TWI681242B - Electrochromic devices - Google Patents

Electrochromic devices Download PDF

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TWI681242B
TWI681242B TW106128807A TW106128807A TWI681242B TW I681242 B TWI681242 B TW I681242B TW 106128807 A TW106128807 A TW 106128807A TW 106128807 A TW106128807 A TW 106128807A TW I681242 B TWI681242 B TW I681242B
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layer
electrochromic
counter electrode
lithium
substrate
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TW106128807A
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TW201738643A (en
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王仲春
普拉達安殊
羅茲畢基羅伯特
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唯景公司
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Priority claimed from US12/772,055 external-priority patent/US8300298B2/en
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    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/15Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect
    • G02F1/153Constructional details
    • G02F1/155Electrodes
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/15Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect
    • G02F1/1514Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material
    • G02F1/1523Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material comprising inorganic material
    • G02F1/1525Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material comprising inorganic material characterised by a particular ion transporting layer, e.g. electrolyte
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/15Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect
    • G02F1/1514Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material
    • G02F1/1523Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material comprising inorganic material
    • G02F1/1524Transition metal compounds

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  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Electrochemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Electrochromic Elements, Electrophoresis, Or Variable Reflection Or Absorption Elements (AREA)

Abstract

Conventional electrochromic devices frequently suffer from poor reliability and poor performance. Improvements are made using entirely solid and inorganic materials. Electrochromic devices are fabricated by forming an ion conducting electronically insulating interfacial region that serves as an IC layer. In some methods, the interfacial region is formedafter formation of an electrochromic and a counter electrode layer. The interfacial region contains an ion conducting electronically insulating material along with components of the electrochromic and/or the counter electrode layer. Materials and microstructure of the electrochromic devices provide improvements in performance and reliability over conventional devices.

Description

電致變色裝置Electrochromic device

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熟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。Electrochromism is a phenomenon in which a material exhibits a reversible change in optical properties when it is in a different electronic energy state (usually by undergoing a voltage change), which is electrochemically mediated. The optical property is usually one or more of color, transmittance, absorbance, and reflectance. For example, a well-known electrochromic material is tungsten oxide (WO 3 ). Tungsten oxide is a cathode electrochromic material, in which a color transition (blue permeation) occurs through electrochemical reduction. Electrochromic materials can be incorporated into, for example, windows and mirrors. The color, transmittance, absorbance and/or reflectivity of these windows and mirrors can be changed by inducing changes in electrochromic materials. For example, a well-known application of electrochromic materials is rearview mirrors in some automobiles. In these electrochromic rearview mirrors, the reflectivity of the mirror changes at night, so that the front lights of other vehicles do not distract the driver’s attention. Although the electrochromic system 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.

典型電致變色裝置包括由對離子高度傳導且對電子高度抵抗之離子傳導(「IC」)層分離的電致變色(「EC」)電極層及對向電極(「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對向電極層之間的短路。該離子傳導層允許電致變色電極及對向電極保持電荷,且藉此維持其褪色狀態或著色狀態。在習知電致變色裝置中,該等組件形成堆疊,其中該離子傳導層夾在該電致變色電極與該對向電極之間。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。因此,該等裝置具有具兩個突變界面之三個相異層。 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,對向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對向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/或組成表示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,為了改良裝置可靠性,可製造電致變色裝置之兩個層(電致變色(EC)層及對向電極(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對向電極層之形成之後形成充當IC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份在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對向電極層,而並不首先在該電致變色層與該對向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對向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。該電致變色層及該對向電極層通常(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。該界面區可含有該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。在一實施例中,該電致變色層包括WO3 。在一些實施例中,該EC層包括WO3 ,該CE層包括氧化鎳鎢(NiWO),且該IC層包括鎢酸鋰(Li2 WO4 )。 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WO3 之情況下,在經由濺鍍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實質上多晶微結構之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,WO3 為實質上多晶的。在一些實施例中,可使用WO3 之富氧層作為該界面區之前驅物。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內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對向電極材料之對向電極層;(b)在該電致變色層或該對向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、該對向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及/或對向電極材料,該中間層不為實質上電絕緣的;(c)形成該電致變色層及該對向電極層中之另一者;及(d)允許該中間層之至少一部分變得實質上電絕緣及實質上離子傳導。用於此方法之形成參數及層特性之詳細內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:(i)含有材料源之第一沈積台,其經配置以沈積包括電致變色材料之電致變色層;及(ii)第二沈積台,其經配置以沈積包括對向電極材料之對向電極層;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對向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配置以在該電致變色層或該對向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對向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該電致變色裝置之一或多個層上之一或多個鋰化台。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。本發明之設備無需具有用於製造離子傳導層之單獨標靶。 本發明之另一態樣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)包括對向電極材料之對向電極層;及(c)在該電致變色層與該對向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、該對向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/或對向電極材料。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對向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))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。A typical electrochromic device includes an electrochromic ("EC") electrode layer and a counter electrode ("CE") layer separated by an ion conducting ("IC") layer that is highly conductive to ions and highly resistant to electrons. In other words, the ion conducting layer allows the transport of ions, but blocks the current. As generally understood, the ion conducting layer thus prevents a short circuit between the electrochromic layer and the counter electrode layer. The ion conductive layer allows the electrochromic electrode and the counter electrode to maintain charge, and thereby maintain their faded or colored state. In the conventional electrochromic device, the components form a stack, wherein the ion conductive layer is sandwiched between the electrochromic electrode and the counter electrode. The boundaries between these three stacked components are defined by sudden changes in composition and/or microstructure. Therefore, these devices have three distinct layers with two abrupt interfaces. Quite surprisingly, the inventors have discovered that high-quality electrochromic devices can be manufactured without depositing an ion-conducting electrically insulating layer. According to certain embodiments, the counter electrode and the electrochromic electrode are formed immediately adjacent to each other (often in direct contact) without depositing an ion conducting layer separately. Xianxin, various 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 serves as at least some of the ion-conducting electrically insulating layers in conventional devices Features. The following describes specific mechanisms that may be key to the formation of the interface area. The interface region usually (though not necessarily) has a heterostructure including at least two discrete components represented by different phases and/or compositions. In addition, the interface region may include gradients among these two or more discrete components. The gradient can provide, for example, variable composition, microstructure, resistivity, dopant concentration (eg, oxygen concentration), and/or stoichiometry. In addition to the above findings, the inventors have observed that in order to improve device reliability, two layers of electrochromic devices (electrochromic (EC) layer and counter electrode (CE) layer) can be fabricated to include each A defined amount of lithium. In addition, careful selection of materials and morphology and/or microstructures of some components of electrochromic devices provides improvements 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 found that the formation of the EC-IC-CE stack does not need to be performed in a conventional sequence (EC→IC→CE or CE→IC→EC), but can be performed in the electrochromic layer and opposite After the formation of the electrode layer, an ion conductive electrically insulating region serving as an IC layer is formed. That is, the EC-CE (or CE-EC) stack is formed first, and then one or a combination of the two layers is formed between the EC layer and the CE layer at the interface between the EC layer and the CE layer. Interface area for some uses to the IC layer. The method of the present invention not only reduces manufacturing complexity and cost by eliminating one or more processing steps, but also provides a device that exhibits improved performance characteristics. Therefore, one aspect of the present invention is a method of manufacturing an electrochromic device, the method comprising: forming an electrochromic layer including an electrochromic material; forming an opposite electrode layer in contact with the electrochromic layer, and Without first providing an ion-conducting electrically insulating layer between the electrochromic layer and the counter electrode layer; and forming an interface region between the electrochromic layer and the counter electrode layer, wherein the interface region is substantially ionic Conductive and substantially electrically insulating. The electrochromic layer and the counter electrode layer are usually (but not necessarily) made of one or more materials that are more conductive than the interface region but may have certain anti-electron properties. The interface region may contain component materials of the EC layer and/or the CE layer, and in some embodiments, the EC layer and the CE layer contain component materials of the interface region. In one embodiment, the electrochromic layer includes WO 3 . In some embodiments, the EC layer includes WO 3 , the CE layer includes nickel tungsten oxide (NiWO), and the IC layer includes lithium tungstate (Li 2 WO 4 ). Heating may be applied during the deposition of at least a portion of the electrochromic layer. In one embodiment, where the EC layer includes WO 3 , heating is applied after each of a series of depositions via sputtering to form an EC layer with a substantially polycrystalline microstructure. In one embodiment, the thickness of the electrochromic layer is between about 300 nm and about 600 nm, but the thickness may vary depending on the desired result of forming the interface region after depositing the EC-CE stack. In some embodiments, WO 3 is substantially polycrystalline. In some embodiments, an oxygen-rich layer of WO 3 can be used as a precursor to the interface region. In other embodiments, the WO 3 layer is a graded layer with varying oxygen concentration in the layer. In some embodiments, lithium is the preferred ionic species for driving electrochromic transitions, and stacking or layer lithiation schemes are described. The 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 manufacturing an electrochromic device, the method comprising: (a) forming an electrochromic layer including an electrochromic material or a counter electrode layer including a counter electrode material; (b) Forming an intermediate layer above the electrochromic layer or the counter electrode layer, wherein the intermediate layer includes an oxygen-rich form of at least one of the electrochromic material, the counter electrode material, and additional materials, wherein the additional materials Including different electrochromic materials and/or counter electrode materials, the intermediate layer is not substantially electrically insulating; (c) forming the other of the electrochromic layer and the counter electrode layer; and ( d) Allow at least a portion of the intermediate layer to become substantially electrically insulating and substantially ionically conductive. The details of the formation parameters and layer characteristics used in this method will also be described in more detail below. Another aspect of the present invention is an apparatus for manufacturing an electrochromic device, which includes: an integrated deposition system, which includes: (i) a first deposition station containing a source of material, which is configured to deposit an electrochromic device An electrochromic layer of a color-changing material; and (ii) a second deposition station configured to deposit an opposite electrode layer including the opposite electrode material; and a controller containing a layer for sequentially depositing the stack on the substrate Transfer the programming instructions of 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 Either or both of the second deposition stations are also configured to deposit the intermediate layer over the electrochromic layer or the counter electrode layer, and wherein the intermediate layer includes the electrochromic material or the counter electrode material Oxygen-rich form, and wherein the first deposition stage and the second deposition stage are interconnected in series and are operable to transfer the substrate from one stage to the next without exposing the substrate to the external environment. In one embodiment, the apparatus of the present invention is operable to transfer the substrate from one stage to the next without breaking the vacuum, and may include operable to deposit lithium from a lithium-containing material source in the electrochromic device One or more lithiation stations on one or more layers. In one embodiment, the apparatus of the present invention is operable to deposit the electrochromic stack on a building glass substrate. The apparatus of the present invention does not need to have a separate target for manufacturing the ion conductive layer. Another aspect of the present invention is an electrochromic device including: (a) an electrochromic layer including an electrochromic material; (b) an opposing electrode layer including an opposing electrode material; and (c) in An interface region between the electrochromic layer and the counter electrode layer, wherein the interface region includes at least one of an electrically insulating ion conductive material and the electrochromic material, the counter electrode material, and additional materials, wherein the The additional materials include different electrochromic materials and/or counter electrode materials. In some embodiments, the additional material is not included; in these embodiments, the interface region includes at least one of the electrochromic material and the counter electrode material. Changes in the composition and morphology and/or microstructure of the interface area will be described in more detail herein. The electrochromic devices described herein can be incorporated into windows (in one embodiment, architectural glass scale windows). These and other features and advantages of the present invention will be described in more detail below with reference to the associated drawings.

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。 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100之示意性橫截面。電致變色裝置100包括基板102、導電層(CL)104、電致變色(EC)層106、離子傳導(IC)層108、對向電極(CE)層110及導電層(CL)112。將元件104、106、108、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「TCO」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TCO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116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、對向電極層、離子傳導層、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102上。接著,EC層106沈積在TCO 104上。接著,IC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110上以形成電致變色裝置100。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,IC層必須沈積在EC層上、繼之以CE層沈積在IC層上,或IC層沈積在CE層上、繼之以EC層沈積在IC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,IC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IC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,IC層係藉由PVD自可能難以製造及使用之陶瓷標靶沈積。 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110,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106經沈積為相異層而很少或沒有至鄰近IC層之組合物滲流。類似地,IC材料108及CE材料110在組成上相異而很少或沒有至鄰近層之滲流。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。習知思想為該三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。 一般熟習此項技術者可認識到,圖1B為理想化描繪,且在實踐意義上,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/或對向電極材料。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對向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對向電極材料)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IC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,該富氧區在沈積對向電極層之後在後續處理時轉換成充當IC層之界面區或層。在一些實施例中,使用包括電致變色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層之界面層。在其他實施例中,使用包括對向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。該富氧CE層之全部或一部分經轉換成界面區。在其他實施例中,使用包括對向電極材料之富氧型式及電致變色材料之富氧形式之相異層來(最終)在EC層與CE層之間形成充當IC層之界面區。換言之,富氧材料之一些或全部充當該充當IC層之界面區之前驅物。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IC層之一或多個功能(特別是對離子之高傳導性及對電子之高電阻率)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WO3 ,但意欲包括WO x ,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(NiWO),且界面區主要包含鎢酸鋰(此處表示為Li2 WO4 ,在另一實施例中,界面區為在約0.5%與約50(原子)%之間的Li2 O、在約5%與約95%之間的Li2 WO4 及約5%與約70%之間的WO3 之奈米複合材料)及某一量之EC材料及/或CE材料。更一般言之,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。由於此原因,本文中有時將充當IC層之界面區稱為「梯度區」、「異質IC層」或「分散式IC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x 軸自左向右移動,吾人可看到,一部分EC材料WO3 (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鎢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IC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IC層功能。發明者已發現,與具有突然過渡之習知裝置相比,此等「異質IC層」改良電致變色裝置之切換特性及可能之熱循環穩定性。此實例中之CE層主要含有氧化鎳鎢作為活性材料,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層作為由鎢酸鋰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2A中所描繪。 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x 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x 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%之氧化鎳鎢及約20%之鎢酸鋰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80%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CE材料均為充當IC層之界面區的重要組份。參看圖2C,自原點開始且沿著x 軸自左向右移動,吾人可看到,一部分EC材料WO3 (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三分之一附近,亦存在增長量之氧化鎳鎢對向電極材料。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80%之鎢酸鋰。在此實例中,EC層與IC層之間或IC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約中間處出現峰值,且因此,此區很可能為界面區之最強電絕緣部分。 如以上[發明內容]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IC層之界面區之分級組合物的三個非限制性實例。一般熟習此項技術者將瞭解,在不脫離本發明之範疇的情況下,許多變化係可能的。在圖2A至圖2C中之實例之每一者中,存在至少一層,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,及對向電極層,其中該裝置之前述兩個層及一個區中之每一者之至少一材料組份以如下量存在於該電致變色層、該界面區及該對向電極層中之每一者中:至少約25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10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%。 界面區中之電致變色材料及/或對向電極材料之量可為顯著的,在一實施例中,多達界面區之50重量%。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/或對向電極材料。在一實施例中,界面區包括在約60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/或對向電極材料。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/或對向電極材料。在一實施例中,界面區包括在約80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/或對向電極材料。 在一些實施例中,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變色材料及/或對向電極材料亦如此。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(超化學計量)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層可包括單一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550 nm厚,其包括富氧層(或區)。若EC層之約150 nm經轉換成界面區,則EC之約27%經轉換成界面區,亦即,150 nm除以550 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)。若富氧金屬氧化物層之全部或一部分經轉換成界面區,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%與約50%之間的用以形成界面區之前驅物區(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IC層具有許多益處。儘管不希望受理論限制,但咸信,藉由具有此等分級區,電致變色過渡之效率得到大大改良。如下文將更詳細描述,存在其他益處。 儘管不希望束縛於理論,但咸信,以下機制中之一或多者可實現EC及/或CE材料至界面區中之IC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一者。此等機制中之每一者與在堆疊之製造期間絕不沈積IC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IC層之材料之單獨標靶。 在第一機制中,電致變色材料或對向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量。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IC功能材料之界面區。該鋰擴散可在整個該第二層已形成之後或在該第二層之僅某一部分已形成之後發生。此外,鋰之擴散及至IC功能性材料之後續轉換在該第一或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層之一些鋰擴散至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EC層以根據上述之該第一機制產生某一IC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IC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IC功能性材料區。 最後,在第四機制中,在EC層與CE層之間流動之電流驅動電致變色材料及對向電極材料中之至少一者轉化為界面區中之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EC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鋰通量可產生鎢酸鋰,其充當IC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,此係因為用於驅動高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300。具體言之,參見305,(在例如TCO之CL上)沈積EC層。接著,參見310,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IC層之界面區。本發明之一實施例為步驟305與310顛倒之類似方法(未描繪)。該方法之要點在於,充當IC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」IC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。 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對向電極層,而並不首先在該電致變色層與該對向電極層之間提供離子傳導電絕緣層,其中該對向電極層包括對向電極材料;及在該電致變色層與該對向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3A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(詳言之,組合物及配置)之WO3 ;CE層包括NiWO,界面區包括Li2 WO4 ,且使用諸如氧化銦錫及經氟化之氧化錫之TCO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Kozlowski等人之題為「Fabrication of Low Defectivity Electrochromic Devices」之美國非臨時專利申請案第12/645,111號及Wang等人之題為「Electrochromic Devices」之美國非臨時專利申請案第12/645,159號中,該兩專利申請案出於所有目的而以引用方式併入本文中。在特定實施例中,本發明之電致變色裝置全部為固態的且係在允許在受控周圍環境中沈積堆疊之一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備中,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中所需之用於沈積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物堆疊(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態材料常常具有的污染物及洩漏問題之優點。應理解,堆疊中之該等層中之任何一或多者可含有某一量之有機材料,但在許多實施中,該等層中之一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言可同樣如此。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3B,參見325,首先沈積WO3 之EC層。圖4A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320形成電致變色裝置之示意性橫截面。具體言之,圖4A至圖4C用以展示包括WO3 之EC層可如何形成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412基本上相同。又,在該三個實施例中之每一者,形成不具有IC層之堆疊,且接著進一步處理該堆疊以便在該堆疊內形成充當IC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400、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,苯乙烯丙烯腈共聚物)、聚(4-甲基-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)銷售的塗有導電層之玻璃。TEC Glass™為塗有經氟化之氧化錫導電層之玻璃。 在一些實施例中,基板402之光學透射率(亦即,透過之輻射或光譜對入射之輻射或光譜之比)為約90%至95%,例如,約90%至92%。基板可具有任何厚度,只要其具有合適機械性質以支撐電致變色裝置即可。雖然基板402可具有任何大小,但在一些實施例中,其為約0.01 mm至10 mm厚,較佳約3 mm至9 mm厚。 在本發明之一些實施例中,基板為建築玻璃。建築玻璃為用作建築材料之玻璃。建築玻璃通常用於商業建築中,但亦可用於居住建築中,且通常(但不必)分離室內環境與室外環境。在特定實施例中,建築玻璃為至少20吋乘以20吋,且可以更大,例如,大達約72吋乘以120吋。建築玻璃通常為至少約2 mm厚。小於約3.2 mm厚之建築玻璃不可回火。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)之鹼石灰玻璃。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%)。可見光譜為典型人眼會回應之光譜,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)由經氟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100 nm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,404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402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。 與圖3B之程序流程320一致,堆疊414a、414b及414c中之每一者包括沈積在第一TCO層404之上之電致變色層。該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(WO3 )、氧化鉬(MoO3 )、氧化鈮(Nb2 O5 )、氧化鈦(TiO2 )、氧化銅(CuO)、氧化銥(Ir2 O3 )、氧化鉻(Cr2 O3 )、氧化錳(Mn2 O3 )、氧化釩(V2 O5 )、氧化鎳(Ni2 O3 )、氧化鈷(Co2 O3 )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-Mo氧化物、W-V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對向電極層轉移之離子。 在一些實施例中,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 x 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(WO3 )不展現電致變色。在一更特定實施例中,將WO x (其中x 小於3.0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 x ,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,Rutherford Backscattering Spectroscopy)之技術可識別包括鍵結至鎢之氧原子及未鍵結至鎢之氧原子之氧原子之總數。在一些例子中,氧化鎢層(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x 為3.0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IC層之離子傳導電絕緣區之前驅物。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 nm(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10至100 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20個)氧化鎢單位晶胞。 因此,為便利起見,圖3B中之程序流程320之剩餘部分將關於第一實施例(包括圖4A中所表示之EC層406之形成)予以進一步描述。接著,將在下文描述圖4B及圖4C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。 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WO3 )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WO3 。在一實施例中,在沈積WO3 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WO3 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WO3 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WO3 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O2 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℃與約450℃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WO3 ,其中該濺鍍氣體包括約50%至約60%之O2 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℃與約350℃之間。在此等實施例中,WO3 層為實質上均質的。在一實施例中,WO3 為實質上多晶的。咸信,在沈積期間至少間歇性地加熱WO3 幫助多晶形式之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,合適離子包括鋰離子(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)氘離子(D+ )、鈉離子(Na+ )、鉀離子(K+ )、鈣離子(Ca++ )、鋇離子(Ba++ )、鍶離子(Sr++ )及鎂離子(Mg++ )。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(WO3-y (0<y£~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,而是可在沈積對向電極層之後添加,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。在一些實施例中,對向電極層410為無機及/或固體。該對向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,對向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,對向電極層由於離子之損失而著色。 在一些實施例中,用於對向電極之合適材料包括氧化鎳(NiO)、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(Cr2 O3 )、氧化錳(MnO2 )及普魯士藍(Prussian blue)。光學被動對向電極包括氧化鈰鈦(CeO2 -TiO2 )、氧化鈰鋯(CeO2 -ZrO2 )、氧化鎳(NiO)、氧化鎳鎢(NiWO)、氧化釩(V2 O5 )及氧化物之混合物(例如,Ni2 O3 與WO3 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)鉭及鎢。因為對向電極層410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,所以對向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。對向電極形態可為晶形、奈米晶形或非晶形。 在一些實施例中,在對向電極層為氧化鎳鎢之情況下,對向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對向電極之晶形對應物相比,已發現該等實質上非晶形之氧化鎳鎢對向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,非晶形氧化鎳鎢係藉由濺鍍製程中之相對較高能量之原子產生。較高能量之原子係(例如)在具有較高標靶功率、較低腔室壓力(亦即,較高真空)及較小的源至基板之距離之濺鍍製程中獲得。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,存在於氧化鎳鎢中之鎳的量可高達氧化鎳鎢之約90重量%。在一特定實施例中,氧化鎳鎢中之鎳與鎢之質量比在約4:6與6:4之間,在一實例中為約1:1。在一實施例中,NiWO包含約15%(原子)與約60%之間的Ni,及在約10%與約40%之間的W。在另一實施例中,NiWO包含約30%(原子)與約45%之間的Ni,及在約15%與約35%之間的W。在另一實施例中,NiWO包含在約30%(原子)與約45%之間的Ni,及在約20%與約30%之間的W。在一實施例中,NiWO包含約42%(原子)之Ni及約14%之W。 在一實施例中,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300 nm之間,在另一實施例中在約200 nm與約250 nm之間,在另一實施例中為約230 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「色彩」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對向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340,鋰(例如,經由濺鍍)添加至NiWO CE層。在一特定實施例中,參見圖3B之345,在已引入足夠鋰以使NiWO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對向電極層褪色所需之量過量約5%與約15%之間。在另一實施例中,添加至CE層之過量鋰為基於使該對向電極層褪色所需之量過量約10%。在沈積CE層410、以鋰使其褪色及添加額外鋰之後,參見圖3B之350,在對向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100 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400,則使其經受將堆疊414a之至少一部分轉換成IC層之熱化學調節(若其歸因於鋰擴散或其他機制而未經轉換)。堆疊414a為前驅物而非電致變色裝置,此係因為該堆疊在EC層406與CE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406之部分經轉換成IC層408以形成功能性電致變色裝置401。參看圖3B,參見355,分層結構400經受MTCC。在一實施例中,該堆疊首先在惰性氛圍(例如,氬氣)下在約150℃與約450℃之間經受加熱歷時約10分鐘與約30分鐘之間,且接著在O2 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℃下在惰性氛圍下加熱歷時約15分鐘,且接著在O2 下加熱約5分鐘。接下來,分層結構400在空氣中經受加熱。在一實施例中,該堆疊在空氣中在約250℃與約350℃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300℃下加熱歷時約30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,且建立功能性電致變色裝置。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之一部分一起組合以形成充當IC層之界面區408。咸信界面區408主要為鎢酸鋰(Li2 WO4 ),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,尚不明確知曉此現象如何發生。存在在多步驟熱化學調節期間必須發生以在EC層與CE層之間形成離子傳導電絕緣區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IC層408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10 nm與約150 nm之間,在另一實施例中在約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)鋰或其他合適離子,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)SiO2 、Nb2 O5 、Ta2 O5 、TiO2 、ZrO2 及CeO2 。在使用鋰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、硼酸鋰鋁、氟化鋰鋁、硼酸鋰、氮化鋰、矽酸鋰鋯、鈮酸鋰、硼矽酸鋰、磷矽酸鋰及其他此等基於鋰之陶瓷材料、矽石或氧化矽(包括氧化鋰矽))可製成為充當IC層之界面區。 如所提及,在一實施例中,離子傳導區之前驅物為經由本文中所描述之鋰化及MTCC轉化成離子傳導/電絕緣區之富氧(超化學計量之)層。儘管不希望束縛於理論,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(Li2 WO4 )、鉬酸鋰(Li2 MoO4 )、鈮酸鋰(LiNbO3 )、鉭酸鋰(LiTaO3 )、鈦酸鋰(Li2 TiO3 )、鋯酸鋰(Li2 ZrO3 )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(WO3+x ,0≤x≤1.5)、氧化鉬(MoO3+x ,0≤x≤1.5)、氧化鈮(Nb2 O5+x ,0≤x≤2)、氧化鈦(TiO2+x ,0≤x≤1.5)、氧化鉭(Ta2 O5+x ,0≤x≤2)、氧化鋯(ZrO2+x ,0≤x≤1.5)及氧化鈰(CeO2+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對向電極層410與電致變色層406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10-10 西門子/公分(Siemens/cm)(或ohm-1 cm-1 )與約10-3 西門子/公分之間的離子電導率及大於105 歐姆-公分之電阻率。在另一實施例中,該離子導體材料具有介於約10-8 西門子/公分與約10-3 西門子/公分之間的離子電導率及大於1010 歐姆-公分之電阻率。雖然離子傳導層應大體上抗漏電流(例如,提供不大於約15 μA/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 μA/cm與約150 μA/cm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IC層之特定實例予以描述。又,如上文所提及,當(例如)鋰擴散或熱將EC及/或CE層之一些轉換成界面區時,具有IC性質之界面區可在製造堆疊期間在原位形成。 通常,在製程中稍後建立離子傳導區存在特定益處。首先,可保護離子傳導材料不受在EC層及CE層之沈積及鋰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IC材料形成移至製程中稍後階段,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IC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。此等條件包括鋰擴散及電極之間的電流。在製程中後期控制此等及其他條件提供額外靈活性以使IC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IC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IC層之習知技術(例如,自IC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一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,在一實例中為約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。此可能可歸因於較大量的安置在界面區及/或分級界面中之可容易地轉移(例如,在EC與界面區之間及/或在CE與界面區之間)之鋰。此等鋰可處於與存在於界面區中之IC相互混之EC及/或CE相中。其亦可能歸因於存在於界面區中之IC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100 μA/cm。 現參看圖4B,在第二實施例中,堆疊414b之最初敷設之EC材料實際上為兩個層:第一WO3 層406,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O2 及約20%與約60%之間的Ar之第一濺鍍氣體濺鍍;及第二WO3 層405,其厚度在約100 nm與約200 nm之間,該第二層係使用鎢標靶及包括約70%與100%之間的O2 及0%與約30%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402至少間歇性地加熱至約150℃與約450℃之間而施加熱,但在第二WO3 層405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50%與約60%之間的O2 及約40%與約50%之間的Ar;第二WO3 層405為約150 nm厚,且該第二濺鍍氣體實質上為純O2 。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℃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WO3 層為實質上多晶的,而該第二WO3 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、添加額外鋰及沈積第二TCO層412以完成分層堆疊403。對分層堆疊403執行類似熱化學調節以提供分層堆疊407、包括離子傳導電絕緣區408a之功能性電致變色裝置。儘管不希望束縛於理論,但在此實例中,咸信WO3 之富氧層405主要充當前驅物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IC層之功能之界面區。 現參看圖4C,在第三實施例中,分層堆疊409包括EC層406a(其具有WO3 之分級組合物(graded composition )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EC-CE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406a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WO3 層,其中該濺鍍氣體在濺鍍電致變色層開始時包括約40%與約80%之間的O2 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O2 及0%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℃與約450℃之間,但不或實質上不在EC層406a之至少一最後部分之沈積期間施加熱。在一更特定實施例中,分級組合物WO3 層為約550 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O2 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O2 ;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200℃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EC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O2 及約40%與約50%之間的Ar調整至實質上純O2 。 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,離子傳導材料及電致變色材料(例如,鎢酸鋰與氧化鎢之混合物))中可包括梯度。該梯度可提供(例如)可變之組合物、微結構、電阻率、摻雜劑濃度(例如,氧濃度)、化學計量、密度及/或晶粒大小範圍。該梯度可具有許多不同形式之過渡,包括線性過渡、S型過渡、高斯過渡等。在一實例中,電致變色層包括過渡至超化學計量氧化鎢區中之氧化鎢區。該超化學計量氧化物區之部分或全部經轉換成界面區。在最後結構中,氧化鎢區為實質上多晶的,且微結構在界面區處過渡至實質上非晶形的。在另一實例中,電致變色層包括過渡至(超化學計量之)氧化鈮區中之氧化鎢區。該氧化鈮區之部分或全部經轉換成界面區。在最後結構中,氧化鎢區為實質上多晶的,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408b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411中充當EC層)之功能性電致變色裝置。儘管不希望束縛於理論,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。儘管不希望束縛於理論,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/或對向電極材料之相對量。 在本文中所描述之各種實施例中,電致變色堆疊經描述為在特定處理階段期間不或實質上不加熱。在一實施例中,在加熱步驟之後,主動或被動地(例如,使用散熱片)冷卻堆疊。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,經由膨脹)氣體之冷卻、致冷單元及其類似者而冷卻之壓板。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。 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對向電極材料之對向電極層;(b)在該電致變色層或該對向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、該對向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對向電極材料,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對向電極層中之另一者;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WO3 。在另一實施例中,(a)包括使用鎢標靶及包括約40%與約80%之間的O2 及約20%與約60%之間的Ar之第一濺鍍氣體濺鍍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150℃與約450℃之間。在另一實施例中,(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O2 及0%與約30%之間的Ar之第二濺鍍氣體濺鍍WO3 以達到在約100 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,該對向電極層包括厚度在約150 nm與約300 nm之間的NiWO。在另一實施例中,將鋰濺鍍至對向電極層上,直至該對向電極層褪色。在另一實施例中,將基於使該對向電極層褪色所需之量過量約5%與約15%之間的額外量之鋰濺鍍至該對向電極層上。在另一實施例中,在該對向電極層之上沈積透明導電氧化物層。在一實施例中,該透明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150℃與約450℃之間加熱歷時約10分鐘與約30分鐘之間,且接著在O2 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250℃與約350℃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MO x 之第一電致變色材料,其中M為金屬或非金屬元素,且x 指示化學計量之氧與M之比,且(b)包括濺鍍式NO y 之第二電致變色材料以作為中間層,其中N為相同或不同之金屬或非金屬元素,且y 指示超化學計量量之氧與N之比。在一實施例中,M為鎢,且N為鎢。在另一實施例中,M為鎢,且N係選自由鈮、矽、鉭、鈦、鋯及鈰組成之群組。 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)包括對向電極材料之對向電極層;及(c)在該電致變色層與該對向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、該對向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對向電極材料。 在一實施例中,該電絕緣離子傳導材料及該電致變色材料、該對向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內。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、該對向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,且該對向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150 nm之間,且該對向電極層之厚度在約150 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20 nm與約100 nm之間,且該對向電極層之厚度在約150 nm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30 nm與約50 nm之間,且該對向電極層之厚度在約200 nm與約250 nm之間。 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O2 及約20%與約60%之間的Ar之濺鍍氣體濺鍍鎢標靶以產生WO3 至在約500 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℃與約450℃之間; 將鋰濺鍍至該電致變色層上,直至盲電荷得到滿足; 在該電致變色層上沈積對向電極層,而並不首先在該電致變色層與該對向電極層之間提供離子傳導電絕緣層,其中該對向電極層包括NiWO; 將鋰濺鍍至該對向電極層上,直至該對向電極層實質上褪色;及 在該電致變色層與該對向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。在一實施例中,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。在一些實施例中,該罩蓋層為SiAlO。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100 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腔室設備(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IC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,發明者對在窗、特別是建築玻璃鱗片窗(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之設備,其包括:整合式沈積系統,其包括:(i)含有材料源之第一沈積台,其經配置以沈積包括電致變色材料之電致變色層;及(ii)第二沈積台,其經配置以沈積包括對向電極材料之對向電極層;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,該堆疊具有夾在該電致變色層與該對向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配置以在該電致變色層或該對向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對向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該電致變色裝置之一或多個層上之一或多個鋰化台。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、該中間層及該對向電極層中之至少一者上沈積來自含鋰材料源之鋰之一或多個鋰化台。在又一實施例中,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狹縫閥門,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配置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500之簡化表示且更詳細地包括內部之剖視圖。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506。存在用於裝載(例如)建築玻璃基板525之入口埠510(真空預抽室504具有對應出口埠)。基板525由沿著軌道515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515支撐,但集裝架520亦可支撐在靠近設備500之底部定位之軌道或(例如)在設備500之頂部與底部中間的軌道之頂上。集裝架520可在系統500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,從而產生多次通過以便達成所要鋰化。然而,此功能不限於鋰標靶,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530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,在每一沈積台中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內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12/645,111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內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者。此等組件並未展示,而是可為一般熟習此項技術者所瞭解。系統500(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。一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統或經由一或多個電腦系統傳送之資料之各種製程。本發明之實施例亦係關於用於執行此等操作之設備、此等電腦及微控制器。此等設備及製程可用以沈積本發明之方法及經設計以實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用於所需目的,或該控制設備可為通用電腦,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配置。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一起使用,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3B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「電致變色裝置前驅物」可具有特別價值。在裝置前驅物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,電致變色裝置前驅物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(提供防潮或抗刮性)以氣密式地密封該裝置前驅物及其類似物。在一實施例中,罩蓋層沈積於該前驅物堆疊之TCO層上。在一些實施例中,該罩蓋層為SiAlO。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100 nm之間。對處於適當位置之頂蓋層之後續處理形成IC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,此係因為內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物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物可具有優點,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一前驅物堆疊導致之靈活性。又,此等前驅物堆疊可用於測試目的,例如,品質控制或研究努力。 因此,本發明之一實施例為一種電致變色裝置前驅物,其包括:(a)基板;(b)該基板上之第一透明導電氧化物層;(c)該第一透明導電氧化物層上之堆疊,該堆疊包括:(i)包括電致變色材料之電致變色層,及(ii)包括對向電極材料之對向電極層;其中該堆疊不包括介於該電致變色層與該對向電極層之間的離子傳導且電絕緣之區;及(d)在該堆疊之上之第二透明導電氧化物層。在一實施例中,該電致變色層包括氧化鎢,且該對向電極層包含氧化鎳鎢。在一實施例中,該堆疊及該電致變色層中之至少一者含有鋰。在另一實施例中,該電致變色層為至少在與該對向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,該堆疊包括在該對向電極層與該電致變色層之間的IC前驅物層,該IC前驅物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IC前驅物層之情況下,該電致變色層之厚度在約500 nm與約600 nm之間,且該對向電極層之厚度在約150 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IC前驅物層之情況下,該電致變色層之厚度在約350 nm與約400 nm之間,該IC前驅物層之厚度在約20 nm與約100 nm之間,且該對向電極層之厚度在約150 nm與約300 nm之間。在一實施例中,本文中所描述之前驅物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)包括對向電極材料之對向電極層,其中該裝置不含有在該電致變色層與該對向電極之間的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,該對向電極材料為氧化鎳鎢,且介於該電致變色層與該對向電極層之間的為包括鎢酸鋰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300 nm與約500 nm之間;該界面區之厚度在約10 nm與約150 nm之間,且該對向電極層之厚度在約150 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x 軸單位為時間/程序流程。在此實例中,製造類似於關於圖4A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WO3 (例如,使用鎢標靶濺鍍,其中濺鍍氣體為約60%之O2 及約40%之Ar),CE層形成於EC層之上且由NiWO製成,且第二TCO為氧化銦錫(ITO)。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(WO3 )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0.07(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0.2。在沈積氧化鎢EC層之後,在EC層上濺鍍鋰,如「Li」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0.4,其指示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NiWO層之沈積,光學密度在此期間增加,此係因為NiWO經著色。由於約230 nm厚之NiWO層之添加,光學密度在NiWO沈積期間自約0.4進一步增加至約0.9。請注意,隨著NiWO沈積,一些鋰可自EC層擴散至CE層。此用來在NiWO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」指示之第二時間週期指示鋰至NiWO EC層之添加。光學密度在此階段期間自約0.9減小至約0.4,此係因為NiWO之鋰化使NiWO褪色。進行鋰化,直至NiWO褪色(包括約0.4光學密度之局部最小值)。光學密度在約0.4開始回升,此係因為WO3 層仍被鋰化且影響光學密度。接下來,如時間週期「額外Li」所指示,將額外鋰濺鍍至NiWO層上,在此實例中,與添加至NiWO之鋰相比約10%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「ITO」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250℃歷時約15分鐘,且接著在O2 下加熱約5分鐘。接著,在空氣中在約300℃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,且尤其用於將鋰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702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濺鍍鎢形成之WO3 ),如上文關於圖6所描述。將鋰添加至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10%過量之鋰。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TEM。如所見,形成離子傳導電絕緣之新區708。 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706a展示EC層為多晶的。圖案708a展示IC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800為形成於玻璃基板(未標記)上之電致變色堆疊。在該玻璃基板上的是經氟化之氧化錫層804,其充當第一TCO(對透明電子導體而言,該層有時被稱為「TEC」層)。氧化鎢EC層806沈積於TCO 804上。在此實例中,層806以約400 nm之厚度形成(亦即,利用氧氣及氬氣經由濺鍍鎢形成之WO3 ,如上文關於圖6所描述),接著沈積富氧前驅物層805至約150 nm之厚度。將鋰添加至層805。接著,添加約230 nm厚之NiWO CE層810,繼而添加鋰以褪色且接著添加約10%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節,如上文關於圖4B所描述。在MSTCC之後,進行此STEM。如所見,形成離子傳導電絕緣之新區808。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之富氧前驅物層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800(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物(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,但所描述之實施例應視為說明性而非限制性的。一般熟習此項技術者將顯而易見,在附加申請專利範圍之範疇內,可實踐特定變化及修改。The present invention claims the rights and priority of the US applications No. 12/772,055 and No. 12/772,075, each filed on April 30, 2010 and entitled "Electrochromic Devices", these applications Each of them is incorporated by reference in full text. The following detailed description can be more fully understood when considered in conjunction with the drawings. FIG. 1A is a schematic cross-section depicting a stack 100 of conventional electrochromic devices. The electrochromic device 100 includes a substrate 102, a conductive layer (CL) 104, an electrochromic (EC) layer 106, an ion conductive (IC) layer 108, a counter electrode (CE) layer 110, and a conductive layer (CL) 112. The elements 104, 106, 108, 110, and 112 are collectively referred to as the electrochromic stack 114. Generally, the CL layers are made of transparent conductive oxide, and are often referred to as "TCO" layers. Since the TCO layer is transparent, the coloring behavior of the EC-IC-CE stack can be observed, for example, through the TCO layer, allowing these devices to be used on windows to obtain reversible shading. A voltage source 116 operable to apply a potential across the electrochromic stack 114 realizes the transition of the electrochromic device from, for example, a faded state (ie, transparent) to a colored state. The order of these layers can be reversed with respect to the substrate. That is, the layers may be in the following order: substrate, transparent conductive layer, counter electrode layer, ion conductive layer, electrochromic material layer, and (another) transparent conductive layer. Referring again to FIG. 1A, in a conventional method of manufacturing an electrochromic stack, individual layers are deposited on top of another layer in a sequential format as depicted in the schematic diagram on the left side of FIG. 1A. That is, the TCO layer 104 is deposited on the substrate 102. Next, the EC layer 106 is deposited on the TCO 104. Next, the IC layer 108 is deposited on the EC layer 106, followed by the CE layer 110 on the IC layer 108, and finally the TCO layer 112 is deposited on the CE layer 110 to form the electrochromic device 100. 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 IC layer must be deposited on the EC layer, followed by the CE layer on the IC layer, or the IC layer is deposited on The CE layer, followed by the EC layer is deposited on the IC layer. The transition between the layers of material in the stack is abrupt. One of the significant challenges of the above procedures is the processing required to form the IC layer. In some previous methods, the IC layer is formed by a sol-gel process that is difficult to incorporate into the CVD or PVD process used to form the EC layer and the CE layer. In addition, IC layers created by sol-gel and other liquid-based processes tend to have defects that degrade the quality of the device and may need to be removed by, for example, engraving. In other methods, the IC layer is deposited by PVD from a ceramic target that may be difficult to manufacture and use. FIG. 1B is a graph depicting the% composition of material versus the position in the electrochromic stack of FIG. 1A (ie, layers 106, 108, and 110, ie, EC layer, IC layer, and CE layer). As mentioned, in conventional electrochromic stacks, the transition between the layers of material in the stack is abrupt. For example, the EC material 106 is deposited as a distinct layer with little or no composition seepage to the adjacent IC layer. Similarly, the IC material 108 and the CE material 110 are different in composition with little or no seepage to adjacent layers. Therefore, these materials are substantially homogeneous (except for the specific composition of CE materials described below) and have abrupt interfaces. The conventional idea is that each of these three layers should be laid as distinct, uniformly deposited and smooth layers to form a stack. The interface between each layer should be "clear", where there is little intermixing of materials from each layer. Those skilled in the art can generally recognize that FIG. 1B is an ideal depiction, and in the practical sense, there is a certain degree of unavoidable material mixing at the layer interface. The point is that in conventional manufacturing methods, any such mixing is unintentional and minimal. The inventors have discovered that an interface region serving as an IC layer can be formed, where the interface region intentionally includes a large amount of one or more electrochromic materials and/or counter electrode materials. This is a fundamental deviation from self-study manufacturing methods. As mentioned above, the inventors have found that the formation of the EC-IC-CE stack does not have to be performed in a conventional sequence (EC→IC→CE or CE→IC→EC), but can be performed in the electrochromic layer and opposite After the deposition of the electrode layer, an interface region serving as an ion conductive layer is formed. That is, the EC-CE (or CE-EC) stack is formed first, and then the layers are used at the interface of the layers (in some embodiments, and/or another electrochromic material or counter electrode material ) One or both components form an interface region between the EC layer and the CE layer (which may possess at least some functions of the IC layer). The interface area serves at least some of the functions of the conventional IC layer because the interface area is substantially ionically conductive and substantially electrically insulating. However, it should be noted that the interface region as described may have a leakage current higher than that accepted by the conventional art, but despite this, these devices exhibit good performance. In one embodiment, the electrochromic layer is formed to have an oxygen-rich region that is converted into an interface region or layer that serves as an IC layer during subsequent processing after depositing the counter electrode layer. In some embodiments, an oxygen-rich dissimilar layer including an electrochromic material is used to (eventually) form an interface layer between the EC layer and the CE layer that acts as an IC layer. In other embodiments, an oxygen-rich dissimilar layer including a counter electrode material is used to (finally) form an interface region between the EC layer and the CE layer that serves as an IC layer. All or part of the oxygen-rich CE layer is converted into an interface area. In other embodiments, a dissimilar layer including an oxygen-rich version of the counter electrode material and an oxygen-rich form of the electrochromic material is used (finally) to form an interface region between the EC layer and the CE layer that acts as an IC layer. In other words, some or all of the oxygen-rich material acts as a precursor to the interface region that serves as the IC layer. The method of the present invention not only reduces processing steps, but also produces electrochromic devices that exhibit improved performance characteristics. As mentioned, Xianxin, some of the EC layer and/or CE layer in the interface area are converted to provide one or more functions of the IC layer (especially high conductivity to ions and high resistivity to electrons) Of material. The IC functional material in the interface region may be, for example, a salt of a conductive cation; for example, a lithium salt. 2A, 2B, and 2C show the composition 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), where the EC material is tungsten oxide (denoted here Is WO 3 , but is intended to include WO x , where x is between about 2.7 and about 3.5, in one embodiment, x is between about 2.7 and about 2.9), the CE material is nickel tungsten oxide (NiWO), and the interface The region mainly includes lithium tungstate (herein expressed as Li 2 WO 4 , in another embodiment, the interface region is between about 0.5% and about 50 (atomic)% Li 2 O, between about 5% and about Between 95% of Li 2 WO 4 and between about 5% and about 70% of WO 3 nanocomposite) and a certain amount of EC material and/or CE material. More generally, the interface region usually (but not necessarily) has a heterostructure including at least two discrete components represented by different phases and/or compositions whose concentration varies across the width of the interface region. For this reason, in this article, the interface region that serves as the IC layer is sometimes referred to as the "gradient region", "heterogeneous IC layer" or "dispersed IC layer". Although described with respect to specific materials, the illustrations in FIGS. 2A, 2B, and 2C more generally represent changes in the composition of any suitable materials used in the electrochromic device of the present invention. FIG. 2A depicts the electrochromic stack of the present invention, where the EC material is an important component serving as the interface region of the IC layer, and the CE material is not an important component. Referring to FIG. 2A, starting from the origin and moving from left to right along the x- axis, one can see that a part of the EC material WO 3 (which is substantially all tungsten oxide) serves as an EC layer. There is a transition into the interface area where there is gradually decreasing tungsten oxide and correspondingly increasing lithium tungstate up to and including the end near the interface area, where there is a substance with a certain minimum amount of tungsten oxide All of the above are parts of lithium tungstate. Although the transition from the EC layer to the interface region is distinguished by a combination of substantially all tungsten oxide and a minimum amount of lithium tungstate, it is obvious that the transition is not as sudden as in conventional devices. In this example, in fact, the transition begins to occur when the composition has a sufficient amount of lithium tungstate to enable the material to perform at least some functions of the IC layer, such as ion conduction and electrical insulation. Undoubtedly, the composition closer to the CE layer (wherein the composition is substantially lithium tungstate) functions as an IC layer, because it is known that lithium tungstate exhibits these properties. However, certain IC layer functions also exist in other parts of the interface area. The inventors have discovered that these "heterogeneous IC layers" improve the switching characteristics and possible thermal cycling stability of electrochromic devices compared to conventional devices with sudden transitions. The CE layer in this example mainly contains nickel tungsten oxide as the active material, and has a relatively sudden transition to the nickel tungsten oxide composition at the edge of the interface region. The method for manufacturing a stack with these interface areas will be described in more detail below. It should be noted that, for example, the nickel tungsten oxide CE layer in FIG. 2A is depicted as having about 20% lithium tungstate. Without wishing to be bound by theory, Xianxin believes that the nickel tungsten oxide CE layer exists as a core or particle of nickel oxide surrounded by a shell or matrix of lithium tungstate (which imparts a fairly good ion conductivity to the CE layer), and thereby Helps the electrochromic transition of the CE layer during the operation of the electrochromic stack. The exact stoichiometry of lithium tungstate in the CE layer can vary significantly between examples. In some embodiments, some tungsten oxide may also be present in the CE layer. Also, because lithium ions travel from the EC layer and the CE layer via the interface region serving as the IC layer, there may be a large amount of lithium tungstate in the EC layer, for example, as depicted in FIG. 2A. FIG. 2B depicts the electrochromic stack of the present invention, in which the CE material is an important component serving as the interface region of the IC layer, and the EC material is not an important component. Referring to FIG. 2B, starting from the origin and moving from left to right along the x- axis, one can see that in this case, substantially all EC materials that are tungsten oxide act as EC layers. There is a sudden transition into the interface region where there is little (if any) tungsten oxide, but there is a large amount of lithium tungstate and at least some nickel tungsten oxide (CE material). The composition of the interface region changes along the x- axis with decreasing lithium tungstate and corresponding increasing nickel tungsten oxide. The transition from the interface area to the CE layer is arbitrarily distinguished by a composition of approximately 80% nickel tungsten oxide and approximately 20% lithium tungstate, but this is only one example of the transition that occurs with a graded composition. When no or few additional changes in the composition occur during further processing of the stack, the interface area can be considered terminated. In addition, the transition actually ends when the composition has a sufficient amount of nickel-tungsten oxide so that the material no longer performs at least a certain function that the different IC layer can perform. Undoubtedly, the composition closer to the CE layer (as distinguished) (where the composition is 80% nickel tungsten oxide) functions as the CE layer. Similarly, the 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. FIG. 2C depicts the electrochromic stack of the present invention, where both the EC material and the CE material are important components that serve as the interface region of the IC layer. Referring to FIG. 2C, starting from the origin and moving from left to right along the x- axis, one can see that a part of the EC material WO 3 (which is substantially all tungsten oxide) serves as an EC layer. There is a transition into the interface region where there is gradually decreasing tungsten oxide and correspondingly increasing lithium tungstate. In this example, there is also a growing amount of nickel tungsten oxide counter electrode material in the vicinity of one-third of the way through the part divided into the interface region. At about the middle position of the portion divided by the interface region, there are about 10% of each of tungsten oxide and nickel tungsten oxide and 80% of lithium tungstate. In this example, there is no abrupt transition between the EC layer and the IC layer or between the IC layer and the CE layer, but there is an interface region with a continuous graded composition of both CE material and EC material. In this example, the lithium tungstate component peaks approximately midway through the interface area, and therefore, this area is likely to be the strongest electrically insulating portion of the interface area. As mentioned in [Summary of the Invention] above, the EC layer and the CE layer may include a material composition that imparts a certain resistivity to the EC layer and the CE layer; at least a certain amount spans all of the materials described in FIGS. 2A to 2C Lithium tungstate in the three regions is an example of such materials that impart resistivity to the EC layer and the CE layer. 2A to 2C only show three non-limiting examples of the graded composition that serves as the interface region of the IC layer in the electrochromic device of the present invention. Those of ordinary skill in the art will understand that many variations are possible without departing from the scope of the present invention. In each of the examples in FIGS. 2A to 2C, there is at least one layer in which there are only two material components and one of the components is the least. The invention is not limited to this approach. Therefore, an embodiment of the present invention is an electrochromic device including an electrochromic layer, an interface region serving as an IC layer, and a counter electrode layer, wherein each of the aforementioned two layers and one region of the device At least one component of the material is present in each of the electrochromic layer, the interface region, and the counter electrode layer in the following amount: at least about 25% by weight, in another embodiment, at least about 15 % By weight, in another embodiment, at least about 10% by weight, in another embodiment, at least about 5% by weight, and in yet another embodiment, at least about 2% by weight. The amount of electrochromic material and/or counter electrode material in the interface area may be significant, in one embodiment, up to 50% by weight of the interface area. However, in many embodiments, the ion-conducting electrically insulating material is usually a plurality of components, and the remaining part of the interface region is the electrochromic material and/or the counter electrode material. In one embodiment, the interface region includes between about 60% and about 95% by weight ionically conductive electrically insulating material, and the remaining portion of the interface region is electrochromic material and/or counter electrode material. In one embodiment, the interface region includes between about 70% and about 95% by weight ionically conductive electrically insulating material, and the remaining portion of the interface region is the electrochromic material and/or counter electrode material. In one embodiment, the interface region includes between about 80% and about 95% by weight ionically conductive electrically insulating material, and the remaining portion of the interface region is an electrochromic material and/or counter electrode material. In some embodiments, the interface regions in the devices described herein may be relatively different, that is, when analyzed, for example, by a microscope, there are relatively distinguishable boundaries at adjacent layers, even if the interface region contains The same is true for a certain amount of electrochromic material and/or counter electrode material. In these embodiments, the thickness of the interface region can be measured. In embodiments where the interface region is formed by the oxygen-rich (superstoichiometric) region of the EC layer and/or 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 One of the zones is measured. 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 mixed homogeneously or heterogeneously in the layer or more diffusion regions. The EC layer is 550 nm thick, which includes an oxygen-rich layer (or region). If about 150 nm of the EC layer is converted into the interface region, then about 27% of the EC is converted into the interface region, that is, 150 nm divided by 550 nm. In another example, the EC layer includes a first metal oxide region (or layer) and an oxygen-rich second metal oxide layer (or region). If all or part of the oxygen-rich metal oxide layer is converted into an 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 the interface region is formed) is Measurement of the interface area. In one embodiment, the interface region includes between about 0.5% and about 50% by thickness of the precursor region (EC and/or CE, including the oxygen-rich portion) used to form the interface region, in another embodiment Between about 1% and about 30%, in yet 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 has many benefits as an IC layer. Although not wishing to be bound by theory, Xianxin, by having such grading zones, the efficiency of electrochromic transition is greatly improved. As will be described in more detail below, there are other benefits. Although not wishing to be bound by theory, Xianxin believes that one or more of the following mechanisms can achieve the conversion of EC and/or CE materials into IC functional materials in the interface region. However, the implementation 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 IC layer material during the manufacturing of the stack. As clearly stated elsewhere herein, the device of the present invention need not have a separate target containing materials for the IC layer. In the first mechanism, direct lithiation of the electrochromic material or the counter electrode material produces an IC material (eg, lithium tungstate) in the interface region. As will be explained more fully below, various embodiments use the direct lithiation of one of these active layers at some point in the manufacturing process between the formation of the EC layer and the CE layer. This operation involves the exposure of the EC layer or the CE layer (formed first) to lithium. According to this mechanism, ion-conducting electron-resistant materials such as lithium salts are generated through the flux of lithium in the EC or CE layer. Heat or other energy can be applied to drive this flux of lithium. The described mechanism converts 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, lithium diffusing from one of EC or CE to another layer causes EC and/or after both layers have been formed and/or during the formation of the second layer on the lithiated first layer The part of one of the CEs is converted to the interface area with IC functional materials at its interface. The lithium diffusion may occur after the entire second layer has been formed or after only a certain portion of the second layer has been formed. In addition, the diffusion of lithium and the subsequent conversion to the functional material of the IC occur in the first or the second deposited layer and in the EC or CE layer. In one example, the EC layer is formed first, and then the EC layer is lithiated. When the CE layer is subsequently deposited over the EC layer, some lithium diffuses from the underlying EC layer toward the CE layer and/or into the CE layer, resulting in conversion into an interface region containing IC functional materials. In another example, an EC layer (with an oxygen-rich upper region as appropriate) is formed first, then, a CE layer is formed and the CE layer is lithiated. Subsequently, some lithium from the CE layer diffuses into the EC layer, where it forms an interface region with IC functional materials. In yet another example, an EC layer is first deposited, and then the EC layer is lithiated to produce a certain IC functional material according to the first mechanism described above. Next, when the CE layer is formed, some lithium diffuses from the underlying EC layer toward the CE layer to produce an IC material in the interface region of the CE layer. In this way, the functional IC material nominally resides in both the CE layer and the EC layer immediately following the interface of the CE layer and the EC layer. In the third mechanism, the EC layer and the CE layer are formed to completion (or at least the moment when the second formed layer is partially completed). Next, the device structure is heated, and the heating converts at least some of the materials in the interface area into IC functional materials (eg, lithium salts). Heating (e.g., as part of the multi-step thermochemical conditioning (MTCC) described further herein) can be performed during deposition or after completion of deposition. In one embodiment, heating is performed after the transparent conductive oxide is formed on the stack. In another embodiment, heating is applied after the second layer is partially or completely completed, but before the transparent conductive oxide is applied to the second layer. In some cases, heating is direct and primarily responsible for conversion. In other cases, heating mainly promotes the diffusion or flow of lithium ions. As described in the second mechanism, this creates an IC functional material area. Finally, in the fourth mechanism, the current flowing between the EC layer and the CE layer drives at least one of the electrochromic material and the counter electrode material into an IC functional material in the interface region. This conversion may occur because, for example, the ion flux associated with the flowing current is so large that it drives the chemical conversion of the EC and/or CE material to the IC material in the interface region. For example, as will be explained below, a large lithium flux through tungsten oxide in the EC layer can produce lithium tungstate, which acts as an IC material. The lithium flux can be introduced, for example, during the initial activation cycle of the newly formed device. However, this need not be the case, because other opportunities for driving high ion fluxes may be more appropriate for achieving the conversion. The method of the present invention can be performed by those skilled in the art without using any one or more of the above mechanisms. FIG. 3A is a program flow 300 of the method according to the present invention. Specifically, see 305, (on the CL of TCO, for example) to deposit an EC layer. Next, referring to 310, a CE layer is deposited. After depositing the EC layer and the CE layer, then, referring to 315, an interface region serving as an IC layer is formed between the EC layer and the CE layer. An embodiment of the present invention is a similar method (not depicted) in which steps 305 and 310 are reversed. The main point of this method is that the interface region serving as the IC layer is formed after the EC layer and the CE layer (in some embodiments, at least part of one of the EC layer and the CE layer is used to form the interface region). For this reason, the interface region formed in this way is sometimes referred to as the "essential" IC layer. In other embodiments, for example, an oxygen-enriched version of EC material or CE material is used to form a different layer between the EC layer and the CE layer, wherein the layer is completely or partially converted into an interface region after forming the EC layer and the CE layer . Various methods for forming the interface region after forming the EC-CE stack will be described below. Therefore, as mentioned, one aspect of the present invention is a method of manufacturing an electrochromic device, the method comprising: forming an electrochromic layer including an electrochromic material; and forming an opposing surface in contact with the electrochromic layer An electrode layer without first providing an ion-conducting electrically insulating layer between the electrochromic layer and the counter electrode layer, wherein the counter electrode layer includes a counter electrode material; and between the electrochromic layer and the pair An interface region is formed between the electrode layers, wherein the interface region is substantially ion conductive and substantially electrically insulating. The interface region may contain the EC layer, the CE layer, or a component material of both. As will be described in more detail below, this interface region can be formed in many ways. FIG. 3B is a process flow showing the process flow according to the method described with respect to FIG. 3A (in detail, a process flow for depositing an EC layer, then depositing a CE layer, and finally forming an interface region serving as an IC layer between the layers) Procedure 320. More specifically, in this embodiment, the EC layer includes WO 3 with various amounts of oxygen (specifically, composition and configuration); the CE layer includes NiWO, the interface region includes Li 2 WO 4 , and uses such as oxidation TCO materials of indium tin and fluorinated tin oxide. It should be noted that the layers of the electrochromic device will be described below with regard to solid materials. Solid-state materials are required due to reliability, consistent characteristics and process parameters, and device performance. Exemplary solid-state electrochromic devices, methods, and equipment for manufacturing the same, and methods for manufacturing electrochromic windows using these devices are described in Kozlowski et al., US Non-Provisional Patent Application entitled "Fabrication of Low Defectivity Electrochromic Devices" No. 12/645,111 and Wang et al. US Non-Provisional Patent Application No. 12/645,159 entitled "Electrochromic Devices". These two patent applications are incorporated herein by reference for all purposes. In certain embodiments, the electrochromic devices of the present invention are all solid state and are manufactured in equipment that allows one or more layers of the stack to be deposited in a controlled ambient environment. That is, in equipment that deposits these layers without leaving the equipment and, for example, without breaking the vacuum between the deposition steps, thereby reducing contaminants and ultimately improving device performance. In a particular embodiment, the device of the present invention does not require the separate target for depositing the IC layer required in the conventional device. As those skilled in the art will understand, the present invention is not limited to these materials and methods. However, in certain embodiments, the materials that make up the electrochromic stack and the precursor stack (as described below) are all inorganic, Solid (that is, 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 provide the advantage of a reliable electrochromic stack that can work for long periods of time. Solid materials also provide the advantage of not having the contaminants and leakage problems that liquid materials often have. It should be understood that any one or more of the layers in the stack may contain a certain amount of organic material, but in many implementations, one or more of the layers contain little or no organic material. The same can be true for liquids that may be present in small amounts in one or more layers. It should also be understood that solid materials can be deposited or otherwise formed by processes using liquid components (such as specific processes using sol-gel or chemical vapor deposition). Referring again to FIG. 3B, see 325, the EC layer of WO 3 is first deposited. 4A to 4C are schematic cross-sections depicting the formation of an electrochromic device according to a specific method and apparatus of the present invention, and in particular, according to the program flow 320. FIG. Specifically, FIGS. 4A to 4C are used to show three non-limiting examples of how an EC layer including WO 3 can be formed as part of a stack, where an interface region serving as an IC layer is formed after depositing other layers of the stack . In each of FIGS. 4A to 4C, the substrate 402, the first TCO layer 404, the CE layer 410, and the second TCO layer 412 are substantially the same. Also, in each of the three embodiments, a stack without an IC layer is formed, and then the stack is further processed to form an interface region serving as an IC layer within the stack between the EC layer and the CE layer . Referring to each of FIGS. 4A to 4C, layered structures 400, 403, and 409 are depicted, respectively. Each of these layered structures includes a substrate 402 that is, for example, glass. As the substrate 402, any material having suitable optical, electrical, thermal, and mechanical properties may be used. Such substrates include, for example, glass, plastic, and mirror materials. Suitable plastic substrates include, for example, acrylic, polystyrene, polycarbonate, allyl diethylene glycol carbonate, SAN (styrene acrylonitrile copolymer), poly(4-methyl-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 silica/polysilicon wear-resistant coating, or the like (such as a coating well known in plastic glazing technology) Layer to provide barrier protection and wear protection. Suitable glasses include transparent or colored soda lime glass, including soda lime floating glass. The glass can be tempered or untempered. In some embodiments, commercially available substrates such as glass substrates contain a transparent conductive layer coating. Examples of such glasses include conductive layer coated glasses sold under the trademarks TEC Glass™ (Pilkington of Toledo, Ohio) and SUNGATE™ 300 and SUNGATE™ 500 (PPG Industries of Pittsburgh, Pennsylvania). TEC Glass™ is glass coated with a conductive layer of fluorinated tin oxide. In some embodiments, the optical transmittance of the substrate 402 (ie, the ratio of transmitted radiation or spectrum to incident radiation or spectrum) is about 90% to 95%, for example, about 90% to 92%. The substrate may have any thickness as long as it has suitable mechanical properties to support the electrochromic device. Although the substrate 402 may have any size, in some embodiments, it is about 0.01 mm to 10 mm thick, preferably about 3 mm to 9 mm thick. In some embodiments of the invention, the substrate is architectural glass. Architectural glass is glass used as a building material. Architectural glass is usually used in commercial buildings, but can also be used in residential buildings, and usually (but not necessarily) separate indoor and outdoor environments. In certain embodiments, the architectural glass is at least 20 inches by 20 inches, and may be larger, for example, up to about 72 inches by 120 inches. Architectural glass is usually at least about 2 mm thick. Architectural glass less than about 3.2 mm thick cannot be tempered. In some embodiments of the invention using architectural glass as the substrate, the substrate can still be tempered even after the electrochromic stack has been fabricated on the substrate. In some embodiments using architectural glass as the substrate, the substrate is soda lime glass from a tin float line. The percentage of transmission in the visible spectrum of architectural glass substrates (ie, overall transmission across the visible spectrum) is generally 80% greater than that of neutral substrates, but it may be lower than the percentage of transmission of colored substrates. Preferably, the percentage transmission of the substrate in the visible spectrum is at least about 90% (eg, about 90% to 92%). The visible spectrum is the spectrum that the typical human eye will respond to, generally about 380 nm (purple) to about 780 nm (red). In some cases, the glass has a surface roughness between about 10 nm and about 30 nm. In one embodiment, the substrate 402 is a soda glass with 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 the layered structures 400, 403, and 409, for example, a first TCO layer 404 made of fluorinated tin oxide or other suitable material (which is especially conductive and transparent) is deposited on the substrate 402. Transparent conductive oxides include metal oxides and metal oxides 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, ruthenium oxide, doped ruthenium oxide and the like. In one embodiment, the thickness of this second TCO layer is between about 20 nm and about 1200 nm, in another embodiment between about 100 nm and about 600 nm, in another embodiment, about 350 nm thick. The TCO layer should have an appropriate sheet resistance (R s ) due to the relatively large area spanned by these layers. In some embodiments, the sheet resistance of the TCO layer is between about 5 ohms and about 30 ohms per square. In some embodiments, the sheet resistance of the TCO layer is about 15 ohms per square. In general, it is desirable that the sheet resistance of each of the two conductive layers is approximately the same. In one embodiment, the two layers (eg, 404 and 412) each have a sheet resistance of about 10-15 ohms per square. Each of the layered structures 400, 403, and 409 includes stacks 414a, 414b, and 414c, respectively, and each of these stacks includes a first TCO layer 404, a CE layer 410, and a second TCO above the substrate 402 Level 412. The difference between each of the layered structures 400, 403, and 409 is how the EC layer is formed, which in each case affects the shape of the resulting interface area. Consistent with the process flow 320 of FIG. 3B, each of the stacks 414a, 414b, and 414c includes an electrochromic layer deposited on the first TCO layer 404. The electrochromic layer may contain any one or more of many different electrochromic materials including metal oxides. Such metal oxides include tungsten oxide (WO 3 ), molybdenum oxide (MoO 3 ), niobium oxide (Nb 2 O 5 ), titanium oxide (TiO 2 ), copper oxide (CuO), iridium oxide (Ir 2 O 3 ) , Chromium oxide (Cr 2 O 3 ), manganese oxide (Mn 2 O 3 ), vanadium oxide (V 2 O 5 ), nickel oxide (Ni 2 O 3 ), cobalt oxide (Co 2 O 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 (eg, W-Mo oxides, WV oxides) can also be used in specific embodiments, that is, the electrochromic layer includes two or more of the above metal oxides. The electrochromic layer including metal oxide can receive ions transferred from the counter electrode layer. In some embodiments, tungsten oxide or doped tungsten oxide is used for the electrochromic layer. In one embodiment of the invention, the electrochromic layer is substantially made of WO x , where " 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 tungsten oxide that is only below the stoichiometric amount exhibits electrochromism; that is, stoichiometric tungsten oxide (WO 3 ) does not exhibit electrochromism. In a more specific embodiment, WO x (where x is less than 3.0 and at least about 2.7) is used for the electrochromic layer. In another embodiment, the electrochromic layer is WO x , where x is between about 2.7 and about 2.9. Techniques such as Rutherford Backscattering Spectroscopy (RBS) can identify the total number of oxygen atoms including oxygen atoms bonded to tungsten and oxygen atoms not bonded to tungsten. In some examples, the tungsten oxide layer (where x is 3 or greater) exhibits electrochromism, which may be due to unbound excess oxygen and sub-stoichiometric tungsten oxide. In another embodiment, the tungsten oxide layer has stoichiometric or more oxygen, where x is from 3.0 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 as a precursor to form an ion-conducting electrically insulating region that acts as an IC layer. In other embodiments, a dissimilar layer of highly oxidized EC material is formed between the EC layer and the CE layer for at least partial final conversion to the ion-conducting electrically insulating interface region. In certain embodiments, the tungsten oxide is crystalline, nanocrystalline, or amorphous. In some embodiments, the tungsten oxide is substantially nanocrystalline and has an average grain size of about 5 nm to 50 nm (or about 5 nm to 20 nm), characterized by transmission electron microscopy (TEM) . The tungsten oxide morphology or microstructure can also be characterized as nanocrystalline using x-ray diffraction (XRD) and/or electron diffraction (such as selected area electron diffraction (SAED)). For example, the nanocrystalline electrochromic tungsten oxide may be characterized by the following XRD characteristics: a crystal size of about 10 to 100 nm (eg, about 55 nm). In addition, nanocrystalline tungsten oxide can exhibit limited long-range order, for example, about several (about 5 to 20) tungsten oxide unit cells. Therefore, for convenience, the remainder of the program flow 320 in FIG. 3B will be further described in relation to the first embodiment (including the formation of the EC layer 406 shown in FIG. 4A). Next, the second and third embodiments shown in FIGS. 4B and 4C, respectively, will be described below, with particular emphasis on the formation and morphology and/or microstructure of their respective EC layers. As mentioned with reference to FIG. 3B, see 325, an EC layer is deposited. In the first embodiment (represented in FIG. 4A), a substantially homogeneous EC layer 406 (including WO 3 ) is formed as part of the stack 414a, where the EC layer is in direct contact with the CE layer 410. In one embodiment, as described above, the EC layer includes WO 3 . In one embodiment, heating is applied during at least part of the deposition of WO 3 . In a particular embodiment, a sputtering target is passed several times, wherein a portion of WO 3 is deposited as each pass passes, and after each deposition, heating is applied to, for example, the substrate 402 to deposit WO 3 on the deposition layer 406 Adjust WO 3 before the next section. In other embodiments, the WO 3 layer can be continuously heated during deposition and can be deposited in a continuous manner instead of going through the sputtering target several times. In one embodiment, 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 embodiment described with respect to FIG. 4A, the EC layer is a tungsten target with a thickness between about 500 nm and about 600 nm and includes between about 40% and about 80% O 2 and about 20% and about Between 60% of the Ar 3 sputter gas sputtered WO 3 , and the substrate in which WO 3 is deposited is heated at least intermittently between about 150° C. and about 450° C. during the formation of the EC layer. In a specific embodiment, the EC layer is about 550 nm thick WO 3 using a tungsten target sputtering, wherein the sputtering gas includes about 50% to about 60% O 2 and about 40% to about 50% Ar, and the substrate on which WO 3 is deposited is heated at least intermittently between about 250°C and about 350°C during the formation of the electrochromic layer. In these embodiments, the WO 3 layer is substantially homogeneous. In one embodiment, WO 3 is substantially polycrystalline. Xianxin, heating the WO 3 at least intermittently during the deposition helps the formation of WO 3 in polycrystalline form. As mentioned, many materials are suitable for the EC layer. In general, in electrochromic materials, the coloration of electrochromic materials (or any optical properties, such as changes in absorbance, reflectance, and transmittance) is through reversible ion insertion (eg, intercalation) into the material ) And the corresponding injection of charge balance electrons. Usually, a small part of the ions responsible for the optical transition are irreversibly bound together in the electrochromic material. As described herein, some or all of the irreversibly bound ions are used to compensate for "blind charge" in the material. In most electrochromic materials, suitable ions include lithium ions (Li + ) and hydrogen ions (H + ) (ie, protons). However, in some cases, other ions will be appropriate. This plasma includes, for example, deuterium ions (D + ), sodium ions (Na + ), potassium ions (K + ), calcium ions (Ca ++ ), barium ions (Ba ++ ), strontium ions (Sr ++ ) And magnesium ions (Mg ++ ). In various embodiments described herein, lithium ions are used to generate electrochromism. The intercalation of lithium ions to tungsten oxide (WO 3-y (0<y£~0.3)) changes tungsten oxide from transparent (fading state) to blue (coloring state). In a typical process where the EC layer includes or is tungsten oxide, a lithium system is deposited on the EC layer 406 (for example, via sputtering) to meet the blind charge (see FIG. 6 and FIG. 7 for more details), see FIG. 3B 330 of the program flow. In one embodiment, lithiation is performed in an integrated deposition system (where vacuum is not broken between deposition steps). It should be noted that in some embodiments, lithium is not added at this stage, but may be added after the counter electrode layer is deposited, or in other embodiments, lithium is added after the TCO is deposited. Referring again to FIG. 4A, next, a CE layer 410 is deposited on the EC layer 406. In some embodiments, the counter electrode layer 410 is inorganic and/or solid. The counter electrode layer may include one or more of many different materials capable of acting as a reservoir of ions when the electrochromic device is in a faded state. During the electrochromic transition initiated by, for example, applying an appropriate potential, the counter electrode layer transfers some or all of the ions it holds to the electrochromic layer, thereby changing the electrochromic layer to a colored state. At the same time, in the case of NiO and/or 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 (NiO), nickel tungsten oxide (NiWO), nickel vanadium oxide, nickel chromium oxide, nickel aluminum oxide, nickel manganese oxide, nickel magnesium oxide, chromium oxide (Cr 2 O 3 ), manganese oxide (MnO 2 ) and Prussian blue. Optical passive counter electrodes include cerium titanium (CeO 2 -TiO 2 ), cerium zirconium oxide (CeO 2 -ZrO 2 ), nickel oxide (NiO), nickel tungsten oxide (NiWO), vanadium oxide (V 2 O 5 ) and A mixture of oxides (for example, a mixture of Ni 2 O 3 and WO 3 ). Doping formulations of these oxides can also be used, where the dopant includes, for example, tantalum and tungsten. Since the counter electrode layer 410 contains ions used to generate electrochromism in the electrochromic material when the electrochromic material is in a faded state, the counter electrode preferably has a high level when it maintains a significant amount of this plasma Transmittance and neutral color. The shape of the counter electrode can be crystalline, nanocrystalline or amorphous. In some embodiments, where the counter electrode layer is nickel tungsten oxide, the counter electrode material is amorphous or substantially amorphous. Compared to the crystalline counterpart of the substantially amorphous nickel-tungsten oxide counter electrode, it has been found that these substantially amorphous nickel-tungsten oxide counter electrodes perform better under certain conditions. As described below, the amorphous state of nickel tungsten oxide can be obtained by using specific processing conditions. Although not wishing to be bound by any theory or mechanism, Xianxin believes that amorphous nickel-tungsten oxide is produced by relatively high-energy atoms in the sputtering process. Higher energy atomic systems are obtained, for example, in sputtering processes with higher target power, lower chamber pressure (ie, higher vacuum), and smaller source-to-substrate distance. Under the described processing conditions, a higher density film with better stability under UV/heat exposure is produced. In certain embodiments, the amount of nickel present in nickel tungsten oxide can be up to about 90% by weight of nickel tungsten oxide. In a particular embodiment, the mass ratio of nickel to tungsten in nickel tungsten oxide is between about 4:6 and 6:4, in one example about 1:1. In one embodiment, NiWO contains between about 15% (atomic) and about 60% Ni, and between about 10% and about 40% W. In another embodiment, NiWO contains between about 30% (atomic) and about 45% Ni, and between about 15% and about 35% W. In another embodiment, NiWO contains between about 30% (atomic) and about 45% Ni, and between about 20% and about 30% W. In one embodiment, NiWO contains about 42% (atomic) Ni and about 14% W. In one embodiment, as described above, referring to 335 of FIG. 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, in another embodiment between about 200 nm and about 250 nm, and in another embodiment about 230 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 non-limiting and implies only one of many examples of electrochromic transitions that may be implemented. Unless otherwise stated herein, whenever a fade-color transition is mentioned, the corresponding device or process covers other optical state transitions such as non-reflective-reflective, transparent-opaque, etc. In addition, the term "fading" refers to an optically neutral state, such as uncolored, transparent, or translucent. Furthermore, unless otherwise stated herein, the "color" of the electrochromic transition is not limited to any particular wavelength or range of wavelengths. As generally understood by those skilled in the art, the selection of appropriate electrochromic materials and counter electrode materials controls the related optical transitions. In a particular embodiment, see 340 of FIG. 3B, lithium (eg, via sputtering) is added to the NiWO CE layer. In a particular embodiment, see 345 of FIG. 3B, an additional amount of lithium is added after sufficient lithium has been introduced to completely fade the NiWO (this procedure is optional, and in one embodiment, at this stage of the procedure Add excess lithium). In one embodiment, this additional amount is between about 5% and about 15% based on the amount required to discolor the counter electrode layer. In another embodiment, the excess lithium added to the CE layer is about 10% excess based on the amount required to discolor the counter electrode layer. After depositing the CE layer 410, discoloring it with lithium, and adding additional lithium, referring to 350 of FIG. 3B, a second TCO layer 412 is deposited over the counter electrode layer. In one embodiment, the transparent conductive oxide includes indium tin oxide. In another embodiment, the TCO layer is indium tin oxide. In one embodiment, the thickness of this second TCO layer is between about 20 nm and about 1200 nm, in another embodiment between about 100 nm and about 600 nm, in another embodiment about 350 nm. Referring again to FIG. 4A, once the layered structure 400 is completed, it is subjected to thermochemical adjustment to convert at least a portion of the stack 414a into an IC layer (if it is not converted due to lithium diffusion or other mechanisms). The stack 414a is a precursor rather than an electrochromic device, because the stack does not yet have an ion conductive/electrically insulating layer (or region) between the EC layer 406 and the CE layer 410. In this particular embodiment, in a two-step process, a portion of the EC layer 406 is converted into an IC layer 408 to form a functional electrochromic device 401. Referring to FIG. 3B and see 355, the layered structure 400 is subjected to MTCC. 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 30 minutes, and then heated under O 2 for a duration 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 under O 2 for about 5 minutes. Next, the layered structure 400 is subjected to heating in air. In one embodiment, the stack is heated in air at between about 250°C and about 350°C for between about 20 minutes and about 40 minutes, in another embodiment, the stack is at about 300°C in air The heating lasted about 30 minutes. The energy required to implement MTCC need not be radiant heat. For example, in one embodiment, MTCC is implemented using ultraviolet radiation. Other energy sources can also be used without departing from the scope of the present invention. After the multi-step thermochemical adjustment, the procedure 320 is completed, and the functional electrochromic device is established. As mentioned, and although not wishing to be bound by theory, it is believed that the lithium in the stack 414a is combined with a portion of the EC layer 406 and/or the CE layer 410 to form an interface region 408 that serves as an IC layer. The Xianxin interface region 408 is mainly lithium tungstate (Li 2 WO 4 ), which is known to have good ion conduction and electrical insulation properties compared to traditional IC layer materials. As discussed above, it is not clear how this phenomenon occurs. There is a chemical reaction that must occur during the multi-step thermochemical conditioning to form an ion-conducting electrically insulating region 408 between the EC layer and the CE layer, but it is also believed that the initial flux of lithium traveling through the stack (eg, as described above The excess lithium added to the CE layer described above) plays a role in the formation of the IC layer 408. The thickness of the ion-conducting electrically 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 10 nm and about 150 nm, in another embodiment between about 20 nm and about 100 nm, and in other embodiments between about 30 nm and Between about 50 nm. As mentioned above, there are many suitable materials for forming the EC layer. Therefore, by using, for example, lithium or other suitable ions in the above method, one can make other interface regions that serve as IC layers starting from the oxygen-rich EC material. Suitable EC materials for this purpose include (but are not limited to) SiO 2 , Nb 2 O 5 , Ta 2 O 5 , TiO 2 , ZrO 2 and CeO 2 . In specific embodiments using lithium ions, ion conducting materials (such as, but not limited to, lithium silicate, lithium aluminum silicate, lithium aluminum borate, lithium aluminum fluoride, lithium borate, lithium nitride, lithium zirconium silicate, Lithium niobate, lithium borosilicate, lithium phosphosilicate and other such lithium-based ceramic materials, silica or silicon oxide (including lithium oxide silicon) can be made to serve as the interface region of the IC layer. As mentioned, in one embodiment, the precursor of the ion conduction region is an oxygen-rich (superstoichiometric) layer converted into an ion conduction/electrical insulation region by lithiation and MTCC as described herein. Although not wishing to be bound by theory, Xianxin believes that after lithiation, excess oxygen forms lithium oxide, which further forms lithium salts (ie, lithium electrolytes), such as lithium tungstate (Li 2 WO 4 ), lithium molybdate (Li 2 MoO 4 ), lithium niobate (LiNbO 3 ), lithium tantalate (LiTaO 3 ), lithium titanate (Li 2 TiO 3 ), lithium zirconate (Li 2 ZrO 3 ) and the like. In one embodiment, the interface region includes at least one of the following: tungsten oxide (WO 3+x , 0≤x≤1.5), molybdenum oxide (MoO 3+x , 0≤x≤1.5), niobium oxide (Nb 2 O 5+x , 0≤x≤2), titanium oxide (TiO 2+x , 0≤x≤1.5), tantalum oxide (Ta 2 O 5+x , 0≤x≤2), zirconium oxide ( ZrO 2+x , 0≤x≤1.5) and cerium oxide (CeO 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 with a low degree of defect and it substantially prevents electrons from passing while allowing ions to pass between the counter electrode layer 410 and the electrochromic layer 406 can. The material can substantially conduct ions and substantially resist electrons. In one embodiment, the ion conductor material has an ion conductivity between about 10 -10 Siemens/cm (or ohm -1 cm -1 ) and about 10 -3 Siemens/cm and is greater than 10 5 ohm-cm resistivity. In another embodiment, the ion conductor material has an ionic conductivity between about 10-8 Siemens/cm and about 10-3 Siemens/cm and a resistivity greater than 10 10 ohm-cm. Although the ion-conducting layer should be substantially resistant to leakage current (for example, providing a leakage current no greater than about 15 μA/cm 2 ), it has been found that some devices manufactured as described herein have surprisingly high leakage currents (for example , Between about 40 μA/cm and about 150 μA/cm), but still provide good color variation across the device and operate efficiently. As mentioned above, there are at least two other ways to establish an ion-conducting electrically insulating region between the EC layer and the CE layer after forming the stack. These additional embodiments will be described below with reference to specific examples of using tungsten oxide for the IC layer. Also, as mentioned above, when, for example, lithium diffusion or heat converts some of the EC and/or CE layers into interface regions, interface regions with IC properties may be formed in situ during the manufacturing stack. Often, there are specific benefits to establishing the ion conducting region later in the process. First, the ion conductive material can be protected from some of the harsh processes that occur during the deposition and lithiation of the EC and CE layers. For example, depositing these layers through a plasma process is often accompanied by a large voltage drop next to the stack, often around 15-20 volts. These large voltages can damage sensitive ion conductive materials or cause decomposition of sensitive ion conductive materials. By moving the IC material formation to a later stage in the process, the material is not exposed to potential damage to voltage extremes. Second, by forming IC materials later in the process, we can better control some processing conditions that are not possible before completing both the EC layer and the CE layer. These conditions include lithium diffusion and current between electrodes. Controlling these and other conditions in the middle and late stages of the process provides additional flexibility to adapt the physical and chemical properties of IC materials to specific applications. Therefore, not all the benefits of the present invention are due to the unique interface area that acts as an IC layer, that is, there are also manufacturing and other benefits. It has been observed that ion conducting materials formed according to some of the embodiments described herein are superior to devices fabricated using conventional techniques for forming IC layers (eg, PVD from IC material targets) efficacy. For example, it has been found that the device switching speed is very fast (eg, less than 10 minutes, in one example about 8 minutes) to achieve a final state of about 80% compared to 20-25 minutes or more for conventional devices. In some examples, the devices described herein have an order of magnitude faster than conventional devices. This may be due to the large amount of lithium disposed in the interface area and/or the graded interface that can be easily transferred (eg, between EC and interface area and/or between CE and interface area). Such lithium may be in EC and/or CE phases that are mixed with ICs present in the interface region. It may also be attributed to the relatively thin layer or network of IC materials present in the interface area. To support this view, it has been observed that some devices manufactured according to the teachings in this article have high leakage currents, but still surprisingly exhibit good color changes and good efficiency. In some cases, the leakage current density of devices that have been robustly implemented has been found to be at least about 100 μA/cm. Referring now to FIG. 4B, in the second embodiment, the initially laid EC material of the stack 414b is actually two layers: the first WO 3 layer 406, which is similar to the layer 406 in FIG. 4A, but with a thickness of about 350 nm Between about 450 nm and the first layer is sputtered with a tungsten target and a first sputtering gas including between about 40% and about 80% O 2 and between about 20% and about 60% Ar ; And the second WO 3 layer 405, whose thickness is between about 100 nm and about 200 nm, the second layer uses a tungsten target and includes between about 70% and 100% of O 2 and 0% and about 30 The second sputtering gas sputtering of Ar between %. In this embodiment, heat is applied by heating the substrate 402 at least intermittently to between about 150°C and about 450°C during the deposition of the first WO 3 layer 406, but during the deposition of the second WO 3 layer 405 No heating or no heating during the period. In a more specific embodiment, the layer 406 is about 400 nm thick, and the first sputtering gas includes between about 50% and about 60% O 2 and between about 40% and about 50% Ar; The two WO 3 layers 405 are about 150 nm thick, and the second sputtering gas is substantially pure O 2 . In this embodiment, heat is applied at least intermittently between about 200°C and about 350°C during the formation of the first WO 3 layer 406, but is not heated or substantially not during the formation of the second WO 3 layer 405 heating. In this way, the first WO 3 layer is substantially polycrystalline, while the second WO 3 layer need not be. Referring again to FIG. 4B, as described above with respect to FIGS. 3B and 4A, the stacking is completed by the following operations: lithiating EC layers 406 and 405 to substantially or substantially satisfy the blind charge, depositing the CE layer 410, lithiating the CE layer To the faded state, additional lithium is added and the second TCO layer 412 is deposited to complete the layered stack 403. Similar thermochemical adjustments are performed on the layered stack 403 to provide a layered stack 407, a functional electrochromic device including an ion-conducting electrically insulating region 408a. Although not wishing to be bound by theory, in this example, the oxygen-rich layer 405 of Xianxin WO 3 mainly charges the source of the current driver material to form the interface region 408a. In this example, the entire oxygen-enriched WO 3 layer is depicted as converted to the 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 to form an interface region that functions as an IC layer. Referring now to FIG. 4C, in the third embodiment, the layered stack 409 includes an EC layer 406a (which has a graded composition of WO 3 and is formed as part of the stack 414c), where the graded composition includes varying content Oxygen. In a non-limiting example, there is a higher oxygen concentration in the EC layer 406a at the interface of the EC-CE layer (410) than at the interface of the TCO layer 404 and the EC layer 406a. In one embodiment, the EC layer 406a is a layered composition WO 3 layer with a thickness of between about 500 nm and about 600 nm using a tungsten target and sputtering gas sputtering, wherein the sputtering gas is electroplated during sputtering The color change layer starts with about 40% and about 80% O 2 and between about 20% and about 60% Ar, and the sputtering gas includes about 70% and about 70% at the end of sputtering the electrochromic layer O 2 between 100% and Ar between 0% and about 30%, and wherein at least intermittently heat is applied to, for example, the substrate 402 to about 150°C and about 450°C during the beginning of the formation of the EC layer 406a Between, but not or substantially not applying heat during the deposition of at least a last portion of the EC layer 406a. In a more specific embodiment, the WO 3 layer of the graded composition is about 550 nm thick; the sputtering gas includes between about 50% and about 60% O 2 and 40% at the beginning of sputtering the electrochromic layer Between about 50% and Ar, and the sputtering gas is substantially pure O 2 at the end of sputtering the electrochromic layer; and wherein at least intermittently heat is applied to the beginning of the formation of the electrochromic layer to For example, the substrate 402 is between about 200°C and about 350°C, but no or substantially no heat is applied 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 gradually decreases to not apply heat when about half of the EC layer is deposited, while the sputtering gas composition is along the The substantially linear rate is adjusted from O 2 between about 50% and about 60% and Ar between about 40% and about 50% to substantially pure O 2 . More generally, the interface region usually (but not necessarily) has a heterostructure including at least two discrete components represented by different phases and/or compositions. In addition, the interface region may include gradients in these two or more discrete components, such as ion conductive materials and electrochromic materials (eg, a mixture of lithium tungstate and tungsten oxide). The gradient can provide, for example, variable composition, microstructure, resistivity, dopant concentration (eg, oxygen concentration), stoichiometry, density, and/or grain size range. The gradient can have many different forms of transition, including linear transition, S-type transition, Gaussian transition, and so on. In one example, the electrochromic layer includes a tungsten oxide region that transitions into a superstoichiometric tungsten oxide region. Part or all of the superstoichiometric oxide zone is converted into an interface zone. In the final structure, the tungsten oxide region is substantially polycrystalline, and the microstructure transitions to substantially amorphous at the interface region. In another example, the electrochromic layer includes a tungsten oxide region that transitions into (superstoichiometric) niobium oxide regions. Part or all of the niobium oxide region is converted into an interface region. In the final structure, the tungsten oxide region is substantially polycrystalline, and the microstructure transitions to substantially amorphous at the interface region. Referring again to FIG. 4C, as described above with respect to FIGS. 3B and 4A, the stacking is completed by the following operations: the lithiated EC layer 406a substantially or substantially meets the blind charge, deposits the CE layer 410, and the lithiated CE layer to a faded state 2. Add additional lithium and deposit the second TCO layer 412 to complete the layered stack 409. A similar multi-step thermochemical adjustment is performed on the layered stack 409 to provide at least a portion of the layered stack 411, including the ion-conducting electrically insulating region 408b, and the original layered EC layer 406a (which serves as an EC in the functional electrochromic device 411 Layer) functional electrochromic device. Although not wishing to be bound by theory, in this example, Xianxin, the uppermost oxygen-rich portion of the graded layer of WO 3 mainly forms a graded interface region 408b. Although not wishing to be bound by theory, there is a possibility that the formation of the interface region is limited by itself and depends on the relative amounts of oxygen, lithium, electrochromic materials, and/or counter electrode materials in the stack. In the various embodiments described herein, the electrochromic stack is described as not or substantially not heated during certain processing stages. In one embodiment, after the heating step, the stack is actively or passively cooled (eg, using heat sinks). The apparatus of the present invention includes active and passive cooling components. For example, active cooling may include a platen cooled by fluid circulation, cooling by exposure to cold (eg, by expanding) gas, a refrigeration unit, and the like. Passive cooling components may include heat sinks, such as metal blocks and the like, or only remove the substrate from heat exposure. Another aspect of the present invention is a method of manufacturing an electrochromic device, the method comprising: (a) forming an electrochromic layer including an electrochromic material or a counter electrode layer including a counter electrode material; (b) Forming an intermediate layer above the electrochromic layer or the counter electrode layer, wherein the intermediate layer includes an oxygen-rich form of at least one of the electrochromic material, the counter electrode material, and additional materials, wherein the additional materials Including different electrochromic materials or counter electrode materials, where the intermediate layer is not substantially electrically insulating; (c) forming the other of the electrochromic layer and the counter electrode layer; and (d ) Allows at least a portion of the intermediate layer to become substantially electrically insulating. In one embodiment, the electrochromic material is WO 3 . In another embodiment, (a) includes sputtering a WO using a tungsten target and a first sputtering gas including between about 40% and about 80% of O 2 and between about 20% and about 60% of Ar 3 to achieve a thickness between about 350 nm and about 450 nm, and at least intermittently heated to between about 150°C and about 450°C during the formation of the electrochromic layer. In another embodiment, (b) includes the use of a tungsten target without heating and second sputtering including between about 70% and 100% of O 2 and between 0% and about 30% of Ar The gas sputters WO 3 to achieve a thickness between about 100 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 one embodiment, the counter electrode layer includes NiWO with a thickness between about 150 nm and about 300 nm. In another embodiment, lithium is sputtered onto the counter electrode layer until the counter electrode layer fades. In another embodiment, an additional amount of lithium between about 5% and about 15% based on the amount required to discolor the counter electrode layer is sputtered onto the counter electrode layer. In another embodiment, a transparent conductive oxide layer is deposited over the counter electrode layer. In one embodiment, the transparent conductive oxide includes 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 heated under Ar at between about 150°C and about 450°C for between about 10 minutes and about 30 minutes, and then heated under O 2 for about 1 Between about 15 minutes and about 15 minutes, and then heated in the air between about 250°C and about 350°C for between about 20 minutes and about 40 minutes. In another embodiment, (a) includes a sputtered MO x first electrochromic material, where M is a metallic or non-metallic element, and x indicates the stoichiometric oxygen to M ratio, and (b) includes The second electrochromic material of sputtered NO y is used as an intermediate layer, where N is the same or different metal or non-metal element, and y indicates the ratio of superstoichiometric oxygen to N. In one embodiment, M is tungsten and N is tungsten. In another embodiment, M is tungsten, and N is selected from the group consisting of niobium, silicon, tantalum, titanium, zirconium, and cerium. Another embodiment of the present invention is an electrochromic device, including: (a) an electrochromic layer including an electrochromic material; (b) an opposing electrode layer including an opposing electrode material; and (c) in An interface region between the electrochromic layer and the counter electrode layer, wherein the interface region includes at least one of an electrically insulating ion conductive material and the electrochromic material, the counter electrode material, and additional materials, wherein the The additional materials include different electrochromic materials or counter electrode materials. In one embodiment, at least one of the electrically insulating ion conductive material and the electrochromic material, the counter electrode material, and the additional material is substantially evenly distributed within the interface area. 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 includes a composition gradient in a direction perpendicular to the layers. In another embodiment, consistent with any of the two previous embodiments, the electrically insulating ion conductive material includes lithium tungstate, the electrochromic material includes tungsten oxide, and the counter electrode material includes nickel tungsten oxide . In one specific implementation of the foregoing embodiment, no additional material is present. In one embodiment, the thickness of the electrochromic layer is between about 300 nm and about 500 nm, the thickness of the interface region is between about 10 nm and about 150 nm, and the thickness of the counter electrode layer is about Between 150 nm and about 300 nm. In another embodiment, the thickness of the electrochromic layer is between about 400 nm and about 500 nm; the thickness of the interface region is between about 20 nm and about 100 nm, and the thickness of the counter electrode layer is between Between about 150 nm and about 250 nm. In yet another embodiment, the thickness of the electrochromic layer is between about 400 nm and about 450 nm; the thickness of the interface region is between about 30 nm and about 50 nm, and the thickness of the counter electrode layer is between Between about 200 nm and about 250 nm. Another embodiment is a method of manufacturing an electrochromic device, the method comprising: by using a sputtering gas containing between about 40% and about 80% of O 2 and between about 20% and about 60% of Ar Sputtering a tungsten target to produce WO 3 to a thickness between about 500 nm and about 600 nm to deposit an electrochromic layer, wherein the substrate on which the WO 3 is deposited is at least intermittently during the formation of the electrochromic layer Heated to between about 150°C and about 450°C; sputtering lithium onto the electrochromic layer until the blind charge is satisfied; depositing an opposing electrode layer on the electrochromic layer without first An ion-conducting electrically insulating layer is provided between the electrochromic layer and the counter electrode layer, wherein the counter electrode layer includes NiWO; sputtering lithium onto the counter electrode layer until the counter electrode layer substantially fades; And forming an interface region between the electrochromic layer and the counter electrode layer, wherein the interface region is substantially ion conductive and substantially electrically insulating. In one embodiment, forming the interface region includes the stack of MTCCs alone or together with the substrate, conductive layer, and/or encapsulation layer. The electrochromic device of the present invention may include one or more additional layers (not shown) such as one or more passive layers (for example) to improve specific optical properties (provide moisture resistance or scratch resistance) in an airtight manner Seal the electrochromic device and the like. Usually (but not necessarily), a capping layer is deposited on the electrochromic stack. In some embodiments, the cap layer is SiAlO. In some embodiments, the cap layer is deposited by sputtering. In one embodiment, the thickness of the cover layer is between about 30 nm and about 100 nm. It should be understood from the above discussion that the electrochromic device of the present invention can be sputtered in a single chamber device (eg, with (for example) tungsten target, nickel target and lithium target, and oxygen and argon sputtering gas) Tool). As mentioned, due to the nature of the interface region formed to serve the purpose of a conventionally distinct IC layer, a separate target for sputtering the IC layer is not necessary. The inventor is particularly interested in, for example, manufacturing the electrochromic device of the present invention in a high-throughput manner. Therefore, there is a need for equipment that can sequentially manufacture the electrochromic device of the present invention when the substrate passes through an integrated deposition system. For example, the inventors are particularly interested in manufacturing electrochromic devices on windows, especially architectural glass slat windows (above). Therefore, another aspect of the present invention is an apparatus for manufacturing an electrochromic device, which includes: an integrated deposition system including: (i) a first deposition station containing a material source, which is configured to deposit including An electrochromic layer of electrochromic material; and (ii) a second deposition station configured to deposit a counter electrode layer including a counter electrode material; and a controller, which contains a substrate for sequentially on the substrate A deposition stack is used to transfer programming commands of 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 Either or both of the stage and the second deposition stage are also configured to deposit the intermediate layer over the electrochromic layer or the counter electrode layer, and wherein the intermediate layer includes the electrochromic material or the pair The oxygen-rich form of the electrode material, and wherein the first deposition stage and the second deposition stage are interconnected in series and are operable to transfer the substrate from one stage to the next stage without exposing the substrate to the external environment. In one embodiment, the apparatus of the present invention is operable to transfer the substrate from one stage to the next without breaking the vacuum, and may include operable to deposit lithium from a lithium-containing material source in the electrochromic device One or more lithiation stations on one or more layers. In one embodiment, the apparatus of the present invention is operable to deposit the electrochromic stack on a building glass substrate. In one embodiment, the apparatus is operable to transfer the substrate from one stage to the next without breaking the vacuum. In another embodiment, the integrated deposition system further includes one operable to deposit one of lithium from a lithium-containing material source on at least one of the electrochromic layer, the intermediate layer, and the counter electrode layer or Multiple lithium stations. 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 a substrate holder and a transport mechanism operable to hold the architectural glass substrate in a vertical orientation when passing the architectural glass substrate through the integrated deposition system. In another embodiment, the apparatus further includes one or more vacuum load locks 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 at least one of the one or more lithium deposition stations and the first deposition station and the second deposition station者 Isolated. In one embodiment, the integrated deposition system includes one or more heaters configured to heat the substrate. 5 depicts a simplified representation of an integrated deposition system 500 in a perspective view and includes a cross-sectional view of the interior in more detail. In this example, the system 500 is a module, wherein the inlet vacuum pre-evacuation chamber 502 and the outlet vacuum pre-evacuation chamber 504 are connected to the deposition module 506. There is an inlet port 510 for loading, for example, a building glass substrate 525 (the vacuum pre-extraction chamber 504 has a corresponding outlet port). The base plate 525 is supported by the pallet 520 traveling along the rail 515. In this example, the pallet 520 is supported by rails 515 via suspension, but the pallet 520 may also be supported on rails located near the bottom of the equipment 500 or (for example) between the rails between the top and bottom of the equipment 500 On top. The pallet 520 can be translated forward and/or backward in the system 500 (as indicated by the double-headed arrow). For example, during lithium deposition, the substrate may move forward and backward in front of the lithium target 530, thereby generating multiple passes to achieve the desired lithiation. However, this function is not limited to a lithium target, for example, a tungsten target can pass through a 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 pallet 520 and the substrate 525 are in a substantially vertical orientation. The substantially vertical orientation is not restrictive, but it can help prevent defects because particulate matter that may be generated, for example, from coalescence of atoms from the sputtering will tend to be subject to gravity and therefore will not be deposited on the substrate 525 . Also, because architectural glass substrates tend to be large, the vertical orientation of the substrate realizes the coating of thinner glass substrates as it traverses the stages of the integrated deposition system, which occurs because of the thicker hot glass There are fewer worries. Target 530 (a cylindrical target in this case) is oriented substantially parallel to and in front of the surface of the substrate on which deposition will occur (for convenience, other sputtering methods are not depicted here). The substrate 525 can translate through the target 530 during deposition, and/or the target 530 can move in front of the substrate 525. The moving path of the target 530 is not limited to translation along the path of the substrate 525. The target 530 can rotate along an axis passing through its length, translate along the path of the substrate (forward and/or backward), translate along the path perpendicular to the path of the substrate, circular in a plane parallel to the substrate 525 Path movement, etc. The target 530 need not be cylindrical, it can be flat or any shape required to deposit the desired layer with the desired properties. Also, there may be more than one target in each deposition station, 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 may be modules, but once connected, they form a continuous system in which a controlled ambient environment is established and maintained to process substrates at various stages within the system. A more detailed description of how to deposit the electrochromic material using the integrated deposition system 500 is described in the aforementioned US Non-Provisional Patent Application Nos. 12/645,111 and 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. These components are not shown, but can be understood by those skilled in the art. The system 500 is controlled by a computer system or other controller represented by an LCD and a keyboard 535 in FIG. 5, for example. Those of ordinary skill in the art will understand that embodiments of the present invention may use various processes involving data stored in or transmitted through one or more computer systems. Embodiments of the present invention also relate to equipment, computers and microcontrollers for performing these operations. Such equipment and processes can be used to deposit the electrochromic materials of the methods of the invention and equipment designed to implement such methods. The control device of the present invention may be specially constructed for the required purpose, or the control device may be a general-purpose computer that is selectively activated or reconfigured by computer programs and/or data structures stored in the computer. The programs presented in this article are not inherently related to any particular computer or other device. In particular, various general-purpose machines can be used with programs written according to the teachings herein, or it may be more convenient for constructing more specific devices to execute and/or control the required methods and procedures. As can be seen from the above description (especially FIGS. 3A to 3B), using the method of the present invention, we can not only manufacture electrochromic devices, but also pre-manufacture layered stacks (e.g., 400, 403, and 409). In this case, it can be converted into an electrochromic device via a subsequent process such as described herein. Although it is not a functional electrochromic device because there is no ion-conducting and electrically insulating region between the EC layer and the CE layer, these "electrochromic device precursors" may have special value. This is particularly the case where the device precursors are manufactured with high purity in an integrated processing facility as described herein, where the material layers are all deposited in a controlled ambient environment where, for example, the vacuum has never been destroyed. In this way, high-purity, low-defect materials are stacked and essentially "sealed" by the final TCO layer and/or cover layer, for example, before leaving the integrated system. Like the electrochromic device of the present invention described above, the electrochromic device precursor 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 resistance or scratch resistance) hermetically seal the device precursors and the like. In one embodiment, a cap layer is deposited on the TCO layer of the precursor stack. In some embodiments, the cap layer is SiAlO. In some embodiments, the cap layer is deposited by sputtering. In one embodiment, the thickness of the cover layer is between about 30 nm and about 100 nm. Subsequent processing of the top cover layer in place forms an IC layer without pollution from the environment, that is, with additional protection of the cover layer. The conversion to a functional electrochromic device can occur outside the integrated system if necessary. This is because the internal stack structure is protected from the external environment, and the slightly lower purity conditions are used to use the precursor Necessary for the final adjustment step of the conversion of the stack into a functional device. These stacked electrochromic device precursors can have advantages, for example, due to the longer lifetime of switching to electrochromic devices only when needed, by having (for example) storable and conversion parameters that depend on the final product The quality standards required and must be met to improve or feed to different conversion chambers and/or consumption points for flexibility resulting from a single precursor stack used for conversion. Again, these precursor stacks can be used for testing purposes, such as quality control or research efforts. Therefore, one embodiment of the present invention is a precursor of an electrochromic device, which includes: (a) a substrate; (b) a first transparent conductive oxide layer on the substrate; (c) the first transparent conductive oxide A stack on a layer, the stack including: (i) an electrochromic layer including an electrochromic material, and (ii) an opposite electrode layer including an opposite electrode material; wherein the stack does not include a layer between the electrochromic layer A region of ion conduction and electrical insulation between the counter electrode layer; and (d) a second transparent conductive oxide layer above the stack. In one embodiment, the electrochromic layer includes tungsten oxide, and the counter electrode layer includes nickel tungsten oxide. In one embodiment, at least one of the stack and the electrochromic layer contains lithium. In another embodiment, the electrochromic layer is tungsten oxide having a superstoichiometric oxygen content at least at the interface with the counter electrode layer. In another embodiment, the stack includes an IC precursor layer between the counter electrode layer and the electrochromic layer, the IC precursor layer includes an oxygen content that has a higher oxygen content than the electrochromic layer Oxygen tungsten oxide. In one embodiment, in the absence of an IC 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 Between about 150 nm and about 300 nm. In another embodiment, where there is an IC precursor layer 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 IC precursor layer is between Between about 20 nm and about 100 nm, and the thickness of the counter electrode layer is between about 150 nm and about 300 nm. In one embodiment, the prior-displacement devices described herein are exposed to heat to convert the devices into functional electrochromic devices. In one embodiment, the heating is part of MTCC. Another embodiment is an electrochromic device, which includes: (a) an electrochromic layer including an electrochromic material; and (b) an opposite electrode layer including an opposite electrode material, wherein the device is not contained in the The electrically insulating ion conducting material between the electrochromic layer and the counter electrode is composed of a homogeneous layer. In one embodiment, the electrochromic material is tungsten oxide, the counter electrode material is nickel tungsten oxide, and between the electrochromic layer and the counter electrode layer are lithium tungstate and tungsten oxide And the interface region of the mixture of at least one of nickel tungsten oxide. In another embodiment, the thickness of the electrochromic layer is between about 300 nm and about 500 nm; the thickness of the interface region is between about 10 nm and about 150 nm, and the thickness of the counter electrode layer is between Between about 150 nm and about 300 nm. Example FIG. 6 is a graph of a procedure flow used as a scheme for manufacturing the electrochromic device of the present invention. The y- axis unit is optical density, and the x- axis unit is time/program flow. In this example, an electrochromic device similar to the electrochromic device described with respect to FIG. 4A was fabricated, in which the substrate was a glass with fluorinated tin oxide as the first TCO, and the EC layer was one with excess oxygen in the matrix WO 3 (for example, using tungsten target sputtering, in which the sputtering gas is about 60% O 2 and about 40% Ar), the CE layer is formed on the EC layer and is made of NiWO, and the second TCO is Indium tin oxide (ITO). Lithium is used as an ion source for electrochromic transition. The optical density is used to determine the end point during the manufacture of the electrochromic device. From the origin of the graph, as the EC layer (WO 3 ) is deposited on the substrate (glass + TCO), the optical density is measured. The optical density of the glass substrate has a baseline optical density of about 0.07 (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 tungsten oxide layer about 550 nm thick, as described above, the optical density rises to about 0.2. After depositing the tungsten oxide EC layer, lithium is sputtered on the EC layer, as indicated by the first time period indicated by "Li". During this period, the optical density further increased to 0.4 along the curve, which indicates that the blind charge of tungsten oxide has been satisfied, because the tungsten oxide is colored with the addition of lithium. The time period indicated by "NiWO" indicates the deposition of the NiWO layer, and the optical density increases during this period, because NiWO is colored. Due to the addition of a NiWO layer about 230 nm thick, the optical density further increased from about 0.4 to about 0.9 during NiWO deposition. Note that as NiWO is deposited, some lithium can diffuse from the EC layer to the CE layer. This serves to maintain the optical density at a relatively low value during NiWO deposition or at least during the initial phase of deposition. The second time period indicated by "Li" indicates the addition of lithium to the NiWO EC layer. The optical density decreased from about 0.9 to about 0.4 during this stage, due to the discoloration of NiWO due to lithiation of NiWO. Lithization is performed until NiWO fades (including a local minimum of about 0.4 optical density). The optical density started to pick up at about 0.4, because the WO 3 layer was still lithiated and affected the optical density. Next, as indicated by the time period "Extra Li", extra lithium is sputtered onto the NiWO layer. In this example, about 10% of the extra lithium compared to the lithium added to the NiWO discolors the NiWO layer. During this stage, the optical density increases slightly. Next, add indium tin oxide TCO as indicated by "ITO" in the graph. Again, the optical density continued to rise slightly to about 0.6 during the formation of the indium tin oxide layer. Next, as indicated by the time period indicated by "MSTCC", the device was heated to about 250 °C under Ar for about 15 minutes, and then heated under O 2 for about 5 minutes. Next, the device was annealed in air at about 300°C for about 30 minutes. During this time, the optical density decreased to about 0.4. Therefore, the optical density is used for manufacturing the device of the present invention (for example, for determining the thickness of the layer based on the deposited material and morphology, and in particular for titrating lithium onto various layers to satisfy the blind charge and/or to achieve discoloration State) is a useful tool. Consistent with the scheme described with respect to FIG. 6, FIG. 7 shows a cross-sectional TEM of an electrochromic device 700 manufactured using the method of the present invention. The device 700 has a glass substrate 702 on which an electrochromic stack 714 is formed. The substrate 702 has an ITO layer 704 serving as a first TCO. The tungsten oxide EC layer 706 is deposited on the TCO 704. Layer 706 is formed with a thickness of about 550 nm (ie, WO 3 formed by sputtering tungsten with oxygen and argon), as described above with respect to FIG. 6. Add lithium to the EC layer. Next, a NiWO CE layer 710 about 230 nm thick is added, followed by lithium to discolor and then about 10% excess lithium. 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 FIG. 4A. After MSTCC, this TEM is performed. As seen, a new zone 708 of ion conduction and electrical insulation is formed. Figure 7 also shows five selected area electron diffraction (SAED) patterns for various layers. First, 704a indicates that the ITO layer is highly crystalline. Pattern 706a shows that the EC layer is polycrystalline. Pattern 708a shows that the IC layer is substantially amorphous. Pattern 710a shows that the CE layer is polycrystalline. Finally, pattern 712a shows that the indium tin oxide TCO layer is highly crystalline. 8 is a cross-section of the device 800 of the present invention analyzed by scanning transmission electron microscope (STEM). In this example, consistent with the solution described with respect to FIG. 4B, the device 800 is manufactured using the method of the present invention. The device 800 is an electrochromic stack formed on a glass substrate (not marked). On the glass substrate is a fluorinated tin oxide layer 804, which serves as the first TCO (for transparent electronic conductors, this layer is sometimes referred to as a "TEC" layer). The tungsten oxide EC layer 806 is deposited on the TCO 804. In this example, the layer 806 is formed with a thickness of about 400 nm (that is, WO 3 formed by sputtering tungsten using oxygen and argon, as described above with respect to FIG. 6), and then depositing the oxygen-rich precursor layer 805 to Thickness of about 150 nm. Add lithium to layer 805. Next, a NiWO CE layer 810 about 230 nm thick is added, followed by lithium to discolor and then about 10% excess lithium. Finally, an indium tin oxide layer 812 is deposited and the stack is subjected to multi-step thermochemical conditioning, as described above with respect to FIG. 4B. After MSTCC, perform this STEM. As seen, a new area 808 of ion-conducting electrical insulation is formed. The difference between this example and the embodiment described with respect to FIG. 4B is that, unlike the similar layer 405 in FIG. 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 serves as an ion conductive layer. 8B and 8C show a "front-to-back" comparison of the device 800 of the present invention (FIG. 8C) and the device precursor (FIG. 8B) before 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 clear in FIG. 8C). Referring again to FIG. 8B, it appears that there is at least lithium concentrated at the interface between the oxygen-rich layer 805 and the CE layer 810 (approximately 10-15 nm thick region), as indicated by 808a. After MTCC (FIG. 8C), it is clear that the interface area 808 has been formed. Although the foregoing invention has been described in some detail to promote understanding, the described embodiments should be considered illustrative rather than restrictive. It will be obvious to those familiar with this technology in general, within the scope of additional patent applications, specific changes and modifications can be practiced.

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(IC)層110‧‧‧對向電極(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WO3 層406‧‧‧EC層406a‧‧‧EC層407‧‧‧分層堆疊408‧‧‧IC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100‧‧‧Electrochromic device 102‧‧‧Substrate 104‧‧‧Conductive layer (CL) 106‧‧‧Electrochromic (EC) layer 108‧‧‧Ion conductive (IC) layer 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 WO 3 layer 406‧‧‧EC layer 406a‧‧‧EC layer 407‧‧ ‧Layered stack 408‧‧‧IC layer/interface area 408a‧‧‧Ion conductive electrical insulation area/interface area 408b‧‧‧ hierarchical interface area 409‧‧‧layer structure 410‧‧‧CE layer 411‧‧‧ points Layer stack/functional electrochromic device 412‧‧‧Second TCO layer 414a‧‧‧Stack 414b‧‧‧Stack 414c‧‧‧Stack 500‧‧‧Integrated deposition system 502‧‧‧Inlet vacuum pre-extraction chamber 504 ‧‧‧Exhaust vacuum pre-exhaust chamber 506‧‧‧Deposition module 510‧‧‧ Entry port 515‧‧‧Orbit 520‧‧‧pallet 525‧‧‧Substrate 530‧‧‧Lithium target 535‧‧‧LCD And keyboard 700‧‧‧Electrochromic device 702‧‧‧glass substrate 704‧‧‧indium tin oxide (ITO) layer 704a‧‧‧pattern 706‧‧‧tungsten oxide EC layer 706a‧‧‧pattern 708‧‧‧ 708a‧‧‧pattern 710‧‧‧CE layer 710a‧‧‧pattern 712‧‧‧indium tin oxide layer 712a‧‧‧pattern 714‧‧‧electrochromic stack 800‧‧‧device 804‧‧‧fluorinated Tin oxide layer 805‧‧‧Oxygen-rich precursor layer 806‧‧‧Tungsten oxide EC layer 808‧‧‧New area/interface area 808a‧‧‧Li 810‧‧‧CE layer 812‧‧‧Indium tin oxide layer

圖1A為描繪電致變色裝置堆疊之習知形成之示意性橫截面。 圖1B為展示習知電致變色堆疊中之EC層、IC層及CE層之組成之曲線圖。 圖2A至圖2C為展示用於本發明之電致變色裝置之代表性組份組合物之曲線圖。 圖3A及圖3B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為展示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8A至圖8C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。FIG. 1A is a schematic cross-section depicting a conventional formation of electrochromic device stacks. FIG. 1B is a graph showing the composition of the EC layer, IC layer, and CE layer in a conventional electrochromic stack. 2A to 2C are graphs showing representative component compositions used in the electrochromic device of the present invention. 3A and 3B are the program flow according to the embodiment of the invention. 4A to 4C are schematic cross sections depicting the formation of an electrochromic device according to certain embodiments of the present invention. Figure 5 depicts the integrated deposition system of the present invention in a perspective view. 6 is a graph showing how program parameters and end point readings are related during the formation of an electrochromic stack according to an embodiment of the invention. 7 and 8A to 8C are actual cross-sections of an electrochromic device manufactured using a method according to an embodiment of the present invention.

320‧‧‧程序流程 320‧‧‧Procedure flow

Claims (18)

一種電致變色裝置,其包含:(a)包含電致變色材料之電致變色層;及(b)包含對向電極材料之對向電極層,其中該對向電極材料可經受電致變色過渡(electrochromic transition);其中該裝置不含有在該電致變色層與該對向電極之間的電絕緣離子傳導材料之組成上均質之層。 An electrochromic device, comprising: (a) an electrochromic layer including an electrochromic material; and (b) an opposite electrode layer including an opposite electrode material, wherein the opposite electrode material can undergo an electrochromic transition (electrochromic transition); wherein the device does not contain a homogeneous layer on the composition of the electrically insulating ion conducting material between the electrochromic layer and the counter electrode. 如請求項1之電致變色裝置,其中該電致變色材料包含氧化鎢,該對向電極材料包含氧化鎳鎢,且在該電致變色層與該對向電極層之間者為包含下列各者之混合物之界面區:(i)鎢酸鋰及/或氧化鋰與(ii)氧化鎢及氧化鎳鎢中之至少一者。 The electrochromic device according to claim 1, wherein the electrochromic material includes tungsten oxide, the counter electrode material includes nickel tungsten oxide, and the one between the electrochromic layer and the counter electrode layer includes the following The interface area of the mixture of: (i) lithium tungstate and/or lithium oxide and (ii) at least one of tungsten oxide and nickel tungsten oxide. 如請求項2之電致變色裝置,其中該電致變色層之厚度在約300nm與約500nm之間;該界面區之厚度在約10nm與約150nm之間,且該對向電極層之厚度在約150nm與約300nm之間。 The electrochromic device according to claim 2, wherein the thickness of the electrochromic layer is between about 300 nm and about 500 nm; the thickness of the interface region is between about 10 nm and about 150 nm, and the thickness of the counter electrode layer is between Between about 150nm and about 300nm. 如請求項1之電致變色裝置,其中該電致變色裝置係完全無機的。 The electrochromic device according to claim 1, wherein the electrochromic device is completely inorganic. 一種電致變色裝置前驅物,其包含:(a)基板;(b)該基板上之第一透明導電氧化物層; (c)該第一透明導電氧化物層上之堆疊,該堆疊包含:(i)包含電致變色材料之電致變色層;(ii)包含對向電極材料之對向電極層,其中該對向電極材料可經受電致變色過渡;其中該堆疊不包含在該電致變色層與該對向電極層之間的離子傳導且電絕緣之區;及(d)在該堆疊之頂部之第二透明導電氧化物層。 A precursor of an electrochromic device, comprising: (a) a substrate; (b) a first transparent conductive oxide layer on the substrate; (c) a stack on the first transparent conductive oxide layer, the stack including: (i) an electrochromic layer including an electrochromic material; (ii) an opposing electrode layer including an opposing electrode material, wherein the pair The electrode material can undergo an electrochromic transition; wherein the stack does not contain a region of ion conduction and electrical insulation between the electrochromic layer and the counter electrode layer; and (d) the second on top of the stack Transparent conductive oxide layer. 如請求項5之電致變色裝置前驅物,其中該電致變色層包含氧化鎢,且該對向電極層包含氧化鎳鎢。 The electrochromic device precursor of claim 5, wherein the electrochromic layer includes tungsten oxide, and the counter electrode layer includes nickel tungsten oxide. 如請求項6之電致變色裝置前驅物,其中該電致變色層及該對向電極層中之至少一者含有鋰。 The electrochromic device precursor of claim 6, wherein at least one of the electrochromic layer and the counter electrode layer contains lithium. 如請求項7之電致變色裝置前驅物,其中該電致變色層包含至少在與該對向電極層之界面處具有超化學計量之含氧量。 The electrochromic device precursor according to claim 7, wherein the electrochromic layer contains an oxygen content having a superstoichiometric amount at least at the interface with the counter electrode layer. 如請求項7之電致變色裝置前驅物,其中該電致變色層之厚度在約500nm與約600nm之間,且該對向電極層之厚度在約150nm與約300nm之間。 The electrochromic device precursor of claim 7, wherein the thickness of the electrochromic layer is between about 500 nm and about 600 nm, and the thickness of the counter electrode layer is between about 150 nm and about 300 nm. 如請求項5之電致變色裝置前驅物,其中該電致變色裝置前驅物係完全無機的。 The electrochromic device precursor according to claim 5, wherein the electrochromic device precursor is completely inorganic. 一種用於製造電致變色裝置之設備,其包含:整合式沈積系統,其包含:(i)含有材料源之第一沈積台,其經配置以沈積包括電致變色材料之電致變色層;(ii)第二沈積台,其經配置以沈積包括對向電極材料之對向電極層,其中該對向電極材料可經受電致變色過渡;及(iii)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,該堆疊包含夾在該電致變色層與該對向電極層之間的中間層;該中間層不為實質上電絕緣的;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配置以在該電致變色層或該對向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對向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。 An apparatus for manufacturing an electrochromic device, comprising: an integrated deposition system, comprising: (i) a first deposition station containing a material source, which is configured to deposit an electrochromic layer including electrochromic materials; (ii) a second deposition station configured to deposit a counter electrode layer including a counter electrode material, wherein the counter electrode material can withstand electrochromic transitions; and (iii) a controller, which contains The programming instructions of the substrate passing through the first deposition table and the second deposition table are sequentially deposited on the substrate in a stacked manner. The stack includes an intermediate layer sandwiched between the electrochromic layer and the counter electrode layer; the The intermediate layer is not substantially electrically insulating; wherein either or both of the first deposition table and the second deposition table are also configured to deposit the intermediate layer over the electrochromic layer or the counter electrode layer , And wherein the intermediate layer includes the electrochromic material or the oxygen-rich form of the counter electrode material, 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 next stage without exposing the substrate to the external environment. 如請求項11之設備,其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。 As in the equipment of claim 11, it is operable to transfer the substrate from one stage to the next without breaking the vacuum. 如請求項12之設備,其中該整合式沈積系統進一步包含可操作以在該電致變色層、該中間層及該對向電極層中之至少一者上沈積來自含鋰材料源之鋰之一或多鋰化台。 The apparatus of claim 12, wherein the integrated deposition system further includes one operable to deposit one of lithium from a lithium-containing material source on at least one of the electrochromic layer, the intermediate layer, and the counter electrode layer Or more lithium stations. 如請求項13之設備,其中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。 The apparatus of claim 13, wherein the integrated deposition system is operable to deposit the stack on a building glass substrate. 如請求項14之設備,其中該整合式沈積系統進一步包含可操作以在使該建築玻璃基板通過該整合式沈積系統時將該建築玻璃基板固持在實質上垂直之定向上之基板固持器及輸送機構。 The apparatus of claim 14, wherein the integrated deposition system further includes a substrate holder and transport operable to hold the architectural glass substrate in a substantially vertical orientation when passing the architectural glass substrate through the integrated deposition system mechanism. 如請求項15之設備,其進一步包含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)。 The apparatus of claim 15, further comprising one or more vacuum pre-exhaust chambers (load locks) for transferring the substrate between the external environment and the integrated deposition system. 如請求項16之設備,其中該整合式沈積系統包含經配置以加熱該基板之一或多個加熱器及經配置而以主動或被動方式冷卻該基板之一或多個冷卻組件。 The apparatus of claim 16, wherein the integrated deposition system includes one or more heaters configured to heat the substrate and one or more cooling components configured to cool the substrate in an active or passive manner. 如請求項11之設備,其中該電致變色裝置係完全無機的。The device of claim 11, wherein the electrochromic device is completely inorganic.
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