201222119 六、發明說明: 本發明主張各自於2010年4月30日申請且題為「電致變 色裝置(Electrochromic Devices)」之美國申請案第 12/772,055號及第12/772,075號之權利及優先權,該等申請 案中之每一者係以全文引用方式併入。 • 【先前技術】 電致變色為一種現象,其中材料在處於不同電子能態下 (通常藉由經受電壓變化)時展現光學性質上的可逆之以電 化學為媒介之變化。光學性質通常為色彩、透射率、吸光 度及反射率中之一或多者。舉例而言,一種熟知電致變色 材料為氧化鎢(WO3)。氧化鎢為陰極電致變色材料,其中 藉由電化學還原而發生著色過渡(藍色可透過)。 電致變色材料可併入至(例如)窗及鏡子中。此等窗及鏡 子之色彩、透射率、吸光度及/或反射率可藉由誘發電致 變色材料之變化來改變。舉例而言,電致變色材料之一個 热知應用為一些汽車中之後視鏡。在此等電致變色後視鏡 中,鏡子之反射率在夜間改變,使得其他車輛之前照燈不 分散駕駛者之注意力。 ' 儘管電致變色係在1960年代發現,但遺憾地,電致變色 裝置仍遭受各種問題且尚未開始實現其全部商業潛能。需 要電致變色技術、設備及製造及/或使用該等設備之相關 方法之進步。 【發明内容】 典型電致變色裝置包括由對離子高度傳導且對電子高度 155961.doc 201222119 抵抗之離子傳導(「IC」)層分離的電致變色(「ec」)電極 層及反電極(「CE」)層。換言之’該離子傳導層准許離子 之輸送’但阻斷電流。如通常所理解,該離子傳導層因此 防止該電致變色層與該反電極層之間的短路。該離子傳導 層允許電致變色電極及反電極保持電荷,且藉此維持其複 色狀態或著色狀態。在習知電致變色裝置中,該等組件形 成堆疊’其中及離子傳導層爽在該電致變色電極與該反電 極之間。此等三個堆疊組件之間的邊界由組成及/或微結 構之突然變化界定β因此,該等裝置具有具兩個突變界面 之二個相異層。 相當令人吃驚地,發明者已發現,可在不沈積離子傳導 電絕緣層之情況下製造高品質電致變色裝置。根據特定實 施例,反電極及電致變色電極係在不分離地沈積離子傳導 層之情況下彼此緊接鄰近地形成(常常直接接觸)。咸信, 各種製造程序及/或物理或化學機制在接觸之電致變色層 與反電極層之間產生界面區,且此界面區起到習知裝置中 之離子傳導電絕緣層的至少一些功能。下文描述可能為形 成界面區之關鍵之特定機制。 該界面區通常(儘管不必)具有包括由不同相及/或組成表 不之至少兩種離散組份之異質結構。此外,該界面區可包 括此等兩種或兩種以上離散組份中之梯度。該梯度可提供 (例如)可變之組成、微結構、電阻率、摻雜劑濃度(例如, 氧濃度)及/或化學計量。 除了以上發現之外,發明者還觀察到,為了改良裝置可 155961.doc 201222119 靠性’可製造電致變色裝置之兩個層(電致變色(EC)層及 反電極(CE)層)以使其各自包括已定義量之鋰,另外,電 致變色裝置之一些組件之材料及形態及/或微結構之小心 選擇提供效能及可靠性之改良。在一些實施例中,裝置之 所有層全部為固體且無機的。 與以上觀察及發現一致’發明者已發現,EC-IC-CE堆疊 之形成無需以習知序列(EC—IC—>CE或CE—>IC-»EC)進行, 而可在電致變色層及反電極層之形成之後形成充當1(:層的 離子傳導電絕緣區。亦即,首先形成EC-CE(或CE-EC)堆 疊’接著在EC層及CE層之界面處使用該等層中之一者或 兩者之組伤在EC層與CE層之間形成起到ic層之一些用途 之界面區。本發明之方法不僅藉由消除一或多個處理步驟 而減少製造複雜性及費用,且提供展示改良之效能特性之 裝置。 因此,本發明之一態樣為一種製造電致變色裝置之方 法,該方法包括:形成包括電致變色材料之電致變色層; 形成與該電致變色層接觸之反電極層,而並不首先在該電 致變色層與該反電極層之間提供離子傳導電絕緣層;及在 該電致變色層與該反電極層之間形成界面區,其中該界面 區為實質上離子傳導且實質上電絕緣的、該電致變色層及 該反電極層通常(但不必)由比該界面區導電性更強但可能 具有一定抗電子特性之一或多種材料製成。該界面區可含 有忒EC層及/或該CE層之組份材料,且在一些實施例中, 該EC層及該CE層含有該界面區之組份材料。在一實施例 155961.doc 201222119 中’該電致變色層包括W03。在一些實施例中,該EC層包 括WO3,該CE層包括氧化鎳鎢(Niw〇),且該1〇:層包括鎢 酸鋰(Li2W〇4)。 可在該電致變色層之至少一部分之沈積期間應用加熱。 在一實施例中’在該EC層包括w〇3之情況下,在經由濺鍵 進行之一系列沈積中之每一者之後應用加熱以便形成具有 貫質上多晶微結構之EC層。在一實施例中,該電致變色層 之厚度在約300 nm與約600 nm之間,但該厚度可取決於預 期在沈積該EC-CE堆疊之後形成該界面區之所要結果而改 變。在一些實施例中’ w〇3為實質上多晶的。在一些實施 例中’可使用W〇3之富氧層作為該界面區之前驅體。在其 他實施例中,該WO3層為層中具有變化之氧濃度之分級 層。在一些實施例中,鋰為用於驅動電致變色過渡之較佳 離子種類,且描述了堆疊或層鋰化方案。形成參數及層特 性之詳細内容將在下文予以更詳細地描述。 本發明之另一態樣為一種製造電致變色裝置之方法,該 方法包括:(a)形成包括電致變色材料之電致變色層或包括 反電極材料之反電極層;⑻在該電致變色層或該反電極層 上方形成中間層,其中該中間層包括該電致變色材料、1 反電極材料及額外材料中之至少一者之富氧形式,其中咳 額外材料包括相異之電致變色材料及/或反電極材料 中間層不為實質上電絕緣的;(c)形成該電致變色層及該反 :極層中之另一者;及⑷允許該中間層之至少一部分變: 實質上電絕緣及實質上離子傳導。用於此方法之形成參數 155961.doc 201222119 及層特性之詳細内容亦將在下文予以更詳細地描述。 本發明之另一態樣為一種用於製造電致變色裝置之設 備,其包括.整合式沈積系統,其包括:(丨)含有材料源之 第一沈積台’其經組態以沈積包括電致變色材料之電致變 色層,及(ii)第二沈積台’其經組態以沈積包括反電極材 料之反電極層;及控制器’其含有用於以在基板上順序地 沈積堆疊之方式傳遞該基板經過該第一沈積台及該第二沈 積台之程式指令,該堆疊具有夾在該電致變色層與該反電 極層之間的中間層,其中該第一沈積台及該第二沈積台中 之任一者或兩者亦經組態以在該電致變色層或該反電極層 上方沈積該中間層,且其中該中間層包括該電致變色材料 或該反電極材料之富氧形式,且其中該第一沈積台及該第 二沈積台串聯互連且可操作以將基板自一個台傳遞至下一 個台而不將該基板曝露於外部環境。在一實施例中,本發 明之設備可操作以將該基板自一個台傳遞至下一個台而不 破壞真空’且可包括可操作以將來自含鋰材料源之鋰沈積 在》亥電致變色裝置之一或多個層上之一或多個經化台。在 實施例中,本發明之設備可操作以在建築玻璃基板上沈 積•亥電致變色堆疊。本發明之設備無需具有用於製造離子 傳導層之單獨標乾。 本發明之另-態樣為一種電致變色裝置,其包括:⑷包 括電致變色材料之電致變色層;(b)包括反電極材料之反電 =層及⑷在該電致變色層與該反電極層之間的界面區, “中該界面區包括電絕緣離子傳導材料及該電致變色材 15596l.doc 201222119 料、該反電極材料及額外材料中之至少一者,其中該額外 材料包括相異之電致變色材料及/或反電極材料。在一些 實施例中,未包括該額外材料;在此等實施例中,該界面 區包括該電致變色材料及該反電極材料中之至少一者。該 界面區之組成及形態及/或微結構之變化將在本文中予以 更詳細地描述。本文中所描述之電致變色裝置可併入至窗 (在一實施例中’建築玻璃鱗片窗(glass scale window:〇 中。 本發明之此等及其他特徵及優點將參看相關聯圖式在下 文予以更詳細地描述。 【實施方式】 以下詳細描述可在結合圖式考慮時得到更全面理解。 圖1A為描繪習知電致變色裝置堆疊ι〇〇之示意性橫截 面。電致變色裝置100包括基板1〇2、導電層(CL)1〇4、電 致變色(EC)層106 '離子傳導(ic)層1〇8、反電極(CE)層110 及導電層(CL)112。將元件1〇4、1〇6、1〇8、110及112共同 稱為電致變色堆疊114。通常,該等CL層係由透明導電氧 化物製成’且通常被稱為「TC0」層。由於TCO層為透明 的’故EC-IC-CE堆疊之著色行為可(例如)經由tc〇層觀 測,從而允許在窗上使用此等裝置以獲得可逆遮光。可操 作以跨電致變色堆疊114施加電位之電壓源丨16實現電致變 色裝置自(例如)褪色狀態(亦即,透明)至著色狀態之過 渡。該等層之次序相對於基板可顛倒。亦即,該等層可處 於以下次序:基板、透明導電層、反電極層、離子傳導 155961.doc 201222119 層、電致變色材料層及(另一)透明導電層。 再次參看圖1A’在製造電致變色堆疊之習知方法中,個 別層係以如圖1A之左側之示意圖中所描繪之順序格式沈積 在另一層之上。亦即’ TCO層104沈積在基板1〇2上。接 著,EC層106沈積在TCO 104上。接著,1C層108沈積在EC 層106上’繼之以CE層110沈積在ic層108上,且最後TCO 層112沈積在CE層11〇上以形成電致變色裝置1〇〇。當然, 步驟之次序可顛倒以形成「反向」堆疊,但要點在於,在 習知方法中,1C層必須沈積在EC層上、繼之以CE層沈積 在1C層上’或1C層沈積在CE層上、繼之以EC層沈積在1C 層上。堆疊中之材料層之間的過渡為突然的。 以上程序之一顯著挑戰為形成IC層所需之處理。在一些 先前方法中’ 1C層係藉由難以併入至用以形成ec層及CE 層之CVD或PVD製程中之溶膠凝膠製程形成。此外,藉由 溶膠凝膠及其他基於液體之製程產生之1(:層易於具有降低 裝置之品質且可能需要藉由(例如)雕刻移除之缺陷。在其 他方法中’ 1C層係藉由pvd自可能難以製造及使用之陶瓷 標乾沈積。 圖1B為描繪材料%組成對圖1A之電致變色堆疊中之位置 (即層106、108及11〇 ’亦即,EC層、IC層及CE層)的曲線 圖°如所提及’在習知電致變色堆疊中,堆疊中之材料層 之間的過渡為突然的《舉例而言,EC材料1〇6經沈積為相 異層而很少或沒有至鄰近1C層之組合物滲流。類似地,ic 材料108及CE材料11〇在組成上相異而很少或沒有至鄰近層 15596l.doc 201222119 之滲流。因此’該等材料為實質上均質的(下文所描述之 CE材料之特定組合物除外)且具有突變界面。習知思想為 s亥二個層中之每一者應作為相異之均勻沈積且平滑之層而 敷設以形成堆疊。每一層之間的界面應為「清楚的」,其 中界面處存在來自每一層之材料之很少互混。 一1熟習此項技術者可認識到,圖1B為理想化描繪,且 在貫踐意義上,層界面處存在一定程度上不可避免的材料 混合。要點在於’在習知製造方法中,任何此混合為非故 意且最少的。發明者已發現,可形成充當IC層之界面區, 其中界面區有意包括大量的一或多種電致變色材料及/或 反電極材料。此為自習知製造方法之根本偏離。 如上文所提及’發明者已發現’ EC-IC-CE堆疊之形成不 必以習知序列(EC —IC —CE或CE—IC—EC)進行,而是可在 電致變色層及反電極層之沈積之後形成充當離子傳導層之 界面區域。亦即’首先形成EC-CE(或CE-EC)堆疊,接 著’在該等層之界面處使用該等層(在一些實施例中,及/ 或另一電致變色材料或反電極材料)中之一者或兩者之組 份在EC層與CE層之間形成界面區(其可擁有IC層之至少一 些功能)。該界面區起到習知1C層之至少一些功能,此係 因為該界面區為實質上離子傳導且實質上電絕緣的。然 而’應注意,如所描述之界面區可具有高於習知所接受之 漏電流的漏電流’但儘管如此,該等裝置展示良好效能。 在一實施例中’電致變色層經形成而具有富氧區,該富 氧區在沈積反電極層之後在後續處理時轉換成充當IC層之 155961.doc -10· 201222119 界面區或層。在-些實施例中,使用包括電致變色材料之201222119 VI. INSTRUCTIONS: The present invention claims the rights and priority of US Application Nos. 12/772,055 and 12/772,075, filed on Apr. 30, 2010, entitled "Electrochromic Devices" Each of these applications is incorporated by reference in its entirety. • [Prior Art] Electrochromism is a phenomenon in which a material exhibits a reversible electrochemical change in optical properties when it is in a different electronic energy state (usually by undergoing a voltage change). Optical properties are typically one or more of color, transmittance, absorbance, and reflectance. For example, one well known electrochromic material is tungsten oxide (WO3). Tungsten oxide is a cathodic electrochromic material in which a color transition (blue permeable) occurs by electrochemical reduction. Electrochromic materials can be incorporated into, for example, windows and mirrors. The color, transmittance, absorbance and/or reflectivity of such windows and mirrors can be varied by inducing changes in the electrochromic material. For example, one of the well-known applications of electrochromic materials is the rearview mirrors in some automobiles. In these electrochromic rearview mirrors, the reflectivity of the mirror changes at night, so that other vehicle headlights do not distract the driver. Although electrochromic was discovered in the 1960s, unfortunately, electrochromic devices still suffer from various problems and have not yet begun to realize their full commercial potential. Advances in electrochromic technology, equipment and related methods of manufacturing and/or using such equipment are required. SUMMARY OF THE INVENTION A typical electrochromic device includes an electrochromic ("ec") electrode layer and a counter electrode separated by an ion-conducting ("IC") layer that is highly conductive to ions and resistant to an electron height of 155961.doc 201222119 (" CE") layer. In other words, the ion conducting layer permits ion transport but blocks current flow. As is generally understood, the ion conducting layer thus prevents short circuits between the electrochromic layer and the counter electrode layer. The ion conducting layer allows the electrochromic electrode and the counter electrode to retain charge and thereby maintain their complex or colored state. In conventional electrochromic devices, the components form a stack' wherein the ion conducting layer is between the electrochromic electrode and the counter electrode. The boundaries between these three stacked components are defined by abrupt changes in composition and/or microstructure. Thus, the devices have two distinct layers with two abrupt interfaces. Quite surprisingly, the inventors have discovered that high quality electrochromic devices can be fabricated without the deposition of ionically conductive electrically insulating layers. According to a particular embodiment, the counter electrode and the electrochromic electrode are formed adjacent to each other (often in direct contact) without the separate deposition of the ion conducting layer. A variety of manufacturing processes and/or physical or chemical mechanisms create an interface region between the contacting electrochromic layer and the counter electrode layer, and this interface region functions as at least some of the functions of the ion conducting electrically insulating layer in conventional devices. . The following describes specific mechanisms that may be key to forming an interface zone. The interfacial region typically, although not necessarily, has a heterostructure comprising at least two discrete components that are represented by different phases and/or compositions. Additionally, the interface region can include gradients in two or more discrete components. The gradient can provide, for example, a variable composition, microstructure, resistivity, dopant concentration (e.g., oxygen concentration), and/or stoichiometry. In addition to the above findings, the inventors have observed that in order to improve the device, two layers (electrochromic (EC) layer and counter electrode (CE) layer) of the electrochromic device can be fabricated by the method of 155961.doc 201222119. Each of them includes a defined amount of lithium, and in addition, careful selection of materials and morphology and/or microstructure of some components of the electrochromic device provides an improvement in performance and reliability. In some embodiments, all layers of the device are all solid and inorganic. Consistent with the above observations and findings, the inventors have discovered that the formation of the EC-IC-CE stack does not need to be performed by conventional sequences (EC-IC->CE or CE->IC-»EC), but can be electro After the formation of the color-changing layer and the counter-electrode layer, an ion-conducting electrically insulating region serving as 1 (: layer is formed. That is, an EC-CE (or CE-EC) stack is first formed] and then the interface is used at the interface between the EC layer and the CE layer. One or both of the equal layers form an interface region between the EC layer and the CE layer for some use of the ic layer. The method of the present invention not only reduces manufacturing complexity by eliminating one or more processing steps And a device for providing improved performance characteristics. Accordingly, one aspect of the present invention is a method of fabricating an electrochromic device, the method comprising: forming an electrochromic layer comprising an electrochromic material; The electrochromic layer contacts the counter electrode layer without first providing an ion conductive electrically insulating layer between the electrochromic layer and the counter electrode layer; and forming between the electrochromic layer and the counter electrode layer An interface region, wherein the interface region is substantially ion conducting and The substantially electrically insulating, electrochromic layer and the counter electrode layer are typically, but not necessarily, made of one or more materials that are more conductive than the interface region but may have some electrical resistance. The interface region may contain germanium. The EC layer and/or the component material of the CE layer, and in some embodiments, the EC layer and the CE layer contain component materials of the interface region. In an embodiment 155961.doc 201222119 'the electrochromic The layer comprises W03. In some embodiments, the EC layer comprises WO3, the CE layer comprises nickel tungsten oxide (Niw〇), and the layer comprises lithium tungstate (Li2W〇4). Heating is applied during deposition of at least a portion of the layer. In one embodiment 'in the case where the EC layer comprises w〇3, heating is applied after each of a series of depositions via a splash bond to form a continuum An epitaxial microstructure of the EC layer. In one embodiment, the electrochromic layer has a thickness between about 300 nm and about 600 nm, but the thickness may depend on the formation of the EC-CE stack after deposition. The desired result of the interface area changes. In some embodiments ' w 〇 3 is substantially polycrystalline. In some embodiments 'an oxygen-rich layer of W 〇 3 can be used as the interface precursor. In other embodiments, the WO 3 layer has a varying oxygen in the layer a grading layer of concentration. In some embodiments, lithium is the preferred ionic species for driving electrochromic transitions, and a stack or layer lithiation scheme is described. Details of the formation parameters and layer characteristics will be described in more detail below. Another aspect of the present invention is a method of fabricating an electrochromic device, the method comprising: (a) forming an electrochromic layer comprising an electrochromic material or a counter electrode layer comprising a counter electrode material; (8) Forming an intermediate layer over the electrochromic layer or the counter electrode layer, wherein the intermediate layer comprises an oxygen-rich form of at least one of the electrochromic material, the counter electrode material, and an additional material, wherein the cough additional material comprises a difference The intermediate layer of electrochromic material and/or counter electrode material is not substantially electrically insulating; (c) forming the other of the electrochromic layer and the counter electrode layer; and (4) allowing at least the intermediate layer Part of the change: Substantially electrically insulating and substantially ion conducting. The details of the formation parameters for this method 155961.doc 201222119 and the layer characteristics are also described in more detail below. Another aspect of the invention is an apparatus for fabricating an electrochromic device comprising: an integrated deposition system comprising: (丨) a first deposition station containing a source of material configured to deposit including electricity An electrochromic layer of a color-changing material, and (ii) a second deposition station configured to deposit a counter electrode layer comprising a counter electrode material; and a controller 'containing a layer for sequentially depositing the stack on the substrate Passing the substrate through the first deposition stage and the second deposition stage, the stack has an intermediate layer sandwiched between the electrochromic layer and the counter electrode layer, wherein the first deposition stage and the first Either or both of the deposition stations are also configured to deposit the intermediate layer over the electrochromic layer or the counter electrode layer, and wherein the intermediate layer comprises the electrochromic material or the counter electrode material is rich An oxygen form, and wherein the first deposition station and the second deposition station are interconnected in series and are operable to transfer the substrate from one station to the next without exposing the substrate to an external environment. In one embodiment, the apparatus of the present invention is operable to transfer the substrate from one station to the next without breaking the vacuum' and may include operable to deposit lithium from a source of lithium-containing material in the electrochromic One or more chemistries on one or more layers of the device. In an embodiment, the apparatus of the present invention is operable to deposit an electrochromic stack on a building glass substrate. The apparatus of the present invention does not require a separate stem for the fabrication of the ion conducting layer. Another aspect of the invention is an electrochromic device comprising: (4) an electrochromic layer comprising an electrochromic material; (b) an anti-electrode layer comprising a counter electrode material; and (4) in the electrochromic layer An interface region between the counter electrode layers, wherein the interface region comprises at least one of an electrically insulating ion conductive material and the electrochromic material, the counter electrode material and an additional material, wherein the additional material Including a dissimilar electrochromic material and/or a counter electrode material. In some embodiments, the additional material is not included; in such embodiments, the interfacial region comprises the electrochromic material and the counter electrode material At least one of the changes in composition and morphology and/or microstructure of the interface region will be described in more detail herein. The electrochromic device described herein can be incorporated into a window (in an embodiment, 'architecture Glass scale window: The same and other features and advantages of the present invention will be described in more detail below with reference to the associated drawings. [Embodiment] The following detailed description can be incorporated in the drawings. Figure 1A is a schematic cross-section depicting a stack of conventional electrochromic devices. Electrochromic device 100 includes substrate 1 2, conductive layer (CL) 1〇4, electro-induced Color change (EC) layer 106 'ion conduction (ic) layer 1〇8, counter electrode (CE) layer 110 and conductive layer (CL) 112. The elements 1〇4, 1〇6, 1〇8, 110 and 112 are common This is called electrochromic stack 114. Typically, these CL layers are made of a transparent conductive oxide 'and are often referred to as 'TC0' layers. Since the TCO layer is transparent', the coloring behavior of the EC-IC-CE stack This can be observed, for example, via a tc layer to allow for the use of such devices on the window to achieve reversible shading. The voltage source 丨 16 that is operable to apply a potential across the electrochromic stack 114 effects the electrochromic device from, for example, fading The transition from the state (ie, transparent) to the colored state. The order of the layers can be reversed relative to the substrate. That is, the layers can be in the following order: substrate, transparent conductive layer, counter electrode layer, ion conduction 155961.doc 201222119 layer, electrochromic material layer and (other) transparent conductive layer Referring again to Figure 1A', in a conventional method of fabricating an electrochromic stack, individual layers are deposited on top of another layer in the sequential format depicted in the schematic of the left side of Figure 1A. That is, the TCO layer 104 is deposited on the substrate. Next, an EC layer 106 is deposited on the TCO 104. Next, a 1C layer 108 is deposited on the EC layer 106, followed by a CE layer 110 deposited on the ic layer 108, and finally a TCO layer 112 deposited on the CE layer. 11〇 to form an electrochromic device 1〇〇. Of course, the order of the steps can be reversed to form a “reverse” stack, but the point is that in the conventional method, the 1C layer must be deposited on the EC layer, followed by The CE layer is deposited on the 1C layer' or the 1C layer is deposited on the CE layer, followed by the EC layer deposited on the 1C layer. The transition between the layers of material in the stack is abrupt. One of the above procedures significantly challenges the processing required to form the IC layer. In some prior methods, the '1C layer was formed by a sol-gel process that was difficult to incorporate into the CVD or PVD process used to form the ec layer and the CE layer. In addition, the sol gel and other liquid-based processes produce 1 (the layer tends to have the disadvantage of reducing the quality of the device and may require removal by, for example, engraving. In other methods the '1C layer is made by pvd Ceramic dry deposits from which it may be difficult to manufacture and use. Figure 1B is a depiction of the % composition of the material in the electrochromic stack of Figure 1A (i.e., layers 106, 108, and 11 〇 ', ie, EC layer, IC layer, and CE The graph of the layer) As mentioned, in the conventional electrochromic stack, the transition between the layers of material in the stack is abrupt. For example, EC material 1〇6 is deposited as a different layer. There is little or no percolation of the composition to the adjacent 1C layer. Similarly, the ic material 108 and the CE material 11〇 differ in composition with little or no percolation to the adjacent layer 15596l.doc 201222119. Therefore, 'these materials are substantial Upper homogenized (except for the specific composition of the CE material described below) and having a mutated interface. It is conventionally thought that each of the two layers of shai should be laid as a uniform uniformly deposited and smooth layer to form Stacking. Interface between each layer To be "clear", there is little intermixing of material from each layer at the interface. One skilled in the art will recognize that Figure 1B is an idealized depiction and, in the sense of practice, the layer interface exists. A certain degree of inevitable material mixing. The point is that 'in the conventional manufacturing method, any such mixing is unintentional and minimal. The inventors have found that an interface region serving as an IC layer can be formed, wherein the interface region intentionally includes a large number of One or more electrochromic materials and/or counter electrode materials. This is a fundamental deviation from the conventional manufacturing method. As mentioned above, the 'inventors have found that the formation of the EC-IC-CE stack does not have to be in the conventional sequence (EC). - IC - CE or CE - IC - EC), but can form an interface region serving as an ion conducting layer after deposition of the electrochromic layer and the counter electrode layer. That is, 'first form EC-CE (or CE-EC) Stacking, then 'using one or both of the layers (in some embodiments, and/or another electrochromic material or counter electrode material) at the interface of the layers at the EC layer Forming an interface region with the CE layer It may have at least some functions of the IC layer. The interface region functions as at least some of the functions of the conventional 1C layer because the interface region is substantially ion-conducting and substantially electrically insulating. However, it should be noted that The described interface regions may have leakage currents that are higher than conventionally accepted leakage currents. However, such devices exhibit good performance. In one embodiment, the electrochromic layer is formed to have an oxygen-rich region, which is rich. The oxygen region is converted to a 155961.doc -10·201222119 interface region or layer that serves as an IC layer after subsequent deposition of the counter electrode layer. In some embodiments, an electrochromic material is used.
富氧型式之相異層來(最終)在EC層與CE層之間形成充當IC 層之界面層。在其他實施例中,使用包括反電極材料之富 氧型式之相異層來(最終)在EC層與CE層之間形成充當IC層 之界面區。言玄f氧CM之全部或一部分經轉換成界面區。 在其他實施例中,使用包括反電極材料之富氧型式及電致 邕色材料之田氧形式之相異層來(最終)在EC層與CE層之間 形成充當1C層之界面區。換言之,富氧材料之一些或全部 充當該充當1C層之界面區之前驅體。本發明之方法不僅可 減少處理步驟,而且產生展示改良之效能特性之電致變色 裝置。 如所提及,咸信,界面區中之EC層及/或CE層之一些經 轉換成提供1C層之一或多個功能(特別是對離子之高傳導 f生及對電子之兩抵抗性)之材料。界面區中之ic功能性材 料可為(例如)導電陽離子之鹽;例如,鋰鹽。 圖2A、圖2B及圖2C展示電致變色裝置堆疊(各自含有EC 層、CE層及充當Ic層之界面區)之三個可能實例之組成曲 線圖,其中EC材料為氧化鎢(此處表示為w〇3,但意欲包 括\νοΛ ’其中x在約2 7與約3 5之間,在一實施例中,X在 約2.7與約2.9之間)’ CE材料為氧化鎳鎢(NiW〇),且界面 區主要包含鎢酸鋰(此處表示為Li2W〇4,在另一實施例 中’界面區為在約0.5%與約5〇(原子)%之間的Li2〇、在約 5 /〇與約95。/。之間的llwO4及約5%與約70%之間的W03之奈 米複合材料)及某一量之EC材料及/或CE材料。更一般言 155961.doc 201222119 之,界面區通常(但不必)具有包括由不同相及/或組成表示 之至少兩個離散組份之異質結構,該等相或組成之濃度在 界面區之寬度上變化。自於此原因,本文中有時將充當ic 層之界面區稱為「梯度區」、「異質冗層」或「分散式^ 層」》雖然關於特定材料加以描述,但圖2A、圖2B及圖 2C中之說明更一般地表示用於本發明之電致變色裝置之任 何合適材料之組成變化。 圖2A描繪本發明之電致變色堆疊,其中Ec材料為充當 ic層之界面區之重要組份,而CE材料並非重要組份。參看 圖2A,自原點開始且沿著^軸自左向右移動,吾人可看 到,一部分EC材料W〇3(其實質上全部為氧化鎢)充當Ec 層。存在至界面區中之過渡,其中存在逐漸減少之氧化嫣 及對應地逐漸增加之鎢酸鋰,直至且包括靠近界面區之末 端,在該末端處,存在具有某一最小量之氧化鎢之實質上 全部為鎢酸鋰之部分。雖然自EC層至界面區之過渡以實質 上全部氧化鎢及最小量之鎢酸鋰之組合物來區分,但顯而 易見,該過渡不像習知裝置中一樣突然。在此實例中,實 際上,該過渡在該組合物具有足夠量之鎢酸鋰之情況下開 始發生以使該材料能夠起到IC層之至少一些功能,例如, 離子傳導及電絕緣。無疑,更接近CE層之組合物(其中該 組合物實質上為鎢酸鋰)起到1(:層之功能,此係因為已知 鎢酸鋰展現此等性質。但在界面區之其他部分中亦存在一 定1C層功能。發明者已發現,與具有突然過渡之習知裴置 相比,此等「異質1C層」改良電致變色裝置之切換特性及 155961.doc 12 201222119 可能之熱循環穩定性。此實例中之CE層主要含有氧化錄鶴 作為活性材料,且具有至界面區之邊緣處之氧化鎳鎢組合 物的相對突然過渡。用於製造具有此等界面區之堆疊之方 法將在下文予以更詳細描述。 應注意’例如’圖2A中之氧化鎳鎢CE層經描繪為具有 約20%之鎢酸鋰。不希望受理論限制,咸信,氧化鎳鎢ce 層作為由鎢酸链之外殼或基質環繞之氧化鎳核心或粒子 (其將相當良好之離子傳導率賦予CE層)而存在,且藉此在 電致變色堆疊之操作期間幫助CE層之電致變色過渡。cE 層中之鎢酸鋰之確切化學計量可在實施例之間顯著改變。 在一些實施例中,CE層中亦可能存在一些氧化鎢。又,因 為鋰離子經由充當IC層之界面區而至及自EC層及ce層行 進,所以EC層中可能存在大量鎢酸鋰,例如,如圖2八中 所描續·。 圖2B描繪本發明之電致變色堆疊,其中CE材料為充當 ic層之界面區之重要組份,而Ec材料並非重要組份。參看 圖2B,自原點開始且沿著文軸自左向右移動,吾人可看 到,在此情況下,實質上全部為氧化鎢之EC材料充當EC 層。存在至界面區中之突然過渡,該界面區中存在很少 (若存在)氧化鎢,但存在大量鎢酸鋰及至少一些氧化鎳鎢 (CE材料)。該界面區之組合物沿著义軸以逐漸減少之鎢酸 鋰及對應之逐漸增多之氧化鎳鎢變化。自界面區至CE層之 過渡以約80%之氧㈣鶴及約2G%之鶴義之組合物任意 地區分,但此僅為過渡以分級組合物發生之情況之一實 155961.doc 201222119 例。當在對堆疊進行進一步處理時無或很少有組合物之額 外變化發生時’界面區可視為終止。另外,過渡實際上在 組合物具有足夠量之氧化鎳鎢之情況下終止,以使得該材 料不再起到相異ic層可起到之至少某一功能。無疑,更接 近CE層之組合物(如所區分)(其中組合物為8〇%之氧化鎳 鎢)起到CE層之功能。同樣地,更接近EC層之界面區之組 合物(其中鎢酸鋰為實質組份)充當離子傳導電絕緣材料。 圖2C描繪本發明之電致變色堆疊,其中Ec材料及(:£材 料均為充當ic層之界面區的重要組份。參看圖2C,自原點The opposite layer of the oxygen-rich pattern (finally) forms an interface layer acting as an IC layer between the EC layer and the CE layer. In other embodiments, a dissimilar layer comprising an oxygen-rich version of the counter electrode material is used (finally) to form an interfacial region that acts as an IC layer between the EC layer and the CE layer. All or part of the meta-oxygen CM is converted into an interface region. In other embodiments, an oxygen-rich version comprising a counter electrode material and a phase layer of the field oxygen form of the electrochromic material are used (finally) to form an interfacial region that acts as a 1C layer between the EC layer and the CE layer. In other words, some or all of the oxygen-rich material acts as a precursor to the interface region that acts as the 1C layer. The method of the present invention not only reduces the number of processing steps, but also produces an electrochromic device that exhibits improved performance characteristics. As mentioned, some of the EC layers and/or CE layers in the interface region are converted to provide one or more functions of the 1C layer (especially for the high conductivity of ions and the resistance to electrons). ) material. The ic functional material in the interfacial zone can be, for example, a salt of a conductive cation; for example, a lithium salt. 2A, 2B, and 2C show compositional curves of three possible examples of electrochromic device stacks (each containing an EC layer, a CE layer, and an interface region serving as an Ic layer), wherein the EC material is tungsten oxide (here indicated Is w〇3, but is intended to include \νοΛ 'where x is between about 27 and about 35, in one embodiment, X is between about 2.7 and about 2.9) 'The CE material is nickel oxide tungsten (NiW〇) And the interface region mainly comprises lithium tungstate (here denoted Li2W〇4, in another embodiment the 'interfacial zone is between about 0.5% and about 5 〇 (atomic)% of Li2〇, at about 5 /〇 and llwO4 between about 95% and about 7% and about 70% of the W03 nanocomposite) and a certain amount of EC material and / or CE material. More generally, 155961.doc 201222119, the interface region typically, but not necessarily, has a heterostructure comprising at least two discrete components represented by different phases and/or compositions, the concentration of the phases or compositions being over the width of the interface region Variety. For this reason, the interface area that serves as the ic layer is sometimes referred to as "gradient zone", "heterogeneous redundancy layer" or "distributed layer" in this paper. Although it describes the specific material, Figure 2A, Figure 2B and The illustration in Figure 2C more generally represents the compositional variation of any suitable material for use in the electrochromic device of the present invention. Figure 2A depicts an electrochromic stack of the present invention in which the Ec material is an important component of the interface region that acts as an ic layer, while the CE material is not an important component. Referring to Fig. 2A, starting from the origin and moving from left to right along the ^ axis, it can be seen that a portion of the EC material W〇3 (which is substantially all tungsten oxide) acts as the Ec layer. There is a transition to the interface region in which there is a gradual decrease in yttrium oxide and a correspondingly increasing amount of lithium tungstate up to and including the end near the interface region where there is a substantial amount of tungsten oxide substantially All of them are part of lithium tungstate. Although the transition from the EC layer to the interface region is distinguished by a combination of substantially all of the tungsten oxide and the minimum amount of lithium tungstate, it is apparent that the transition is not as abrupt as in conventional devices. In this example, in practice, the transition begins with the composition having a sufficient amount of lithium tungstate to enable the material to function as at least some of the IC layer, such as ion conduction and electrical insulation. Undoubtedly, a composition closer to the CE layer (wherein the composition is substantially lithium tungstate) functions as a layer (1: layer because it is known that lithium tungstate exhibits such properties. But in other parts of the interface region There is also a certain 1C layer function. The inventors have found that the switching characteristics of these "heterogeneous 1C layers" improved electrochromic devices compared with the conventional devices with sudden transitions and 155961.doc 12 201222119 possible thermal cycling Stability. The CE layer in this example mainly contains an oxide-recorded crane as an active material and has a relatively abrupt transition to the nickel-tungsten oxide composition at the edge of the interface region. A method for fabricating a stack having such interface regions will It will be described in more detail below. It should be noted that 'for example, the nickel-nickel-tungsten CE layer of Figure 2A is depicted as having about 20% lithium tungstate. Without wishing to be bound by theory, it is believed that the nickel-tungsten oxide ce layer acts as tungsten. The outer shell of the acid chain or the nickel oxide core or particles surrounding the matrix, which imparts a relatively good ionic conductivity to the CE layer, exists and thereby assists in the electrochromic transition of the CE layer during operation of the electrochromic stack. The exact stoichiometry of lithium tungstate in the cE layer can vary significantly between the examples. In some embodiments, some tungsten oxide may also be present in the CE layer. Again, because lithium ions pass through the interface region that acts as the IC layer And traveling from the EC layer and the ce layer, so there may be a large amount of lithium tungstate in the EC layer, for example, as depicted in Figure 2-8. Figure 2B depicts the electrochromic stack of the present invention, wherein the CE material acts as an ic layer The important component of the interface area, and the Ec material is not an important component. Referring to Figure 2B, starting from the origin and moving from left to right along the axis, we can see that in this case, substantially all of the oxidation The tungsten EC material acts as an EC layer. There is a sudden transition into the interface region where there is little, if any, tungsten oxide, but a large amount of lithium tungstate and at least some nickel oxide tungsten (CE material) are present. The composition of the zone varies along the sense axis with a gradual decrease in lithium tungstate and a corresponding increase in nickel oxide tungsten. The transition from the interface zone to the CE layer is a combination of about 80% oxygen (four) cranes and about 2G% of cranes. Objects are arbitrarily divided, but this is only a transition One of the conditions in which the composition occurs is 155961.doc 201222119. The interface zone can be considered to be terminated when no additional changes to the composition occur when further processing of the stack occurs. Additionally, the transition actually has in the composition Sufficient amount of nickel oxide tungsten is terminated so that the material no longer functions as at least one of the functions of the distinct ic layer. Undoubtedly, the composition of the CE layer is closer (as distinguished) (wherein the composition is 8 〇% of nickel oxide tungsten) functions as a CE layer. Likewise, a composition closer to the interface region of the EC layer (where lithium tungstate is a substantial component) acts as an ion conducting electrically insulating material. Figure 2C depicts the invention The electrochromic stack, in which the Ec material and the material are all important components of the interface region of the ic layer. See Figure 2C, from the origin
開始且沿著X軸自左向右移動,吾人可看到,一部分ECM 料WO3(其實質上全部為氧化鎢)充當£(:層。存在至界面區 中之過渡,其中存在逐漸減少之氧化鎢及對應地逐漸增多 之鎢酸鋰。在此實例中,在通過區分為界面區之部分之路 途的二分之一附近,亦存在增長量之氧化鎳鎢反電極材 料。在通過區分為界面區之部分的約中間位置處,存在各 自約10%之氧化鎢及氧化鎳鎢及8〇%之鎢酸鋰。在此實例 中,EC層與1C層之間或1(:層與CE層之間不存在突然過 渡,而是存在具有CE材料及EC材料兩者之連續分級組合 物之界面區。在此實例中,鎢酸鋰組份在通過界面區之约 中間處出現峰值,且因此,此區很可能為界面區之最強電 絕緣部分。 如以上[發明内容]中所提及,EC層及CE層可包括將某一 電阻率賦予EC層及CE層之材料組份;圖2A至圖2C中所描 述之至少以某一量跨越所有三個區之鎢酸鋰為將電阻率賦 155961.doc 201222119 予EC層及CE層之此等材料之一實例。 圖2A至圖2C僅表示本發明之電致變色裝置中之充當【c 層之界面區之分級組合物的三個非限制性實例。一般&習 此項技術者將瞭解,在不脫離本發明之範疇的情況許 多變化係可能的。在圖2A至圖2C中之實例之每一者中, 存在至H其中僅存在兩種材料組份且該等組份中之 一者為最少的。本發明不限於此方式。因此,本發明之一 實施例為一種電致變色裝置,其包括電致變色層'充當IC 層之界面區,及反電極層,纟中該裝置之前述兩個層及一 個區中之每—者之至少—材料組份以如下量存在於該電致 變色層、該界面區及該反電極層中之每一者中:至少約 重量%,在另一實施例中,至少約15重量%,在另一實施 例中’至少約1〇重量%,在另一實施例中,至少約5重量 %,在又一實施例中,至少約2重量0/〇。 界面區中之電致t色材料及/或反電極材料之量可為顯 著的’在一實施例中’多達界面區之5〇重量0/〇。然而,在 許多實施例中,離子傳導電絕緣材料通常為多數組份,而 界面區之剩餘部分為電致變色材料及/或反電極材料。在 一實施例中,界面區包括在約6〇重量%與約95重量%之間 的離子傳導電絕緣材料,而界面區之剩餘部分為電致變色 材料及/或反電極材料。在一實施例中,界面區包括在約 70重量%與約95重量%之間的離子傳導電絕緣材料,而界 面區之剩餘部分為電致變色材料及/或反電極材料。在一 實施例中’界面區包括在約8G f f %與約95重量%之間的 155961.doc •15· 201222119 離子傳導電、、,邑緣材料,而界面區之剩餘部分為電致變色材 料及/或反電極材料。 在-些實施例中’本文中所描述之裝置中之界面區可為 相對相異的,亦即,當(例如)藉由顯微鏡分析時,鄰接層 處存在相對可區別之邊界,即使界面區含有某一量之電致 支色材料及/或反電極材料亦如此。在此等實施例中,可 量測界面區之厚度。在界面區係由EC層及,或CE層之富氧 學計4)區形成之實施例中’界面區之厚度與形成界 面區之該層或該等層之比為用於特性化界面區之一量度。 舉例而言,電致變色層經沈積具有富氧上層。EC層可包括 單金屬氧化物或在層或更多擴散區中均質或異質地混合 之兩種或兩種以上金屬氧化物。EC層為55〇 nm厚其包括 虽氧層(或區)。若EC層之約15〇 nm經轉換成界面區,則Ec 之約27%經轉換成界面區,亦即,丨5〇 nm除以wo nm。在 另一實例中,EC層包括第一金屬氧化物區(或層)及富氧之 第二金屬氧化物層(或區)β若富氧金屬氧化物層之全部或 口Ρ分經轉換成界面區’則界面區之厚度除以該第一金屬 氧化物層及該第二金屬氧化物層之總厚度(在形成界面區 之前)為界面區之量度。在一實施例中,界面區包括以厚 度計約0.5〇/〇與約50%之間的用以形成界面區之前驅體區 (EC及/或CE ’包括富氧部分),在另一實施例中在約1 %與 約30%之間’在又一實施例中在約2%與約10%之間,且在 另一實施例中在約3%與約7%之間。 發明者已發現,分級組合物充當1(:層具有許多益處。儘 155961.doc •16- 201222119 B不希望文理淪限制,但咸信,冑由具有此等分級區,電 致變色過渡之效率得到大大改良。如y文將更詳細描述, 存在其他益處。 儘管不希望束缚於理論,但咸信,以下機制中之一或多 者可貫現EC及/或CE材料至界面區中之1(:功能性材料之轉 化。然而,本發明之執行或應用並不限於此等機制中之任 者此等機制中之每一者與在堆疊之製造期間絕不沈積 1C層材料之製程一致。如本文中其他處清楚表示,本發明 之設備無需具有包含用於1(:層之材料之單獨標靶。 在第一機制中,電致變色材料或反電極材料之直接鋰化 產生界面區中之IC材料(例如,鎢酸鋰)。如下文將更充分 解釋,各種實施例在EC層及CE層之形成之間的製造程序 中之某時刻使用該等作用層中之一者之直接鋰化。此操作 涉及EC層或CE層(首先形成者)於鋰之曝露。根據此機制, 通過EC或CE層之鋰之通量產生離子傳導之抵抗電子之材 料,諸如,鋰鹽。可施加熱或其他能量以驅動鋰之此通 里。所描述之此機制在形成第二層(CE或EC層)之前轉換首 先形成之層(EC或CE層)之頂部或曝露部分。 在第二機制中,自EC或CE中之一者擴散至另一層之鋰 在兩個層皆已形成之後及/或在經鋰化之第一層上形成第 二層期間導致EC及/或CE中之一者之部分在其界面處轉換 至具有1C功能材料之界面區》該經擴散可在整個該第二層 已形成之後或在该苐一層之僅某一部分已形成之後發生。 此外’鋰之擴散及至1C功能性材料之後續轉換在該第一或 155961.doc •17· 201222119 該第二沈積層中及在EC或CE層中發生。在一實例中,首 先形成EC層’且接著鋰化該EC層。當隨後將CE層沈積在 EC層之上時,一些鋰自下伏EC層朝著CE層擴散及/或擴散 至CE層中,從而導致轉化成含有IC功能性材料之界面區。 在另一實例中,首先形成EC層(視情況具有富氧上部區), 接著’形成CE層且鋰化該CE層。隨後,來自Ce層之一些 經擴散至EC層中,在此處其形成具有IC功能性材料之界面 區。在又一實例中,首先沈積EC層,且接著鋰化該£(:層 以根據上述之該第一機制產生某一 1C功能性材料。接著, 當形成CE層時,一些鋰自下伏EC層朝著CE層擴散以在CE 層之界面區中產生某一 1C材料。以此方式,IC功能性材料 名義上緊接CE層與EC層之界面駐留於CE層及EC層兩者 中。 在第三機制中’形成EC層及CE層至完成(或至少到達第 二形成之層部分完成之時刻)。接著,加熱裝置結構,且 該加熱將界面區中之材料之至少一些轉換成IC功能性材料 (例如,鋰鹽)。加熱(例如,作為本文中進一步描述之多步 驟熱化學調節(MTCC)之部分)可在沈積期間或在沈積完成 之後執行。在一實施例中,在於堆疊上形成透明導電氧化 物之後執行加熱。在另一實施例中,在該第二層部分或完 全完成之後,但在將透明導電氧化物塗覆至該第二層之前 應用加熱。在一些情況下,加熱直接且主要負責轉化。在 其他情況下,加熱主要促進鋰離子之擴散或流動,如該第 二機制中所描述’此建立1C功能性材料區。 155961.doc 18- 201222119 最後,在第四機制中,在Ec層與CE層之間流動之電产 驅動電致變色材料及反電極材料中之至少一者轉化為界: 區中之IC功能性材料。此轉化可能發生,此係因為(例如) 與流動電流相關聯之離子通量很大,以致其驅動沉及,或 CE材料至界面區中之IC材料之化學轉化。舉例而言,如下 文將解釋’穿過EC層中之氧化鎢之大的鐘通量可產生鶴酸 鋰,其充當1C材料。鋰通量可(例如)在新形成之裝置之初 始活化循環期間引入。然而,情況不必如&,此係因為用 於驅動咼離子通量之其他機會對實現該轉換而言可能更適 當。本發明之方法可由一般熟習此項技術者在不採用以上 機制中之任何一或多者之情況下執行。 圖3A為根據本發明之方法之程序流程3〇〇。具體言之, 參見305,(在例如TC〇2 CL上)沈積£(:層。接著,參見 31〇,沈積CE層。在沈積Ec層及cE層之後,接著,參見 315,在EC層與CE層之間形成充當1(::層之界面區。本發明 之一實施例為步驟305與3 10顛倒之類似方法(未描繪)。該 方法之要點在於’充當1C層之界面區係在EC層及CE層之 後形成(在一些實施例中,使用EC層及CE層中之一者之至 少部分形成界面區)。為此,有時將以此方式形成之界面 區稱為「本質」1C層。在其他實施例中,例如使用EC材料 或CE材料之富氧型式在ec層與CE層之間形成相異層,其 中該層再次在形成EC層及CE層之後被完全或部分轉換成 界面區。用以在形成EC-CE堆疊之後形成界面區之各種方 法將在下文予以描述。 155961.doc •19- 201222119 因此,如所提及,本發明之一態樣為一種製造電致變色 裝置之方法’該方法包括:形成包括電致變色材料之電致 變色層;形成與該電致變色層接觸之反電極層,而並不首 先在該電致變色層與該反電極層之間提供離子傳導電絕緣 層’其中該反電極層包括反電極材料;及在該電致變色層 與該反電極層之間形成界面區,其中該界面區為實質上離 子傳導且實質上電絕緣的。該界面區可含有EC層、CE層 或兩者之組份材料。如下文將更詳細描述,該界面區可以 許多方式形成。 圖3B為展示根據關於圖3 A所描述之方法之程序流程(詳 言之’用於沈積EC層、接著沈積Ce層且最終在該等層之 間形成充當ic層之界面區之程序流程)的程序流程320。更 特定言之,在此實施例中,EC層包括具有各種量之氧(詳 s之’組合物及組態)之w〇3 ; CE層包括NiWO,界面區包 括LhWO4,且使用諸如氧化銦錫及經氟化之氧化錫之TC〇 材料。應注意,將在下文關於固態材料來描述電致變色裝 置之層。固態材料由於可靠性、一致特性及程序參數及裝 置效能而為所需的。例示性固態電致變色裝置、方法及用 於製造其之設備以及用此等裝置製造電致變色窗之方法描 述於 K〇Zl〇Wski 等人之題為「FabHcati〇n 〇f L〇w DefectivityStarting and moving from left to right along the X axis, we can see that a portion of the ECM material WO3 (which is essentially all tungsten oxide) acts as a £: layer. There is a transition into the interface region where there is a gradual decrease in oxidation. Tungsten and correspondingly increasing lithium tungstate. In this example, there is also a growth amount of nickel oxide tungsten counter electrode material in the vicinity of one-half of the path divided into portions of the interface region. At about the middle of the portion of the region, there are about 10% each of tungsten oxide and nickel oxide tungsten and 8% by weight of lithium tungstate. In this example, between the EC layer and the 1C layer or 1 (: layer and CE layer) There is no abrupt transition between them, but there is an interfacial zone with a continuous grading composition of both the CE material and the EC material. In this example, the lithium tungstate component peaks around the middle of the interface region, and thus This region is likely to be the strongest electrically insulating portion of the interface region. As mentioned in the above [Summary], the EC layer and the CE layer may include a material component that imparts a certain resistivity to the EC layer and the CE layer; Crossing at least a certain amount as described in Figure 2C There are three regions of lithium tungstate which are examples of such materials which impart a resistivity of 155961.doc 201222119 to the EC layer and the CE layer. Figures 2A to 2C show only the [c layer] in the electrochromic device of the present invention. Three non-limiting examples of hierarchical compositions of the interface regions. It will be appreciated by those skilled in the art that many variations are possible without departing from the scope of the invention. Examples in Figures 2A-2C In each of them, there are only two material components present in H and one of the components is the least. The present invention is not limited to this manner. Therefore, an embodiment of the present invention is an electrochromic. a device comprising an electrochromic layer 'acting as an interface region of an IC layer, and a counter electrode layer, wherein at least one of the two layers of the device and one of the regions - the material component is present in the amount In each of the electrochromic layer, the interfacial region, and the counter electrode layer: at least about wt%, in another embodiment, at least about 15 wt%, and in another embodiment, at least about 1 wt. %, in another embodiment, at least about 5% by weight, in yet In embodiments, at least about 2 weights per Å. The amount of electrochromic t-color material and/or counter electrode material in the interface region can be significant 'in one embodiment' up to 5 〇 weight of the interface region 0/ However, in many embodiments, the ionically conductive electrically insulating material is typically in multiple layers, and the remainder of the interface region is an electrochromic material and/or a counter electrode material. In one embodiment, the interface region is included Between 6% by weight and about 95% by weight of the ionically conductive electrically insulating material, and the remainder of the interface region is an electrochromic material and/or a counter electrode material. In one embodiment, the interface region is comprised at about 70% by weight. The ion conductive electrically insulating material is between about 95% by weight, and the remainder of the interface region is an electrochromic material and/or a counter electrode material. In one embodiment, the 'interface region includes about 8 G ff % and about 95 wt. Between 5%, 155961.doc •15· 201222119 ion-conducting electricity, and rim materials, while the remainder of the interface region is an electrochromic material and/or a counter electrode material. In some embodiments, the interface regions in the devices described herein can be relatively distinct, that is, when analyzed, for example, by microscopy, there are relatively distinguishable boundaries at adjacent layers, even if the interface region The same applies to a certain amount of electrochromic material and/or counter electrode material. In these embodiments, the thickness of the interface region can be measured. In the embodiment in which the interface region is formed by the EC layer and or the oxygen-rich meter 4) region of the CE layer, the ratio of the thickness of the interface region to the layer or layers forming the interface region is used to characterize the interface region. One measure. For example, the electrochromic layer is deposited with an oxygen-rich upper layer. The EC layer may include a single metal oxide or two or more metal oxides which are homogeneously or heterogeneously mixed in one or more diffusion regions. The EC layer is 55 〇 nm thick and includes an oxygen layer (or region). If about 15 〇 nm of the EC layer is converted into an interface region, about 27% of Ec is converted into an interface region, that is, 丨5〇 nm divided by wo nm. In another example, the EC layer includes a first metal oxide region (or layer) and an oxygen-enriched second metal oxide layer (or region) β if the oxygen-rich metal oxide layer is all or the enthalpy is converted into The interface region 'the thickness of the interface region divided by the total thickness of the first metal oxide layer and the second metal oxide layer (before forming the interface region) is a measure of the interface region. In one embodiment, the interface region comprises between about 0.5 Å/〇 and about 50% of the thickness to form the interface region precursor region (EC and/or CE 'including the oxygen-rich portion), in another implementation In an example between about 1% and about 30% 'in another embodiment between about 2% and about 10%, and in another embodiment between about 3% and about 7%. The inventors have found that the graded composition acts as a 1 (: layer has many benefits. 155961.doc • 16-201222119 B does not wish to limit the literary arts, but Xianxin, 胄 by having such grading areas, the efficiency of electrochromic transition Greatly improved. There are other benefits as described in more detail in y. Although not wishing to be bound by theory, it is believed that one or more of the following mechanisms can be used to achieve EC and/or CE materials in the interface region. (: Conversion of Functional Materials. However, the execution or application of the present invention is not limited to any of these mechanisms. Each of these mechanisms is consistent with the process of never depositing 1 C layer material during fabrication of the stack. As is clear elsewhere herein, the apparatus of the present invention need not have a separate target comprising a material for the layer (1: layer). In the first mechanism, direct lithiation of the electrochromic material or counter electrode material creates an interface region. IC material (eg, lithium tungstate). As will be more fully explained below, various embodiments use direct lithium in one of the active layers at some point in the manufacturing process between the formation of the EC layer and the CE layer. Chemical. The operation involves the exposure of the EC layer or the CE layer (formerly formed) to lithium. According to this mechanism, an ion-conducting electron-resistant material, such as a lithium salt, is generated by the flux of lithium in the EC or CE layer. Heat or other may be applied. Energy to drive the lithium. This mechanism describes the conversion of the top or exposed portion of the first formed layer (EC or CE layer) before forming the second layer (CE or EC layer). In the second mechanism, One of the EC or CE that diffuses to another layer after the formation of both layers and/or during the formation of the second layer on the lithiated first layer results in a portion of one of the EC and/or CE Switching to an interface region having a 1C functional material at its interface" may occur after the entire second layer has been formed or after only a portion of the layer has been formed. Further 'lithium diffusion and to 1C functionality Subsequent conversion of the material occurs in the first deposited layer of the first or 155961.doc • 17· 201222119 and in the EC or CE layer. In one example, the EC layer is first formed 'and then the EC layer is lithiated. Then when the CE layer is deposited on top of the EC layer, some The underlying EC layer diffuses and/or diffuses into the CE layer toward the CE layer, resulting in conversion to an interfacial region containing the IC functional material. In another example, the EC layer is first formed (as appropriate with an oxygen-rich upper region) Then, 'the CE layer is formed and the CE layer is lithiated. Subsequently, some of the layer from the Ce layer is diffused into the EC layer where it forms an interfacial region with an IC functional material. In yet another example, the first deposition An EC layer, and then lithiation of the £ (: layer to produce a certain 1C functional material according to the first mechanism described above. Then, when the CE layer is formed, some of the lithium diffuses from the underlying EC layer toward the CE layer to A certain 1C material is produced in the interface region of the CE layer. In this manner, the interface of the IC functional material nominally next to the CE layer and the EC layer resides in both the CE layer and the EC layer. In the third mechanism, the formation of the EC layer and the CE layer is completed (or at least the time when the layer portion of the second formation is completed). Next, the device structure is heated and the heating converts at least some of the material in the interface region into an IC functional material (e.g., a lithium salt). Heating (e.g., as part of a multi-step thermochemical conditioning (MTCC) as further described herein) can be performed during deposition or after deposition is complete. In an embodiment, the heating is performed after the transparent conductive oxide is formed on the stack. In another embodiment, heating is applied after the second layer portion is fully completed, but prior to applying the transparent conductive oxide to the second layer. In some cases, the heating is directly and primarily responsible for the conversion. In other cases, heating primarily promotes the diffusion or flow of lithium ions, as described in this second mechanism, which establishes a region of functional material. 155961.doc 18- 201222119 Finally, in the fourth mechanism, at least one of the electro-chromic-driven electrochromic material and the counter-electrode material flowing between the Ec layer and the CE layer is transformed into a boundary: IC functionality in the region material. This conversion may occur because, for example, the ion flux associated with the flow current is so large that it drives the sink, or chemical conversion of the CE material to the IC material in the interface region. For example, as will be explained below, the large clock flux through the tungsten oxide in the EC layer can produce lithium oleate, which acts as a 1C material. Lithium flux can be introduced, for example, during the initial activation cycle of a newly formed device. However, the situation does not have to be as & this is because other opportunities for driving the cesium ion flux may be more appropriate to achieve this conversion. The method of the present invention can be performed by those of ordinary skill in the art without employing any one or more of the above mechanisms. Figure 3A is a flow diagram of a process in accordance with the method of the present invention. Specifically, see 305, (for example, on TC〇2 CL) deposit £(: layer. Next, see 31〇, depositing the CE layer. After depositing the Ec layer and the cE layer, then, see 315, in the EC layer with An interface region serving as a 1 (:: layer) is formed between the CE layers. An embodiment of the present invention is a similar method (not depicted) in which steps 305 and 3 10 are reversed. The main point of the method is that 'the interface region serving as the 1C layer is The EC layer and the CE layer are formed after (in some embodiments, at least part of one of the EC layer and the CE layer is used to form an interface region). For this reason, the interface region formed in this way is sometimes referred to as "essence" 1C layer. In other embodiments, an oxygen-rich version, such as an EC material or a CE material, is used to form a distinct layer between the ec layer and the CE layer, wherein the layer is again fully or partially converted after forming the EC layer and the CE layer. Interfacial zone. Various methods for forming an interfacial zone after forming an EC-CE stack will be described below. 155961.doc • 19- 201222119 Thus, as mentioned, one aspect of the present invention is an electrical fabrication Method of color changing device 'This method includes: forming including electricity An electrochromic layer of a color changing material; forming a counter electrode layer in contact with the electrochromic layer without first providing an ion conducting electrically insulating layer between the electrochromic layer and the counter electrode layer, wherein the counter electrode layer Including a counter electrode material; and forming an interface region between the electrochromic layer and the counter electrode layer, wherein the interfacial region is substantially ionically conductive and substantially electrically insulating. The interfacial region may comprise an EC layer, a CE layer or The component materials of both. As will be described in more detail below, the interface region can be formed in a number of ways. Figure 3B is a flow diagram showing the process described in relation to Figure 3A (detailed 'for depositing an EC layer, then A program flow 320 of depositing a Ce layer and ultimately forming a program flow that acts as an interface region for the ic layer between the layers. More specifically, in this embodiment, the EC layer includes oxygen having various amounts (detailed 'Composition and configuration' w〇3; CE layer includes NiWO, interface region includes LhWO4, and TC〇 material such as indium tin oxide and fluorinated tin oxide is used. It should be noted that the following will be about solid materials. Description of electrical alteration A layer of a color device that is required for reliability, consistent characteristics, and program parameters and device performance. Exemplary solid state electrochromic devices, methods, and devices for making the same, and fabricating electrochromic devices therewith The method of the window is described in K〇Zl〇Wski et al. entitled "FabHcati〇n 〇f L〇w Defectivity
Electrochiromic Deviees」之美國非臨時專利申請案第 12/645,111 號及 Wang 等人之題為「Electr〇chr〇mic 之美國非臨時專利申請案第12/645,159號中,該兩專利申 清案出於所有目的而以引用方式併入本文中。在特定實施 155961.doc •20· 201222119 例令,本發明之電致變色裝置全部為固態的且係在允許在 文控周圍環境中沈積堆疊之—或多個層之設備中製造。亦 即,在係在不離開設備且(例如)不破壞沈積步驟之間的真 空之情況下沈積該等層之設財,藉此減少污染物且最終 改善裝置效能。在特定實施例中,本發明之設備不需要習 知設備令所需之用於沈積IC層之單獨標靶。如一般熟習此 項技術者將瞭解,本發明並不限於此等材料及方法,然. 而’在特定實施例中,組成電致變色堆疊及前驅體堆疊 (如下文所描述)之材料全部為無機、固體(亦即,為固態) 或無機且固體的。 因為有機材料傾向於隨時間推移而降級,例如當曝露於 與窗應用相關聯之紫外光及熱時,所以無機材料提供可工 作達長時間段之可靠電致變色堆疊之優點。固態材料亦提 供不具有液癌材料常常具有的污染物及泡漏問題之優點。 應理解’堆疊中之該等層中之任何—或多者可含有某一量 之有機材料’但在許多實施中,該㈣巾之—或多者含有 很少或不含有有機物質。對於可能以小量存在於一或多個 層中之液體而S可同樣如此。亦應理解,固態材料可藉由 使用液體組份之製程(諸如,使用溶膠-凝膠或化學氣相沈 積之特定製程)沈積或以其他方式形成。 再次參看圖3Β,參見325,首先沈積w〇3之㈣。圖 至圖4C為描繪根據本發明之特定方法及設備且具體言之根 據程序流程32G形成電致變色裝置之示意性橫截面。具體 。之’圖4Α至圖4C用以展示包括w〇,EC層可如何形成 155961.doc -21- 201222119 為堆疊之部分之三個非限制性實例,其中充當ic層之界面 區係在沈積該堆疊之其他層之後形成。在圖4A至圖4C中 之每一者中,基板402、第一 TCO層404、CE層410及第二 TCO層41 2基本上相同。又,在該三個實施例中之每一 者,形成不具有1C層之堆疊,且接著進一步處理該堆疊以 便在該堆疊内形成充當1C層之界面區,其在EC層與CE層 之間。 參看圖4A至圖4C中之每一者,分別描繪了分層結構 4〇0、403及409。此等分層結構中之每一者包括為(例如)玻 璃之基板402。可使用具有合適光學、電、熱及機械性質 之任何材料作為基板402。此等基板包括(例如)玻璃、塑膠 及鏡材料。合適塑膠基板包括(例如)丙烯酸、聚苯乙烯、 聚碳酸酯、烯丙基二乙二醇碳酸酯、SAN(styrene acrylonitrile copolymer,苯乙烯丙稀腈共聚物)、聚(4-曱 基-1-戊烯)、聚酯、聚醯胺等,且較佳地,塑膠應能夠耐 受高溫處理條件。若使用塑膠基板,則其較佳使用(例如) 類鑽石保護塗層、矽石/聚矽氧耐磨塗層或其類似者(諸 如,塑膠上光技術中所熟知之塗層)之硬塗層來加以障壁 #\ 保護及磨損保護。合適玻璃包括透明或有色鹼石灰玻璃, 包括鹼石灰漂浮玻璃。玻璃可為經回火或未經回火的。在 一些實施例中,諸如玻璃基板之市售‘基板含有透明導電層 塗層。此等玻璃之實例包括以商標TEC Glass™(Pilkington of Toledo, Ohio)及 SUNGATE™ 300 及 SUNGATE™ 500 (PPG Industries of Pittsburgh, Pennsylvania)銷售的塗有導 155961.doc -22· 201222119 電層之玻璃 之玻璃。Electrochiromic Deviees, U.S. Non-Provisional Patent Application No. 12/645,111, and Wang et al., entitled "Electr〇chr〇mic, US Non-Provisional Patent Application No. 12/645,159, the two patents The invention is incorporated herein by reference for all purposes. In the specific implementation 155961.doc • 20 201222119, the electrochromic devices of the present invention are all solid and are capable of depositing a stack in a documented environment. - or multiple layers of equipment. That is, depositing the layers without leaving the equipment and, for example, without breaking the vacuum between the deposition steps, thereby reducing contaminants and ultimately improving Device Effectiveness. In a particular embodiment, the apparatus of the present invention does not require the conventional apparatus to require a separate target for depositing an IC layer. As will be appreciated by those of ordinary skill in the art, the present invention is not limited to such materials. And methods, but in a particular embodiment, the materials comprising the electrochromic stack and the precursor stack (as described below) are all inorganic, solid (ie, solid) or inorganic and solid. Because organic materials tend to degrade over time, such as when exposed to ultraviolet light and heat associated with window applications, inorganic materials offer the advantage of a reliable electrochromic stack that can operate for extended periods of time. It also provides the advantage of not having the contaminants and bubble problems that liquid cancer materials often have. It should be understood that 'any of the layers in the stack—or more may contain a certain amount of organic material' but in many implementations, The (four) towel may contain little or no organic matter. S may be the same for liquids that may be present in small amounts in one or more layers. It should also be understood that solid materials may be used by using liquid groups. a portion of the process (such as a specific process using sol-gel or chemical vapor deposition) is deposited or otherwise formed. Referring again to Figure 3A, see 325, first depositing (4) of w〇3. Figure to Figure 4C is a depiction based on A particular method and apparatus of the present invention, and in particular a schematic cross-section of an electrochromic device formed according to program flow 32G, is specifically shown in Figures 4A through 4C to illustrate the inclusion of w〇, EC. How to form 155961.doc -21 - 201222119 are three non-limiting examples of portions of the stack in which the interface region acting as the ic layer is formed after depositing the other layers of the stack. Each of Figures 4A-4C The substrate 402, the first TCO layer 404, the CE layer 410, and the second TCO layer 41 2 are substantially identical. Again, in each of the three embodiments, a stack having no 1C layer is formed, and then The stack is further processed to form an interfacial region that acts as a 1C layer within the stack, between the EC layer and the CE layer. Referring to each of Figures 4A-4C, a hierarchical structure 4〇0, 403 is depicted, respectively. And 409. Each of these layers includes, for example, a substrate 402 of glass. Any material having suitable optical, electrical, thermal, and mechanical properties can be used as the substrate 402. Such substrates include, for example, glass, plastic, and mirror materials. Suitable plastic substrates include, for example, acrylic acid, polystyrene, polycarbonate, allyl diethylene glycol carbonate, SAN (styrene acrylonitrile copolymer), poly(4-mercapto-1) -pentene), polyester, polyamide, etc., and preferably, the plastic should be able to withstand high temperature processing conditions. If a plastic substrate is used, it is preferably hard coated with, for example, a diamond-like protective coating, a vermiculite/polyoxygen wear resistant coating or the like (such as a coating well known in plastic glazing techniques). Layers come with barriers #\ protection and wear protection. Suitable glasses include clear or colored soda lime glass, including soda lime floating glass. The glass can be tempered or untempered. In some embodiments, a commercially available 'substrate, such as a glass substrate, contains a transparent conductive layer coating. Examples of such glasses include those sold under the trademark TEC GlassTM (Pilkington of Toledo, Ohio) and SUNGATETM 300 and SUNGATETM 500 (PPG Industries of Pittsburgh, Pennsylvania) coated with a conductive layer of 155961.doc -22· 201222119 Glass.
TECTEC
Glass™為塗有經氟化 之氧化錫導電層 j—二實施例中,基板術之光學透射率(亦即,透過之 輪射或光譜對人射之輻射或光譜之比)為物%至㈣例 如,約鄉至92%。基板可具有任何厚度只要其具有合 適機械性質以支擇電致變色裝置即可。雖然基板術可且 有任何大小,但在-些實施财,其為約⑽錢 mm厚,較佳約3 mm至9 mm厚。 在本發明之-些實施例中,基板為建築玻璃。建築玻璃 為用作建築材料之玻璃。建築玻璃通f用於商業建築中, 但亦可用於居住建築中’且通常(但不必)分離室内環境與 室外環境。在特定實施例中,建築玻璃為至少2〇吋乘以2〇 吋,且可以更大,例如,大達約72吋乘以12〇吋。建築玻 璃通常為至少約2 mm厚。小於約3.2 mm厚之建築玻璃不 了回火在以建築玻璃作為基板之本發明之一些實施例 中,即使在已在基板上製造電致變色堆疊之後,基板仍可 經回火《在以建築玻璃為基板之一些實施例中,基板為來 自錫浮法生產線(tin float line)之驗石灰玻璃《建築玻璃基 板之可見光譜上之透射百分率(亦即,跨越可見光譜之整 體透射)一般比中性基板大80%,但其可能低於著色基板之 透射百分率。較佳地,基板在可見光譜上之透射百分率為 至少約90°/。(例如’約90%至92%)。可見光譜為典型人目艮會 回應之光譜’一般為約380 nm(紫色)至約780 nm(紅色)。 在一些.情況下,玻璃具有在約10 nm與約30 nm之間的表面 155961.doc •23- 201222119 粗糙度。在一實施例中,基板402為具有鈉擴散障壁(未圖 示)以防止鈉離子擴散至電致變色裝置中之鈉玻璃。為此 描述之目的’將此配置稱為「基板402」。 再次參看分層結構400、403及409,(例如)由經敗化之 氧化錫或其他合適材料(其尤其為導電且透明的)製成之第 一 TCO層404沈積在基板402之上。透明導電氧化物包括金 屬氧化物及摻雜一或多種金屬之金屬氧化物。此等金屬氧 化物及經摻雜之金屬氧化物之實例包括氧化銦、氧化銦 錫、經摻雜之氧化銦、氧化錫、經摻雜之氧化錫、氧化 鋅、氧化鋁鋅、經摻雜之氧化鋅、氧化釕、經摻雜之氧化 釕及其類似者。在一實施例中,此第二TCO層之厚度在約 20 nm與約1200 nm之間,在另一實施例中在約1〇〇11111與約 600 nm之間,在另一實施例中,約350 nm厚。TCO層由於 該等層所跨越之相對較大區域而應具有適當之薄層電阻 (Rs)。在一些實施例中,TCO層之薄層電阻在每平方約5歐 姆與約30歐姆之間。在一些實施例中,TCO層之薄層電阻 為每平方約15歐姆。一般而言,希望兩個導電層中之每一 者之薄層電阻大致相同》在一實施例中,兩個層(例如, 4〇4及412)各自具有約每平方10_15歐姆之薄層電阻。 分層結構400、403及409中之每一者分別包括堆疊 414a、414b及414c,該等堆疊中之每一者包括在基板4〇2 之上之第一 TCO層404、CE層410及第二TCO層412。分層 結構400、403及409中之每一者之差異在於EC層係如何形 成的,在每一情形下,此又影響所得界面區之形態。 155961.doc -24- 201222119 與圖3B之程序流程320 一致,堆疊41乜、41朴及41钧中 之母者包括沈積在第一 TCO層404之上之電致變色層。 "亥電致變色層可含有包括金屬氧化物之許多不同電致變色 材料中之任何一或多者。此等金屬氧化物包括氧化鎢 (W〇3)、氧化鉬(Mo〇3) ' 氧化鈮(Nb2〇5)、氧化鈦(Ti〇2)、 氧化銅(Cu〇)、氧化銥(11>2〇3)、氧化鉻(Cr2〇3)、氧化錳 (Mn2〇3)、氧化飢(v2〇5)、氧化錄(Ni2〇3)、氧化始(c〇2〇3) 及其類似者。在一些實施例中,金屬氧化物摻雜有一或多 種摻雜劑,諸如鋰、鈉、鉀、鉬、鈮、釩、鈦及/或其他 合適金屬或含有金屬之化合物。混合氧化物(例如,w_m〇 氧化物、W-ν氧化物)亦可在特定實施例中使用,亦即, 電致變色層包括上述金屬氧化物中之兩者或兩者以上。包 括金屬氧化物之電致變色層能夠接收自反電極層轉移之離 子。 在些貫施例中,將氧化鎢或經摻雜之氧化鎢用於電致 變色層。在本發明之一實施例中,電致變色層實質上由 wo,製成,其中「x」指代電致變色層中之氧與鎢之原子 比,且X在約2.7與3.5之間。已提出僅低於化學計量之氧化 鎢展現電致變色;亦即,化學計量之氧化鎢(w〇3)不展現 電致變色°在-更特定實施例中,將湘工(其中χ小於3〇且 為至少約2.7)用於電致變色層。在另一實施例中,電致變 色層為WO,,其中X在約.2.7與約2.9之間。諸如拉塞福背向 散射光譜測定法(RBS,Rutherf〇rd BackscatteHngGlassTM is a conductive layer coated with fluorinated tin oxide. In the embodiment, the optical transmittance of the substrate (that is, the ratio of the transmitted radiation or the spectrum to the radiation or spectrum of the human being) is (d) For example, about township to 92%. The substrate may have any thickness as long as it has suitable mechanical properties to support the electrochromic device. Although the substrate can be of any size, it is about (10) money mm thick, preferably about 3 mm to 9 mm thick. In some embodiments of the invention, the substrate is architectural glass. Building glass is glass used as building materials. Building glass is used in commercial buildings, but can also be used in residential buildings' and usually (but not necessarily) separates indoor and outdoor environments. In a particular embodiment, the architectural glass is at least 2 inches by 2 inches, and may be larger, for example, up to about 72 inches by 12 inches. Architectural glass is typically at least about 2 mm thick. Building glass less than about 3.2 mm thick can not be tempered. In some embodiments of the invention in which architectural glass is used as a substrate, the substrate can be tempered after the electrochromic stack has been fabricated on the substrate. In some embodiments of the substrate, the substrate is a lime glass from a tin float line. "The percentage of transmission in the visible spectrum of the architectural glass substrate (ie, the overall transmission across the visible spectrum) is generally better than neutral. The substrate is 80% larger, but it may be lower than the transmission percentage of the colored substrate. Preferably, the substrate has a percent transmission in the visible spectrum of at least about 90°/. (e.g. 'about 90% to 92%). The visible spectrum is a typical human eye that responds to a spectrum 'typically from about 380 nm (purple) to about 780 nm (red). In some cases, the glass has a surface between about 10 nm and about 30 nm 155961.doc • 23- 201222119 roughness. In one embodiment, substrate 402 is a soda glass having a sodium diffusion barrier (not shown) to prevent sodium ions from diffusing into the electrochromic device. For the purpose of this description, this configuration is referred to as "substrate 402." Referring again to layered structures 400, 403 and 409, a first TCO layer 404, for example made of defeated tin oxide or other suitable material, which is especially conductive and transparent, is deposited over substrate 402. The transparent conductive oxide includes a metal oxide and a metal oxide doped with one or more metals. Examples of such metal oxides and doped metal oxides include indium oxide, indium tin oxide, doped indium oxide, tin oxide, doped tin oxide, zinc oxide, aluminum zinc oxide, doped Zinc oxide, cerium oxide, doped cerium oxide and the like. In one embodiment, the thickness of the second TCO layer is between about 20 nm and about 1200 nm, and in another embodiment between about 1〇〇11111 and about 600 nm, in another embodiment, About 350 nm thick. The TCO layer should have an appropriate sheet resistance (Rs) due to the relatively large area spanned by the layers. In some embodiments, the TCO layer has a sheet resistance between about 5 ohms and about 30 ohms per square. In some embodiments, the TCO layer has a sheet resistance of about 15 ohms per square. In general, it is desirable that the sheet resistance of each of the two conductive layers be substantially the same. In one embodiment, the two layers (eg, 4〇4 and 412) each have a sheet resistance of about 10-15 ohms per square. . Each of the layered structures 400, 403, and 409 includes a stack 414a, 414b, and 414c, each of which includes a first TCO layer 404, a CE layer 410, and a portion over the substrate 4? Two TCO layers 412. The difference in each of the hierarchical structures 400, 403, and 409 is in how the EC layer is formed, which in each case affects the morphology of the resulting interface region. 155961.doc -24- 201222119 Consistent with the program flow 320 of FIG. 3B, the mothers of the stacks 41, 41, and 41 include an electrochromic layer deposited on the first TCO layer 404. " The electrochromic layer may contain any one or more of a number of different electrochromic materials including metal oxides. These metal oxides include tungsten oxide (W〇3), molybdenum oxide (Mo〇3) 'Nb2〇5), titanium oxide (Ti〇2), copper oxide (Cu〇), yttrium oxide (11). 2〇3), chromium oxide (Cr2〇3), manganese oxide (Mn2〇3), oxidative hunger (v2〇5), oxidation record (Ni2〇3), oxidation start (c〇2〇3) and the like . In some embodiments, the metal oxide is doped with one or more dopants such as lithium, sodium, potassium, molybdenum, niobium, vanadium, titanium, and/or other suitable metals or metal containing compounds. Mixed oxides (e.g., w_m〇 oxide, W-ν oxide) may also be used in certain embodiments, i.e., the electrochromic layer includes two or more of the above metal oxides. An electrochromic layer comprising a metal oxide is capable of receiving ions transferred from the counter electrode layer. In some embodiments, tungsten oxide or doped tungsten oxide is used in the electrochromic layer. In one embodiment of the invention, the electrochromic layer is substantially made of wo, wherein "x" refers to the atomic ratio of oxygen to tungsten in the electrochromic layer, and X is between about 2.7 and 3.5. It has been proposed that only below stoichiometric tungsten oxide exhibits electrochromism; that is, stoichiometric tungsten oxide (w〇3) does not exhibit electrochromism. In a more specific embodiment, Xianggong (where χ is less than 3) And at least about 2.7) for the electrochromic layer. In another embodiment, the electrochromic layer is WO, wherein X is between about .2.7 and about 2.9. Such as Rutherford backscattering spectrometry (RBS, Rutherf〇rd BackscatteHng
Spectroscopy)之技術可識別包括鍵結至鎢之氧原子及未鍵 155961.doc •25- 201222119 結至鎢之氧原子之氧原子之總數。在一些例子中,氧化鶴 層(其中X為3或更大)展現電致變色,其可能係歸因於未結 合之過量氧以及低於化學計量之氧化鎢。在另一實施例 中’氧化鎢層具有化學計量或更多之氧,其中欠為3〇至約 3.5。在本發明之一些實施例中,EC層之至少一部分具有 過量之氧。將EC層之此更高度氧化之區用作形成充當1(:層 之離子傳導電絕緣區之前驅體。在其他實施例中,高度氧 化之EC材料之相異層形成於EC層與ce層之間以用於至少 部分地至離子傳導電絕緣界面區之最終轉換。 在特定實施例中,氧化鎢為晶形、奈米晶形或非晶形 的。在一些實施例中,氧化鎢為實質上奈米晶形的,且具 有平均約5 nm至50 rim(或約5 nm至20 nm)之晶粒大小,以 透射電子顯微學(TEM)為特性。氧化鎢形態或微結構亦可 使用X光繞射(XRD)及/或電子繞射(諸如,選定區域電子繞 射(SAED))特性化為奈米晶形的。舉例而言,奈米晶形電 致變色氧化鎢之特性可能在於以下XRD特徵:約1〇至1〇〇 nm(例如,約55 nm)之晶體大小。此外,奈米晶形氧化鎢 可展現有限之長程有序性,例如,約若干(約5至2〇個)氧化 鎢單位晶胞。 因此,為便利起見,圖3B中之程序流程32〇之剩餘部分 將_第_實_ (包㈣4A中所表示之冗層伽之形幻 予以進一步描述。接著,將在下文描述圖4β及圖牝中分 別表示之第二實施例及第三實施例,其尤其著重於其各別 EC層之形成及形態及/或微結構。 155961.doc -26- 201222119 如參看圖3B所提及,參見325,沈積EC層。在第一實施 例(圖4A中所表示)中,實質上均質之EC層406(包括W03) 經形成作為堆疊414a之部分,其中該EC層與CE層410直接 接觸。在一實施例中,如上所述,該EC層包括W03。在一 實施例中,在沈積W03之至少一部分期間應用加熱。在一 特定實施例中,經過濺鍍標靶若干遍,其中在每一遍經過 時沈積W〇3之一部分,且在每一遍沈積之後將加熱應用於 (例如)基板402以在沈積層406之W03之下一部分之前調節 WO3。在其他實施例中,可在沈積期間連續加熱w〇3層, 且可以連續方式進行沈積,而非經過濺鍍標靶若干遍。在 一實施例中,該EC層之厚度在約300 nm與約600 nm之 間。如所提及,該EC層之厚度取決於所要結果及形成ic層 之方法。 在關於圖4A所描述之實施例中,EC層為厚度在約500 nm與約600 nm之間的使用鎢標靶及包括約40%與約80%之 間的〇2及約20%與約60%之間的Ar之濺鍍氣體濺鍍之 WO3 ’且其中沈積有WO3之基板在形成EC層期間被至少間 歇性地加熱至約150°C與約450°C之間。在一特定實施例 中,EC層為約550 nm厚之使用鎢標靶濺鍍之w〇3,其中該 濺鍍氣體包括約50%至約60%之〇2及約40%至約50%之Ar, 且沈積有WO3之基板在形成該電致變色層期間被至少間歇 性地加熱至約250°C與約350°C之間。在此等實施例中, W〇3層為實質上均質的。在一實施例中,w〇3為實質上多 晶的。咸信,在沈積期間至少間歇性地加熱W〇3幫助多晶 155961.doc -27- 201222119 形式之wo3之形成。 如所提及,許多材料適合於EC層。一般而言,在電致 變色材料中,電致變色材料之著色(或任何光學性質,例 如’吸光度、反射率及透射率之變化)係藉由至材料中之 可逆離子插入(例如,夾插)及電荷平衡電子之對應注入引 起。通常,負責光學過渡之離子之某一小部分在電致變色 材料中不可逆地結合在一起。如本文中所描述,不可逆地 結合之離子之一些或全部用以補償材料中之「盲電荷 (blind charge)」。在大部分電致變色材料中,合適離子包 括鐘離子(Li+)及氫離子(H+)(亦即,質子)。然而,在一些 情況下,其他離子將為合適的。此等離子包括(例如)氣離 子(D+)、鈉離子(Na+)、鉀離子(κ+)、鈣離子(ca++)、鎖離 子(Ba++)、锶離子(Sr++)及鎂離子(Mg++p在本文中所描述 之各種實施例中’鋰離子用以產生電致變色現象。鋰離子 至氧化鎢(W〇3_y(0<yS〜0.3))中之夾插使氧化鎢自透明(褪 色狀態)改變為藍色(著色狀態)。在EC層包括或為氧化鎢 之典型製程中’鋰係(例如)經由濺鍍沈積在EC層406上以 滿足盲電荷(如下文參看圖6及圖7將更詳細論述),參見圖 3B中之程序流程之330。在一實施例中,鋰化係在整合式 沈積系統(其中真空在沈積步驟之間未被破壞)中執行。應 注意’在一些實施例中’鋰並不在此階段添加,而是可在 沈積反電極層之後添加’或在其他實施例中,鋰係在沈積 TCO之後添加。 再次參看圖4A’接下來’在EC層406上沈積CE層410。 155961.doc -28- 201222119 在一些實施例中,反電極層410為無機及/或固體。該反電 極層可包括在電致變色裝置處於褪色狀態下時能夠充當離 子之儲集器之許多不同材料中之一或多者。在藉由(例如) 施加適當電位起始之電致變色過渡期間,反電極層將其保 持之離子中之一些或全部轉移至電致變色層,從而使電致 變色層改變為著色狀態。同時,在NiO及/或NiWO之情況 下’反電極層由於離子之損失而著色。 在一些實施例中,用於反電極之合適材料包括氧化鎳 (犯〇)、氧化鎳鎢(NiWO)、氧化鎳釩、氧化鎳鉻、氧化鎳 鋁、氧化鎳錳、氧化鎳鎂、氧化鉻((>2〇3)、氧化錳(Mn〇2) 及普魯士藍(Prussian blue)。光學被動反電極包括氧化鈽 鈦(Ce〇2-Ti〇2)、氧化錦錯(ce〇2_Zr〇2)、氧化錄(Ni〇)、氧 化鎳鎢(NiW〇)、氧化釩(V2〇5)及氧化物之混合物(例如, 犯2〇3與WO;之混合物)。亦可使用此等氧化物之摻雜調配 物,其中摻雜劑包括(例如)钽及鎢。因為反電極層41〇含有 用以在電致變色材料處於褪色狀態下時在電致變色材料中 產生電致變色現象之離子,所以反電極在其保持顯著量之 此等離子時較佳具有高透射率及中性色彩。反電極形態可 為晶形、奈米晶形或非晶形。 在些貫施例中,在反電極層為氧化鎳鎢之情況下,反 電極材料為非晶形或實質上非晶形的。與實質上非晶形之 氧化鎳鎢反電極之晶形對應物相比’已發現該等實質上非 曰曰形之氧化鎳鎢反電極在一些條件下較佳地執行。如下文 所描述,可藉由使用特定處理條件獲得氧化鎳鎢之非晶形 15596] .doc •29· 201222119 狀態。儘管不希望束縛於任何理論或機制,但咸信,非晶 形氧化鎳鶴係藉由濺鐘製程中之相對較高能量之原子^曰 生。較高能量之原子係(例如)在具有較高標靶功率、較低 腔室屋力(亦即,較高真空)及較小的源至基板之距離之滅 鍍製程中獲得。在所描述之處理條件下,產生在uv/熱曝 露下具有更佳穩定性之較高密度薄膜。 在特定實施例中,存在於氧化鎳鶴中之鎮的量可高達氧 化錦鎢之約90重量%。在一特定實施例中,氧化錄鶴中之 鎳與嫣之質量比在約4:6與6:4之間,在一實例中為約Η。 在—實施例中,NiWO包含約15%(原子)與約6〇%之間的 价,及在約10%與約4〇%之間的w。在另一實施例中, NiWO包含約3〇%(原子)與約45%之間的州,及在約15%與 約35%之間的w。在另一實施例中,Niw〇包含在約 30%(原子)與約45%之間的Ni,及在約2〇%與約3〇%之間的 W。在一實施例中’ NiWO包含約42%(原子)之Ni及約14% 之W。 在一貫施例中,如上所述’參見圖3B之335,CE層410 為NiWO。在一實施例中,ce層之厚度在約150 nm與約 3 00 nm之間,在另一實施例中在約2〇〇 nrn與約250 nm之 間’在另一實施例中為約23〇 nm。 在典型製程中,亦將鋰塗覆至CE層,直至CE層褪色。 應理解’對著色狀態與褪色狀態之間的過渡之述及為非限 制性的且暗示可能實施之電致變色過渡之許多實例中之僅 一個實例。除非本文中另有說明,否則無論何時述及褪 155961.doc -30- 201222119 色-著色過渡’對應之裝置或製程涵蓋諸如非反射-反射、 透明-不透明等之其他光學狀態過渡,此外,術語「褪 色」指代光學中性狀態,例如未著色、透明或半透明。更 進一步,除非本文中另有說明,否則電致變色過渡之「色 a」不限於任何特定波長或波長範圍 如一般熟習此項技 術者所理解,適當電致變色材料及反電極材料之選擇控管 相關光學過渡。 在一特定實施例中,參見圖3B之34〇,鋰(例如,經由滅 鍵)添加至NiWO CE層。在一特定實施例中,參見圖把之 345,在已引入足夠鋰以使Niw〇完全褪色之後添加額外量 之鋰(此程序為可選的,且在一實施例中,在程序之此階 段不添加過量鋰)。在一實施例中,此額外量在基於使該 反電極層褪色所需之量過量約5%與約1 5%之間。在另一實 方&例中,添加至CE層之過量經為基於使該反電極層褪色所 需之量過量約10%。在沈積〇^層410、以鋰使其褪色及添 加額外链之後’參見圖3B之350,在反電極層之上沈積第 二TCO層412。在一實施例中,透明導電氧化物包括氧化 銦錫’在另一實施例中,TCO層為氧化銦錫。在一實施例 中’此第二TCO層之厚度在約20 nm與約1200 nm之間,在 另一實施例中在約1〇〇 nm與約600 nm之間,在另一實施例 中為約350 nm。 再次參看圖4A ’ 一旦完成分層結構4〇〇,則使其經受將 堆疊414a之至少一部分轉換成1(:層之熱化學調節(若其歸 因於裡擴散或其他機制而未經轉換)。堆疊414a為前驅體 155961.doc •31· 201222119 而非電致變色裝置,此係因為該堆疊在Ec層4〇6與層 410之間尚未具有離子傳導/電絕緣層(或區)^在此特定實 施例中,在兩步驟之程序中,EC層4〇6之部分經轉換成… 層408以形成功能性電致變色裝置4〇1。參看圖3b,參見 355,分層結構4〇〇經在一實施例中,該堆疊首 先在惰性氛圍(例如,氬氣)下在約150°C與約450°C之間經 受加熱歷時約10分鐘與約3〇分鐘之間,且接著在〇2下加熱 歷時約1分鐘與約15分鐘之間。在另一實施例中,該堆疊 在約250°C下在惰性氛圍下加熱歷時約15分鐘且接著在 〇2下加熱約5分鐘。接下來,分層結構4〇〇在空氣中經受加 熱。在—實施例中,該堆疊在空氣中在約25(rc與約35〇<t 之間加熱歷時約20分鐘與約40分鐘之間,在另一實施例 中該堆疊在空氣中在約3 00。匚下加熱歷時約3 0分鐘。實 施MTCC所需之能量不必為輻射熱能。舉例而言,在一實 施例中,使用紫外輻射來實施MTCC。在不脫離本發明之 範疇的情況下亦可使用其他能量源。 在多步驟熱化學調節之後,程序流程320完成,且建立 功倉b 1±電致變色裝置。如所提及,且儘管不希望受理論限 制’但咸信’堆疊414a中之鋰與EC層406及/或CE層410之 刀起組合以形成充當1C層之界面區408。咸信界面 區408主要為鎢酸鋰(Li2W〇4),已知其相對於傳統ic層材 料具有良好的離子傳導及電絕緣性質。如上文所論述,尚 不月確知曉此現象如何發生。存在在多步驟熱化學調節期 門必/頁發生以在Ec層與CE層之間形成離子傳導電絕緣區 155961.doc -32- 201222119 408之化學反應,但亦認為,行進穿過堆疊之鋰之初始通 量(例如,由如上所述之添加至CE層之過量鋰提供)在1(:層 4〇8之形成中起作用。離子傳導電絕緣區之厚度可取決於 所使用之材料及用於形成該層之處理條件而改變。在一些 實施例中’界面區408之厚度在約1〇 nni與約丨5〇 nm之間, 在另一貫施例中在約20 nm與約100 nm之間,且在其他實 施例中在約30 nm與約50 nm之間。 如上文所提及’存在用於形成EC層之許多合適材料。 因而,在上述方法中使用(例如)裡或其他合適離子,吾人 可自富氧EC材料開始製成充當ic層之其他界面區。用於此 用途之合適EC材料包括(但不限於)Si〇2、Nb2〇5、Ta205、 Ti〇2、Zr〇2及Ce〇2。在使用經離子之特定實施例中,離子 傳導材料(諸如,但不限於,矽酸鋰、矽酸鋰鋁、硼酸鋰 紹、氟化鋰鋁、硼酸鋰、氮化鋰、矽酸鋰锆、鈮酸鋰、蝴 石夕酸裡、鱗石夕酸經及其他此等基於裡之陶瓷材料、石夕石或 氧化矽(包括氧化鋰矽))可製成為充當1C層之界面區。 如所提及’在一實施例中,離子傳導區之前驅體為經由 本文中所描述之裡化及MTCC轉化成離子傳導/電絕緣區之 富氧(超化學計量之)層。儘管不希望束缚於理論,但咸 信,在鋰化後’過量氧形成氧化鋰,其進一步形成鋰鹽 (亦即,鋰電解質),諸如,鎢酸鋰(Li2W04)、鉬酸鋰 (Li2Mo04)、鈮酸鋰(LiNb03)、鈕酸鋰(LiTa03)、鈦酸鋰 (LizTiO3)、锆酸鋰(LizZrO3)及其類似物。在一實施例中, 界面區包含下列各者中之至少一者:氧化鎢(W〇3+x , 155961.doc •33- 201222119 OSxSl.5)、氧化翻(m〇03+x,〇sd5)、氧化鈮(Nb2〇5+x, 〇SxS2)、氧化欽(Ti02+x,(^d.5)、氧化钽(Ta2〇5+x, 〇$x$2)、氧化錘(Zr02+x,〇sd .5)及氧化鈽(Ce〇2+x ’ 0<x<1.5) ° 然而,任何材料可用於離子傳導界面區,只要該材料可 經製造而具有低缺陷度且其在實質上阻止電子通過的同時 允許離子在反電極層410與電致變色層4〇6之間通過即可。 該材料可以實質上傳導離子且實質上抵抗電子為特性。在 一實施例中,該離子導體材料具有介於約1〇-1〇西門子/公 分(Siemens/cm)(或ohn^cnT丨)與約ι〇-3西門子/公分之間的 離子電導率及大於1〇5歐姆-公分之電子抵抗性。在另一實 施例中,a亥離子導體材料具有介於約1 〇·8西門子/公分與約 1〇·3西門子/公分之間的離子電導率及大於i 〇1Q歐姆公分之 電子抵抗性。雖然離子傳導層應大體上抗漏電流(例如, 提供不大於約1 5 μΑ/cm2之漏電流),但已發現,如本文中 所描述而製造之一些裝置具有驚人的高之漏電流(例如, 在約40 μΑ/cm與約150 μΑ/ειη之間),但仍提供跨越裝置之 良好色彩變化且有效地操作。 如上文所提及’存在在形成堆疊之後,於EC層與ce層 之間建立離子傳導電絕緣區之至少兩種其他方式。此等額 外實施例將在下文參考將氧化鎢用於1〇:層之特定實例予以 描述又,如上文所提及,當(例如)經擴散或熱將EC及/ 或CE層之—些轉換成界面區時,具有ic性質之界面區可在 製造堆疊期間在原位形成。 155961.doc •34· 201222119 通常’在製財_建立離子傳㈣存在特定益處。首 先’可保4離子傳導材料不受在Ec層及ce層之沈積及鐘 化期間發生的苛刻處理中之一些影響。舉例而言,藉由電 漿製程沈積此等層常常伴隨著緊接堆疊之大的電壓降,常 在15 20伏特上下。此等大電壓可損害敏感離子傳導材料 或造成敏感離子傳導材料之分解。藉由將㈣料形成移至 製程中稱後階段,該材料即不曝露於潛在之損害電壓極 值。其次’藉由在製程中稍後形成1C材料,吾人可更佳地 控制在完成EC層及CE層兩者之前所不可能的一些處理條 件。此等條件包括鐘擴散及電極之間的電流。在製程中後 』控制此等及其他條件提供額外靈活性以使材料之物理 性質及化學性質適合特定應用。因此,並非本發明之所有 益處皆歸因於充當1C層之獨特界面區,亦即,亦存在製造 及其他益處。 已觀測到’與使用用於形成1C層之習知技術(例如,自 1C材料標靶之PVD)製造之裝置相比,根據本文中所描述 之實施例中之"'些形成之離子傳導材料具有優異效能。舉 例而言,已發現,與傳統裝置之20_25分鐘或以上相比, 裝置切換速度非常快(例如,小於10分鐘,在-實例中為 約8分鐘)以達成約80%之最終狀態。在一些例子中,本文 中所描述之裝置具有優於習知裝置之切換速度數量級。此 可2可歸因於較大量的安置在界面區及/或分級界面中之 ^谷易地轉移(例如,在此與界面區之間及/或在ce與界面 區之間)之Μ °此等鋰可處於與存在於界面區中之1C相互 155961.doc •35· 201222119 混之EC及/或CE相中。其亦可能歸因於存在於界面區中之 1C材料之相對較薄層或網路。為支持此觀點,已觀測到’ 根據本文中之教示製造之一些裝置具有高漏電流,但仍驚 人地展現良好色彩變化及良好效率。在一些情況下,已發 現穩健執行之裝置之漏電流密度為至少約丨〇〇 pA/cm。 現參看圖4Β,在第二實施例中,堆疊41仆之最初敷設之 EC材料實際上為兩個層:第一 w〇3層4〇6 ’其類似於圖4A 中之層406 ’但厚度在約350 nm與約450 nm之間,該第一 層係使用鎢標靶及包括約40%與約80%之間的〇2及約2〇0/〇 與約60%之間的Ar之第一濺鍍氣體濺鍍;及第二w〇3層 405 ’其厚度在約1〇〇 nm與約2〇〇 nm之間,該第二層係使 用鎢標靶及包括約70%與1〇〇%之間的〇2及〇%與約3〇%之間 的Ar之第二濺鍍氣體濺鍍。在此實施例中,藉由在第一 WO3層406之沈積期間將基板4〇2至少間歇性地加熱至約 150 C與約450°C之間而施加熱,但在第二冒〇3層4〇5之沈 積期間不加熱或實質上不加熱。在一更特定實施例中,層 406為約400 nm厚,且該第一濺鍍氣體包括約5〇%與約6〇% 之間的〇2及約40%與約50%之間的Ar ;第二W〇3層405為約 150 nm厚’且該第二濺鍍氣體實質上為純〇2。在此實施例 中,在第一 WO3層406之形成期間至少間歇性地施加熱至 約200°C與約350。(:之間,但在第二WO3層405之形成期間 不加熱或實質上不加熱。以此方式,該第一 w〇3層為實質 上多晶的,而該第二W〇3層不必如此。 再次參看圖4B,如上文關於圖3B及圖4A所描述,藉由 155961.doc -36. 201222119 以下操作來完成堆疊:鋰化EC層406及405以大致或實質上 滿足盲電荷、沈積CE層410、將CE層鋰化至褪色狀態、添 加額外鐘及沈積第二丁<:0層412以完成分層堆疊4〇3 ^對分 層堆疊403執行類似熱化學調節以提供分層堆疊4〇7、包括 離子傳導電絕緣區408a之功能性電致變色裝置。儘管不希 望束缚於理論,但在此實例中,咸信W〇3之富氧層405主 要充當前驅體材料之源以形成界面區408a。在此實例中, 整個富氧WO3層經描繪為轉換成界面區408a,然而,已發 現,情況並不始終如此。在一些實施例中,富氧層之僅一 部分經轉換而形成起到1C層之功能之界面區。 現參看圖4C,在第三實施例中,分層堆疊4〇9包括EC層 406a(其具有\v〇3之分級組合物⑶讲尸似⑴’⑽)且形成 為堆疊414c之部分)’其中該分級組合物包括變化含量之 氧°在一非限制性實例中,在^(:<£層(410)界面處存在比 TCO層404與EC層406a之界面處高的EC層406a中之氧濃 度。 在一實施例中’ EC層4〇6a為厚度在約500 nm與約600 nm之間的使用鎢標靶及濺鍍氣體濺鍍之分級組合物w〇3 層’其中該濺鍍氣體在濺鍍電致變色層開始時包括約4〇% 與約80%之間的〇2及約20%與約60%之間的Ar,且該濺鍍 氣體在濺鍍該電致變色層結束時包括約70%與100%之間的 〇2及〇%與約30%之間的Ar,且其中在ec層406a之形成之 開始期間至少間歇性地施加熱至(例如)基板402至約150°C 與約450°C之間’但不或實質上不在£(:層4〇6a之至少一最 155961.doc -37- 201222119 後力之沈積期間施加熱。在一更特定實施例中,分級組 合物W〇3層為約55〇 nm厚;該濺鍍氣體在濺鍍該電致變色 層開始時包括約50%與約60%之間的〇2及40%與約50%之間 的Ar ’且該濺鍍氣體在濺鍍該電致變色層結束時為實質上 純〇2 ’且其中在電致變色層之形成之開始期間至少間歇性 地施加熱至(例如)基板402至約200eC與約350。(:之間,但不 或實質上不在電致變色層之至少一最後部分之沈積期間施 加熱。在一實施例中,在沈積開始時在所述溫度範圍下施 加熱,且逐漸減小至在沈積了約一半之£(:層時不施加熱, 而濺鍍氣體組合物在EC層之沈積期間沿著實質上線性之速 率自約50%與約60%之間的ο:及約4〇%與約5〇%之間的旭調 整至實質上純〇2。 料及電致變色材料(例如 包括梯度。該梯唐可裎 更一般地,該界面區通常(但不必)具有包括由不同相及/ 或組成表示之至少兩個離散組份之異質結構。此外,該界 面區在此等兩個或兩個以上離散組份(諸如,離子傳導材 如,鎢酸鋰與氧化鎢之混合物))中可The technique of Spectroscopy can identify the total number of oxygen atoms that are bonded to the oxygen atom of tungsten and the unbonded 155961.doc •25- 201222119 oxygen atom bound to tungsten. In some instances, the oxidized crane layer (where X is 3 or greater) exhibits electrochromism, which may be due to uncombined excess oxygen and less than stoichiometric tungsten oxide. In another embodiment, the tungsten oxide layer has a stoichiometric or more oxygen, wherein the amount is from about 3 Torr to about 3.5. In some embodiments of the invention, at least a portion of the EC layer has excess oxygen. This more highly oxidized region of the EC layer is used to form a precursor that acts as an ion conducting electrically insulating region of the layer (in other embodiments, a highly oxidized EC material is formed in the EC layer and the ce layer). Between the final conversion for at least partially to the ionically conductive electrically insulating interface region. In a particular embodiment, the tungsten oxide is crystalline, nanocrystalline or amorphous. In some embodiments, the tungsten oxide is substantially Rice crystal-shaped, with an average grain size of about 5 nm to 50 rim (or about 5 nm to 20 nm), characterized by transmission electron microscopy (TEM). X-rays can also be used for tungsten oxide morphology or microstructure. Diffraction (XRD) and/or electron diffraction (such as selected area electron diffraction (SAED)) are characterized as nanocrystalline. For example, the characteristics of nanocrystalline electrochromic tungsten oxide may lie in the following XRD features. : crystal size of about 1 〇 to 1 〇〇 nm (for example, about 55 nm). In addition, nanocrystalline tungsten oxide can exhibit limited long-range order, for example, about several (about 5 to 2 〇) tungsten oxide. Unit cell. Therefore, for the sake of convenience, the program flow in Figure 3B The remainder of 32 进一步 will further describe the illusion of cues represented by ____ (package (4) 4A. Next, the second embodiment and the third respectively shown in Fig. 4β and Fig. 2 will be described below. Examples, which are particularly focused on the formation and morphology and/or microstructure of their respective EC layers. 155961.doc -26- 201222119 As mentioned with reference to Figure 3B, see 325, Deposition of the EC layer. In the first embodiment ( In Fig. 4A), a substantially homogeneous EC layer 406 (including W03) is formed as part of stack 414a, wherein the EC layer is in direct contact with CE layer 410. In one embodiment, as described above, the EC The layer includes W03. In one embodiment, heating is applied during at least a portion of the deposition W03. In a particular embodiment, the sputtering target is passed through several times, wherein one portion of the W〇3 is deposited at each pass, and Heating is applied to, for example, substrate 402 after deposition for each pass to adjust WO3 prior to a portion below W03 of deposited layer 406. In other embodiments, the layer of w〇3 may be continuously heated during deposition and may be deposited in a continuous manner. Instead of being sputtered In a number of embodiments, the thickness of the EC layer is between about 300 nm and about 600 nm. As mentioned, the thickness of the EC layer depends on the desired result and the method of forming the ic layer. In the depicted embodiment, the EC layer is a tungsten target having a thickness between about 500 nm and about 600 nm and includes between about 40% and about 80% 〇2 and between about 20% and about 60%. The sputtered gas sputtered WO3' of Ar and the substrate in which WO3 is deposited are at least intermittently heated to between about 150 ° C and about 450 ° C during formation of the EC layer. In a particular embodiment, the EC layer is about 550 nm thick using tungsten target sputtering, wherein the sputtering gas comprises from about 50% to about 60% 〇2 and from about 40% to about 50%. Ar, and the substrate deposited with WO3 is at least intermittently heated to between about 250 ° C and about 350 ° C during formation of the electrochromic layer. In these embodiments, the W〇3 layer is substantially homogeneous. In one embodiment, w 〇 3 is substantially polycrystalline. Xianxin, at least intermittently heating W〇3 during the deposition to help the formation of polycrystalline 155961.doc -27- 201222119 form of wo3. As mentioned, many materials are suitable for the EC layer. In general, in electrochromic materials, the coloring of an electrochromic material (or any optical property, such as a change in 'absorbance, reflectance, and transmittance') is caused by reversible ion insertion into the material (eg, intercalation). And the corresponding injection of charge balance electrons. Typically, a small portion of the ions responsible for the optical transition are irreversibly bonded together in the electrochromic material. As described herein, some or all of the irreversibly combined ions are used to compensate for the "blind charge" in the material. Among most electrochromic materials, suitable ions include clock ions (Li+) and hydrogen ions (H+) (i.e., protons). However, in some cases, other ions will be suitable. The plasma includes, for example, gas ions (D+), sodium ions (Na+), potassium ions (κ+), calcium ions (ca++), lock ions (Ba++), barium ions (Sr++), and magnesium ions (Mg++p). In the various embodiments described herein, 'lithium ions are used to generate electrochromism. The intercalation of lithium ions to tungsten oxide (W〇3_y (0<yS~0.3)) makes the tungsten oxide self-transparent (faded state) Change to blue (colored state). In the typical process of the EC layer including or for tungsten oxide, 'lithium' is deposited, for example, on the EC layer 406 via sputtering to meet the blind charge (see Figures 6 and 7 below). As will be discussed in more detail), see program flow 330 of Figure 3B. In one embodiment, the lithiation is performed in an integrated deposition system in which the vacuum is not destroyed between deposition steps. It should be noted that 'in some In the embodiment, 'lithium is not added at this stage, but may be added after depositing the counter electrode layer' or in other embodiments, the lithium system is added after depositing the TCO. Referring again to FIG. 4A 'next' on the EC layer 406 Depositing CE layer 410. 155961.doc -28- 201222119 In some implementations The counter electrode layer 410 is inorganic and/or solid. The counter electrode layer may comprise one or more of a number of different materials capable of acting as a reservoir of ions when the electrochromic device is in a discolored state. During the electrochromic transition initiated by the application of a suitable potential, for example, the counter electrode layer transfers some or all of the ions it retains to the electrochromic layer, thereby changing the electrochromic layer to a colored state. Meanwhile, at NiO And/or in the case of NiWO, the counter electrode layer is colored due to the loss of ions. In some embodiments, suitable materials for the counter electrode include nickel oxide (nickel), nickel tungsten oxide (NiWO), nickel vanadium oxide, Nickel oxide chromium, nickel aluminum oxide, nickel manganese oxide, nickel magnesium oxide, chromium oxide ((>2〇3), manganese oxide (Mn〇2), and Prussian blue. The optical passive counter electrode includes titanium ruthenium oxide. a mixture of (Ce〇2-Ti〇2), oxidized 〇(ce〇2_Zr〇2), oxidized (Ni〇), nickel oxynitride (NiW〇), vanadium oxide (V2〇5) and oxide (for example , a mixture of 2〇3 and WO;) can also be used for such oxidation Doping formulations, wherein the dopant comprises, for example, tantalum and tungsten, because the counter electrode layer 41 contains ions for generating electrochromism in the electrochromic material when the electrochromic material is in a discolored state Therefore, the counter electrode preferably has a high transmittance and a neutral color when it maintains a significant amount of the plasma. The counter electrode form may be a crystal form, a nano crystal form or an amorphous form. In some embodiments, the counter electrode layer is In the case of nickel oxide tungsten, the counter electrode material is amorphous or substantially amorphous. Compared to the crystalline counterpart of the substantially amorphous nickel-tungsten tungsten counter electrode, the substantially non-曰曰-shaped oxidation has been found. The nickel tungsten counter electrode is preferably performed under some conditions. As described below, the amorphous form of nickel tungsten oxide can be obtained by using specific processing conditions. 15596] .doc • 29· 201222119 state. Although not wishing to be bound by any theory or mechanism, it is believed that amorphous nickel oxide cranes are produced by relatively high energy atoms in the splash clock process. Higher energy atomic systems are obtained, for example, in a blanking process with higher target power, lower chamber home power (i.e., higher vacuum), and smaller source to substrate distance. Under the described processing conditions, a higher density film with better stability under uv/thermal exposure is produced. In a particular embodiment, the amount of town present in the nickel oxide crane can be as high as about 90% by weight of the oxidized strontium tungsten. In a particular embodiment, the mass ratio of nickel to rhenium in the oxidized log crane is between about 4:6 and 6:4, in one example about Η. In an embodiment, NiWO comprises a valence between about 15% (atoms) and about 6%, and between about 10% and about 4,000%. In another embodiment, the NiWO comprises between about 3% (atoms) and about 45% of the states, and between about 15% and about 35% of w. In another embodiment, Niw(R) comprises between about 30% (atoms) and about 45% Ni, and between about 2% and about 3%. In one embodiment, 'NiWO contains about 42% (atomic) Ni and about 14% W. In a consistent embodiment, as described above, see 335 of Figure 3B, the CE layer 410 is NiWO. In one embodiment, the thickness of the ce layer is between about 150 nm and about 300 nm, and in another embodiment between about 2 〇〇 nrn and about 250 nm 'in another embodiment, about 23 〇nm. In a typical process, lithium is also applied to the CE layer until the CE layer fades. It should be understood that the description of the transition between the colored state and the faded state is merely one of many examples of non-limiting and suggesting possible electrochromic transitions. Unless otherwise stated herein, whenever a 155961.doc -30-201222119 color-coloring transition' corresponds to a device or process that covers other optical state transitions such as non-reflective-reflective, transparent-opaque, etc., "Fad" refers to an optically neutral state such as uncolored, transparent or translucent. Furthermore, unless otherwise stated herein, the "color a" of the electrochromic transition is not limited to any particular wavelength or range of wavelengths, as understood by those skilled in the art, the selection of suitable electrochromic materials and counter electrode materials. Tube related optical transitions. In a particular embodiment, referring to 34 of Figure 3B, lithium (e.g., via a bond) is added to the NiWO CE layer. In a particular embodiment, referring to FIG. 345, an additional amount of lithium is added after sufficient lithium has been introduced to completely fade Niw ( (this procedure is optional, and in one embodiment, at this stage of the process Do not add excess lithium). In one embodiment, the additional amount is between about 5% and about 5% excess based on the amount required to fade the counter electrode layer. In another example & example, the excess added to the CE layer is about 10% excess based on the amount required to fade the counter electrode layer. After depositing the layer 410, dissolving it with lithium, and adding additional chains, see 350 of Figure 3B, a second TCO layer 412 is deposited over the counter electrode layer. In one embodiment, the transparent conductive oxide comprises indium tin oxide. In another embodiment, the TCO layer is indium tin oxide. In one embodiment 'this second TCO layer has a thickness between about 20 nm and about 1200 nm, in another embodiment between about 1 〇〇 nm and about 600 nm, in another embodiment About 350 nm. Referring again to Figure 4A', once the layered structure 4 is completed, it is subjected to converting at least a portion of the stack 414a to 1 (the thermochemical adjustment of the layer (if it is not converted due to diffusion or other mechanism) The stack 414a is the precursor 155961.doc • 31·201222119 instead of the electrochromic device because the stack does not have an ion conducting/electrical insulating layer (or region) between the Ec layer 4〇6 and the layer 410. In this particular embodiment, in a two-step process, a portion of the EC layer 4〇6 is converted into a layer 408 to form a functional electrochromic device 4〇1. Referring to Figure 3b, see 355, Layered Structure 4〇 In one embodiment, the stack is first subjected to heating between about 150 ° C and about 450 ° C under an inert atmosphere (eg, argon) for between about 10 minutes and about 3 minutes, and then Heating at 〇 2 lasts between about 1 minute and about 15 minutes. In another embodiment, the stack is heated at about 250 ° C under an inert atmosphere for about 15 minutes and then heated at 〇 2 for about 5 minutes. Next, the layered structure 4 is subjected to heating in air. The stack is heated between about 25 (rc and about 35 Torr) for about 20 minutes and about 40 minutes in air, and in another embodiment the stack is about 300 in air. The heating takes about 30 minutes. The energy required to implement the MTCC need not be radiant heat. For example, in one embodiment, the MTCC is implemented using ultraviolet radiation. Other energies may be used without departing from the scope of the invention. After the multi-step thermochemical conditioning, program flow 320 is complete and the work chamber b 1 ± electrochromic device is established. As mentioned, and although not wishing to be bound by theory, the lithium in the stack 414a The knives of the EC layer 406 and/or the CE layer 410 combine to form an interface region 408 that acts as a 1C layer. The smectic interface region 408 is primarily lithium tungstate (Li2W〇4), which is known to be good relative to conventional ic layer materials. Ion conduction and electrical insulation properties. As discussed above, it is not known how this phenomenon occurs. There is a multi-step thermochemical conditioning period that must occur/page to form ion-conducting electrical insulation between the Ec layer and the CE layer. District 155961.doc -32- 201222119 408 The reaction, but it is also believed that the initial flux of lithium traveling through the stack (eg, provided by excess lithium added to the CE layer as described above) acts in the formation of 1 (: layer 4 〇 8). The thickness of the insulating region may vary depending on the materials used and the processing conditions used to form the layer. In some embodiments, the thickness of the interface region 408 is between about 1 〇 nni and about 〇 5 〇 nm, in another It is consistent between about 20 nm and about 100 nm in a consistent embodiment, and between about 30 nm and about 50 nm in other embodiments. As mentioned above, there are many suitable materials for forming an EC layer. Thus, in the above methods, for example, or other suitable ions, we can make other interface regions that act as ic layers starting from the oxygen-rich EC material. Suitable EC materials for this purpose include, but are not limited to, Si〇2, Nb2〇5, Ta205, Ti〇2, Zr〇2, and Ce〇2. In particular embodiments in which ions are used, ion conducting materials such as, but not limited to, lithium niobate, lithium aluminum niobate, lithium borate, lithium aluminum fluoride, lithium borate, lithium nitride, lithium zirconium niobate, Lithium niobate, ruthenium acid, scaly acid and other such ceramic materials based on ceramsite, or cerium oxide (including lithium lanthanum oxide) can be made into an interface region serving as a 1C layer. As mentioned, in one embodiment, the ion-conducting region precursor is an oxygen-rich (superstoichiometric) layer that is converted to an ion conducting/electrically insulating region via the nucleation and MTCC described herein. Although not wishing to be bound by theory, it is believed that after lithiation, excess oxygen forms lithium oxide, which further forms a lithium salt (ie, a lithium electrolyte), such as lithium tungstate (Li2W04), lithium molybdate (Li2Mo04). Lithium niobate (LiNb03), lithium nitrite (LiTa03), lithium titanate (LizTiO3), lithium zirconate (LizZrO3) and the like. In one embodiment, the interface region comprises at least one of: tungsten oxide (W〇3+x, 155961.doc • 33-201222119 OSxSl.5), oxidized turn (m〇03+x, 〇sd5) ), yttrium oxide (Nb2〇5+x, 〇SxS2), oxidized chin (Ti02+x, (^d.5), yttrium oxide (Ta2〇5+x, 〇$x$2), oxidized hammer (Zr02+x) , 〇sd .5) and yttrium oxide (Ce 〇 2+ x ' 0< x < 1.5) ° However, any material can be used for the ion-conducting interface region as long as the material can be manufactured to have low defectivity and it is substantially Blocking electrons while allowing ions to pass between the counter electrode layer 410 and the electrochromic layer 4〇6. The material can conduct ions substantially and be substantially resistant to electrons. In one embodiment, the ion conductor The material has an ionic conductivity between about 1〇-1〇Siemens/cm (or ohn^cnT丨) and about ι〇-3 Siemens/cm and an electron greater than 1〇5 ohm-cm Resistance. In another embodiment, the a ion conductor material has an ionic conductivity between about 1 〇·8 Siemens/cm and about 1 〇3 Siemens/cm. Electrical resistance greater than i 〇 1Q ohm centimeters. Although the ion conducting layer should be substantially resistant to leakage current (e.g., providing a leakage current of no more than about 15 μΑ/cm 2 ), it has been found to be fabricated as described herein. Some devices have surprisingly high leakage currents (eg, between about 40 μΑ/cm and about 150 μΑ/ειη), but still provide good color variation across the device and operate efficiently. As mentioned above, After forming the stack, at least two other ways of establishing an ion conducting electrically insulating region between the EC layer and the ce layer are provided. These additional embodiments will be described below with reference to a specific example of using tungsten oxide for a layer: As mentioned above, when, for example, diffusion or heat is used to convert the EC and/or CE layers into interfacial regions, interface regions having ic properties can be formed in situ during fabrication of the stack. 155961.doc • 34· 201222119 Usually there is a specific benefit in 'making money _ establishing ion transmission (4). First of all, 'enable 4 ion-conducting materials are not affected by some of the harsh treatments that occur during the deposition and clocking of the Ec and ce layers. In other words, the deposition of such layers by a plasma process is often accompanied by a large voltage drop immediately adjacent to the stack, often above and below 15 20 volts. Such large voltages can damage sensitive ion conducting materials or cause decomposition of sensitive ion conducting materials. By moving the (four) material formation to the post-stage phase of the process, the material is not exposed to the potential damage voltage extremes. Secondly, by forming the 1C material later in the process, we can better control the completion of the EC layer and Some processing conditions that were previously impossible for the CE layer. These conditions include clock diffusion and current flow between the electrodes. Controlling these and other conditions during the process provides additional flexibility to tailor the physical and chemical properties of the material to the particular application. Therefore, not all of the benefits of the present invention are due to the unique interface area that acts as the 1C layer, i.e., there are manufacturing and other benefits as well. It has been observed that 'the formation of ion conduction according to the embodiments described herein is compared to devices made using conventional techniques for forming a 1C layer (eg, PVD from a 1C material target). The material has excellent performance. For example, it has been found that the device switches very fast (e.g., less than 10 minutes, in the example - about 8 minutes) to achieve a final state of about 80% compared to 20-15 minutes or more of conventional devices. In some examples, the devices described herein have an order of magnitude that is superior to conventional devices. This can be attributed to a larger amount of placement in the interface zone and/or the grading interface (eg, between the interface zone and/or between the ce and the interface zone). These lithium may be in the EC and/or CE phase mixed with the 1C mutual 155961.doc • 35· 201222119 present in the interface region. It may also be due to a relatively thin layer or network of 1C material present in the interface region. To support this view, it has been observed that some devices fabricated according to the teachings herein have high leakage currents, but still surprisingly exhibit good color variations and good efficiency. In some cases, devices that have been found to perform robustly have a leakage current density of at least about 丨〇〇 pA/cm. Referring now to Figure 4A, in the second embodiment, the initially laid EC material of the stack 41 is actually two layers: a first w〇3 layer 4〇6' which is similar to layer 406' in Figure 4A but thickness Between about 350 nm and about 450 nm, the first layer uses a tungsten target and includes between about 40% and about 80% of 〇2 and between about 2〇0/〇 and about 60% of Ar. a first sputter gas sputtering; and a second w 〇 3 layer 405 ′ having a thickness between about 1 〇〇 nm and about 2 〇〇 nm, the second layer using a tungsten target and including about 70% and 1第二2 between 〇2 and 〇% with about 3〇% of Ar's second sputtering gas sputtering. In this embodiment, heat is applied by at least intermittently heating the substrate 4〇2 to between about 150 C and about 450 °C during deposition of the first WO3 layer 406, but in the second layer of the third The deposition of 4〇5 is not heated or substantially not heated. In a more specific embodiment, layer 406 is about 400 nm thick, and the first sputtering gas comprises between about 5% and about 6% of 〇2 and between about 40% and about 50% of Ar. The second W 〇 3 layer 405 is about 150 nm thick 'and the second sputtering gas is substantially pure 〇 2 . In this embodiment, heat is applied at least intermittently to about 200 ° C and about 350 during formation of the first WO 3 layer 406. (: between, but not heated or substantially not heated during the formation of the second WO3 layer 405. In this way, the first w〇3 layer is substantially polycrystalline, and the second W〇3 layer does not have to Referring again to Figure 4B, as described above with respect to Figures 3B and 4A, the stacking is accomplished by the following operations: lithiated EC layers 406 and 405 to substantially or substantially satisfy blind charge, deposition. The CE layer 410, the CE layer is lithiated to a faded state, an additional clock is added, and a second layer <:0 layer 412 is deposited to complete the layered stack 4〇3 ^ Performing a similar thermochemical adjustment on the layered stack 403 to provide delamination Stack 4〇7, a functional electrochromic device comprising an ion-conducting electrically insulating region 408a. Although not wishing to be bound by theory, in this example, the oxygen-rich layer 405 of the salt-like W〇3 is primarily a source of current precursor material. To form interface region 408a. In this example, the entire oxygen-rich WO3 layer is depicted as being converted into interface region 408a, however, it has been found that this is not always the case. In some embodiments, only a portion of the oxygen-rich layer is converted And form an interface area that functions as a 1C layer. Referring to FIG. 4C, in the third embodiment, the layered stack 4〇9 includes an EC layer 406a (which has a hierarchical composition of \v〇3 (3) and is formed as part of the stack 414c) The graded composition includes varying levels of oxygen. In a non-limiting example, there is an EC layer 406a at the interface of the layer (410) that is higher than the interface between the TCO layer 404 and the EC layer 406a. Oxygen concentration. In one embodiment, the 'EC layer 4〇6a is a graded composition w〇3 layer using a tungsten target and a sputtering gas sputtering thickness between about 500 nm and about 600 nm, where the sputtering The gas comprises between about 4% and about 80% of 〇2 and between about 20% and about 60% of Ar at the beginning of the sputtered electrochromic layer, and the sputtering gas is sputtered on the electrochromic layer Included between about 70% and 100% of 〇2 and 〇% and about 30% of Ar, and wherein at least intermittently applies heat to, for example, substrate 402 during the beginning of formation of ec layer 406a Apply heat between about 150 ° C and about 450 ° C 'but not substantially or substantially not at least one of the most 155961.doc -37 - 201222119 after the deposition of the layer. In an embodiment, the graded composition W 〇 3 layer is about 55 〇 nm thick; the sputtering gas comprises between about 50% and about 60% 〇 2 and 40% and about 100% of the beginning of sputtering the electrochromic layer. Between 50% of Ar' and the sputtering gas is substantially pure '2' at the end of sputtering of the electrochromic layer and wherein at least intermittently applies heat to the beginning of the formation of the electrochromic layer (eg Substrate 402 to about 200 eC and about 350. (between, but not or substantially not during the deposition of at least a final portion of the electrochromic layer. In one embodiment, heat is applied at the temperature range at the beginning of deposition and is gradually reduced to about half of the deposit (the layer is not applied with heat, and the deposition of the sputtering gas composition in the EC layer) During the period of substantially linear, from about 50% to about 60%, and between about 4% and about 5%, to a substantially pure 〇2 material and electrochromic material (eg In addition, the interface region generally (but not necessarily) has a heterostructure comprising at least two discrete components represented by different phases and/or compositions. Furthermore, the interface region is herein One or more discrete components (such as ion conductive materials such as a mixture of lithium tungstate and tungsten oxide)
155961.doc •38· 201222119 括過渡至(超化學計量之)氧化鈮區中之氧化鎢區。該氧化 銳區之部分或全部經轉換成界面區。在最後結構中,氧化 鶴區為實質上多晶的,且微結構在界面區處過渡至實質上 非晶形的。 再次參看圖4C’如上文關於圖3B及圖4A所描述,藉由 以下操作來完成堆疊:鋰化EC層406a以大致或實質上滿足 盲電荷、沈積CE層410、鋰化CE層至褪色狀態、添加額外 鋰及沈積第二TCO層412以完成分層堆疊409。對分層堆疊 409執行類似之多步驟熱化學調節以提供分層堆疊411、包 括離子傳導電絕緣區4〇8b及原始分層EC層406a之至少一部 分(其在功能性電致變色裝置41 i中充當EC層)之功能性電 致’變色裝置《儘管不希望束缚於理論,但在此實例中,咸 信,WO3之分級層之最上層富氧部分主要形成分級界面區 408b。儘官不希望束缚於理論,但存在如下可能性:界面 區之形成為受自身限制的且取決於堆疊中之氧、鋰、電致 變色材料及/或反電極材料之相對量。 在本文中所描述之各種實施例中,電致冑色堆疊經描述 為在特定處理階段期間不或實f上不加熱。在1 = 中:在加熱步驟之後,主動或被動地(例如,使用散熱γ 冷部堆疊。本發明之設備包括主動及被動冷卻組件,例 如’主動冷卻可包括經由流體循環、曝露於冷(例如,扣 由膨脹)氣體之冷卻、致冷單元及其類似者而冷卻之: :。被動冷卻組件可包括散熱片,諸如金屬塊及其類似 者,或僅自於熱之曝露移除基板。 155961.doc •39· 201222119 本發明之另一態樣為一種製造電致變色裝置之方法,該 方法包括:(a)形成包括電致變色材料之電致變色層或包括 反電極材料之反電極層;(13)在該電致變色層或該反電極層 上方形成中間層,其中該中間層包括該電致變色材料、該 反電極材料及額外材料中之至少一者之富氧形式,其中該 額外材料包括相異之電致變色材料或反電極材料,其中該 中間層不為實質上電絕緣的;(c)形成該電致變色層及該反 電極層中之另一者,及(d)允許該中間層之至少一部分變得 實質上電絕緣。在一實施例中,該電致變色材料為w〇3。 在另一實施例中,(a)包括使用鎢標靶及包括約4〇%與約 80〇/。之間的〇2及约20%與约60%之間的心之第一濺鑛氣體 減鑛WO3以達到在約350 nm與約450 nm之間的厚度,及在 該電致變色層之形成期間至少間歇性地加熱至約1 5〇β(:與 約450°C之間。在另_實施例中’(b)包括在不加熱的情況 下使用鎢標靶及包括約70%與100%之間的〇2及〇%與約3〇0/〇 之間的Ar之第二濺鍍氣體濺鍍W〇3以達到在約1〇〇 nm與約 200 nm之間的厚度。在又一實施例中,該方法進一步包括 將鋰濺鍍至該中間層上,直至盲電荷大致或實質上得到滿 足。在一實施例中,該反電極層包括厚度在約15〇 nm與約 300 nm之間的NiWO。在另一實施例中,將鋰濺鍍至反電 極層上,直至該反電極層褪色。在另—實施例中,將基於 使該反電極層褪色所需之量過量約5%與約丨5%之間的額外 量之鋰濺鍍至該反電極層上。在另一實施例中,在該反電 極層之上沈積透明導電氧化物層。在—實施例中,該透明 155961.doc •40· 201222119 導電氧化物包括氧化銦錫,在另一實施例中,該透明導電 氧化物為氧化銦錫。在另一實施例中,將根據以上實施例 形成之堆疊在Ar下在約15〇。(:與約45CTC之間加熱歷時約10 分鐘與約30分鐘之間,且接著在〇2下加熱歷時約1分鐘與 約15分鐘之間’且接著在空氣中在約25〇。〇與約35〇cc之間 加熱歷時約20分鐘與約40分鐘之間。 在另一實施例中,(a)包括濺鍍式Μ〇χ之第一電致變色材 料’其中Μ為金屬或非金屬元素,且χ指示化學計量之氧 與Μ之比’且(b)包括濺鐘式N〇y之第二電致變色材料以作 為十間層,其中N為相同或不同之金屬或非金屬元素,且少 指不超化學計量量之氧與N之比。在一實施例中,M為 鶴,且N為鶴。在另一實施例中,μ為鶴,且n係選自由 銳、矽、鈕、鈦、锆及鈽組成之群組。 本發明之另一實施例為一種電致變色裝置,其包括:(a) 包括電致變色材料之電致變色層;(b)包括反電極材料之反 電極層,及(c)在該電致變色層與該反電極層之間的界面 區’其中該界面區包括電絕緣離子傳導材料及該電致變色 材料、該反電極材料及額外材料中之至少一者,其中該額 外材料包括相異之電致變色材料或反電極材料。 在一實施例中,該電絕緣離子傳導材料及該電致變色材 料、該反電極材料及該額外材料中之至少一者實質上均勻 地分佈於該界面區内。在另一實施例中,該電絕緣離子傳 導材料及該電致變色材料、該反電極材料及該額外材料中 之至少一者包括在垂直於該等層之方向上之組成梯度。在 155961.doc •41 · 201222119 另一實施例中’與兩個前述實施例中之任一者一致,該電 絕緣離子傳導材料包括鎢酸鋰,該電致變色材料包括氧化 鎢,且該反電極材料包括氧化鎳鎢。在前述實施例之一特 定實施中,不存在額外材料。在一實施例中,該電致變色 層之厚度在約300 nm與約500 nm之間,該界面區之厚度在 約10 nm與約15〇 nm之間,且該反電極層之厚度在約15〇 nm與約300 nm之間。在另一實施例中,該電致變色層之厚 度在約400 nm與約500 nm之間;該界面區之厚度在約2〇 nm與約100 nm之間,且該反電極層之厚度在約15〇 ^^爪與 約250 nm之間。在又一實施例中,該電致變色層之厚度在 約400 nm與約450 nm之間;該界面區之厚度在約3〇 nm與 約50 nm之間,且該反電極層之厚度在約2〇〇 nm與約25〇 nm之間0 另一實施例為一種製造電致變色裝置之方法,該方法包 括: 藉由用包含約40%與約80%之間的〇2及約2〇%與約6〇%之 間的Ar之濺鍍氣體濺鍍鎢標靶以產生w〇3至在約5〇〇 nm與 約600 nm之間的厚度來沈積電致變色層,其中沈積有該 WO3之基板在該電致變色層之形成期間被至少間歇性地加 熱至約150°C與約450°C之間; 將裡濺鐘至該電致變色層上,直至盲電荷得到滿足; 在a亥電致變色層上沈積反電極層,而並不首先在該電致 變色層與該反電極層之間提供離子傳導電絕緣層,其中該 反電極層包括NiWO ; 155961.doc •42· 201222119 將經濺鍍至該反電極層上,直至該反電極層實質上褪 色;及 在該電致變色層與該反電極層之間形成界面區,其中該 界面區為實質上離子傳導且實質上電絕緣的。在—實施例 中’形成該界面區包括該堆疊單獨或與基板、導電層及/ 或囊封層一起之MTCC。 本發明之電致變色裝置可包括諸如一或多個被動層之一 或多個額外層(未圖示例如)以改良特定光學性質(提供防 潮或抗刮擦性)以氣密式地密封該電致變色裝置及其類似 物。通常(但不必),罩蓋層沈積於該電致變色堆疊上。在 些貫例中,該罩蓋層為SiAl〇。在一些實施例中,該 罩蓋層係藉由濺鍍沈積。在一實施例中,罩蓋層之厚度在 約30 nm與約1〇〇 nm之間。 自上文之論述應瞭解,本發明之電致變色裝置可在單一 辟室設備(例如,具有(例如)鎢標靶、鎳標靶及鋰標靶以及 氧氣及氬氣濺鍍氣體之濺鍍工具)中製造。如所提及,歸 因於經形成以起到習知相異IC層之用途的界面區之性質, 用於濺鍍1C層之單獨標靶並非必需的。發明者特別感興趣 的是(例如)以高產量方式製造本發明之電致變色裝置,因 此,需要具有可在基板通過整合式沈積系統時順序地製造 本發明之電致變色裝置之設備。舉例而言,發明者對在 曲特別疋建築玻璃鱗片窗(上述)上製造電致變色裝置特 別感興趣。 因此本發明之另一態樣為一種用於製造電致變色裝置 155961.doc -43· 201222119 之設備,#包括:整合式沈積系統,其包括:⑴含有材料 源之第-沈積台’其經組態以沈積包括電致變色材料之電 致變色層;及(ii)第二沈積台,其緩 ”生組態以沈積包括反電 極材料之反電極層;及控制器’其含有用於以在該基板上 順序地沈積堆疊之方式傳遞該基板經過該第一沈積台及該 第二沈積台之程式指令’該堆疊具有失在該電致變色層也 該反電極層之間的中間層;$中該第—沈積台及該第二沈 積台中之任-者或兩者亦經組態以在該電致變色層或該反 電極層上方沈積該中間層,且其中該中間層包括該電致變 色材料或該反電極材料之宮童4Π i 例了叶之虽軋形式,且其中該第一沈積台 及該第二沈積台串聯互連且可操作以將基板自一個台傳遞 至下-個台而不將該基板曝露於外部環境。在一實施例 中,本發明之設備可操作以將該基板自一個台傳遞至下一 個台而不破壞真空,且可包括可操作以將來自含鐘材料源 之鋰沈積在該電致變色裝置之一或多個層i之一或多個鋰 化台η在一實施例中,本發明之設備可操作以在建築玻璃 基板上沈積該電致變色堆疊。 在一實施例中,該設備可操作以將該基板自一個台傳遞 至下一個台而不破壞真空。在另一實施例中,該整合式沈 積系統進一步包括可操作以在該電致變色層、該中間層及 該反電極層中之至少—者上沈積來自含㈣料源之經之一 或多個H化台。在又-實施例巾,該整合式沈積系統可操 作以在建築玻璃基板上沈積該堆疊。在另一實施例中,該 整合式沈積系統進一步包括可操作以在使該建築玻璃基板 155961.doc •44· 201222119 通過該整合式沈積系統時將該建築玻璃基板固持在垂直定 向上之基板固持器及輸送機構。在另一實施例中,該設備 進一步包括用於在外部環境與該整合式沈積系統之間傳遞 該基板之一或多個真空預抽室(load lock)。在另一實施例 中,該設備進一步包括至少一狭縫閥門,該至少一狹縫閥 門可操作以准許該一或多個鋰沈積台與該第一沈積台及該 第二沈積台中之至少一者隔離。在一實施例中,該整合式 沈積系統包括經組態以加熱該基板之一或多個加熱器》 圖5以透視圖描繪整合式沈積系統5〇〇之簡化表示且更詳 細地包括内部之剖視圖。在此實例中,系統500為模組, 其中入口真空預抽室502及出口真空預抽室504連接至沈積 模組5〇6。存在用於裝載(例如)建築玻璃基板525之入口皡 51〇(真空預抽室504具有對應出口埠)。基板525由沿著軌道 5 15行進之集裝架520支撐。在此實例中,集裝架520係經 由懸掛而由軌道5 1 5支撐,但集裝架520亦可支撐在靠近設 備500之底部定位之轨道或(例如)在設備5〇〇之頂部與底部 中間的軌道之頂上。集裝架52〇可在系統5〇〇中向前及/或 向後平移(如雙頭箭頭所指示)^舉例而言,在鋰沈積期 間’基板可在鋰標靶530前面向前及向後移動,從而產生 多-人通過以便達成所要鐘化。然而,此功能不限於鐘標 靶,例如,鎢標靶可通過基板多次,或該基板可在該鎢標 靶前面經由向前/向後運動路徑通過以沈積(例如)電致變色 層。集裝架520及基板525處於實質上垂直之定向上。實質 上垂直之定向並非限制性的,但其可幫助防止缺陷,此係 155961.doc -45- 201222119 因為可能(例如)自來自濺鍍之原子之聚結產生之顆粒物質 將傾向於受到重力且因此不沈積在基板525上。又,因為 建築玻璃基板傾向於為大的,所以基板之垂直定向在其橫 越該整合式沈積系統之該等台時實現較薄玻璃基板之塗 佈,此係因為對關於較厚熱玻璃發生之下垂之擔憂較少。 標靶530(在此情況下為圓柱形標靶)係經定向而實質上 平行於將發生沈積之基板表面且在該基板表面前面(為便 利起見,此處未描繪其他濺鍍手段)^基板525在沈積期間 可平移通過標靶530,及/或標靶53〇可在基板525前面移 動。標靶530之移動路徑不限於沿著基板525之路徑平移。 標靶530可沿著通過其長度之軸線旋轉、沿著基板之路徑 (向前及/或向後)平移、沿著垂直於基板之路徑之路徑平 移、在平行於基板525之平面中以圓形路徑移動等。標靶 530不必為圓柱形的,其可為平坦的或沈積具有所要性質 之所要層所需之任何形狀。又,在每一沈積台令可能存在 一個以上之標靶,‘及/或標靶可取決於所要製程而在台之 間移動。本發明之整合式沈積系統之各種台可為模組,但 其一旦連接即形成連續系統,其中建立且維持受控周圍環 境以便在系統内之各種台處處理基板。 如何使用整合式沈積系統500沈積電致變色材料之更詳 細態樣描述於前述之美國非臨時專利申請案第12/645,丨工^ 號及第12/645,159號中。 整合式沈積系統500亦具有建立且維持系統内之受控周 圍環境之各種真空泵、氣體入口、壓力感測器及其類似 I55961.doc •46· 201222119 ί解=件並未展示’而是可為-般熟習此項技術者所 ' …5GG(例如)係經由圖5中由LCD及鍵盤535所表示 之電腦系統或其他控制器控制。—般熟習此項技術者將瞭 解本發明之實施例可使用涉及儲存於一或多個電腦系统 或經由—或多個電腦系統傳送之資料之各種製程。本發明 之貫施例亦係關於用於執行此等操作之設備、此等電腦及 微控制$此等&備及製程可用以沈積本發明之方法及經 设相貫施該等方法之設備之電致變色材料。本發明之控 制設備可經特殊建構以詩所需目的,或該㈣設備可為 通用電腦’其藉由儲存於該電腦中之電腦程式及/或資料 結構而選擇性地啟動或重組態。本文中所呈現之該等程序 並不固有地與任何特定電腦或其他設備相關。詳言之,各 種通用機器可與根據本文中之教示撰寫之程式—起使用, 或其對建構更特定設備以執行及/或控制所需方法及程序 而言可能更便利。 自以上(特別是圖3A至圖化之)描述可見,利用本發明之 方法,吾人不僅可製造電致變色裝置,而且可預先製造分 層堆疊(例如,400、403及409),其在一些情況下可經由例 如本文中所描述之後續處理轉換成電致變色裝置。儘管由 於在EC層與CE層之間不具有離子傳導且電絕緣之區而並 非功能性電致變色裝置,但此等「電致變色裝置前驅體」 可具有特別價值。在裝置前驅體係以高純度在如本文中所 描述之整合式處理設備中製造之情況下尤其如此,其中材 料層全部在(例如)真空始終未被破壞之受控周圍環境下沈 155961.doc •47- 201222119 積。以此方式,高純度之低缺陷材料經堆疊且基本上(例 如)在離開整合式系統之前由最後TCO層及/或罩蓋層「密 封」。 與上述之本發明之電致變色裝置一樣,電致變色裝置前 驅體亦可包括諸如一或多個被動層之一或多個額外層(未 圖示)(例如)以改良特定光學性質(提供防潮或抗到性)以氣 密式地密封該裝置前驅體及其類似物。在一實施例中,罩 蓋層沈積於該前驅體堆疊之TC0層上。在一些實施例中, 该罩蓋層為hAlO。在—些實施例中,該罩蓋層係藉由賤 鍍沈積。在一實施例中,罩蓋層之厚度在約3〇 nm與約ι〇〇 nm之間。對處於適當位置之頂蓋層之後續處理形成π層而 無來自環境之污染,亦即,具有罩蓋層之額外保護。 至功能性電致變色裝置之轉換必要時可在該整合式系統 之外發生,此係因為内部堆疊結構受保護而不受外部環境 影響,且稍微較低嚴格純度之條件係用以將前驅體堆疊轉 換成功能性裝置之最末調節步驟所必需的。此等堆疊之電 致變色裝置前驅體可具有優點,例如,歸因於僅在需要時 轉換至電致變色裝置之較長壽命、由具有(例如)可儲存且 在轉換參數取決於最後產品之需要及必須滿足之品質標準 而改良或饋送至不同轉換腔室及/或消費點以用於轉換時 使用之單-前驅體堆疊導致之靈活性。又,此等前驅體堆 疊可用於測試目的’例如,品質控制或研究努力。 因此,本發明之—實施例為—種電致變色裝置前驅體, 其包括’⑷基板’(b)該基板上之第一透明導電氧化物 15596I.doc •48· 201222119 層;(c)該第一透明導電氧化物層上之堆疊’該堆疊包括: (:)包括電致變色材料之電致變色層,及⑼包括反電極材 料之反電極層,其中該堆疊不包括介於該電致變色層與玆 反電極層之間的離子傳導且電絕緣之區;及⑷在該:疊: 上之第二透明導電氧化物層。在-實施例中,該電致變色 層包括氧化鶴,且該反電極層包含氧化鎳鎢。在_實施例 中,該堆疊及該電致變色層中之至少—者含有鐘。在另一 實施例中,該電致變色層為至少在與該反電極層之界面處 具有超化學計量之含氧量之氧化鎢。在另一實施例中,該 堆疊包括在該反電極層與該電致變色層之間的lc前驅體 層,S亥1C前驅體層包括具有比該電致變色層之含氧量高的 含氧量之氧化鎢。在一實施例中,在於Ec層與CE層之間 不存在1C前驅體層之情況下,該電致變色層之厚度在約 500 nm與約600 nm之間,且該反電極層之厚度在約15〇 nm 與約300 nm之間。在另一實施例中,在於EC層與CE層之 間存在1C前驅體層之情況下’該電致變色層之厚度在約 350 nm與約400 nm之間,該1C前驅體層之厚度在約2〇 nm 與約100 nm之間’且該反電極層之厚度在約15〇 11111與約 300 nm之間。在一實施例中,本文中所描述之前驅體裝置 曝露於加熱以將該等裝置轉換成功能性電致變色裝置。在 一實施例中,加熱為MTCC之部分。 另一實施例為一種電致變色裝置,其包括:(a)包括電致 變色材料之電致變色層;及(b)包括反電極材料之反電極 層,其中該裝置不含有在該電致變色層與該反電極之間的 155961.doc -49· 201222119 電絕緣離子傳導材料之組成上均質之層。在一實施例中, 該電致變色材料為氧化鎢,該反電極材料為氧化鎳鎢,且 介於該電致變色層與該反電極層之間的為包括鶴酸經與氧 化鎢及氧化鎳鎢中之至少一者之混合物之界面區。在另一 實施例中’該電致變色層之厚度在約3〇〇 nm與約5〇〇 nm之 間;該界面區之厚度在約1〇 nm與約15〇 nm之間,且該反 電極層之厚度在約15〇 nm與約300 nm之間。 實例 圖6為用作用於製造本發明之電致變色裝置之方案之程 序流程之曲線圖。y軸單位為光學密度,且λ軸單位為時間/ 程序流程。在此實例中,製造類似於關於圖4 Α所描述之電 致變色裝置之電致變色裝置,其中基板為以經氟化之氧化 錫作為第一 TCO之玻璃’ Ec層為基質中具有過量氧之 W〇3(例如,使用鎢標靶濺鍍,其中濺鍍氣體為約60%之〇2 及約40%之Ar),CE層形成於EC層之上且由Niw〇製成,且 第一 TCO為氧化銦錫(IT〇)。將鋰用作用於電致變色過渡 之離子源。 光學密度用以在電致變色裝置之製造期間判定終點。自 曲線圖之原點開始,隨著Ec層(w〇3)沈積在基板(玻璃+ TCO)上,量測光學密度。玻璃基板之光學密度具有為約 〇.〇7(吸光度單位)之基線值光學密度。隨著Ec層建置,光 學密度自該點增加,因為氧化鎢(雖然實質上透明)吸收一 些可見光。針對約550 nm厚之氧化鎢層之所要厚度,如上 所述,光學密度上升至約〇 2 ^在沈積氧化鎢Ec層之後, 15596I.doc •50· 201222119 在EC層上濺鍍鋰,如「Lij指示之第一時間週期所指示。 在此週期期間,光學密度沿著曲線進一步增加至〇4,其 指不氧化鎢之盲電荷已得到滿足,此係因為氧化鎢隨著鋰 添加而著色。「NiWO」指示之時間週期指示Niw〇層之沈 積,光學密度在此期間增加,此係因為NiW〇經著色。由 於約230 nm厚之NiWO層之添加,光學密度在Niw〇沈積期 間自約0.4進一步增加至約〇.9。請注意,隨著Niw〇沈積, 一些鋰可自EC層擴散至匚丑層。此用來在Niw〇沈積期間或 至少在沈積之初始階段期間將光學密度維持在相對較低 值。 「Li」指不之第二時間週期指示鋰至Niw〇 Ec層之添 加。光學密度在此階段期間自約〇.9減小至約〇 4,此係因 為NiWO之鋰化使NiWO褪色。進行鋰化,直至Niw〇褪色 (包括約0_4光學密度之局部最小值)。光學密度在約〇4開 始回升’此係因為W〇3層仍被鐘化且影響光學密度。接下 來,如時間週期「額外U」所指示’將額外鋰濺鍍至 NiWO層上,在此實例中,與添加至Niw〇之鋰相比約1〇% 之額外鋰使NiWO層褪色。在此階段期間,光學密度稍微 增加。接下來’添加氧化銦錫TCO,如曲線圖中「IT0」 所指示。再次,光學密度在氧化銦錫層之形成期間繼續稍 微上升至約0.6。接下來,如「MSTCC」指示之時間週期 所指示,在Ar下將裝置加熱至約25〇〇c歷時約15分鐘,且 接著在〇2下加熱約5分鐘。接著,在空氣中在約;^^^下將 裝置退火歷時約30分鐘。在此時間期間,光學密度減小至 155961.doc -51 _ 201222119 約0.4 »因此,光學密度為用於製造本發明之裝置(例如, 用於基於所沈積之材料及形態判定層厚度,且尤其用於將 鐘滴定至各種層上以用於滿足盲電荷及/或達到褪色狀態) 之有用工具。 與關於圖6所描述之方案一致,圖7展示使用本發明之方 法製造的電致變色裝置700之橫截面TEM。裝置700具有玻 璃基板702’電致變色堆疊714形成於該玻璃基板上。基板 7〇2具有充當第一 TCO之ITO層704。氧化鎢EC層706沈積 於TCO 704上。層706以約550 nm之厚度形成(亦即,利用 氧氣及氬氣經由錢鑛鶴形成之W03),如上文關於圖6所描 述。將鐘添加至EC層。接著,添加約230 nm厚之NiWO CE層710 ’繼而添加鋰以褪色且接著添加約1〇%過量之 經。最後,沈積氧化銦錫層712,且使堆疊經受多步驟熱 化學調節’如上文關於圖4A所描述。在MSTCC之後,進 行此TEJV^如所見,形成離子傳導電絕緣之新區7〇8。 圖7亦展示各種層之五個選定區域電子繞射(SAED)圖 案。首先,704a指示ITO層為高度晶形的。圖案7〇6a展示 EC層為多晶的。圖案708a展示1C層為實質上非晶形的。圖 案710a展示CE層為多晶的。最後,圖案712a展示氧化銦錫 TCO層為高度晶形的。 圖8為藉由掃描透射電子顯微鏡(STEM)分析的本發明之 裝置800之橫截面。在此實例中,與關於圖4B描述之方案 一致,裝置800係使用本發明之方法製造。裝置8〇〇為形成 於玻璃基板(未標記)上之電致變色堆疊。在該玻璃基板上 155961.doc •52· 201222119 的是經氟化之氧化錫層804,其充當第一Tc〇(對透明電子 導體而。„玄層有時被稱為r TEC」層)。氧化鎢EC層祕 沈積於TCO 804上。在此實例t,層_以約彻nm之厚度 开^/成(亦即,利用氧氣及氬氣經由錢鍍鶴形成之界〇3,如 上文關於圖6所描述),接著沈積富氧前驅體層8〇5至約15〇 nm之厚度《將鋰添加至層8〇5。接著’添加約23〇 nm厚之 NiWO CE層81G,繼而添加鐘以褪色且接著添加約1〇%過 量之鋰。最後,沈積氧化銦錫層812且使堆疊經受多步驟 熱化學調郎,如上文關於圖4B所描述。在MSTCC之後, 進行此S TEM »如所見’形成離子傳導電絕緣之新區8 〇 8。 此實例與關於圖4B所描述之實施例之間的差異在於,不同 於圖4B中之類似層405,富氧層805僅部分地轉換成界面區 808。在此情況下,150 nm之富氧前驅體層405中僅約40 nm轉換成充當離子傳導層之區。 圖8B及圖8C展示本發明之裝置8〇〇(圖8C)與如STEM所分 析的在多步驟熱化學調節之前的裝置前驅體(圖8B)之「前 後」比較。在此實例中,僅描繪層804-810(EC至CE)。該 等層與圖8A中相同地編號,但有些例外。圖8B中之點線 用以大致地區分EC層806與富氧層805之界面(此在圖8C中 更清楚)。再次參看圖8B,看起來至少存在集中在富氧層 805與CE層810之界面處之鋰(大致10-15 nm厚之區),如 808a所指示。在MTCC之後(圖8C),很明顯,界面區808已 形成。 雖然已稍微詳細地描述前述發明以促進理解,但所描述 155961.doc •53· 201222119 之實施例應視為說明性而非限制 者將顯而易見,在附加申請專利圍:::熟習此項技術 定變化及修改。 4圍之範鳴内’可實踐特 【圖式簡單說明】 圖1A為描繪電致變色裝 面0 置隹疊之習知形成之示意性橫截 圖1B為展示習知電致變色堆叠 之組成之曲線圖。 中之EC層、1C層及CE層 圖2A至圖2C為展示用於本發明 性組份組合物之曲線圖。 之電致變色裝置之代表 圖3 A及圖3 B為根據本發明之實施例之程序流程。 圖4A至圖4C為描繪根據本發明之特定實施例之電致變 色裝置之形成的示意性橫截面。 圖5以透視圖描繪本發明之整合式沈積系統。 圖6為展不程序參數與終點示值讀數在根據本發明之實 施例之電致變色堆疊之形成期間如何相關的曲線圖。 圖7及圖8 A至圖8 C為使用根據本發明之實施例之方法製 造之電致變色裝置的實際橫截面。【主要元件符號說明】 100 電致變色裝置 102 基板 104 導電層(CL) 106 電致變色(EC)層 108 離子傳導(1C)層 155961.doc -54 - 201222119 110 反電極(CE)層 112 導電層(CL) 114 電致變色堆疊 116 電壓源 300 程序流程 320 程序流程 400 分層結構 401 功能性電致變色裝置 402 基板 403 分層結構 404 第一 TCO層 405 第二W03層 406 EC層 406a EC層 407 分層堆疊 408 1C層/界面區 408a 離子傳導電絕緣區/界面區 408b 分級界面區 409 分層結構 410 CE層 411 分層堆疊/功能性電致變色裝置 412 第二TCO層 414a 堆疊 414b 堆疊 155961.doc -55- 201222119 414c 堆疊 500 整合式沈積系統 502 入口真空預抽室 504 出口真空預抽室 506 沈積模組 510 入口埠 515 軌道 520 集裝架 525 基板 530 鋰標靶 535 LCD及鍵盤 700 電致變色裝置 702 玻璃基板 704 氧化銦錫(ITO)層 704a 圖 '案 706 氧化鎢EC層 706a 圖案 708 新區 708a 圖案 710 CE層 710a 圖案 712 氧化銦錫層 712a 圖案 714 電致變色堆疊 -56- 155961.doc 201222119 800 裝置 804 經氟化之氧化錫層 805 富氧前驅物層 806 氧化鎢EC層 808 新區/界面區 808a 鋰 810 CE層 812 氧化銦錫層 155961.doc -57-155961.doc •38· 201222119 Includes a transition to the tungsten oxide zone in the (superstoichiometric) yttrium oxide zone. Part or all of the oxidized sharp region is converted into an interface region. In the final structure, the oxidized crane region is substantially polycrystalline and the microstructure transitions to substantially amorphous at the interfacial region. Referring again to FIG. 4C', as described above with respect to FIG. 3B and FIG. 4A, the stacking is accomplished by lithochemical EC layer 406a to substantially or substantially satisfy the blind charge, deposit CE layer 410, lithiated CE layer to a faded state. Additional lithium is deposited and a second TCO layer 412 is deposited to complete the layered stack 409. A similar multi-step thermochemical conditioning is performed on the layered stack 409 to provide a layered stack 411 comprising at least a portion of the ion conducting electrically insulating region 4 8b and the original layered EC layer 406a (which is in the functional electrochromic device 41 i In the present example, in the example, the uppermost oxygen-rich portion of the graded layer of WO3 mainly forms the graded interface region 408b. It is not desirable to be bound by theory, but there is a possibility that the formation of the interface region is self-limiting and depends on the relative amounts of oxygen, lithium, electrochromic material and/or counter electrode material in the stack. In various embodiments described herein, the electrochromic stack is described as not being heated during a particular processing stage. In 1 =: after the heating step, active or passive (for example, using a heat-dissipating γ cold section stack. The apparatus of the present invention includes active and passive cooling components, such as 'active cooling may include circulation via fluid, exposure to cold (eg The fuse is cooled by the expansion of the gas, the cooling unit, and the like: The passive cooling assembly may include a heat sink, such as a metal block and the like, or the substrate may only be removed from the heat exposure. .doc •39· 201222119 Another aspect of the invention is a method of making an electrochromic device, the method comprising: (a) forming an electrochromic layer comprising an electrochromic material or a counter electrode layer comprising a counter electrode material (13) forming an intermediate layer over the electrochromic layer or the counter electrode layer, wherein the intermediate layer comprises an oxygen-rich form of at least one of the electrochromic material, the counter electrode material, and additional material, wherein Additional materials include dissimilar electrochromic materials or counter electrode materials, wherein the intermediate layer is not substantially electrically insulating; (c) forming the electrochromic layer and the other of the counter electrode layers One, and (d) allows at least a portion of the intermediate layer to become substantially electrically insulated. In one embodiment, the electrochromic material is w 〇 3. In another embodiment, (a) includes the use of tungsten The target and the first splashing gas between the 〇2 and about 20% and about 60% between about 4% and about 80% are reduced by the WO3 to reach about 350 nm and about 450 nm. The thickness between, and during the formation of the electrochromic layer, is at least intermittently heated to between about 15 〇β (: and about 450 ° C. In another embodiment - (b) included without heating In the case of using a tungsten target and a second sputtering gas comprising W between about 70% and 100% between 〇2 and 〇% and about 3〇0/〇, the sputtering is performed to achieve about 1 A thickness between 〇〇nm and about 200 nm. In yet another embodiment, the method further includes sputtering lithium onto the intermediate layer until the blind charge is substantially or substantially satisfied. In an embodiment, the The counter electrode layer comprises NiWO having a thickness between about 15 〇 nm and about 300 nm. In another embodiment, lithium is sputtered onto the counter electrode layer until the counter electrode layer fades. In an example, an excess amount of lithium between about 5% and about 5% excess of the amount required to fade the counter electrode layer is sputtered onto the counter electrode layer. In another embodiment, in the opposite A transparent conductive oxide layer is deposited over the electrode layer. In an embodiment, the transparent 155961.doc • 40· 201222119 conductive oxide comprises indium tin oxide, and in another embodiment, the transparent conductive oxide is indium tin oxide. In another embodiment, the stack formed according to the above embodiment is stacked at Ar at about 15 Torr. (: heating between about 45 CTC and about 45 minutes between about 10 minutes and about 30 minutes, and then heating at 〇2 It lasts between about 1 minute and about 15 minutes' and then in the air at about 25 inches. Heating between about 〇 and about 35 cc takes about 20 minutes and about 40 minutes. In another embodiment, (a) includes a first electrochromic material of the sputtered crucible 'where germanium is a metallic or non-metallic element, and χ indicates a stoichiometric ratio of oxygen to hydrazine' and (b) A second electrochromic material comprising a splash-type N〇y is used as ten layers, wherein N is the same or a different metal or non-metal element, and less refers to a ratio of oxygen to N that is not superstoichiometric. In one embodiment, M is a crane and N is a crane. In another embodiment, μ is a crane and n is selected from the group consisting of sharp, enamel, button, titanium, zirconium, and hafnium. Another embodiment of the invention is an electrochromic device comprising: (a) an electrochromic layer comprising an electrochromic material; (b) a counter electrode layer comprising a counter electrode material, and (c) at the electricity An interface region between the discoloration layer and the counter electrode layer, wherein the interface region comprises at least one of an electrically insulating ion conducting material and the electrochromic material, the counter electrode material, and additional materials, wherein the additional material comprises a phase Different electrochromic materials or counter electrode materials. In one embodiment, at least one of the electrically insulating ion conducting material and the electrochromic material, the counter electrode material, and the additional material are substantially uniformly distributed within the interface region. In another embodiment, at least one of the electrically insulating ion conducting material and the electrochromic material, the counter electrode material, and the additional material comprise a compositional gradient in a direction perpendicular to the layers. In another embodiment, in accordance with any of the two preceding embodiments, the electrically insulating ion conducting material comprises lithium tungstate, the electrochromic material comprises tungsten oxide, and the counter The electrode material includes nickel tungsten oxide. In a particular implementation of one of the foregoing embodiments, there is no additional material. In one embodiment, the electrochromic layer has a thickness between about 300 nm and about 500 nm, the interface region has a thickness between about 10 nm and about 15 nm, and the thickness of the counter electrode layer is about Between 15 〇 nm and about 300 nm. In another embodiment, the electrochromic layer has a thickness between about 400 nm and about 500 nm; the interface region has a thickness between about 2 nm and about 100 nm, and the thickness of the counter electrode layer is About 15 〇 ^ ^ claws and about 250 nm. In still another embodiment, the electrochromic layer has a thickness between about 400 nm and about 450 nm; the interface region has a thickness between about 3 〇 nm and about 50 nm, and the thickness of the counter electrode layer is Another embodiment is between about 2 〇〇 nm and about 25 〇 nm. Another embodiment is a method of fabricating an electrochromic device, the method comprising: comprising between about 40% and about 80% 〇2 and about 2溅% and about 6〇% of the sputtering gas of Ar is sputtered with a tungsten target to produce w〇3 to a thickness between about 5 〇〇 nm and about 600 nm to deposit an electrochromic layer, wherein the deposited The substrate of the WO3 is at least intermittently heated to between about 150 ° C and about 450 ° C during formation of the electrochromic layer; the clock is splashed onto the electrochromic layer until the blind charge is satisfied; Depositing a counter electrode layer on the a-electrochromic layer without first providing an ion-conducting electrically insulating layer between the electrochromic layer and the counter-electrode layer, wherein the counter-electrode layer comprises NiWO; 155961.doc • 42 · 201222119 will be sputtered onto the counter electrode layer until the counter electrode layer is substantially discolored; and in the electrochromic layer and the counter electrode It is formed between the interface region, wherein the interfacial region is substantially ion-conducting and electrically substantially insulating. Forming the interface region in the embodiment includes the stack of MTCC alone or with the substrate, conductive layer and/or encapsulation layer. The electrochromic device of the present invention may include one or more additional layers (such as, for example, one or more passive layers) to improve specific optical properties (providing moisture or scratch resistance) to hermetically seal the Electrochromic devices and the like. Typically, but not necessarily, a cap layer is deposited on the electrochromic stack. In some instances, the cap layer is SiAl. In some embodiments, the cap layer is deposited by sputtering. In one embodiment, the thickness of the cap layer is between about 30 nm and about 1 〇〇 nm. It should be understood from the above discussion that the electrochromic device of the present invention can be used in a single chamber device (for example, with, for example, a tungsten target, a nickel target, a lithium target, and a sputtering of oxygen and argon sputtering gases). Manufactured in the tool). As mentioned, due to the nature of the interface region formed to serve the purpose of the conventional IC layer, a separate target for sputtering the 1C layer is not necessary. Of particular interest to the inventors is the fabrication of the electrochromic devices of the present invention, for example, in a high throughput manner, and therefore there is a need for an apparatus that can sequentially fabricate the electrochromic devices of the present invention as it passes through an integrated deposition system. For example, the inventors are particularly interested in the manufacture of electrochromic devices on curved glass window (described above). Therefore, another aspect of the present invention is an apparatus for manufacturing an electrochromic device 155961.doc-43 201222119, including: an integrated deposition system comprising: (1) a first-deposition table containing a source of material Configuring to deposit an electrochromic layer comprising an electrochromic material; and (ii) a second deposition station configured to deposit a counter electrode layer comprising a counter electrode material; and a controller 'containing And sequentially transferring the substrate on the substrate to transfer the substrate through the first deposition stage and the second deposition stage; the stack has an intermediate layer between the electrochromic layer and the counter electrode layer; Any one or both of the first deposition stage and the second deposition stage are configured to deposit the intermediate layer over the electrochromic layer or the counter electrode layer, and wherein the intermediate layer includes the electricity The color change material or the counter electrode material of the palace is exemplified by a rolled form of the leaf, and wherein the first deposition stage and the second deposition stage are interconnected in series and operable to transfer the substrate from one stage to the bottom - Station without exposing the substrate Environment. In one embodiment, the apparatus of the present invention is operable to transfer the substrate from one station to the next without disrupting the vacuum, and may include being operable to deposit lithium from the source of the clocked material in the electrolysis One or more layers of one or more layers i of a color changing device. In one embodiment, the apparatus of the present invention is operable to deposit the electrochromic stack on a building glass substrate. In an embodiment, the The apparatus is operable to transfer the substrate from one station to the next without breaking the vacuum. In another embodiment, the integrated deposition system further includes an operative layer in the electrochromic layer, the intermediate layer, and the counter At least one of the electrode layers is deposited from one or more H-stages containing the source of (iv). In yet another embodiment, the integrated deposition system is operable to deposit the stack on a building glass substrate. In another embodiment, the integrated deposition system further includes an operable to hold the architectural glass substrate in a vertical orientation when the architectural glass substrate 155961.doc • 44 201222119 is passed through the integrated deposition system The substrate holder and transport mechanism. In another embodiment, the apparatus further includes one or more vacuum preload chambers for transferring the substrate between the external environment and the integrated deposition system. In another embodiment, the apparatus further includes at least one slit valve operable to permit the one or more lithium deposition stations and at least one of the first deposition station and the second deposition station Isolation. In one embodiment, the integrated deposition system includes one or more heaters configured to heat the substrate. Figure 5 depicts a simplified representation of the integrated deposition system 5' in a perspective view and includes in more detail Internal cross-sectional view. In this example, system 500 is a module in which inlet vacuum pre-extraction chamber 502 and outlet vacuum pre-extraction chamber 504 are coupled to deposition module 5〇6. There is an inlet port 51 for loading, for example, a building glass substrate 525 (the vacuum pre-extraction chamber 504 has a corresponding outlet port). The substrate 525 is supported by a pallet 520 that travels along the track 5 15 . In this example, the pallet 520 is supported by the track 515 via suspension, but the pallet 520 can also support a track positioned near the bottom of the device 500 or, for example, at the top and bottom of the device 5 On top of the middle track. The pallet 52 can be translated forward and/or backward in the system 5 (as indicated by the double-headed arrow). For example, during lithium deposition, the substrate can move forward and backward in front of the lithium target 530. , thereby producing a multi-person pass in order to achieve the desired bell. However, this function is not limited to a clock target, for example, the tungsten target can pass through the substrate multiple times, or the substrate can pass in front of the tungsten target via a forward/backward motion path to deposit, for example, an electrochromic layer. The carrier 520 and the substrate 525 are in a substantially vertical orientation. The substantially vertical orientation is not limiting, but it can help prevent defects, which is 155961.doc -45-201222119 because particulate matter that may, for example, arise from agglomeration of atoms from sputtering will tend to be subject to gravity and Therefore, it is not deposited on the substrate 525. Also, because the architectural glass substrate tends to be large, the vertical orientation of the substrate enables coating of the thinner glass substrate as it traverses the stations of the integrated deposition system, as is the case with respect to thicker hot glass. There are fewer concerns about drooping. Target 530 (in this case a cylindrical target) is oriented substantially parallel to the surface of the substrate where deposition will occur and in front of the surface of the substrate (for convenience, other sputtering means are not depicted herein)^ The substrate 525 can be translated through the target 530 during deposition, and/or the target 53 can be moved in front of the substrate 525. The path of movement of the target 530 is not limited to translation along the path of the substrate 525. Target 530 can be translated along a path through its length, along a path of the substrate (forward and/or backward), along a path perpendicular to the path of the substrate, in a plane parallel to substrate 525. Path moves, etc. The target 530 need not be cylindrical, it can be flat or deposit any shape desired for the desired layer of the desired properties. Also, there may be more than one target at each deposition station, and 'and/or the target may move between stations depending on the desired process. The various stages of the integrated deposition system of the present invention can be modular, but once connected, form a continuous system in which a controlled ambient environment is established and maintained to process the substrate at various stages within the system. A more detailed description of how to deposit an electrochromic material using the integrated deposition system 500 is described in the aforementioned U.S. Non-Provisional Patent Application Serial No. 12/645, filed on Apr. No. 12/645,159. The integrated deposition system 500 also has various vacuum pumps, gas inlets, pressure sensors, and the like that establish and maintain a controlled surrounding environment within the system. I55961.doc • 46· 201222119 ί solution = piece not shown 'but may be The 5GG (for example) is generally controlled by a computer system or other controller represented by LCD and keyboard 535 in FIG. Those skilled in the art will appreciate that embodiments of the present invention may utilize various processes involving the storage of data stored on one or more computer systems or via one or more computer systems. The embodiments of the present invention are also directed to apparatus for performing such operations, such computers and micro-controls, such & preparations and processes for depositing the methods of the present invention and apparatus for performing such methods Electrochromic material. The control device of the present invention may be specially constructed for the purpose required by the poem, or the (4) device may be a general purpose computer' selectively activated or reconfigured by a computer program and/or data structure stored in the computer. The programs presented herein are not inherently related to any particular computer or other device. In particular, various general purpose machines may be used with programs written in accordance with the teachings herein, or may be more convenient for constructing more specific devices to perform and/or control desired methods and procedures. As can be seen from the above description (in particular, FIG. 3A to FIG. 3), with the method of the present invention, not only can an electrochromic device be fabricated, but also a layered stack (eg, 400, 403, and 409) can be pre-manufactured, in some The case can be converted to an electrochromic device via subsequent processing such as described herein. Although "non-functional electrochromic devices" are not provided between the EC layer and the CE layer without ion conduction and electrical insulation, such "electrochromic device precursors" may have particular value. This is especially the case when the device precursor system is manufactured in high purity in an integrated processing apparatus as described herein, wherein the material layers are all sunk in a controlled surrounding environment where, for example, the vacuum is never destroyed 155961.doc • 47- 201222119 Product. In this manner, high purity, low defect materials are stacked and substantially "sealed" by the last TCO layer and/or cap layer, for example, prior to exiting the integrated system. As with the electrochromic devices of the present invention described above, the electrochromic device precursors may also include one or more additional layers (not shown) such as one or more passive layers (for example) to improve specific optical properties (provided) Moisture-proof or resistant) seals the device precursor and the like in a gas-tight manner. In one embodiment, a cap layer is deposited on the TC0 layer of the precursor stack. In some embodiments, the cap layer is hAlO. In some embodiments, the cap layer is deposited by ruthenium plating. In one embodiment, the thickness of the cap layer is between about 3 〇 nm and about ι 〇〇 nm. Subsequent processing of the cap layer in place forms a π layer without environmental contamination, i.e., with additional protection of the cap layer. Conversion to a functional electrochromic device can occur outside of the integrated system if necessary because the internal stack structure is protected from the external environment and a slightly lower stringency condition is used to drive the precursor The stack is converted to the necessary adjustment steps for the functional device. Such stacked electrochromic device precursors may have advantages, for example, due to the longer lifetime of switching to an electrochromic device only when needed, by having, for example, storable and depending on the final product. Flexibility due to the single-precursor stack used for conversion or improvement to different conversion chambers and/or consumption points for quality standards that are required and must be met. Again, such precursor stacks can be used for testing purposes' such as quality control or research efforts. Accordingly, an embodiment of the present invention is an electrochromic device precursor comprising '(4) substrate' (b) a first transparent conductive oxide 15596I.doc • 48· 201222119 layer on the substrate; (c) a stack on the first transparent conductive oxide layer 'The stack includes: (:) an electrochromic layer comprising an electrochromic material, and (9) a counter electrode layer comprising a counter electrode material, wherein the stack does not include the electro-electrode a region of ion-conducting and electrically insulating between the color-changing layer and the counter electrode layer; and (4) a second transparent conductive oxide layer on the stack:. In an embodiment, the electrochromic layer comprises an oxidized crane and the counter electrode layer comprises nickel tungsten oxide. In an embodiment, at least one of the stack and the electrochromic layer contains a clock. In another embodiment, the electrochromic layer is a tungsten oxide having a superstoichiometric amount of oxygen at least at the interface with the counter electrode layer. In another embodiment, the stack includes an lc precursor layer between the counter electrode layer and the electrochromic layer, and the S1 1C precursor layer includes an oxygen content having a higher oxygen content than the electrochromic layer. Tungsten oxide. In one embodiment, in the case where there is no 1C precursor layer between the Ec layer and the CE layer, the thickness of the electrochromic layer is between about 500 nm and about 600 nm, and the thickness of the counter electrode layer is about Between 15 〇 nm and about 300 nm. In another embodiment, in the case where a 1C precursor layer exists between the EC layer and the CE layer, the thickness of the electrochromic layer is between about 350 nm and about 400 nm, and the thickness of the 1C precursor layer is about 2 Between 〇nm and about 100 nm' and the thickness of the counter electrode layer is between about 15 〇 11111 and about 300 nm. In one embodiment, the precursor devices described herein are exposed to heat to convert the devices into functional electrochromic devices. In one embodiment, the heating is part of the MTCC. Another embodiment is an electrochromic device comprising: (a) an electrochromic layer comprising an electrochromic material; and (b) a counter electrode layer comprising a counter electrode material, wherein the device is not contained in the electro-optical layer A compositionally homogeneous layer of 155961.doc -49· 201222119 electrically insulating ion conducting material between the color changing layer and the counter electrode. In one embodiment, the electrochromic material is tungsten oxide, and the counter electrode material is nickel oxide tungsten, and between the electrochromic layer and the counter electrode layer, including erbium acid and tungsten oxide, and oxidation An interface region of a mixture of at least one of nickel tungsten. In another embodiment, the thickness of the electrochromic layer is between about 3 〇〇 nm and about 5 〇〇 nm; the thickness of the interfacial region is between about 1 〇 nm and about 15 〇 nm, and the inverse The thickness of the electrode layer is between about 15 〇 nm and about 300 nm. EXAMPLES Figure 6 is a graph showing the flow of a procedure for use in the manufacture of the electrochromic device of the present invention. The y-axis unit is optical density, and the λ-axis unit is time/program flow. In this example, an electrochromic device similar to the electrochromic device described with respect to FIG. 4A is fabricated, wherein the substrate has excess oxygen in the matrix of the glass 'Ec layer with fluorinated tin oxide as the first TCO. W〇3 (for example, using tungsten target sputtering, in which the sputtering gas is about 60% 〇 2 and about 40% Ar), the CE layer is formed on the EC layer and made of Niw ,, and One TCO is indium tin oxide (IT〇). Lithium is used as an ion source for electrochromic transition. The optical density is used to determine the endpoint during manufacture of the electrochromic device. From the origin of the graph, the optical density was measured as the Ec layer (w〇3) was deposited on the substrate (glass + TCO). The optical density of the glass substrate has a baseline optical density of about 〇.〇7 (absorbance unit). As the Ec layer is built, the optical density increases from this point because tungsten oxide (although substantially transparent) absorbs some visible light. For the desired thickness of the 550 nm thick tungsten oxide layer, as described above, the optical density increases to about ^2 ^ after depositing the tungsten oxide Ec layer, 15596I.doc •50· 201222119 is sputtered on the EC layer, such as " Lij indicates the first time period indicated. During this period, the optical density is further increased along the curve to 〇4, which means that the blind charge of non-oxidized tungsten has been satisfied because the tungsten oxide is colored with lithium addition. The time period indicated by "NiWO" indicates the deposition of the Niw layer, and the optical density increases during this period because the NiW is colored. Due to the addition of a NiWO layer of about 230 nm thick, the optical density further increased from about 0.4 to about 〇9 during the Niw〇 deposition period. Note that as Niw〇 deposits, some of the lithium can diffuse from the EC layer to the ugly layer. This is used to maintain the optical density at a relatively low value during Niw(R) deposition or at least during the initial stage of deposition. "Li" means that the second time period indicates that the lithium to Niw〇 Ec layer is added. The optical density decreased from about 9.9 to about 〇4 during this stage because NiWO was discolored by lithiation of NiWO. Lithiation is performed until Niw fading (including a local minimum of about 0-4 optical density). The optical density starts to rise at about 〇4. This is because the W〇3 layer is still clocked and affects the optical density. Next, additional lithium is sputtered onto the NiWO layer as indicated by the time period "Extra U". In this example, about 1% of the additional lithium added to the Niw(R) lithium discolors the NiWO layer. During this phase, the optical density increases slightly. Next, add indium tin oxide TCO as indicated by "IT0" in the graph. Again, the optical density continues to rise slightly to about 0.6 during the formation of the indium tin oxide layer. Next, the apparatus was heated to about 25 〇〇c for about 15 minutes under Ar as indicated by the time period indicated by "MSTCC", and then heated at 〇 2 for about 5 minutes. Next, the device was annealed in air for about 30 minutes at about; During this time, the optical density is reduced to 155961.doc -51 _ 201222119 about 0.4 » Therefore, the optical density is used to fabricate the device of the invention (for example, for determining the layer thickness based on the deposited material and morphology, and in particular A useful tool for titrating a clock onto various layers for satisfying blind charge and/or reaching a faded state. Consistent with the scheme described with respect to Figure 6, Figure 7 shows a cross-sectional TEM of an electrochromic device 700 fabricated using the method of the present invention. Apparatus 700 has a glass substrate 702' an electrochromic stack 714 formed on the glass substrate. The substrate 7〇2 has an ITO layer 704 serving as a first TCO. A tungsten oxide EC layer 706 is deposited on the TCO 704. Layer 706 is formed at a thickness of about 550 nm (i.e., W03 formed by a gas mine with oxygen and argon) as described above with respect to Figure 6. Add the clock to the EC layer. Next, a NiWO CE layer 710' of about 230 nm thick was added followed by lithium to fade and then an excess of about 1% excess was added. Finally, an indium tin oxide layer 712 is deposited and the stack is subjected to multi-step thermochemical conditioning' as described above with respect to Figure 4A. After the MSTCC, the TEJV^ is as seen, forming a new region 7-8 of ion-conducting electrical insulation. Figure 7 also shows five selected area electronic diffraction (SAED) patterns for various layers. First, 704a indicates that the ITO layer is highly crystalline. Pattern 7〇6a shows that the EC layer is polycrystalline. Pattern 708a shows that the 1C layer is substantially amorphous. Pattern 710a shows that the CE layer is polycrystalline. Finally, pattern 712a exhibits an indium tin oxide TCO layer that is highly crystalline. Figure 8 is a cross section of an apparatus 800 of the present invention as analyzed by scanning transmission electron microscopy (STEM). In this example, in accordance with the approach described with respect to Figure 4B, device 800 is fabricated using the method of the present invention. Device 8 is an electrochromic stack formed on a glass substrate (not labeled). On the glass substrate 155961.doc • 52· 201222119 is a fluorinated tin oxide layer 804 which acts as a first Tc (for a transparent electronic conductor. The layer is sometimes referred to as a r TEC layer). The tungsten oxide EC layer is deposited on the TCO 804. In this example t, the layer _ is opened at a thickness of about tens of nanometers (i.e., using the oxygen and argon gas to form a boundary 〇3 via a money-plated crane, as described above with respect to Figure 6), followed by deposition of an oxygen-rich precursor. The thickness of the bulk layer from 8 〇 5 to about 15 〇 nm "addition of lithium to the layer 8 〇 5. Next, a NiWO CE layer 81G of about 23 Å thick was added, followed by the addition of a clock to fade and then add about 1% excess lithium. Finally, an indium tin oxide layer 812 is deposited and the stack is subjected to a multi-step thermochemical grading as described above with respect to Figure 4B. After the MSTCC, perform this S TEM » as seen, forming a new region of ion-conducting electrical insulation 8 〇 8. The difference between this example and the embodiment described with respect to Figure 4B is that, unlike the similar layer 405 of Figure 4B, the oxygen-rich layer 805 is only partially converted into the interface region 808. In this case, only about 40 nm of the 150 nm oxygen-rich precursor layer 405 is converted into a region that acts as an ion conducting layer. Figures 8B and 8C show a "front-back" comparison of the device precursor (Figure 8C) of the present invention with the device precursor (Figure 8B) prior to multi-step thermochemical conditioning as analyzed by STEM. In this example, only layers 804-810 (EC to CE) are depicted. These layers are numbered the same as in Figure 8A, with some exceptions. The dotted line in Fig. 8B is used to roughly distinguish the interface between the EC layer 806 and the oxygen-rich layer 805 (this is more clearly seen in Figure 8C). Referring again to Figure 8B, it appears that there is at least lithium concentrated at the interface of the oxygen-rich layer 805 and the CE layer 810 (a region approximately 10-15 nm thick) as indicated by 808a. After the MTCC (Fig. 8C), it is apparent that the interface region 808 has been formed. Although the foregoing invention has been described in some detail to facilitate an understanding, the embodiments of the 155961.doc.53.201222119 are described as illustrative and not limiting, and in the appended claims::: Changes and modifications. 4 围范鸣内's practical [simplified description of the drawings] Figure 1A is a schematic cross-sectional view showing the conventional formation of electrochromic surface 0 stacking. Figure 1B shows the composition of a conventional electrochromic stack. Graph. EC layer, 1C layer and CE layer in Figs. 2A to 2C are graphs showing compositions for use in the present invention. Representative of Electrochromic Device Figures 3A and 3B are program flows in accordance with an embodiment of the present invention. 4A-4C are schematic cross sections depicting the formation of an electrochromic device in accordance with certain embodiments of the present invention. Figure 5 depicts the integrated deposition system of the present invention in a perspective view. Figure 6 is a graph of how the program parameters and endpoint readings are correlated during formation of an electrochromic stack in accordance with an embodiment of the present invention. Figures 7 and 8A through 8C are actual cross sections of an electrochromic device fabricated using a method in accordance with an embodiment of the present invention. [Main component symbol description] 100 Electrochromic device 102 Substrate 104 Conductive layer (CL) 106 Electrochromic (EC) layer 108 Ion conduction (1C) layer 155961.doc -54 - 201222119 110 Counter electrode (CE) layer 112 Conductive Layer (CL) 114 Electrochromic Stack 116 Voltage Source 300 Program Flow 320 Program Flow 400 Layered Structure 401 Functional Electrochromic Device 402 Substrate 403 Layered Structure 404 First TCO Layer 405 Second W03 Layer 406 EC Layer 406a EC Layer 407 Layered Stack 408 1C Layer/Interface Zone 408a Ion Conduction Electrical Insulation Zone/Interface Zone 408b Graded Interface Zone 409 Layered Structure 410 CE Layer 411 Layered Stack/Functional Electrochromic Device 412 Second TCO Layer 414a Stack 414b Stacking 155961.doc -55- 201222119 414c Stacking 500 Integrated Deposition System 502 Inlet Vacuum Pre-Draining Chamber 504 Outlet Vacuum Pre-Pulling Chamber 506 Deposition Module 510 Inlet 埠 515 Track 520 Cartridge 525 Substrate 530 Lithium Target 535 LCD and Keyboard 700 electrochromic device 702 glass substrate 704 indium tin oxide (ITO) layer 704a Figure 'case 706 tungsten oxide EC layer 706a pattern 708 new Region 708a Pattern 710 CE Layer 710a Pattern 712 Indium Tin Oxide Layer 712a Pattern 714 Electrochromic Stack - 56-155961.doc 201222119 800 Device 804 Fluorinated Tin Oxide Layer 805 Oxygen-rich Precursor Layer 806 Tungsten Oxide EC Layer 808 New District /Interface area 808a Lithium 810 CE layer 812 Indium tin oxide layer 155961.doc -57-