齊標誌之位置。在光束聚集組 合透鏡的元件之構造中也列入考慮的柑反於傳統的虛點 源(qugsi-point source)1的是多束來源(陰極陣· 列)是密集的在它的橫斷面的尺寸上,以及此光束聚集 組合的其他特徵是,例如在目標上的此變動的光束電 流。如根據本發明中所使用的橫斷式密集源其可靠的電 子透鏡投射係已經在電子束投射微影中出現過,請參閱 Μ· B. Her it a g e ’ 在 J _ V a c · S c i. T e chn ο 1 ·,1 2 6 (Nov/Dec 1 9 7 5 ) p p . 1135-1140 及 B. Lischke 等人’在 Op tik 5 4 ( 1 9 7 9 ) ( 4 ) pp . 3 2 5 - 3 4 1 所發 表的文件,此兩文獻也在此被倂爲本案的參考文件。 另外在習知技藝中,依據本發明還有其他的稜鏡及 偏折鏡的設計是適合使k的則另'外還包括活動的接物透 鏡鏡片(Moving Objective Lens)如在 J. Vac. Sci. T e chn ο 1. 15(3) ( M a y / J u n e 1 9 7 8 ) 8 4 9 - 5 2 中 所述;可變軸稜鏡(Variable Axis Lens ),如在J. Vac. Sci. Techno 1. 19(4) (Nov./Dec. 1981) . 105 8-6 3中所述;可變軸.瘴入稜鏡(Variab.le Axis Immersion Lens ),如於 Microcircuit 10 本紙張尺度適用中國國家標準(CNS ) Λ4規格(210X 297公t ) (讀先閱讀背面.之注意事項再填寫本頁) #1I 4 Page 1 Alignment This paper size applies to Chinese National Standard (CNS) Λ4 specification (210X2W public narrative) Λ7 Five 'invention description (8) Consumption cooperation between employees of the Central Standards Bureau of the Ministry of Economic Affairs Du printed profit number 4,902,8 The procedure described in 98 (US Pat. No. 4, 902, 898) for making ion emitter arrays has also been incorporated as a reference in this case. Therefore, according to the present invention, a multi-beam optical system includes a multi-beam generator for generating a focused combination of electron beams, and a (light) beam-focusing electron optics (lens) for dualizing it as a single and integral beam Accelerate and guide the beam to focus and combine on a target, such as a semiconductor wafer or a reticle substrate '. The multi-beam generator includes a radiation array (an array of field emitter cathodes) and a radiation control array to control the amount of this radiation current, both of which are formed on a single (eg, silicon) substrate . In a specific embodiment, the control array is an integrated selector / blanker electrode array following the field emitter (that is, radiated along the space in this space). A sequence of light beams). In a specific embodiment, the multi-beam generator includes an electrostatic deflector array, and the individual beams are deflected by an appropriate number, and in some embodiments, a following edge The mirror array is also integrally formed on this same substrate. The focusing (lens) optics of this (light) beam will consider the necessity of transmitting a relatively high level of all beam currents in a short complete beam path length, thereby accelerating this beam macro combination to a desired Energy of the last beam. This final beam energy was then selected to reduce the internal interaction of the internal beam, thereby allowing the radiation array and the paper size to apply the Chinese National Standard (CNS) Λ4 specification (210X297 mm). Please fill in the back Ί % Order line Λ7 Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs 5. Description of the invention (9) The extension of the space between the targets. By increasing the length, it is possible to use traditional electron optics (lenses) for focusing and deflection. This beam energy is also selected so that it can penetrate the traditional thickness of the photoresist material to expose the photoresist and develop the backscattered signal, which is used to determine the position of the alignment mark that may be located under the photoresist. . Also considered in the structure of the beam-gathering combination lens element is that the multi-beam source (cathode array · array) is dense in its cross section as opposed to the traditional qugsi-point source 1 In terms of size, and other characteristics of this beam-gathering combination, such as this fluctuating beam current on the target. A reliable electron lens projection system such as a transversal dense source used in the present invention has appeared in electron beam projection lithography, see M. B. Her it age 'in J _ V ac · S c i T e chn ο 1 ·, 1 2 6 (Nov / Dec 1 9 7 5) pp. 1135-1140 and B. Lischke et al. 'In Op tik 5 4 (1 9 7 9) (4) pp. 3 2 5-3 4 1 Published documents, these two documents are also cited as reference documents for this case. In addition, in the conventional art, according to the present invention, there are other design of the 稜鏡 and deflection lens are suitable to make k's, in addition to moving objective lens (Moving Objective Lens) as in J. Vac. Sci. T e chn ο 1. 15 (3) (M ay / J une 1 9 7 8) 8 4 9-5 2; Variable Axis Lens, as in J. Vac. Sci. Techno 1. 19 (4) (Nov./Dec. 1981). 105 8-6 3; Variab.le Axis Immersion Lens, as in Microcircuit 10 paper Dimensions are applicable to Chinese National Standards (CNS) Λ4 specifications (210X 297g t) (Read the back and read the precautions before filling this page) # 1

、1T 線_ Λ7 B7 五、發明説明(10)、 1T line_ Λ7 B7 V. Description of the invention (10)

Engineering 83 ( 1 9 8 3 ) 106-16,J. Vac. Sci. T e chn ο 1. B 6 ( 6 ) (Nov./Dec. 1988) 1995-8; J . Vac. Sci. T e c h η ο 1. B 8 8 ( 6 ) (Nov./Dec. 1 9 9 0 ); 1 ό 8 2 - 5等中所述。 上述及其他的本發明之目的、特徵及優點藉由下述 之本發明的細節描述及結合相關圖式說明將會更爲淸楚 顯著。 第一圖係根據本發明的一多束光學(透鏡)系統圖; 第二圖係根據本發明的一多束場放射源的一部份的橫斷 面視圖;,_ . _ _ 第三圖Α所示係一指端形的陰極及第三圖Β所示係一帶狀 陰極(strip cathode);其等係當作第二圖中的來 源; 、 第四圖A係根據本發明的一(光)束聚集組合光學(透 鏡)圖;及_ 第四圖B係光束聚集組合光學(透鏡)的一更詳細的細節 • ·. 圖式。 . 此一多束圖樣產生器包括有一來源它是一個充電粒 子源元素的陣列。一整合的引出器/空白閃爍器 (extra ct or/blank er )電極控制陣列在此等充電粒子 源之後("之後"意味著在空間上序列的沿著此一放射的 充電粒子束或是11下游"的軸),一個具有一電子偏向器 的具體實施例伴隨於後去提供橫斷於此光束路徑之個別 11 本紙張尺度適用中國國家標準(CNS ) A4規格(210X 297公t ) (讀先閱讀背面之注意事項再填寫P頁Engineering 83 (1 9 8 3) 106-16, J. Vac. Sci. T e chn ο 1. B 6 (6) (Nov./Dec. 1988) 1995-8; J. Vac. Sci. T ech η ο 1. B 8 8 (6) (Nov./Dec. 1 9 9 0); 1 ό 8 2-5 etc. The above and other objects, features, and advantages of the present invention will be more apparent through the following detailed description of the present invention and the combination of related drawings. The first diagram is a diagram of a multi-beam optical (lens) system according to the present invention; the second diagram is a cross-sectional view of a portion of a multi-beam field radiation source according to the present invention; _. _ _ Third diagram A shows a finger-shaped cathode and the third figure B shows a strip cathode; these are taken as the source in the second figure; and the fourth figure A is a (Light) beam focusing combination optics (lens) diagram; and _ The fourth figure B series beam focusing combination optics (lens) a more detailed detail • ·. Schematic. This multi-beam pattern generator includes an array of sources which are a source of charged particles. An integrated extractor / blank er electrode control array after these charged particle sources (" after " means a sequence of charged particle beams or Is the axis of the downstream 11), a specific embodiment with an electronic deflector is provided to provide an individual 11 that traverses this beam path. This paper size is applicable to the Chinese National Standard (CNS) A4 specification (210X 297mm t ) (Read the notes on the back before filling in page P

、tT 線 經濟部中央標準局員工消費合作社印装 ΑΊ 、^、__— Β7 五、發明説明(11 ) ~~一 — 的偏向光束’之後在一具體實施例係伴隨有一稜鏡陣列 於後。此一來源陣列結構更與電氣連接(electrical connections)整合藉以適當的控制電子,此等電氣連 1 接提供控制訊號並控制加速電壓,或者此等電氣連接也 可以與此放射器陣列本身部分的整合在—起。此稜鏡陣 列僅爲某些具體實施例所需要,例如若發自此來源元件 的此放射圖樣對此下游光束聚集組合光學(透鏡)的接 收度在其空間或是速度不甚匹配時。 不具此偏向器陣列的此來源陣列可以被用來當作一 II 點矩陣"圖樣產生器,當作微影的應用,誠如列爲本發明 之篸考資料的美國專利4,153,843 (U.s. Patent 4 153,8 4 3 )所述。 經濟部中央標準局員工消費合作社印製 因此在一具體實施例中的多束產生器包括了有在一 來源中之具有被製作在上面的微空白器(micro-blanker) 及微偏向器 (micro-deflector) 的電子場 放射器,的陣列(或是一蕭特基輔助陰極放射器陣列(a Schott ky-assisted cathode emitter array))以. 及一習知設計的電子光學稜鏡藉以形成一陣列影像在一 目標基材上。場放射器用作陰極元件基本上可容許陰極 影像(在無其他的元件下)。習用的多束光學透鏡需要 此陰極之下游的光學元件,然而由此會導致—不希望出 現的偏差的束飄移以及其他的效應。而本多束產生器僅 在(光)束源形成並處理此個別的(光)束,如此被建‘ 12 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) Λ7 B7 五、發明説明(12 ) 構成將(光)束飄移及其他效應最小化。所以此居於下 游的光束聚集組合透鏡以如同它們係單一化般的,也就 是將它們視爲一整體光束般的影響此等光束,因此沒有 任何偏差效果的來源存在於此多束來源其本身之上。 第一圖係被包含在一傳統的眞空箱中(未示.出)的 一多束圖樣產生器系統1的圖形,以及還包括一多束電子 源2 (於此之後被當作是此多束源)它產生電子(光)束 ό的一聚集組合,還有束聚集組合光學(透鏡)4去導引 此(光)束6的聚集組合到一目標上,也就是一工作物 (work piece)或是被固定在一傳統的可移動之χ_γ平. 台(精密運動桌)5之上的一晶圓。習用的回散射電子偵 測器(backscattered electron detector ) 7提供來 偵測由此目標3所散射回的電子。 此多束源2其中僅有一小部份的細節横斷面係如第二 圖所述,包括有配置成,例如一矩形陣列(就未示出的 . 平面束圖而言)的一微陰極的電子場放射陣列202,及, 引出陰極陣列2 0 3。此兩個微陰極陣列2 0 2及引出陰極陣 列2 0 3被成型在一砂基材(或是其他適當的材料)2 0 1 上。陰極202藉由一作用電壓而被帶到一參考電壓Vr。 ' 引出陰極2〇3則藉由一第二作用電壓被帶到一相對於此 參考電壓VR的一正引出電位VE。引出陰極203.中的任一 , 個爲由陰極2 0 1所放射出的電子其通道界定出.一孔。在. 一具體實施例中的多束來源2包括一陽極陣列2 0 4,此陽 13 本纸張尺度適用中國國家標準(CNS ) Λ4規格(210X 297公釐) (請先閲讀背面之注意事項再填寫本頁, TT line Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs ΑΊ, ^, __— B7 V. Description of the invention (11) ~~ — A deflected beam ′ is followed by a specific embodiment with an array of arrays behind. This source array structure is further integrated with electrical connections to provide appropriate control electronics. These electrical connections provide control signals and control the acceleration voltage, or these electrical connections can also be integrated with this radiator array itself From-on. This chirped array is only required for some specific embodiments, for example, if the radiation pattern from this source element is not compatible with its downstream beam-gathering combination optics (lens) in space or speed. This source array without this deflector array can be used as an II-point matrix " pattern generator, as a lithography application, as shown in U.S. Patent No. 4,153,843, which is the reference material for this invention (Us Patent 4 153, 8 4 3). Printed by the Consumer Standards Cooperative of the Central Standards Bureau of the Ministry of Economics. Therefore, the multi-beam generator in a specific embodiment includes a source with a micro-blanker and a micro deflector. -deflector) array of electron field emitters (or a Schottky-assisted cathode emitter array), and a conventionally designed electron optics to form an array The image is on a target substrate. The use of a field emitter as a cathode element basically allows a cathode image (without other elements). Conventional multi-beam optical lenses require optical elements downstream of this cathode, but this can result in undesired beam drift and other effects. The multi-beam generator only forms and processes this individual (light) beam at the (light) beam source, so it is built. '12 This paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) Λ7 B7 V. SUMMARY OF THE INVENTION (12) The composition minimizes (light) beam drift and other effects. Therefore, the downstream beam-concentrating combination lenses act as if they are singular, that is, they are treated as a whole beam to affect these beams, so there is no source of any deviation effect in this multi-beam source itself. on. The first picture is a diagram of a multi-beam pattern generator system 1 contained in a conventional hollow box (not shown.) And also includes a multi-beam electron source 2 (hereafter referred to as the multi-beam (Beam source) It produces a gathering combination of electron (light) beams, and a beam gathering combination optics (lens) 4 to guide the gathering combination of this (light) beam 6 to a target, which is a work (work piece) or a wafer fixed on a traditional movable χ_γ flat table (precision sports table) 5. A conventional backscattered electron detector 7 is provided to detect the electrons scattered by the target 3. Only a small part of the detailed cross section of the multi-beam source 2 is as described in the second figure, and includes a microcathode configured, for example, in a rectangular array (in the case of a planar beam diagram). The electron field emission array 202 and the cathode array 203 are drawn. The two microcathode arrays 202 and the lead-out cathode arrays 203 are formed on a sand substrate (or other suitable material) 203. The cathode 202 is brought to a reference voltage Vr by an applied voltage. The extraction cathode 203 is brought to a positive extraction potential VE with respect to this reference voltage VR by a second applied voltage. Lead out any one of the cathodes 203. A hole is defined by a channel of the electrons emitted by the cathode 201. In a specific embodiment, the multi-beam source 2 includes an anode array 204, and this anode 13 paper size is applicable to the Chinese National Standard (CNS) Λ4 specification (210X 297 mm) (Please read the precautions on the back first Fill this page again

、1T 線 經濟部中央標準局員工消費合作社印製 Λ7Line 1T Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs Λ7

經濟部中央標率局員工消費合作社印製 發明説明(13 ) 極陣列係一加速器並被帶到相對於此引出電壓V E的一正 電位VA且爲此等電子束的通道界定出孔。 在一具體實施例中,偏向器陣列(deflector a r r a y )包括一._ X -偏向器陣列.2 0 5及一具有相關_的整合 控制電子2 3 0的y-偏向器陣列2 0 6皆與自此陽極陣列 ' . ' .... 2 0 4起且相對於此個別的放射光束之傳播方向而整合在 一起且被_定位在下游(downstream ).處(也就是0.1 到10/zm),而根據系統的設計因素,藉由適當的 比例量去偏折此等個別的光束使之橫斷於此光束路徑。 引出電極2 0 3,陽極2 0 4及X,y偏向器電極2 0 5, 2 0 6係以一傳統的1C製造技術形成在基材2 0 1上而成 型一連續的絕緣及傳導層,誠如第二圖所示。此等絕緣 層207,208,209係如二氧化矽或其他在1C製造技藝 中所習知的介電材料。此等傳導層2 0 3,2 0 4,2 0 5及 2 0 6係爲傳統的沉積定型鋁或是其合金,其他的傳導材 料,例如複晶矽,鈦-鈀-金(Ti-Pd-Au ),鈦-鉑-金 ' , ; (Ti-Pt-Au )及鈦-鎢(Ti-W )皆可使用。 由於適當的來源(source)就本技藝而言是眾所週 知的,所以此來源之結構及製.作的更多細節並不在此說 明。請看,例如Epstein等人的美國專利編號5,0 7 0, 2 8 2 ( Epstein et a 1. U. S. Patent No. 5,070, 282),還有Newman等人發表在J.Vac. Sci. Technology,131(4) Oct.-Dec. 1983,pp. 993 的 14 本紙張尺度適用中國國家標準(CNS ) A4規格(210X 297公t ) (諳先聞讀背面之注意事項再填寫本頁) §丨 訂 線; I . Λ7 ___ Β7 五、發明説明(14 ) "點矩陣電子束微影.("Dot Matrix _Ele.ctro.ii beam Lithography".)"等,及 MacDonald 等人在 SRC Workshop ; Dallas, Texas, 1991, p . 241 所發表 的"可定址陣列陰極用作投射電子束微影 ("Addressable Array Cathodes for Projection . .. .. ...... . .... . ··Printed by the Employees' Cooperative of the Central Standards Bureau of the Ministry of Economics. Description of the invention (13) The polar array is an accelerator and is brought to a positive potential VA which leads to the voltage V E and defines a hole for the channel of these electron beams. In a specific embodiment, the deflector array includes a ._X-deflector array. 2 0 5 and a y-deflector array 2 0 6 with integrated control electronics 2 3 0 and From this anode array '.' .... 2 0 4 and integrated with respect to the propagation direction of this individual radiation beam and are positioned _ downstream (that is, 0.1 to 10 / zm). According to the design factors of the system, these individual beams are deflected by an appropriate proportion to make them cross the beam path. The lead-out electrode 2 0 3, the anode 2 0 4 and the X, y deflector electrode 2 05, 2 0 6 are formed on the substrate 2 1 by a conventional 1C manufacturing technology to form a continuous insulating and conductive layer. As shown in the second picture. These insulating layers 207, 208, 209 are, for example, silicon dioxide or other dielectric materials known in 1C manufacturing techniques. These conductive layers 2 0 3, 2 0 4, 2 0 5 and 2 0 6 are traditionally deposited and shaped aluminum or alloys thereof, and other conductive materials such as polycrystalline silicon, titanium-palladium-gold (Ti-Pd -Au), titanium-platinum-gold ', (Ti-Pt-Au) and titanium-tungsten (Ti-W) can be used. Since appropriate sources are well known in the art, the structure and production of this source are not described in more detail here. See, for example, US Patent No. 5,0 7 0, 2 8 2 (Epstein et a 1. US Patent No. 5,070, 282) by Epstein et al., And Newman et al. Published in J. Vac. Sci. Technology, 131 (4) Oct.-Dec. 1983, pp. 993 of 14 This paper size is applicable to the Chinese National Standard (CNS) A4 specification (210X 297 g) (谙 Please read the precautions on the back before filling this page) § 丨 line; I. Λ7 ___ Β7 V. Description of the invention (14) " Dot Matrix _Ele.ctro.ii beam Lithography ". &Quot; etc., and MacDonald et al. SRC Workshop; Dallas, Texas, 1991, p. 241 " Addressable Array Cathodes for Projection ........... .. ···

Electron Beam L i t h o g r a p li y ·’)"等..皆被倂入於此 ' 當作相關的參考文獻,用來說明此來源的結構及製作細 節。 在第二圖中所示的結構,是要去提供於各種放射器 之間的輸出電流及電流變異量的放射穩定性。還有也是 要去擴展此放射器的生命週期使其免於燒毀。是以在本 發明的範圍中便是要設置有贅餘的放射器。在一個具體 實施例中,此放射器係以群組的方式聯合而成,任一個 群組包括至少一個贅餘的放射器元素,而任一道實際的 光束係由此群組中的所有的放射器所發出的放射光所合 .成。因此若有一放射器燒毀,而又要保持一個準位的輸 I · 出電流時,一贅餘的放射器可以用來取代。 因爲任一個個別的電子源(放射器或是陰極元件) 係個別的由空白非空白及偏向所控制,且任一個定義出 一個別的光束並進而可以被用來創建一精緻的紋理圖 樣。因此,在一具體實施例中,例如藉由脈衝調諧 . (p u 1 s e m 〇 d 111 a t i 0 n ) ’對此個別敗射器的電流準位 係被控制成可以去提供一灰階的尺度(可變化強度)效 15 本紙張尺度適用中國國家標準(CNS ) Λ4規格(210X 297公t ) (請先?4讀背δ之注意事項再填窍.尽頁 、?τ 線、 經濟部中央標準局員工消費合作社印製 經濟部中央標準局員工消費合作社印製 Λ7 B7 五、發明説明(15) 應。由於此個別的放射器可以被控制,根據本發明的圖 樣產生器則是容許非常高速產量之圖樣成像的一高速的 平行構造。 微陰極2 0 2是’例如指端形的陰極或是帶狀的,其. 等是一習知技術’誠如分別於第三圖A及第三圖B所例 舉°還有.其他的陰極型態_,例如成讀狀的模形也可使 用。_此帶狀的陰極係在S p a 11 a s .及.MacDonald在 .IEDM. Technical Digest, 1991,中戶斤述,此文章.亦 被列爲參考於下。 第三圖A中描述一指端狀的陰極,一個鈦化鎢 (TiW)的引出陰極3〇3環繞在一矽陰極指端301上。 在第二圖B中描述一帶狀陰極.,一砂基3 10定義出一較低 的矽帶3 1 2,它並由一平行的鈦化鎢引出陰極3 2 4所環 繞。指端狀的陰極是被描述於本技藝中之微陰極的最普 通的型態,帶狀及環狀楔形較此指端狀者具有較大的放 射面積並產生較大的全電流。 微陰極2 0 2係使用一熟知的側向高溫熱氧化程序而 成型。由此而成型的微陰極係先天地,在高度上,外形 及曲率半徑上是爲均勻,還有此引出陰極係自我對齊。 具有非常銳利的指端及非常小的指端到引出電極距離的 陰極,當產生非常大、穩定的平均電流密度時,容許使 用非常低的操作電壓來操作。甩來製作此微陰極的過程 順序係基於被開發來製作矽於絕緣體(SOI)島询過程 16 本紙張尺度適用中國國家標準(CNS ) A4規格(2丨〇/ 297公t ) (請先閱讀背面之注意事項再填寫本頁) 訂 線 經^「部中央標準局員工消費合作社印製 Λ7 B7 五、發明説明(16 ) 順序而來。Spallas 及 MacDonald 在 IEDM Technical Digest, Washington, D.C. 1991,ρρ· 2 0 9所發表的"矽場放射陰極陣列的製作及操作 ("Fabrication and Operation of S i 1 i e on Field E m i s s i o.ii. .C a til o d e A r r a y _s." ) _ "中揭露 了此製程的細 節,此文章並在此被倂爲本案的參考文獻。 —控制的電極陣列(未示出)可以被設置在引出陰 極陣列2 0 3及陽極陣列2 0 4之間,並被帶到相對於此引出 電極的一個負控制電位V c以便去降低此放射電流到部 份的未被控制的放射電流。對某些圖樣產生器的應用來 說,如上述的,一稜鏡陣列(未示出)係沿著此等光束 的方向整合到此偏向器陣列2 0 5、2 0 6下游的多束源2 上。請看美國專利 5, 126,827 (U.S. Patent 5, 126,827)及 Ν· C. MacDonald 等人發表於 Proceeding SPIE 2 5 2 2 (July 1 9 9 5 ) pp . 2 2 0 -2 2 9之有關此種整合的文章,此兩文章也在此被倂爲本 案的參考文獻。此來源結構2係更進一步的對習用的控制 電子220提供有電氣連接(未示出,其係位在本平面圖 式的之外)。控制電子2 2 0對多束源2提供控制訊號及控 制加速電壓,而在一個具體實施例中其係以電路構成, 例如藉由傳統的積體電路製造技術所形成,還有此電路 至少是有部分地被整合到此基材20 1上。 .. (光)束的聚集組合6,係由多束源2所產生,之後‘ 17 本紙張尺度適用中國國家標準(CNS ) A4規格(21〇X 297公摄) (請先閲讀背面之注意事項再填寫本頁) 、1T. 線. 經濟部中央標準局員工消費合作社印製 ______ ^ B7 五、發明説明(”) ' 便通過光聚集組合光學(透鏡)4。第四圖A顯示一般的 光束及組合光學透鏡4之斷面。光束的聚集組合光學(透 鏡)4以一個單元的方式(也就是如同它是一單一的光束 般的),以一個較佳而短的光束路徑由此來源2傳輸光束 聚集組合6到此目標3,進而使此光束的交互作用最小 化。在一具體實施例中的此光束聚集組合光學(透鏡)6 包括有一習用的充電粒子光束加速器401去後加速光束 聚集組合6到一所要的最後(光)束能量,一習用的聚焦 系統(稜鏡)4 0 2用來聚焦(或解焦)(光)束聚集組 合6,還有一習用的χ-γ偏向器4〇4用來偏折光束聚集 組合6到此目標4 0 3的一特定位置上。光束聚集組合光學 (透鏡)4係習用在電子束圖樣產生器中,就算計設計因 素來說,例如本電子源2相反於習用的虛點電子源 (quasi-point electron source)而在其橫斷尺寸上 是密集的,還有一個短的、完全的(光)束路徑長度也 是所希望的,還有其他的(光)束聚集組合的,觀點,例 ' 如變化的光束電流等。由於此光束聚集組合光學(透 鏡)4係以如同它們係爲一單一的(光)束來處理此等 (光)束,因此毫無任何差異效應的原因會存在於此^ 源2的下游處。 第四圖B顯示附加的細節,藉之得以較佳的解釋第四 圖A中的結構.,。粒子源2產生電子光束_,相對於此來源2 ‘ 之中的陰極陣列的一個正電位,其等通過在加速器電極' 本纸張尺度適用中國國家標準.(CNS ) A4規格(210X297公蝥) (請先閱讀背面之注意事項再填寫本頁) 、-° 線 A7 B7 五、發明説明(18 ) 401上的一開口。一個限制小孔(limiting aperture) 4 12則被設置。偏向線圏,之後則由一射透 鏡4 0 2所伴隨。(在此處請注意,此偏向及聚焦稜鏡結 構係與第四圖A中有不同的次序)。目標物未示於第四圖Electron Beam L i t h o g r a p li y · ’) " etc. are all incorporated here as' relevant references to illustrate the structure of this source and the details of its production. The structure shown in the second figure is to provide radiation stability of the output current and the amount of current variation between various radiators. There is also a need to extend the life cycle of this emitter to prevent it from being burned. Therefore, it is within the scope of the present invention to provide a redundant radiator. In a specific embodiment, the radiators are combined in a group manner. Each group includes at least one redundant radiator element, and any actual beam is emitted by all the radiation in the group. The radiation emitted by the device is combined. Therefore, if one radiator is burned and a level of output I · is maintained, a redundant radiator can be used instead. Because any individual electron source (radiator or cathode element) is individually controlled by blank non-blank and deflection, and any one defines a different beam and can then be used to create a delicate texture pattern. Therefore, in a specific embodiment, for example, by pulse tuning. (Pu 1 sem 〇d 111 ati 0 n) 'The current level of the individual defeater is controlled to provide a gray scale ( The intensity can be changed. 15 This paper size is applicable to the Chinese National Standard (CNS) Λ4 specification (210X 297g t) (please read the precautions for δ before reading the δ. Please complete the page, the? Τ line, and the central standard of the Ministry of Economic Affairs Printed by the Consumer Cooperative of the Bureau of the People's Republic of China Printed by the Consumer Standards of the Central Standards Bureau of the Ministry of Economic Affairs Λ7 B7 V. Description of the invention (15) Yes. Since this individual radiator can be controlled, the pattern generator according to the present invention allows very high-speed output A high-speed parallel structure imaged by a pattern. The microcathode 202 is 'for example, a terminal cathode or a strip-shaped cathode, and so on. It is a conventional technique', as shown in Figure 3 and Figure 3, respectively. B is exemplified. There are other types of cathodes, for example, the shape of the reading can also be used. This strip-shaped cathode is in Spa 11 as. And MacDonald in IEDM. Technical Digest, 1991 This article is also listed as a reference for The third figure A depicts a finger-shaped cathode, and a tungsten titanate (TiW) lead-out cathode 303 surrounds a silicon cathode finger end 301. The second figure B describes a strip-shaped cathode., A sand base 3 10 defines a lower silicon ribbon 3 1 2 and is surrounded by a parallel tungsten titanate cathode 3 2 4. Finger-shaped cathodes are described in this art as microcathodes. The most common type, band-shaped and ring-shaped wedges have a larger radiation area and generate a larger full current than the finger-shaped ones. The microcathode 2 0 2 uses a well-known lateral high temperature thermal oxidation process and Molding. The microcathode formed in this way is inherently uniform in height, shape and radius of curvature, and the lead-out cathode system is self-aligned. It has very sharp finger tips and very small finger tips to the lead-out electrode The distance of the cathode, when producing a very large and stable average current density, allows operation with very low operating voltages. The process sequence for making this microcathode is based on the process of developing a silicon-on-insulator (SOI) island 16 This paper size applies to Chinese national standards ( CNS) A4 specification (2 丨 〇 / 297 g t) (Please read the notes on the back before filling this page) Scripture ^ "Printed by the Ministry of Standards Bureau Consumer Cooperatives Λ7 B7 V. Description of the invention (16) Sequence "Sparlas and MacDonald's" Fabrication and Operation of S i 1 ie on Field E missi "published in IEDM Technical Digest, Washington, DC 1991, ρ ·· 2 09 The details of this process are disclosed in o.ii. .C a til ode A rray _s. ") _ ", and this article is hereby incorporated by reference. -The controlled electrode array (not shown) can be placed between the extraction cathode array 203 and the anode array 204, and brought to a negative control potential Vc relative to this extraction electrode in order to reduce this radiation Current to part of uncontrolled radiation current. For some pattern generator applications, as described above, a beam array (not shown) is integrated along the direction of these beams into a multi-beam source downstream of the deflector array 2 05, 2 06 2 on. See U.S. Patent 5,126,827 (US Patent 5,126,827) and NC MacDonald et al. Published in Proceeding SPIE 2 5 2 2 (July 1 9 9 5) pp. 2 2 0 -2 2 9 Articles on such integration are also hereby cited as references in this case. This source structure 2 is for further control of the conventional control electronics 220 (not shown, which is located outside of this plan). The control electron 2 2 provides a control signal and a control acceleration voltage to the multi-beam source 2. In a specific embodiment, it is constituted by a circuit, for example, formed by a traditional integrated circuit manufacturing technology, and the circuit is at least Partially integrated on this substrate 201. .. (light) beam clustering combination 6, generated by multi-beam source 2, then '17 This paper size applies Chinese National Standard (CNS) A4 specification (21〇X 297 photo) (Please read the note on the back first Please fill in this page again), 1T. Line. Printed by the Consumer Cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs ______ ^ B7 V. Description of the invention (") 'Then the optical (lens) is combined by light focusing 4. The fourth figure A shows the general Beam and the cross section of the combined optical lens 4. The focusing of the combined light (lens) 4 is in a unit (that is, as if it is a single beam), with a better and shorter beam path. Source 2 transmits a beam-gathering combination 6 to this target 3, thereby minimizing the interaction of the beam. In a specific embodiment, the beam-gathering combination optics (lens) 6 includes a conventional charged particle beam accelerator 401 to accelerate Beam focusing combination 6 to a desired final (light) beam energy, a conventional focusing system (稜鏡) 4 0 2 is used to focus (or defocus) (light) beam focusing combination 6, and a conventional χ-γ Bias 4〇4 is used to deflect the beam focusing combination 6 to a specific position of this target 403. The beam focusing combination optics (lens) 4 is used in the electron beam pattern generator. For design factors, such as this Electron source 2 is opposite to the conventional quasi-point electron source and is dense in its cross-sectional size. A short, complete (light) beam path length is also desirable, and Other (light) beam-gathering combinations, viewpoints, such as changing beam currents, etc. Because of this beam-gathering combination, optical (lens) 4 systems treat these (light) as if they were a single (light) beam ) Beam, so there is no reason for any difference effect to exist downstream of this source 2. The fourth figure B shows additional details to better explain the structure in the fourth figure A. .. particle source 2 Generate an electron beam_, a positive potential relative to the cathode array in this source 2 ', which passes through the accelerator electrode' This paper size applies Chinese national standards. (CNS) A4 size (210X297 cm) (Please Read the note on the back first Please fill in this page for further information),-° line A7 B7 V. An opening on the 401 (18) 401. A limiting aperture 4 12 is set. It is biased towards the line, and then by a shot lens 4 Accompanied by 0 2. (Please note here that this biased and focused 稜鏡 structure is in a different order from that in Figure 4A.) The target is not shown in Figure 4

I B中。 在另外一個具體實施例中的此多束產生器包括有在 此來源中之具有所被製造的微空白器(micro-blanker) 及微偏向器 (micro-deflector) 的一離子 放射器陣列另有一(習知設計的)加速離子的光學稜鏡 去形成一陣列影像在一目標基材上。在此技藝上一適當 的粒子源是眾所週知的,請看例如Jones等人的美國專 利編號 4, 9 0 2, 9 8 9 ( U. S . Patent No. 4,902, 898),此專利亦在此被列爲本案的參考文獻。(請特 別參閱第八、九、十圖◊)。適當的加速離子光學(透 鏡)結構係本技藝的習用技術。請參閱,例如S t en g 1 '等人的美國專利編號4, 985,634 (U.S. PatentI B. In another embodiment, the multi-beam generator includes an ion emitter array with a micro-blanker and a micro-deflector manufactured in this source. (Conventional design) Accelerates the optical depletion of ions to form an array image on a target substrate. A suitable particle source is well known in this art. See, for example, U.S. Patent No. 4,902, 898 to Jones et al. It is hereby incorporated by reference. (Please refer in particular to Figures VIII, IX, and XX). Appropriate accelerated ion optics (lens) structures are conventional techniques in this art. See, for example, US Patent No. 4,985,634 (U.S. Patent

No· 4,985,634),在此也被倂爲本案的參考文獻。 本發明是適用於各種應用包括微影,檢視及顯微鏡 檢測。其中充電粒子束需要具有高解析度,高平均電流 及(光)束控制。 經濟部中央標準局員Η消費合作社印製 (.請先閱讀背面之注意事項.再填离本頁) 線- 雖然本發明已經藉特定的具體實施例加以敘述及舉 例’但可淸楚了解這只是舉例說明,本發明並不受限於 此笋例示。本發明的精神及範圍則如所附申請專利範圍 所示。 19 本紙張尺度適用中國國家標準(CNS ) Λ4規格(210X 297公綠)No. 4,985,634), also referred to herein as a reference. The invention is suitable for various applications including lithography, inspection and microscopy. The charged particle beam needs to have high resolution, high average current and (light) beam control. Printed by a member of the Central Standards Bureau of the Ministry of Economic Affairs and a Consumer Cooperative (Please read the notes on the back. Then leave this page) Line-Although the present invention has been described and exemplified by specific embodiments, it is clear that this is only By way of illustration, the present invention is not limited to this bamboo shoot illustration. The spirit and scope of the present invention are shown in the scope of the attached patent application. 19 This paper size applies to Chinese National Standard (CNS) Λ4 specification (210X 297 male green)

Claims (1)

S Π 〇5 7 4 9 Α8 Β8 C8 D8 經濟部中央榡準局員工消#合作、社印製 申請專利範圍 1. 一種圖樣產生器,包括: 一電子來源,該來源包括一個別之場放射元素的陣列, 任一個該元素產生一個別的電子束; 一束聚集組合光學(透鏡)被設置並當作一聚集組合來 ..... 1 接收該等個別的電子束去加速及控制該等假別的電子 束;及 * 一目標位置坐落在該束聚集組合透鏡,導引集中該等束 的聚集組合之處。 2 .如申請專利範圍第1項所述的圖樣產生器,其中該等個別 之放射元素的陣列是一個二維陣列。 3 .如申g靑專利範圍第1項所述的圖樣產生器’其中任一個該 放射元素係獨立地明暗閃爍(空白及非空白)。 4 .如申請專利範圍第1項所述的圖樣產生器,其中該電子來 源亮暗閃爍該群的放射元素。 5 .如申請專利範圍第1項所述的圖樣產生器,其中任一個該 放射元素係被供應有一來源電位,以及任一個該放射元 素的該來源電位係被獨立的控制。 6 .如申請專利範圍第1項所述的圖樣產生器,其中任一個該 放射元素係被供應有一引出電位),以及任一個該放射 元素的該引出電位係被獨立的控制。 > 7 ·如申請專利範圍第1項所述的圖樣產生器,相關於任一個 該放射元素更包括一獨立的偏向元素用來偏向由該放射 元素所放射出的電子。 20 (請先閎讀背面之注意事項再填寫本頁)S Π 〇5 7 4 9 Α8 Β8 C8 D8 Employees of the Central Bureau of Standards and Quarantine Bureau of the Ministry of Economic Affairs # Cooperation and printing of the patent application scope 1. A pattern generator, including: an electronic source, the source includes a radioactive element from another field Array, any one of the elements generates another electron beam; a beam-combining combination optics (lens) is set up and used as a beam-combining combination ..... 1 receives the individual electron beams to accelerate and control the False electron beams; and * A target position is located at the beam-combining-combining lens, which guides the focused combination of these beams. 2. The pattern generator according to item 1 of the scope of patent application, wherein the array of the individual radioactive elements is a two-dimensional array. 3. Any of the pattern generators described in item 1 of the patent scope of claim g ', the radioactive element blinks independently (blank and non-blank). 4. The pattern generator according to item 1 of the scope of the patent application, wherein the electron source flashes the radioactive elements of the group brightly and darkly. 5. The pattern generator according to item 1 of the scope of patent application, wherein any one of the radioactive elements is supplied with a source potential, and the source potential of any of the radioactive elements is independently controlled. 6. The pattern generator according to item 1 of the scope of the patent application, wherein any one of the radioactive elements is supplied with an extraction potential), and the extraction electric potential system of any of the radiation elements is independently controlled. > 7 · The pattern generator described in item 1 of the scope of patent application, which relates to any one of the radioactive elements further includes an independent biasing element for biasing the electrons emitted by the radioactive element. 20 (Please read the notes on the back before filling in this page) ^&度通用中~ 國國家標隼(〇奶)六4規格(210父297公釐) 經濟部中央標率局員工消費合作社印製 A8 BS , G8 DS 々、申請專利範圍 8 ·如申請專利範圍第1項所述的圖樣產生器,更包括與該電 .子來源整合在一起的一偏向器陣列,用來偏折個別的電. 子束。 9.如申請專利範圍第8項所述的圖樣產生器,其中該偏向器 陣列包括與任一假該等個別的放射元素相關聯的第一及 第二偏向器用來將發自該放射元素的該電子束偏折成兩 個正交_(. orthogonal)的方向_。 1 0 .如申請專利範圍第1項所述的圖樣產生器,更包括與該 電子來源整合在一起的一加速器陣列用來個別地加速該 等電子束。 ]1 .如申請專_範圍第1項所述的圖樣產生器,其中該束聚 集組合光學(透鏡)包括一偏向器用來偏折整個該等個 別的電子束之聚集組合。 12.如申請專利範爵第7項所述的圖樣產生器,其中該偏向 器係本質上等同地偏折任一個該電子束。 1 3 .如申請專利範圍第1項所述的圖樣產生器,其中該束聚 集組合光學(透鏡)包括一聚焦元件用來聚焦餐個該等 個別的電子束之聚集組合。 1 4 ·如申請專利範圍第1項所述的圖樣產生器,其中該束聚 集組合光學(透鏡)藉由一加速器元件加速該等個別的 電子束。 1 5 ·如申請專利範圔第1項所述的圖樣產生器,其中該圖樣 產生器藉由一向量掃描而在工作物上形成一圖'樣。. 本纸張尺度適用中國國家標準(CNS ) A4规格(21 〇 X 297公釐) (請先閲讀背面之注告2事項再填寫本頁) 、言 線 A8 B8 386248 .___S___^________— 六、申請專利範園 1 6 .如申請專利範圍第1項所述的圖樣產生器,其中該圖樣 產生器藉由一光柵掃描而在工作物上形成—圖樣。' 1 7 .如申請專利範圍第1項所述的圖樣產生器’其中該目標 位置係一基材的一支撐物。 , . ' 18. —種用來提供一多束聚集組合之方法’包括下述步驟:_ 提供一電子的場放射源其係配置來產生一多束於一陣列 .中: 操縱產生自該陣列中的個別的電子束在一密切接近於該 放射源之處;及 之後如同該多束係一單一電子束一般的導引並加速該被 操縱的多束到一目標上。 19. 如申請專利範圍第18項所述的方法,其中該操縱步驟包 括引出該等個別的電子束。 2 0 .如申請專利範圍第1 8項所述的方法,其中該操縱步驟包 括獨立地加速該等個別的電子束。 2 1 .如申請專利範圍第1 8項所述的方法,其中該操縱步驟包 括獨立地偏折該等個別的電子束橫向(transversely)於 該等個別的電子束的一傳播方向。 2 2 .如申請專利範圍第1 8項所述的方法,其中加速步驟包括 加速該多束到一預定的最後能量。 經濟部中央標準局員工消費合作社印装 2 3 .如申請專利範圍第1 8項所述的方法,其中該導引步驟包 括聚焦該多束到該目標上,。 2 4 .如申請專利範圍第1 8項所述的方法,其中該導引步驟 包括偏折該多束到該目標的一特定位置上。 22 本紙張尺度適用中國K家標準(CNS ) A4規格(210X297公釐)^ & General Chinese ~ National standard (0 milk) 6 4 specifications (210 father 297 mm) Printed by the Consumer Standards Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs A8 BS, G8 DS 々, patent scope 8 · If applied The pattern generator described in the first item of the patent scope further includes an array of deflectors integrated with the electric source to deflect individual electric beams. 9. The pattern generator according to item 8 of the scope of the patent application, wherein the deflector array includes first and second deflectors associated with any of the individual radioactive elements to use the The electron beam is deflected into two orthogonal directions (. Orthogonal). 10. The pattern generator according to item 1 of the scope of the patent application, further comprising an accelerator array integrated with the electron source for individually accelerating the electron beams. ] 1. The pattern generator as described in item 1 of the application, wherein the beam-concentrating combination optics (lens) includes a deflector for deflecting the entire combination of these individual electron beams. 12. The pattern generator of claim 7, wherein the deflector essentially deflects any one of the electron beams equally. 1 3. The pattern generator as described in item 1 of the scope of the patent application, wherein the beam-concentrating combination optics (lens) includes a focusing element for focusing the focusing combination of the individual electron beams. 1 4 The pattern generator according to item 1 of the scope of patent application, wherein the beam-concentrating combination optics (lens) accelerates the individual electron beams by an accelerator element. 1 5. The pattern generator according to item 1 of the patent application, wherein the pattern generator forms a pattern on the work by a vector scan. . This paper size applies to China National Standard (CNS) A4 specification (21 〇X 297 mm) (please read the note 2 on the back before filling out this page), speech line A8 B8 386248 .___ S ___ ^ ________— VI. Patent application park 16. The pattern generator according to item 1 of the patent application scope, wherein the pattern generator forms a pattern on a work by a raster scan. '17. The pattern generator according to item 1 of the scope of patent application ', wherein the target position is a support of a substrate. '. 18. A method for providing a multi-beam clustering combination' includes the following steps: _ providing an electron field radiation source configured to generate a multi-beam in an array. In: manipulation generated from the array The individual electron beams in it are in close proximity to the radiation source; and thereafter, the multiple beams are guided as a single electron beam and accelerated to the target. 19. The method of claim 18, wherein the manipulating step includes eliciting the individual electron beams. 20. The method of claim 18, wherein the manipulating step includes independently accelerating the individual electron beams. 2 1. The method as described in item 18 of the scope of patent application, wherein the manipulation step includes independently deflecting the individual electron beams transversely in a propagation direction of the individual electron beams. 22. The method of claim 18, wherein the step of accelerating comprises accelerating the plurality of beams to a predetermined final energy. Printed by the Consumer Standards Cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs 2 3. The method as described in item 18 of the scope of patent application, wherein the guiding step includes focusing the multi-bundle onto the target. 24. The method as described in claim 18, wherein the guiding step includes deflecting the plurality of beams to a specific position of the target. 22 This paper size is applicable to China K-house standard (CNS) A4 specification (210X297 mm)
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