TWI417410B - A manufacturing method of electric conduction film - Google Patents

A manufacturing method of electric conduction film Download PDF

Info

Publication number
TWI417410B
TWI417410B TW100123337A TW100123337A TWI417410B TW I417410 B TWI417410 B TW I417410B TW 100123337 A TW100123337 A TW 100123337A TW 100123337 A TW100123337 A TW 100123337A TW I417410 B TWI417410 B TW I417410B
Authority
TW
Taiwan
Prior art keywords
conductive film
target
aluminum
zinc oxide
zinc
Prior art date
Application number
TW100123337A
Other languages
Chinese (zh)
Other versions
TW201303061A (en
Inventor
Yu Zen Tsai
Na Fu Wang
Chien Hsien Yang
Original Assignee
Univ Cheng Shiu
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Univ Cheng Shiu filed Critical Univ Cheng Shiu
Priority to TW100123337A priority Critical patent/TWI417410B/en
Publication of TW201303061A publication Critical patent/TW201303061A/en
Application granted granted Critical
Publication of TWI417410B publication Critical patent/TWI417410B/en

Links

Description

導電薄膜製作方法Conductive film manufacturing method

本發明係關於一種導電薄膜製作方法,特別是一種具有高載子遷移率而可提高電導率及透光度之導電薄膜製作方法。The present invention relates to a method for fabricating a conductive film, and more particularly to a method for fabricating a conductive film having high carrier mobility and improved electrical conductivity and transmittance.

由於氧化鋅具有寬能隙的特性,能夠於可見光範圍具有較高穿透率,因此近幾年來,以氧化鋅作為透明導電薄膜廣泛應用於光電半導體產業,如平面顯示器、太陽能電池等相關領域。Since zinc oxide has a wide energy gap and can have a high transmittance in the visible light range, in recent years, zinc oxide has been widely used as a transparent conductive film in an optoelectronic semiconductor industry, such as a flat panel display, a solar cell, and the like.

然該氧化鋅薄膜之電阻率通常介於1至100歐姆之間,故多數業者為求提高該氧化鋅導電薄膜的導電性,通常係於該氧化鋅薄膜中另摻雜有其他金屬(如鋁、鎵或銦等),以期望降低該氧化鋅導電薄膜之電阻率,而可以在不影響該氧化鋅導電薄膜光學特性之情況下,達到增強該氧化鋅導電薄膜導電性之目的。However, the resistivity of the zinc oxide film is usually between 1 and 100 ohms. Therefore, in order to improve the conductivity of the zinc oxide conductive film, most of the zinc oxide film is usually doped with other metals (such as aluminum). , gallium or indium, etc., in order to reduce the resistivity of the zinc oxide conductive film, and to enhance the conductivity of the zinc oxide conductive film without affecting the optical properties of the zinc oxide conductive film.

傳統上多以陽離子摻雜於該氧化鋅導電薄膜中,然由半導體物理概念得知,由-1價之陰離子取代-2價之氧離子,同樣可以提高氧化鋅導電薄膜的導電性,尤其係以離子半徑與氧離子相似之氟離子摻雜最受矚目。以往多用化學噴霧法沉積摻雜有氟之氧化鋅薄膜,然所獲得之導電薄膜係存在有導電性不足之困擾,故陸續有研究使用真空電弧電漿蒸鍍、磁控共濺鍍法等,以期望成長具有高品質及較佳導電性的氧化鋅導電薄膜。Traditionally, cations are mostly doped in the zinc oxide conductive film. However, it is known from the semiconductor physical concept that the substitution of a -1 valence anion with a -2 valent oxygen ion can also improve the conductivity of the zinc oxide conductive film, especially Fluoride ion doping with ionic radii similar to oxygen ions is most noticeable. In the past, chemical vapor deposition was used to deposit a film of fluorine-doped zinc oxide. However, the conductive film obtained has the problem of insufficient conductivity. Therefore, vacuum arc plasma evaporation and magnetron sputtering have been studied. It is desired to grow a zinc oxide conductive film having high quality and excellent conductivity.

如Choi等人於2005年所發表之研究指出,利用磁控共濺鍍法,以摻有鋁之氧化鋅靶材與摻有氟之氧化鋅靶材進行共濺鍍,在基板上成形共摻有鋁及氟的一氧化鋅導電薄膜,且於10-6 托耳之高真空環境下,經300℃退火2小時後,該共摻有鋁及氟之氧化鋅導電薄膜係可以具有較低的電阻率,證實氟摻雜可以增強摻鋁氧化鋅導電薄膜之導電性。For example, the research published by Choi et al. in 2005 pointed out that co-sputtering with aluminum-doped zinc oxide target and fluorine-doped zinc oxide target by magnetron co-sputtering method is used to form co-doped on the substrate. A zinc oxide conductive film having aluminum and fluorine, and after being annealed at 300 ° C for 2 hours in a high vacuum environment of 10 -6 Torr, the zinc oxide conductive film co-doped with aluminum and fluorine may have a lower The resistivity confirms that fluorine doping can enhance the conductivity of the aluminum-doped zinc oxide conductive film.

然而,以上述摻有氟之氧化鋅靶材進行共濺鍍時,必須於含氟之氧化鋅靶材燒結之前,便決定其中的氟摻雜量,以致於進行共濺鍍的過程,無法依需求改變該氟離子於基板的沉積濃度,往往必須重新燒結一個新的靶材,才能製備出摻雜有不同氟離子含量之氧化鋅導電薄膜,故上述研究所揭露之手段係無法透過氟離子的沉積濃度變化,而徹底達到改變該氧化鋅導電薄膜之電阻率,以具有較佳導電性之功效。However, when the above-mentioned fluorine-doped zinc oxide target is used for co-sputtering, the fluorine doping amount must be determined before the fluorine-containing zinc oxide target is sintered, so that the process of co-sputtering cannot be performed. The demand changes the deposition concentration of the fluoride ion on the substrate, and it is often necessary to re-sinter a new target to prepare a zinc oxide conductive film doped with different fluoride ion content. Therefore, the method disclosed in the above research is not capable of transmitting fluorine ions. The deposition concentration is changed, and the resistivity of the zinc oxide conductive film is completely changed to have a better conductivity.

再者,由於鋁摻雜主要是取代鋅原子,然而鋁離子半徑和鋅離子半徑差異較大,因此鋁摻雜雖可提高載子濃度,但卻容易使晶格變形,造成載子在移動時發生散射,導致載子遷移率降低;相反地,氟原子摻雜主要是取代氧原子,然而氟離子半徑和氧離子半徑差異不大,因此氟摻雜除可提高載子濃度之外,相較鋁摻雜亦可有效提高載子遷移率。由於濺鍍過程中氟容易自基板上薄膜表面溢散而被抽氣系統抽除,導致該含氟靶材之氟含量無法充份沉積於該基板表面,使得該氧化鋅導電薄膜內所摻雜之氟含量不足;故上述研究所揭露之手段僅能透過鋁摻雜,而提高該氧化鋅導電薄膜內的載子濃度,無法有效利用氟摻雜的優勢。Furthermore, since aluminum doping mainly replaces zinc atoms, the difference between aluminum ion radius and zinc ion radius is large, so aluminum doping can increase the carrier concentration, but it is easy to deform the crystal lattice, causing the carrier to move. Scattering occurs, resulting in a decrease in carrier mobility; conversely, fluorine atom doping is mainly to replace the oxygen atom, but the difference between the fluoride ion radius and the oxygen ion radius is not large, so the fluorine doping can increase the carrier concentration, Aluminum doping can also effectively improve carrier mobility. Since the fluorine is easily removed from the surface of the film on the substrate during the sputtering process, the fluorine content of the fluorine-containing target is not sufficiently deposited on the surface of the substrate, so that the zinc oxide conductive film is doped. The fluorine content is insufficient; therefore, the method disclosed in the above research can only increase the carrier concentration in the zinc oxide conductive film by doping with aluminum, and cannot effectively utilize the advantage of fluorine doping.

有鑑於此,確實有必要發展一種導電薄膜製作方法,以期望解決如上所述之問題,而獲得具有較佳透光度及導電性的導電薄膜。In view of the above, it is indeed necessary to develop a method of fabricating a conductive film in order to solve the above problems and obtain a conductive film having better light transmittance and conductivity.

本發明之主要目的乃改良上述缺點,以提供一種導電薄膜製作方法,其係能夠任意調配摻雜於該導電薄膜中的氟含量,以提升該導電薄膜的載子遷移率而降低其電阻率。The main object of the present invention is to improve the above disadvantages to provide a method for fabricating a conductive film which is capable of arbitrarily adjusting the fluorine content doped in the conductive film to increase the carrier mobility of the conductive film and reduce its resistivity.

本發明之次一目的係提供一種導電薄膜製作方法,係能夠以鋁摻雜穩定該導電薄膜的載子濃度,以維持該導電薄膜之透光度,且同時提升其導電性。A second object of the present invention is to provide a method for fabricating a conductive film which is capable of stabilizing the carrier concentration of the conductive film with aluminum doping to maintain the transmittance of the conductive film while improving its conductivity.

為達到前述發明目的,本發明之導電薄膜製作方法,係包含:一電漿生成步驟,於一真空腔室內通入一電漿生成氣體,使該電漿生成氣體於該真空腔室內解離,而形成富含高能離子之電漿態;及一轟擊步驟,係以該電漿態中的高能離子,同時轟擊一摻鋁之氧化鋅靶材及一氟化鋅靶材,使得該二靶材中的鋁原子、氟原子、鋅原子及氧原子同時受濺射溢出靶材表面,以共同沉積於一基板,而獲得共摻有鋁及氟的一氧化鋅導電薄膜;其中,係以一擋板控制該氟化鋅靶材受轟擊後,該氟原子濺射溢出而沉積至該基板之含量。In order to achieve the above object, the method for fabricating an electroconductive film of the present invention comprises: a plasma generating step, wherein a plasma is generated in a vacuum chamber to generate a gas, and the plasma generating gas is dissociated in the vacuum chamber, and Forming a plasma state rich in high-energy ions; and a bombardment step, in which high-energy ions in the plasma state are simultaneously bombarded with an aluminum-doped zinc oxide target and a zinc fluoride target, so that the two targets are The aluminum atom, the fluorine atom, the zinc atom and the oxygen atom are simultaneously sputtered onto the surface of the target to be co-deposited on a substrate, thereby obtaining a zinc oxide conductive film co-doped with aluminum and fluorine; wherein, a baffle is used After controlling the bombardment of the zinc fluoride target, the fluorine atoms are sputtered and deposited to the content of the substrate.

本發明之導電薄膜製作方法還可以於該轟擊步驟後另操作一後處理步驟,係將該共摻有鋁及氟的氧化鋅導電薄膜,進行熱退火處理,使得該氧化鋅導電薄膜的晶格重新排列,其中該熱退火處理之溫度為400~600℃。The conductive film manufacturing method of the present invention may further operate a post-processing step after the bombarding step, wherein the zinc oxide conductive film doped with aluminum and fluorine is subjected to thermal annealing treatment to make the crystal lattice of the zinc oxide conductive film. Rearranged, wherein the temperature of the thermal annealing treatment is 400 to 600 °C.

再且,於本發明之導電薄膜製作過程中,係將該摻鋁的氧化鋅靶材係置於一直流濺鍍鎗,且於該直流濺鍍鎗內通入5~30瓦之直流功率,另將該氟化鋅靶材係置於一射頻濺鍍鎗,且於該射頻濺鍍鎗通入50~150瓦之射頻功率。Moreover, in the manufacturing process of the conductive film of the present invention, the aluminum-doped zinc oxide target is placed in a continuous sputtering gun, and a DC power of 5 to 30 watts is applied to the DC sputtering gun. In addition, the zinc fluoride target is placed in an RF sputtering gun, and the RF sputtering gun is supplied with an RF power of 50 to 150 watts.

為讓本發明之上述及其他目的、特徵及優點能更明顯易懂,下文特舉本發明之較佳實施例,並配合所附圖式,作詳細說明如下:請參照第1圖所示,其係一反應式磁控共濺鍍機台1,該反應式磁控共濺鍍機台1係於一腔室10內設有二濺鍍鎗11、12,且該二濺鍍鎗11、12各位於陰極處,以供給其一濺鍍鎗11適當之直流功率,及供給另一濺鍍鎗12適當之射頻功率,且於該陽極處另設有一基板13,用以沉積本發明之導電薄膜。其中,該反應式磁控共濺鍍機台1之設計,係為所屬技術領域具有通常知識者可輕易思及,且非本發明欲強調之特徵,此處僅為初略說明,以供於下詳述本發明之導電薄膜製作方法的步驟之用,故不加以贅述,更不以此機台為限。The above and other objects, features, and advantages of the present invention will become more apparent from the aspects of the appended claims. It is a reactive magnetron co-sputtering machine 1 , which is provided with a double sputter gun 11 , 12 in a chamber 10 , and the double sputter gun 11 12 are each located at the cathode to supply a suitable DC power of a sputtering gun 11 and an appropriate RF power to another sputtering gun 12, and a substrate 13 is additionally provided at the anode for depositing the conductive material of the present invention. film. The design of the reactive magnetron co-sputtering machine 1 is easily understood by those skilled in the art and is not intended to be emphasized by the present invention. The steps of the method for fabricating the conductive film of the present invention are described in detail below, and thus are not described again, and are not limited to this machine.

請參照第1及2圖所示,其為本發明一較佳實施例,以上述反應式磁控共濺鍍機台1進行操作,該導電薄膜製作方法係包含一電漿生成步驟S1及一轟擊步驟S2。Referring to FIGS. 1 and 2, which is a preferred embodiment of the present invention, the reactive magnetron sputtering apparatus 1 is operated. The conductive film manufacturing method includes a plasma generating step S1 and a Bombardment step S2.

該電漿生成步驟S1係於一真空腔室10內通入一電漿生成氣體,使該電漿生成氣體於該真空腔室10內解離,而形成富含高能離子之電漿態。更詳言之,係以一幫浦14對該腔室10抽氣,使得該腔室10形成真空狀態,以確保該腔室10內不存在有任何外界之氣體,形成該真空腔室10後通入該電漿生成氣體G(如第3a圖所示),再緩慢提升該二濺鍍鎗11、12的直流及射頻功率,以於該真空腔室10內產生反應所需之電場,透過游離電子撞擊該電漿生成氣體,以破壞該電漿生成氣體原子或分子間的鍵結,而解離形成電漿態。其中,該幫浦14係可以選擇機械幫浦或冷凝幫浦,且該電漿生成氣體G可以為氬氣、氮氣、氫氣或氧氣等。The plasma generating step S1 is to pass a plasma generating gas into a vacuum chamber 10 to dissociate the plasma generating gas in the vacuum chamber 10 to form a plasma state rich in high energy ions. More specifically, the chamber 10 is evacuated by a pump 14, so that the chamber 10 is in a vacuum state to ensure that there is no external gas in the chamber 10, and the vacuum chamber 10 is formed. Passing the plasma generating gas G (as shown in FIG. 3a), and slowly increasing the DC and RF power of the two sputtering guns 11, 12 to generate an electric field required for the reaction in the vacuum chamber 10, Free electrons impinge on the plasma generating gas to destroy the plasma to form gas atoms or intermolecular bonds, and dissociate to form a plasma state. Wherein, the pump 14 system can select a mechanical pump or a condensing pump, and the plasma generating gas G can be argon gas, nitrogen gas, hydrogen gas or oxygen gas.

舉例而言,本發明係先以該幫浦14抽氣至該腔室10之壓力為2×10-6 托耳,確保該腔室10係為絕對真空狀態後,通入氧氣混摻氬氣,且以流量控制器15限定其氧氣流量分率為10~20%,使得該真空腔室10內的壓力值維持5×10-3 托耳之工作壓力,以維持較佳的電漿生成率;再於該二濺鍍鎗11、12之電極間各別輸入5~30瓦之直流功率及50~150瓦之射頻功率,使得該真空腔室10內可以產生適當的電場,以由該電場所產生的高能游離電子撞擊該氬氣,而破壞該氬氣的分子鍵結而形成電漿態。本實施例較佳之直流功率係為10瓦,且較佳之射頻功率係為90瓦,藉此產生較適當的電漿生成電場,且可以於後續該轟擊步驟S2時,達到較佳的靶材轟擊效果。For example, in the present invention, the pump 14 is first evacuated to the chamber 10 at a pressure of 2×10 -6 Torr, ensuring that the chamber 10 is in an absolute vacuum state, and oxygen is mixed with argon gas. And the flow controller 15 defines the oxygen flow rate of 10-20%, so that the pressure value in the vacuum chamber 10 maintains a working pressure of 5×10 −3 Torr to maintain a better plasma generation rate. And then inputting 5 to 30 watts of DC power and 50 to 150 watts of RF power between the electrodes of the two sputtering guns 11, 12, so that an appropriate electric field can be generated in the vacuum chamber 10 to The high-energy free electrons generated by the site impinge on the argon gas, and the molecular bonds of the argon gas are broken to form a plasma state. The preferred DC power of the embodiment is 10 watts, and the preferred RF power is 90 watts, thereby generating a more suitable plasma generating electric field, and achieving better target bombardment in the subsequent bombardment step S2. effect.

請再配合3b及3c圖所示,該轟擊步驟S2係以該電漿態中的高能離子G,同時轟擊一摻鋁之氧化鋅靶材T1及一氟化鋅靶材T2,使得該二靶材中的鋁原子A、氟原子F、鋅原子及氧原子同時受濺射溢出靶材表面,以共同沉積於一基板13,而獲得共摻有鋁及氟的一氧化鋅導電薄膜M。其中,係以一擋板121控制該氟化鋅靶材T2受轟擊後,該氟原子F濺射溢出而沉積至該基板13之含量。更詳言之,為提升傳統氧化鋅導電薄膜的導電率,且同時維持該氧化鋅導電薄膜的透明度,本發明係選擇以該摻鋁的氧化鋅靶材T1及氟化鋅靶材T2進行共濺鍍,以將該摻鋁的氧化鋅靶材T1置於該直流濺鍍鎗11,且將該氟化鋅靶材T2置於該射頻濺鍍鎗12,藉此避免通入直流電源產生電漿高能離子G轟擊該氟化鋅靶材T2時,產生正電荷累積於該氟化鋅靶材T2所衍生的問題;再且,本發明以氟化鋅作為其一濺鍍靶材T2時,係可以隨意改變該氟化鋅靶材T2受轟擊,而沉積於該基板13上的氟含量,以藉由該氟離子與氧離子相接近之離子半徑,取代該氧化鋅導電薄膜中的氧;更可以透過摻有鋁之氧化鋅靶材T1,同時於該基板13上沉積鋁離子,以穩定該氧化鋅導電薄膜的氟摻雜濃度,達到提升載子遷移率而增加薄膜導電率之功效。 Please cooperate with the 3b and 3c diagrams, the bombardment step S2 is to bombard an aluminum-doped zinc oxide target T1 and a zinc fluoride target T2 by the high-energy ion G in the plasma state, so that the two targets are The aluminum atom A, the fluorine atom F, the zinc atom and the oxygen atom in the material are simultaneously sputtered over the surface of the target to be deposited on a substrate 13 to obtain a zinc oxide conductive film M doped with aluminum and fluorine. Wherein, after a baffle 121 controls the zinc fluoride target T2 to be bombarded, the fluorine atom F is sputtered and deposited to the content of the substrate 13. More specifically, in order to improve the conductivity of the conventional zinc oxide conductive film while maintaining the transparency of the zinc oxide conductive film, the present invention selects the aluminum-doped zinc oxide target T1 and the zinc fluoride target T2. Sputtering, placing the aluminum-doped zinc oxide target T1 on the DC sputtering gun 11, and placing the zinc fluoride target T2 on the RF sputtering gun 12, thereby avoiding the power generation by the DC power source When the high-energy ion G bombards the zinc fluoride target T2, a problem arises in that a positive charge is accumulated in the zinc fluoride target T2; further, when the present invention uses zinc fluoride as a sputtering target T2, The fluorine content of the zinc fluoride target T2 can be arbitrarily changed, and the fluorine content deposited on the substrate 13 is substituted for the oxygen in the zinc oxide conductive film by the ionic radius of the fluoride ion and the oxygen ion; Further, the aluminum-doped zinc oxide target T1 can be used to deposit aluminum ions on the substrate 13 to stabilize the fluorine doping concentration of the zinc oxide conductive film, thereby improving the carrier mobility and increasing the film conductivity.

舉例而言,本發明係於工作壓力為5×10-3托耳之真空腔室10內置入該基板13,使得該基板13位於陽極處,且以該檔板121限制該氟化鋅靶材T2之氟離子F受濺射溢出,而沉積於該基板13之含量,本實施例係控制該氟化鋅靶材T2的檔板121開啟時間,係佔該導電薄膜總製程時間的25%、50%、75%及100%。以於該些時間內,透過該電漿所生成之高能離子G同時轟擊該摻鋁之氧化鋅靶材 T1及氟化鋅靶材T2,使得該高能離子G之能量可以傳遞至該二靶材T1、T2表面,以自該二靶材T1、T2表面各濺射出該鋁原子A、氟原子F、鋅原子及氧原子而沉積於該基板13上,而能夠獲得不同鋁及氟含量共摻之氧化鋅導電薄膜。其中,該摻鋁之氧化鋅靶材T1及氟化鋅靶材T2的純度皆為99.99%,且該二靶材T1、T2的直徑皆為3吋,而可以自該二靶材T1、T2獲得品質較佳的氧化鋅導電薄膜;該基板13係可以選擇為玻璃基板,且控制該基板13之溫度維持於150~250℃,藉以增加該鋁、氟、鋅及氧原子或鋁、氟鋅及氧離子沉積於該基板13的均勻度。 For example, the present invention is built into the substrate 13 at a working pressure of 5×10 −3 Torr, such that the substrate 13 is located at the anode, and the zinc fluoride target is restricted by the baffle 121 The fluoride ion F of T2 is spattered by sputtering, and is deposited on the substrate 13. The present embodiment controls the opening time of the baffle 121 of the zinc fluoride target T2, which accounts for 25% of the total process time of the conductive film. 50%, 75% and 100%. During the time, the high-energy ion G generated by the plasma simultaneously bombards the aluminum-doped zinc oxide target T1 and the zinc fluoride target T2, so that the energy of the high-energy ion G can be transmitted to the two targets. The surface of T1 and T2 is deposited on the substrate 13 by sputtering the aluminum atom A, the fluorine atom F, the zinc atom and the oxygen atom from the surfaces of the two targets T1 and T2, thereby obtaining different aluminum and fluorine content co-doping. Zinc oxide conductive film. The purity of the aluminum-doped zinc oxide target T1 and the zinc fluoride target T2 is 99.99%, and the diameters of the two targets T1 and T2 are both 3吋, and the two targets T1 and T2 can be used. Obtaining a zinc oxide conductive film with better quality; the substrate 13 can be selected as a glass substrate, and the temperature of the substrate 13 is controlled to be maintained at 150-250 ° C, thereby increasing the aluminum, fluorine, zinc and oxygen atoms or aluminum, fluorine zinc And the uniformity of oxygen ions deposited on the substrate 13.

此外,請參照第4圖所示,於該轟擊步驟S2後還可以另操作一後處理步驟S3,該後處理步驟S3係將該共摻有鋁及氟的氧化鋅導電薄膜,進行熱退火處理,使得該氧化鋅導電薄膜的晶格重新排列。更詳言之,係於該真空腔室10內抽氣至壓力為1×10-3托耳,升高該真空腔室10之溫度為400~600℃,本實施例較佳係控制該真空腔室10之溫度為500℃,以對該共摻有鋁及氟的氧化鋅導電薄膜進行熱退火處理,且以每秒升溫6℃之速率,持續退火時間為10~20分鐘。藉此,係可以改變該共摻有鋁及氟的氧化鋅導電薄膜之光電特性,以獲得具有較佳透光度及導電性的氧化鋅導電薄膜。 In addition, as shown in FIG. 4, after the bombardment step S2, a post-processing step S3 may be further performed, and the post-processing step S3 is performed by thermally annealing the zinc oxide conductive film doped with aluminum and fluorine. The lattice of the zinc oxide conductive film is rearranged. More specifically, the vacuum chamber 10 is evacuated to a pressure of 1×10 -3 Torr, and the temperature of the vacuum chamber 10 is raised to 400-600 ° C. This embodiment preferably controls the vacuum. The temperature of the chamber 10 is 500 ° C, and the zinc oxide conductive film doped with aluminum and fluorine is thermally annealed, and the annealing time is 10 to 20 minutes at a rate of 6 ° C per second. Thereby, the photoelectric characteristics of the zinc oxide conductive film doped with aluminum and fluorine can be changed to obtain a zinc oxide conductive film having better transmittance and conductivity.

再且,請再參照第4圖所示,本發明亦可以於該電漿生成步驟S1之前另操作一前置步驟S01,該前置步驟S01係洗去該基板13表面之附著物。更詳言之,本實施例係將該基板13浸於丙酮中,進行超音波震動5~10分鐘,以完成第一次清洗;接著,再將該基板13置於甲醇溶液中,以重複超音波震動5~10分鐘,以完成第二次清洗;最後,再將該基板13移至去離子水中,進行第三次的超音波震盪5~10分鐘,於此徹底去除附著於該基板13表面之髒汙、灰塵或油漬等,再以高壓氮氣烘乾,放置於120℃之精密烤箱烘烤1小時,以去除該基板13表面之水氣,藉此維持該基板13表面所生成之氧化鋅導電薄膜的品質。甚至,於該電漿生成步驟S1中還可以透過預濺鍍之手段,以去除該二靶材T1、T2上的污染源,達到穩定後續鍍膜製程之較佳功效。Further, referring to FIG. 4 again, the present invention may further operate a pre-step S01 before the plasma generating step S1. The pre-step S01 washes off the deposit on the surface of the substrate 13. More specifically, in this embodiment, the substrate 13 is immersed in acetone, subjected to ultrasonic vibration for 5 to 10 minutes to complete the first cleaning; then, the substrate 13 is placed in a methanol solution to repeat the super The sound wave is shaken for 5~10 minutes to complete the second cleaning; finally, the substrate 13 is moved to the deionized water for the third ultrasonic shock for 5-10 minutes, thereby completely removing the surface attached to the substrate 13 Dirty, dust or oil stains, etc., and then dried under high pressure nitrogen, and placed in a precision oven at 120 ° C for 1 hour to remove moisture on the surface of the substrate 13, thereby maintaining the zinc oxide formed on the surface of the substrate 13. The quality of the conductive film. Even in the plasma generating step S1, the pre-sputtering means can be used to remove the pollution source on the two targets T1 and T2 to achieve a better effect of stabilizing the subsequent coating process.

經由上述得知,本發明之導電薄膜製作方法,不僅可以透過該摻鋁的氧化鋅靶材T1濺射出鋁原子或鋁離子,更可以藉由該氟化鋅靶材T2濺射出足量的氟原子或氟離子,而形成共摻有鋁及氟之氧化鋅導電薄膜;由於氟離子半徑和氧離子半徑差異不大,因此藉由充分的氟摻雜,除了可提高載子濃度之外,並可提升載子遷移率。根據霍爾效應量測原理得知,該電阻率係與載子遷移率及載子濃度的乘積呈現負相關,故本發明於電子濃度維持穩定之情況下,係能夠經由該載子遷移率的提升,降低該共摻有鋁及氟之氧化鋅導電薄膜的電阻率,以於不改變該氧化鋅導電薄膜透光度的同時,達到提升該氧化鋅導電薄膜導電率之功效。甚至,本發明係可以隨意改變該氟化鋅靶材濺射至該基板表面的氟含量,不須重新製作新的含氟靶材,便可以調整於該氧化鋅導電薄膜中的較佳氟含量,以方便取得共摻鋁及氟的較佳比例,而省去含氟靶材再次購買或製備所需耗費的時間及成本。According to the above, the conductive film manufacturing method of the present invention can not only sputter aluminum atoms or aluminum ions through the aluminum-doped zinc oxide target T1, but also can sputter a sufficient amount of fluorine by the zinc fluoride target T2. Atom or fluoride ion, forming a zinc oxide conductive film co-doped with aluminum and fluorine; since the difference between the radius of the fluoride ion and the radius of the oxygen ion is small, by sufficiently doping with fluorine, in addition to increasing the concentration of the carrier, Can improve carrier mobility. According to the Hall effect measurement principle, the resistivity system has a negative correlation with the product of the carrier mobility and the carrier concentration. Therefore, in the case where the electron concentration is maintained stable, the present invention is capable of mobility through the carrier. The electrical resistivity of the zinc oxide conductive film doped with aluminum and fluorine is increased to improve the conductivity of the zinc oxide conductive film without changing the transmittance of the zinc oxide conductive film. In addition, the present invention can arbitrarily change the fluorine content of the zinc fluoride target sputtered onto the surface of the substrate, and can adjust the preferred fluorine content in the zinc oxide conductive film without re-making a new fluorine-containing target. In order to facilitate the better ratio of co-doped aluminum and fluorine, the time and cost required for the fluorine target to be purchased or prepared again is omitted.

為證實本發明之導電薄膜可以透過摻鋁之氧化鋅靶材與氟化鋅靶材共濺鍍之方法,而於該基板上沉積出共摻有鋁及氟的氧化鋅導電薄膜,且本發明之導電薄膜係具有較佳的導電性及光穿透效率。於此,係針對沉積有不同濃度氟原子之氧化鋅導電薄膜進行分析,以獲得載子濃度、載子遷移率、電阻率及光穿透率之量測數值,結果詳見於第5及8圖。In order to confirm that the conductive film of the present invention can be co-sputtered through the aluminum-doped zinc oxide target and the zinc fluoride target, a zinc oxide conductive film co-doped with aluminum and fluorine is deposited on the substrate, and the present invention The conductive film has better conductivity and light penetration efficiency. Here, the zinc oxide conductive film deposited with different concentrations of fluorine atoms is analyzed to obtain the measured values of carrier concentration, carrier mobility, resistivity and light transmittance. The results are detailed in 5 and 8. Figure.

請參照第5圖所示,其係為本發明之導電薄膜載子濃度,與該氟化鋅靶材的擋板開啟時間百分比分析圖。其中,該氟化鋅靶材的擋板開啟時間百分比,可代表該氟化鋅靶材受該高能電漿離子轟擊後,該氟原子自該氟化鋅靶材濺射溢出而沉積於基板之含量。由第5圖的結果得知,不論該氟化鋅靶材的擋板開啟時間百分比為何,該共摻有鋁及氟之氧化鋅導電薄膜的載子濃度約於3.34×1020 /cm3 至3.62×1020 /cm3 之間,其顯示於該基板上的不同的氟原子沉積濃度,並不足以影響本發明導電薄膜的載子濃度。Please refer to FIG. 5 , which is a graph of the concentration of the conductive film carrier of the present invention and the percentage of the opening time of the baffle of the zinc fluoride target. The percentage of the baffle opening time of the zinc fluoride target may represent that after the bombardment of the zinc fluoride target by the high-energy plasma ion, the fluorine atom is sputtered from the zinc fluoride target and deposited on the substrate. content. From the results of FIG. 5, regardless of the percentage of the baffle opening time of the zinc fluoride target, the carrier concentration of the zinc oxide conductive film doped with aluminum and fluorine is about 3.34×10 20 /cm 3 . Between 3.62 × 10 20 /cm 3 , the different fluorine atom deposition concentrations shown on the substrate are not sufficient to affect the carrier concentration of the electroconductive thin film of the present invention.

請參照第6圖所示,其係為本發明之導電薄膜載子遷移率,與該氟化鋅靶材的擋板開啟時間百分比分析圖。其中,該氟化鋅靶材的擋板開啟時間百分比,即代表該氟化鋅靶材受該高能電漿離子轟擊後,該氟原子自該氟化鋅靶材濺射溢出而沉積於基板之含量。由第6圖的結果得知,未開啟該氟化鋅靶材的擋板時,其氧化鋅導電薄膜的載子遷移率僅為18.3cm2 /V-s,隨著該氟化鋅靶材的擋板開啟時間百分比增加,該共摻有鋁及氟的氧化鋅導電薄膜之載子遷移率明顯逐漸提升,且於該氟化鋅靶材的擋板開啟時間百分比達75%時,係可以獲得高達30.3 cm2 /V-s之載子遷移率。Please refer to FIG. 6 , which is a graph showing the mobility of the conductive film carrier of the present invention and the percentage of the opening time of the baffle of the zinc fluoride target. Wherein, the percentage of the baffle opening time of the zinc fluoride target, that is, after the zinc fluoride target is bombarded by the high-energy plasma ion, the fluorine atom is sputtered from the zinc fluoride target and deposited on the substrate. content. From the results of Fig. 6, it is known that when the baffle plate of the zinc fluoride target is not opened, the carrier mobility of the zinc oxide conductive film is only 18.3 cm 2 /Vs, with the blocking of the zinc fluoride target. The percentage of plate opening time increases, and the carrier mobility of the zinc oxide conductive film doped with aluminum and fluorine is gradually increased, and when the percentage of baffle opening time of the zinc fluoride target reaches 75%, the system can obtain up to Carrier mobility of 30.3 cm 2 /Vs.

請參照第7圖所示,其係為本發明之導電薄膜電阻率,與該氟化鋅靶材的擋板開啟時間百分比分析圖。其中,該氟化鋅靶材的擋板開啟時間百分比,即代表該氟化鋅靶材受該高能電漿離子轟擊後,該氟原子自該氟化鋅靶材濺射溢出而沉積於基板之含量。由第7圖的結果得知,未開啟該氟化鋅靶材的擋板時,其氧化鋅導電薄膜的電阻率僅為1.02×10-3 Ω-cm,隨著該氟化鋅靶材的擋板開啟時間百分比增加,該共摻有鋁及氟的氧化鋅導電薄膜之電阻率明顯逐漸降低,且於該氟化鋅靶材的擋板開啟時間百分比達75%時,係可以獲得低於5.69×10-4 Ω-cm之電阻率。Please refer to FIG. 7 , which is a graph of the resistivity of the conductive film of the present invention and the percentage of the baffle opening time of the zinc fluoride target. Wherein, the percentage of the baffle opening time of the zinc fluoride target, that is, after the zinc fluoride target is bombarded by the high-energy plasma ion, the fluorine atom is sputtered from the zinc fluoride target and deposited on the substrate. content. From the results of Fig. 7, it is known that when the baffle plate of the zinc fluoride target is not opened, the resistivity of the zinc oxide conductive film is only 1.02 × 10 -3 Ω-cm, along with the target of the zinc fluoride target. The percentage of the opening time of the baffle is increased, and the resistivity of the zinc oxide conductive film doped with aluminum and fluorine is gradually decreased gradually, and when the percentage of the baffle opening time of the zinc fluoride target is 75%, the lowering time can be obtained. 5.69 × 10 -4 Ω-cm resistivity.

藉此顯示,根據霍爾效應量測原理得知,該電阻率係與載子遷移率及載子濃度的乘積呈現負相關之情況下,證實本發明共摻有鋁及氟之氧化鋅導電薄膜,係可以透過氟原子的摻雜提升該導電薄膜之載子遷移率,且配合鋁原子的摻雜穩定該導電薄膜之載子濃度,以此降低該導電薄膜之電阻率,達到有效提升該導電薄膜導電率之功效。According to the Hall effect measurement principle, it is confirmed that the resistivity system has a negative correlation with the product of the carrier mobility and the carrier concentration, and it is confirmed that the present invention is co-doped with the zinc oxide conductive film of aluminum and fluorine. The carrier mobility of the conductive film can be improved by doping with fluorine atoms, and the carrier concentration of the conductive film is stabilized by doping with aluminum atoms, thereby reducing the resistivity of the conductive film, thereby effectively improving the conductivity. The effect of film conductivity.

請參照第8圖所示,其係為本發明之導電薄膜光穿透率,與該氟化鋅靶材的擋板開啟時間百分比分析圖。其中,該氟化鋅靶材的擋板開啟時間百分比,即代表該氟化鋅靶材受該高能電漿離子轟擊後,該氟原子自該氟化鋅靶材濺射溢出而沉積於基板之含量。由第8圖的結果得知,不論該氟化鋅靶材的擋板開啟時間百分比為何,於該光波長為360奈米時,皆呈現有明顯的吸收邊界,且該吸收邊界處的能量係與氟化鋅3.3 eV之能隙相近似,故本發明之導電薄膜的吸收邊界係為氧化鋅直接能隙吸收所造成之結果。再且,於光波長為300~900奈米處,不論該氟化鋅靶材的擋板開啟時間百分比為何,其平均光穿透率均維持於93%以上,藉此證實該共摻有鋁及氟之氧化鋅導電薄膜係具有較佳的光穿透效率。Please refer to FIG. 8 , which is a graph showing the light transmittance of the conductive film of the present invention and the percentage of the shutter opening time of the zinc fluoride target. Wherein, the percentage of the baffle opening time of the zinc fluoride target, that is, after the zinc fluoride target is bombarded by the high-energy plasma ion, the fluorine atom is sputtered from the zinc fluoride target and deposited on the substrate. content. From the results of Fig. 8, it is known that regardless of the percentage of the baffle opening time of the zinc fluoride target, when the wavelength of the light is 360 nm, there is a significant absorption boundary, and the energy system at the absorption boundary Similar to the energy gap of 3.3 eV of zinc fluoride, the absorption boundary of the conductive film of the present invention is the result of direct absorption of zinc oxide. Moreover, at a wavelength of 300 to 900 nm, regardless of the percentage of the baffle opening time of the zinc fluoride target, the average light transmittance is maintained above 93%, thereby confirming that the co-doped aluminum And the fluorine zinc oxide conductive film has better light penetration efficiency.

本發明之導電薄膜製作方法,其係能夠任意調配摻雜於該導電薄膜中的氟含量,以提升該導電薄膜的載子遷移率,達到降低該導電薄膜電阻率之功效。The method for preparing a conductive film of the present invention is capable of arbitrarily adjusting the fluorine content doped in the conductive film to improve the carrier mobility of the conductive film and to reduce the resistivity of the conductive film.

本發明之導電薄膜製作方法,係能夠以鋁摻雜穩定該導電薄膜的載子濃度,以維持該導電薄膜之透光度,且同時達到提升其導電性之功效。The method for fabricating the conductive film of the present invention is capable of stabilizing the carrier concentration of the conductive film with aluminum doping to maintain the transmittance of the conductive film and at the same time achieving the effect of improving the conductivity thereof.

雖然本發明已利用上述較佳實施例揭示,然其並非用以限定本發明,任何熟習此技藝者在不脫離本發明之精神和範圍之內,相對上述實施例進行各種更動與修改仍屬本發明所保護之技術範疇,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。While the invention has been described in connection with the preferred embodiments described above, it is not intended to limit the scope of the invention. The technical scope of the invention is protected, and therefore the scope of the invention is defined by the scope of the appended claims.

[本發明][this invention]

S1...電漿生成步驟S1. . . Plasma generation step

S2...轟擊步驟S2. . . Bombardment step

S3...後處理步驟S3. . . Post processing step

S01...前置步驟S01. . . Pre-step

1...直流反應式磁控共濺鍍機台1. . . DC reactive magnetron co-sputtering machine

10...腔室10. . . Chamber

11...濺鍍鎗11. . . Sputter gun

111...擋板111. . . Baffle

12...濺鍍鎗12. . . Sputter gun

121...擋板121. . . Baffle

13...基板13. . . Substrate

14...幫浦14. . . Pump

15...流量控制器15. . . Flow controller

T1...摻鋁之氧化鋅靶材T1. . . Aluminum-doped zinc oxide target

T2...氟化鋅靶材T2. . . Zinc fluoride target

G...電漿生成氣體/電漿態高能粒子G. . . Plasma generated gas/plasma high energy particles

A...鋁原子A. . . Aluminum atom

F...氟原子F. . . Fluorine atom

M...導電薄膜M. . . Conductive film

第1圖:本發明使用之直流反應式磁控共濺鍍機台示意圖。Figure 1: Schematic diagram of a DC reactive magnetron co-sputtering machine used in the present invention.

第2圖:本發明之操作流程圖。Figure 2: Flow chart of the operation of the present invention.

第3a-3c圖:本發明之操作流程示意圖。3a-3c: Schematic diagram of the operational flow of the present invention.

第4圖:本發明之操作流程圖又一。Fig. 4 is a flow chart showing the operation of the present invention.

第5圖:本發明之導電薄膜載子濃度分析圖。Fig. 5 is a graph showing the concentration analysis of the conductive film carrier of the present invention.

第6圖:本發明之導電薄膜載子遷移率分析圖。Fig. 6 is a graph showing the mobility analysis of the conductive film of the present invention.

第7圖:本發明之導電薄膜電阻率分析圖。Figure 7 is a graph showing the electrical resistivity analysis of the conductive film of the present invention.

第8圖:本發明之導電薄膜透光率分析圖。Fig. 8 is a graph showing the transmittance of a conductive film of the present invention.

S1...電漿生成步驟S1. . . Plasma generation step

S2...轟擊步驟S2. . . Bombardment step

Claims (10)

一種導電薄膜製作方法,係包含:一電漿生成步驟,於一真空腔室內通入一電漿生成氣體,使該電漿生成氣體於該真空腔室內解離,而形成富含高能離子之電漿態;及一轟擊步驟,係以該電漿態中的高能離子,同時轟擊一摻鋁之氧化鋅靶材及一氟化鋅靶材,使得該二靶材中的鋁原子A、氟原子F、鋅原子及氧原子同時受濺射溢出靶材表面,以共同沉積於一基板,而獲得共摻有鋁及氟的一氧化鋅導電薄膜;其中,係以一擋板控制該氟化鋅靶材受轟擊後,該氟原子濺射溢出而沉積至該基板之含量。A method for fabricating a conductive film, comprising: a plasma generating step, introducing a plasma into a vacuum chamber to generate a gas, dissolving the plasma generating gas in the vacuum chamber, and forming a plasma rich in high energy ions And a bombardment step, in which the high-energy ions in the plasma state are simultaneously bombarded with an aluminum-doped zinc oxide target and a zinc fluoride target, such that the aluminum atom A and the fluorine atom F in the two targets The zinc atom and the oxygen atom are simultaneously sputtered onto the surface of the target to be co-deposited on a substrate to obtain a zinc oxide conductive film co-doped with aluminum and fluorine; wherein the zinc fluoride target is controlled by a baffle After the material is bombarded, the fluorine atoms are sputtered and deposited to the content of the substrate. 依申請專利範圍第1項所述之導電薄膜製作方法,於該轟擊步驟後另操作一後處理步驟,係將該共摻有鋁及氟的氧化鋅導電薄膜,進行熱退火處理,使得該氧化鋅導電薄膜的晶格重新排列。According to the method for manufacturing a conductive film according to the first aspect of the patent application, after the bombardment step, a post-processing step is performed, and the zinc oxide conductive film doped with aluminum and fluorine is subjected to thermal annealing treatment to cause the oxidation. The lattice realignment of the zinc conductive film. 依申請專利範圍第2項所述之導電薄膜製作方法,其中該熱退火處理之溫度係為400~600℃。The method for producing a conductive film according to claim 2, wherein the temperature of the thermal annealing treatment is 400 to 600 °C. 依申請專利範圍第1或2項所述之導電薄膜製作方法,其中該摻鋁的氧化鋅靶材係置於一直流濺鍍鎗,且於該直流濺鍍鎗內通入5~30瓦之直流功率,該氟化鋅靶材係置於一射頻濺鍍鎗,且於該射頻濺鍍鎗通入50~150瓦之射頻功率。The method for producing a conductive film according to claim 1 or 2, wherein the aluminum-doped zinc oxide target is placed in a continuous sputtering gun, and 5 to 30 watts are introduced into the DC sputtering gun. For DC power, the zinc fluoride target is placed in an RF sputtering gun, and the RF sputtering gun is supplied with RF power of 50 to 150 watts. 依申請專利範圍第1或2項所述之導電薄膜製作方法,其中該摻鋁的氧化鋅靶材之純度為99.99%,且該摻鋁的氧化鋅靶材之直徑為3吋。The method for producing an electroconductive thin film according to claim 1 or 2, wherein the aluminum-doped zinc oxide target has a purity of 99.99%, and the aluminum-doped zinc oxide target has a diameter of 3 Å. 依申請專利範圍第1或2項所述之導電薄膜製作方法,其中該氟化鋅靶材之純度為99.99%,且該氟化鋅靶材之直徑為3吋。The method for producing a conductive film according to claim 1 or 2, wherein the zinc fluoride target has a purity of 99.99%, and the zinc fluoride target has a diameter of 3 Å. 依申請專利範圍第1或2項所述之導電薄膜製作方法,其中該真空腔室內的壓力值係為5×10-3 托耳。The method for producing an electroconductive film according to claim 1 or 2, wherein the pressure in the vacuum chamber is 5 × 10 -3 Torr. 依申請專利範圍第1或2項所述之導電薄膜製作方法,其中該基板之溫度維持於150~250℃。The method for producing a conductive film according to claim 1 or 2, wherein the temperature of the substrate is maintained at 150 to 250 °C. 依申請專利範圍第1或2項所述之導電薄膜製作方法,於該電漿生成步驟中另透過預濺鍍之手段,以去除靶材上的污染源且穩定後續之轟擊步驟。According to the method for manufacturing a conductive film according to claim 1 or 2, in the plasma generating step, a pre-sputtering method is further adopted to remove the pollution source on the target and stabilize the subsequent bombardment step. 依申請專利範圍第1或2項所述之導電薄膜製作方法,於該電漿生成步驟之前另操作一前置步驟,該前置步驟係洗去該基板表面之附著物。According to the method for producing a conductive film according to claim 1 or 2, before the plasma generating step, a pre-step is performed, which washes off the deposit on the surface of the substrate.
TW100123337A 2011-07-01 2011-07-01 A manufacturing method of electric conduction film TWI417410B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
TW100123337A TWI417410B (en) 2011-07-01 2011-07-01 A manufacturing method of electric conduction film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW100123337A TWI417410B (en) 2011-07-01 2011-07-01 A manufacturing method of electric conduction film

Publications (2)

Publication Number Publication Date
TW201303061A TW201303061A (en) 2013-01-16
TWI417410B true TWI417410B (en) 2013-12-01

Family

ID=48137948

Family Applications (1)

Application Number Title Priority Date Filing Date
TW100123337A TWI417410B (en) 2011-07-01 2011-07-01 A manufacturing method of electric conduction film

Country Status (1)

Country Link
TW (1) TWI417410B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115181944A (en) * 2022-06-28 2022-10-14 北京航空航天大学 Metal-doped fluorine-containing alumina-based target, transparent high-hydrophilicity film and preparation method

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009001835A (en) * 2007-06-19 2009-01-08 Sumitomo Bakelite Co Ltd Aluminum-added zinc oxide-based transparent conductive film
TW201025448A (en) * 2008-12-16 2010-07-01 Ind Tech Res Inst Transparent conductive films and fabrication methods thereof

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009001835A (en) * 2007-06-19 2009-01-08 Sumitomo Bakelite Co Ltd Aluminum-added zinc oxide-based transparent conductive film
TW201025448A (en) * 2008-12-16 2010-07-01 Ind Tech Res Inst Transparent conductive films and fabrication methods thereof

Also Published As

Publication number Publication date
TW201303061A (en) 2013-01-16

Similar Documents

Publication Publication Date Title
JP5005772B2 (en) Conductive laminate and manufacturing method thereof
Lu et al. Remote plasma sputtering deposited Nb-doped TiO2 with remarkable transparent conductivity
JP2004511655A (en) Preparation method of indium tin oxide thin film using magnetron negative ion sputtering source
US20120160663A1 (en) Sputter Deposition and Annealing of High Conductivity Transparent Oxides
Chan et al. The Effect of annealing on nanothick indium tin oxide transparent conductive films for touch sensors
CN109082631B (en) Ga2O3Transparent conductive film and preparation method thereof
Kiristi et al. Radio frequency-H2O plasma treatment on indium tin oxide films produced by electron beam and radio frequency magnetron sputtering methods
Mian et al. Improvement of the uniformity of structural and electrical properties of transparent conductive Al-doped ZnO thin films by inductively coupled plasma-assisted radio frequency magnetron sputtering
US8512860B2 (en) Housing and method for making the same
TWI417410B (en) A manufacturing method of electric conduction film
CN110331367B (en) Preparation method of stannous tungstate film
US8512859B2 (en) Housing and method for making the same
US8568907B2 (en) Housing and method for making the same
JP2012138228A (en) Transparent conductive thin film and method for manufacturing the same
JP4229803B2 (en) Method for producing transparent conductive film
JP2017193755A (en) Method of manufacturing transparent conductive film, and transparent conductive film
TWI433948B (en) A radio frequency plasma assisted pulsed laser deposition system and a method for preparing a thin film from its system
Wang et al. Influence of O2 flux on compositions and properties of ITO films deposited at room temperature by direct-current pulse magnetron sputtering
US8597782B2 (en) Housing and method for making the same
US8597804B2 (en) Housing and method for making the same
US8568905B2 (en) Housing and method for making the same
US8568906B2 (en) Housing and method for making the same
US8568904B2 (en) Housing and method for making the same
He et al. Properties of ITO thin films prepared by APS-assisted EB evaporation
CN111139439B (en) Method for preparing film on large-area substrate through magnetron sputtering