CN102386045A - Field emission cathode array with grid control function and manufacturing method thereof - Google Patents
Field emission cathode array with grid control function and manufacturing method thereof Download PDFInfo
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Abstract
本发明涉及一种带有栅控作用的场发射阴极阵列,其特征在于:在玻璃基板同一平面设置相互交替的阴极和栅极,栅极是由多列相互平行的栅极电极构成,栅极电极由纵向电极和数个横向带构成,阴极是由多列相互平行的条状阴极电极以及在各列条状阴极电极上交替设置电子发射层和介质层构成,栅极电极上的横向带与相邻的带有电子发射层的阴极电极平行相对。该带有栅控作用的场发射阴极阵列可以实现低压调控,降低场发射阴极阵列的开启电场,提高电子发射的均匀性和电子发射效率,而且结构简单、制造工艺容易、成本低廉、制造过程稳定可靠的优点。本发明还公开一种带有栅控作用的场发射阴极阵列的制造方法。
The invention relates to a field emission cathode array with a gate control function, which is characterized in that alternate cathodes and grids are arranged on the same plane of a glass substrate, the grid is composed of multiple columns of grid electrodes parallel to each other, and the grid The electrode is composed of a longitudinal electrode and several transverse strips. The cathode is composed of multiple rows of strip cathode electrodes parallel to each other and electron emission layers and dielectric layers are alternately arranged on each strip cathode electrode. Adjacent cathode electrodes with electron emission layers face each other in parallel. The field emission cathode array with gate control function can realize low-voltage control, reduce the open electric field of the field emission cathode array, improve the uniformity and efficiency of electron emission, and has simple structure, easy manufacturing process, low cost and stable manufacturing process Reliable advantages. The invention also discloses a manufacturing method of the field emission cathode array with gate control function.
Description
技术领域 technical field
本发明涉及真空微电子器件制造技术领域,特别是具有栅极调控的场发射阴极阵列装置及其制造方法。 The invention relates to the technical field of manufacturing vacuum microelectronic devices, in particular to a field emission cathode array device with gate regulation and a manufacturing method thereof.
the
背景技术 Background technique
场致发射显示器(Field Emission Display,FED)是一种新型的平板显示技术,它是阴极射线管(Cathode Ray Tube,CRT)技术的延伸,其工作原理是靠很强的外部电场来压抑物体表面的势垒,使势垒高度降低,宽度变窄,当势垒的宽度窄到可以同电子的波长相比拟时,电子通过隧道效应穿透势垒逸入真空而轰击阳极荧光粉发光。 Field Emission Display (Field Emission Display, FED) is a new type of flat panel display technology. It is an extension of Cathode Ray Tube (CRT) technology. Its working principle is to suppress the surface of objects by a strong external electric field. The potential barrier reduces the height of the potential barrier and narrows the width. When the width of the potential barrier is narrow enough to be comparable to the wavelength of electrons, the electrons penetrate the potential barrier through the tunnel effect and escape into the vacuum to bombard the anode phosphor to emit light.
场发射阴极阵列是场致发射显示器的核心,常用的阴极结构可分为二极式和三极式结构。二极式场发射阴极的制作工艺虽然简单,但阳极需要高压才能给电子足够能量轰击荧光粉实现高亮度,另一方面阳极电极又充当调制电极,连接驱动电路又需要低压调制,因此存在发光亮度和调制电压之间的不可调和的矛盾,必须在二极结构的基础上引入调制栅极,由栅极进行电压调制,由阳极控制亮度。三极式场发射阴极阵列按位置不同,可分为前栅型阴极结构、后栅型阴极结构和平面型阴极结构。前栅极结构的制作较为困难,制备需要3-5次掩膜工艺,而且在制作过程中场致发射源容易受到破坏,栅极由于加的正电压使得场发射电子可能打在栅极而被截获并且阴极发射对介质层厚度、调制极开口等参数都很敏感。后栅型结构是将栅极埋在阴极之下,解决了前栅结构的制作困难问题,但是该结构失去了栅极对阳极的屏蔽作用而使阴极容易受到离子轰击,且阳极电压不能太高,否则栅极调控作用减弱甚至蜕变为二极FED。前栅和后栅场致发射显示器都需要制作阴栅绝缘层,而大面积的绝缘层制作对工艺要求很高,且绝缘性能很难保证,故器件成本高,不易实现大面积显示。平面型结构是指其栅极和阴极处在同一个平面上,结构制作简单,成本低,极适合大面积制作和未来工业化生产。 The field emission cathode array is the core of the field emission display, and the commonly used cathode structures can be divided into two-pole and three-pole structures. Although the manufacturing process of the two-pole field emission cathode is simple, the anode needs high voltage to give electrons enough energy to bombard the phosphor to achieve high brightness. On the other hand, the anode electrode acts as a modulation electrode, and the connection to the driving circuit requires low-voltage modulation, so there is luminous brightness. The irreconcilable contradiction between the modulation voltage and the modulation voltage must introduce a modulation grid on the basis of the diode structure, the voltage is modulated by the grid, and the brightness is controlled by the anode. The three-pole field emission cathode array can be divided into front grid type cathode structure, rear grid type cathode structure and planar type cathode structure according to different positions. The fabrication of the front gate structure is relatively difficult, and requires 3-5 masking processes, and the field emission source is easily damaged during the fabrication process, and the field emission electrons may hit the gate due to the positive voltage applied to the gate and be destroyed. Both interception and cathode emission are sensitive to parameters such as dielectric layer thickness and modulator opening. The gate-back structure is to bury the gate under the cathode, which solves the difficulty of making the front gate structure, but this structure loses the shielding effect of the gate on the anode and makes the cathode vulnerable to ion bombardment, and the anode voltage cannot be too high , otherwise the gate control function is weakened or even transformed into a two-pole FED. Both front-gate and rear-gate field emission displays need to make a cathode-gate insulating layer, and the production of a large-area insulating layer requires high technology, and the insulating performance is difficult to guarantee, so the cost of the device is high, and it is difficult to realize large-area display. The planar structure means that the grid and cathode are on the same plane, the structure is simple to manufacture, and the cost is low, which is very suitable for large-area production and future industrial production.
平面型阴极结构中的阴极和栅极位于同一个平面,阴极和栅极之间由真空间隙隔开,采用传统的光刻技术能一次性在基板上完成阴极和栅极的制作。已知现有技术的平面型场发射阴极的立体图和结构示意图分别见附图1和附图2,平面型场发射阴极包括阴极基板200,设置在阴极基板200上的阴极210和栅极220,其中阴极210由阴极电极211和设置在阴极电极211上的电子发射层212所构成,其中阴极210和栅极220相互平行。但是,传统的平面型场发射阴极结构的开启电压高,要降低阵列的工作电压,必须要减少阴极210和栅极220之间的距离,增加了制作工艺的难度和成本;同时电子发射层212很难控制均匀分布在阴极电极211表面,从而影响场发射阴极阵列的电子发射均匀性。
In the planar cathode structure, the cathode and the grid are located on the same plane, and the cathode and the grid are separated by a vacuum gap. The cathode and the grid can be fabricated on the substrate at one time by using traditional photolithography technology. The perspective view and structural schematic view of the known prior art planar field emission cathode are shown in accompanying drawings 1 and 2 respectively. The planar field emission cathode comprises a
综上所述,有必要提供一种带栅控作用的新型场发射阵列,其阴极和栅极的制作工艺简单,电子发射层能均匀、图形化地沉积在阴极电极表面,栅极调控电压低、同时阴极电极表面的电子发射层在均匀的电场作用能实现均匀发射,有效地提高场发射阴极阵列的电子发射均匀性和电子发射效率。 In summary, it is necessary to provide a new type of field emission array with a gate control function. The fabrication process of the cathode and grid is simple, the electron emission layer can be uniformly and graphically deposited on the surface of the cathode electrode, and the gate control voltage is low. , At the same time, the electron emission layer on the surface of the cathode electrode can realize uniform emission under the action of a uniform electric field, effectively improving the electron emission uniformity and electron emission efficiency of the field emission cathode array.
发明内容 Contents of the invention
本发明的目的在于克服现有技术的不足,提供一种制造工艺简单且带有栅控作用的场发射阴极阵列及其制造方法,该场发射阵列阴极不仅可以实现栅极低压调控,电子发射均匀和效率高,而且制造工艺极其简单,易于实现大面积的具有栅极调控作用的场发射阴极阵列生产制造。 The purpose of the present invention is to overcome the deficiencies of the prior art and provide a field emission cathode array with a simple manufacturing process and a grid control function and its manufacturing method. The field emission array cathode can not only realize grid low voltage regulation, but also uniform electron emission And the efficiency is high, and the manufacturing process is extremely simple, and it is easy to realize the production and manufacture of a large-area field emission cathode array with a grid regulation function.
为实现上述目的,本发明的技术方案是: For realizing the above object, technical scheme of the present invention is:
一种带有栅控作用的场发射阴极阵列,包括玻璃基板,设置于玻璃基板上的阴极和栅极,其特征在于:所述的阴极和栅极设置在玻璃基板同一平面上,阴极是由多列相互平行的条状阴极电极以及在各列条状阴极电极上交替设置电子发射层和介质层构成,所述的介质层是等间距地设置在阴极电极上,所述的电子发射层是等间距地设置在未被介质层电所覆盖的阴极电极上,所述的栅极是由多列相互平行的栅极电极构成,所述各列的栅极电极由纵向电极和数个横向带构成,所述的栅极电极和阴极电极交替设置在玻璃基板上,所述的位于各列阴极电极的电子发射层与相邻栅极电极的横向带平行相对。 A field emission cathode array with a gate control function, comprising a glass substrate, a cathode and a grid arranged on the glass substrate, characterized in that: the cathode and the grid are arranged on the same plane of the glass substrate, and the cathode is made of Multiple rows of strip cathode electrodes parallel to each other and electron emission layers and dielectric layers are alternately arranged on each row of strip cathode electrodes, the dielectric layers are arranged on the cathode electrodes at equal intervals, and the electron emission layers are Arranged at equal intervals on the cathode electrodes that are not covered by the dielectric layer, the grid is composed of multiple columns of grid electrodes parallel to each other, and the grid electrodes of each column are composed of longitudinal electrodes and several transverse strips. The configuration is that the grid electrodes and cathode electrodes are arranged alternately on the glass substrate, and the electron emission layers located in each row of cathode electrodes are parallel to and opposite to the lateral strips of the adjacent grid electrodes.
优选的,每列栅极电极的横向带等间距对称地设置在栅极电极的纵向电极两侧,横向带垂直于纵向电极,横向带的宽度为1μm-1mm,横向带的长度为100μm-2mm,各列栅极电极上的相邻横向带之间的距离100μm-2mm。 Preferably, the horizontal strips of each row of grid electrodes are symmetrically arranged on both sides of the vertical electrodes of the grid electrodes at equal intervals, the horizontal strips are perpendicular to the longitudinal electrodes, the width of the horizontal strips is 1 μm-1 mm, and the length of the horizontal strips is 100 μm-2 mm , the distance between adjacent lateral strips on each column of gate electrodes is 100 μm-2 mm.
优选的,设置于阴极电极上的电子发射层的长度与相邻栅极电极的横向带的宽度一致,电子发射层与相邻栅极电极的横向带之间的距离为0.01μm-200μm。 Preferably, the length of the electron emission layer disposed on the cathode electrode is consistent with the width of the lateral strip of the adjacent gate electrode, and the distance between the electron emission layer and the transverse strip of the adjacent gate electrode is 0.01 μm-200 μm.
优选的,所述介质层是覆盖在阴极电极上的矩形状介质层,或是覆盖在阴极电极、玻璃基板和栅极电极的纵向电极上的条状介质层,介质层厚度为10nm-100nm,构成介质层材料包含SiO2、Ta2O5、AlN、Al2O3、Si3N4、BN、TiO2中的一种或者两种及其以上的组合。 Preferably, the dielectric layer is a rectangular dielectric layer covering the cathode electrode, or a strip dielectric layer covering the cathode electrode, the glass substrate and the longitudinal electrodes of the gate electrode, and the thickness of the dielectric layer is 10nm-100nm, The material constituting the dielectric layer includes one or a combination of two or more of SiO 2 , Ta 2 O 5 , AlN, Al 2 O 3 , Si 3 N 4 , BN, and TiO 2 .
优选的,所述电子发射层包含碳纳米管、氧化锌、氧化锡、氧化镁、氧化铋中的一种或者两种及其以上的组合。 Preferably, the electron emission layer contains one or a combination of two or more of carbon nanotubes, zinc oxide, tin oxide, magnesium oxide, and bismuth oxide.
优选的,电子发射层可以掺杂纳米银颗粒、纳米金颗粒、纳米铜颗粒、纳米锡颗粒、纳米氧化锌颗粒、纳米镍颗粒中的一种或者两种及其以上的组合,颗粒直径为0.1nm-10μm。 Preferably, the electron emission layer can be doped with one or a combination of two or more of nano-silver particles, nano-gold particles, nano-copper particles, nano-tin particles, nano-zinc oxide particles, and nano-nickel particles, and the particle diameter is 0.1 nm-10μm.
本发明还公开一种带有栅控作用的场发射阴极阵列的制造方法,其特征在于,包括以下步骤: The invention also discloses a method for manufacturing a field emission cathode array with gate control function, which is characterized in that it includes the following steps:
(1)对整个玻璃进行划片,清洗; (1) Scribing and cleaning the entire glass;
(2)在玻璃基板上采用镀膜、光刻或印刷、光刻、烧结的方法制备栅极和阴极电极; (2) Prepare the grid and cathode electrodes on the glass substrate by coating, photolithography or printing, photolithography, and sintering;
(3)在带有阴极电极和栅极的玻璃基板上采用光刻、镀膜、剥离技术制备介质层; (3) Prepare the dielectric layer on the glass substrate with cathode electrodes and grids by photolithography, coating, and lift-off techniques;
(4)在未被介质层所覆盖的阴极电极上采用电泳沉积、烧结或印刷、光刻、烧结或印刷、烧结制备表面具有场致电子发射性能的电子发射层。 (4) Electrophoretic deposition, sintering or printing, photolithography, sintering or printing and sintering are used to prepare an electron emission layer with field electron emission properties on the surface of the cathode electrode not covered by the dielectric layer.
优选的,在所述步骤(4)中的电泳沉积是采用栅极作为电泳阳极,采用阴极电极作为电泳阴极,通过改变电泳时电压来改变电场大小,使得电子发射层均匀地沉积在未被介质层所覆盖的阴极电极表面,从而形成图形化的电子发射层。 Preferably, the electrophoretic deposition in the step (4) uses the gate as the electrophoretic anode, and the cathode electrode as the electrophoretic cathode, and changes the electric field by changing the voltage during electrophoresis, so that the electron emission layer is uniformly deposited on the undisturbed medium Layer covered cathode electrode surface, thus forming a patterned electron emission layer.
本发明的有益效果是提供一种带栅控作用的场发射阴极阵列,该场发射阴极阵列的电子发射源能够均匀地实现图形化生长,且与栅极电极的横向带相互平行,有利于提高场发射阴极阵列的电子发射均匀性和电子发射效率;此外,该场发射阴极阵列采用普通的镀膜和光刻工艺就可以在基片上完成阴极电极和栅极的制作,采用电泳沉积、烧结或印刷、光刻、烧结或印刷、烧结就可以制备阵列电子发射层,其制造工艺简单,其大大降低了工艺的复杂性及难度,不仅易于生产而且制造成本低,极适合大面积制作和未来工业化生产,具有广阔的市场应用前景。 The beneficial effect of the present invention is to provide a field emission cathode array with a gate control function, the electron emission source of the field emission cathode array can realize patterned growth uniformly, and is parallel to the transverse strip of the gate electrode, which is beneficial to improve The electron emission uniformity and electron emission efficiency of the field emission cathode array; in addition, the field emission cathode array can complete the cathode electrode and grid on the substrate by using ordinary coating and photolithography processes, using electrophoretic deposition, sintering or printing , photolithography, sintering or printing, and sintering can prepare the array electron emission layer. The manufacturing process is simple, which greatly reduces the complexity and difficulty of the process. It is not only easy to produce but also low in manufacturing cost. It is very suitable for large-scale production and future industrial production. , has a broad market application prospect.
附图说明 Description of drawings
图1为现有技术的平面型结构的场发射阴极俯视图。 FIG. 1 is a top view of a field emission cathode with a planar structure in the prior art.
图2为现有技术的平面型结构的场发射阴极的剖面图。 Fig. 2 is a cross-sectional view of a field emission cathode with a planar structure in the prior art.
图3为本发明第一优选实施例的带有栅控作用的场发射阴极阵列的结构示意图。 Fig. 3 is a schematic structural diagram of a field emission cathode array with gate control function according to the first preferred embodiment of the present invention.
图4为本发明第一优选实施例的带有栅控作用的场发射阴极阵列的俯视图。 Fig. 4 is a top view of a field emission cathode array with gate control function according to the first preferred embodiment of the present invention.
图5为本发明第一优选实施例的制备电子发射层前的带有栅控作用的场发射阴极阵列结构的光学显微镜图。 Fig. 5 is an optical micrograph of the field emission cathode array structure with gate control function before the electron emission layer is prepared according to the first preferred embodiment of the present invention.
图6为本发明第一优选实施例的制备电子发射层的场发射阴极阵列的光学显微镜图。 Fig. 6 is an optical micrograph of the field emission cathode array for preparing the electron emission layer according to the first preferred embodiment of the present invention.
图7为本发明第一优选实施例的带有栅控作用的场发射阴极阵列与阳极荧光屏配合,在真空中场发射的阳极荧光屏发光图。 Fig. 7 is a luminescent diagram of the anode fluorescent screen emitting in a vacuum field by cooperating the field emission cathode array with grid control function and the anode fluorescent screen according to the first preferred embodiment of the present invention.
图8为本发明第二优选实施例的带有栅控作用的场发射阴极阵列的结构示意图。 FIG. 8 is a schematic structural diagram of a field emission cathode array with a gate control function according to a second preferred embodiment of the present invention.
图9为本发明第二优选实施例的带有栅控作用的场发射阴极阵列的俯视图。 FIG. 9 is a top view of a field emission cathode array with gate control function according to the second preferred embodiment of the present invention.
图10为本发明第二优选实施例的带有栅控作用的场发射阴极阵列的剖面图。 Fig. 10 is a cross-sectional view of a field emission cathode array with gate control function according to the second preferred embodiment of the present invention.
the
【主要组件符号说明】 [Description of main component symbols]
200—玻璃基板;210—阴极;211—阴极电极;212—电子发射层;213—介质层;220—栅极;221—纵向电极;222—横向带。 200—glass substrate; 210—cathode; 211—cathode electrode; 212—electron emission layer; 213—dielectric layer; 220—grid; 221—longitudinal electrode; 222—transverse strip.
具体实施方式 Detailed ways
下面结合附图3-7对本发明的优选实施例一的一种带栅控作用的场发射阴极阵列及其制造方法进行阐述。 A field emission cathode array with gate control function and its manufacturing method according to the preferred embodiment 1 of the present invention will be described below with reference to the accompanying drawings 3-7.
如图3、4所示,本发明的一种带有栅控作用的场发射阴极阵列,包括玻璃基板200,设置于玻璃基板200上的阴极210和栅极220,所述的阴极210和栅极220设置在玻璃基板200同一平面上,阴极210是由多列相互平行的条状阴极电极211以及在各列条状阴极电极211上交替设置电子发射层212和介质层213构成,所述的介质层213是等间距地设置在阴极电极211上,且介质层213是覆盖在阴极电极211、玻璃基板200和栅极220的纵向电极211上的条状介质层,所述的介质层213厚度为10nm-100nm,构成介质层213材料包含SiO2、Ta2O5、AlN、Al2O3、Si3N4、BN、TiO2中的一种或者两种及其以上的组合。所述的电子发射层212是等间距地设置在介质层213所覆盖的阴极电极211上,所述的栅极220是由多列相互平行的栅极电极构成,所述各列的栅极电极由纵向电极221和数个横向带222构成,所述的栅极电极和阴极电极211交替设置在玻璃基板200上,所述的位于各列阴极电极211的电子发射层212与相邻栅极电极的横向带222平行相对。设置于阴极电极211上的电子发射层212的长度与相邻栅极电极的横向带222的宽度一致,电子发射层212与相邻栅极电极的横向带222之间的距离为0.01μm-200μm。电子发射层包含碳纳米管、氧化锌、氧化锡、氧化镁、氧化铋中的一种或者两种及其以上的组合。电子发射层212还可以掺杂纳米银颗粒、纳米金颗粒、纳米铜颗粒、纳米锡颗粒、纳米氧化锌颗粒、纳米镍颗粒中的一种或者两种及其以上的组合,颗粒直径为0.1nm-10μm。
As shown in Figures 3 and 4, a field emission cathode array with gate control function of the present invention includes a
本发明优选实施例一提供的一种带栅控作用的场发射阴极阵列的制备方法包括下列步骤: A method for preparing a field emission cathode array with gate control function provided by the preferred embodiment 1 of the present invention comprises the following steps:
(S11)玻璃基板200的准备:对整个玻璃进行划片,清洗; (S11) Preparation of the glass substrate 200: scribing and cleaning the entire glass;
(S12)阴极电极211和栅极220的制作,具体过程包括:
(S12) Fabrication of the
(S121)划片后的玻璃基板200上采用溅射沉积或印刷、光刻、烧结制作导电薄膜。
( S121 ) Fabricate a conductive film on the
在基板200表面形成阴极电极211和栅极220,其所用材料可以选用Cu,W,Co,Ni,Ta,TaN,Ti,Zn,Al,Cr,感光银浆中的一种金属电极或者两种及其以上的组合的复合金属电极。本实施例优选采用磁控溅射方法沉积CrNi复合薄膜。
The
(S122)光刻胶旋涂。利用旋涂工艺将RZJ-304光刻胶转移至带有CrNi复合薄膜的玻璃基片200表面,并在110℃保温25min。
(S122) Photoresist spin coating. The RZJ-304 photoresist was transferred to the surface of the
(S123)曝光。预烘干的光刻胶膜层自然冷却至室温后进行曝光,将所需图形的掩膜版遮盖在光刻胶膜层上,在光强为4.4mW/cm2光刻机上曝光11秒,光刻胶的光敏剂呈正性,所以受紫外光照的图形被光溶解,不受紫外光照的图形保持不变。 (S123) exposure. After the pre-dried photoresist film layer is naturally cooled to room temperature, it is exposed, and the mask plate of the required pattern is covered on the photoresist film layer, and the photoresist film layer is exposed for 11 seconds on a photolithography machine with a light intensity of 4.4mW/ cm2 . The photosensitizer of the photoresist is positive, so the pattern subjected to ultraviolet light is dissolved by light, and the pattern not subjected to ultraviolet light remains unchanged.
(S124)显影。用浓度为3%的RZX-3038溶液显影,被光固化的光刻胶被RZX-3038溶液除去,留下所需的图形。 (S124) Developing. Develop with a concentration of 3% RZX-3038 solution, and the photoresist cured by light is removed by RZX-3038 solution, leaving the desired pattern.
(S125)湿法刻蚀。用15-20克硝酸铈,5ml冰乙酸,100毫升水所组成的混合溶液在50℃水浴中刻蚀。 (S125) Wet etching. Etching in a water bath at 50°C with a mixed solution consisting of 15-20 grams of cerium nitrate, 5 ml of glacial acetic acid, and 100 ml of water.
(S126)退胶。将湿法刻蚀后的基片浸泡丙酮溶液中,电极表面的光刻胶因溶于丙酮而脱落,形成阴极电极211和栅极220。
(S126) Unglue. The wet-etched substrate is immersed in an acetone solution, and the photoresist on the electrode surface is peeled off due to being dissolved in acetone, forming a
(S13)介质层213的制作。在该第一优选实施例中带栅控作用的场发射阴极阵列中的介质层213是覆盖在阴极电极211上的矩形状213,也可以是覆盖在阴极电极211、玻璃基板200和栅极电极的纵向电极221上的条状介质层213,介质层213厚度为10nm-100nm,构成介质层213材料包含SiO2、Ta2O5、AlN、Al2O3、Si3N4、BN、TiO2中的一种或者两种及其以上的组合。本实施例优先选用SiO2条状介质层213。(S13)具体实现步骤如下:
( S13 ) Fabrication of the
(S131)光刻胶旋涂。利用旋涂工艺将RZJ-304光刻胶转移至带有阴极电极211和栅极220的玻璃基片上,在烘箱中进行烘烤,烘烤温度110℃,保温时间25min;
(S131) Photoresist spin coating. Transfer the RZJ-304 photoresist to the glass substrate with the
(S132)曝光显影。预烘干的光刻胶膜层自然冷却至室温后进行曝光,将制备好的掩模版盖在光刻胶膜层上,在光强为4.4mW/cm2光刻机上曝光11秒,用浓度为3%的RZX-3038溶液显影,被光固化的光刻胶被RZX-3038溶液除去,留下覆盖栅极电极上的横向带222、且与阴极电极211垂直的条状光刻胶图案;
(S132) Exposure and development. The pre-dried photoresist film layer was naturally cooled to room temperature and then exposed. The prepared mask was covered on the photoresist film layer and exposed for 11 seconds on a photolithography machine with a light intensity of 4.4mW/ cm2 . Developing the 3% RZX-3038 solution, the photoresist cured by light is removed by the RZX-3038 solution, leaving a striped photoresist pattern covering the
(S133)SiO2介质薄膜镀制。利用溅射或电子束蒸发在上述所制的玻璃基片上沉积一层厚度为10nm-100nmSiO2介质薄膜; (S133) SiO 2 dielectric thin film plating. Using sputtering or electron beam evaporation to deposit a layer of thickness on the above-mentioned glass substrate is 10nm-100nmSiO Dielectric thin film;
(S134)光刻胶剥离。将镀有SiO2介质薄膜基片浸泡在丙酮溶液中,覆盖栅极电极的横向带222、且与阴极电极211垂直的光刻胶会被丙酮溶解而除去其表面上的SiO2介质层,留下所需的条状介质层213,此时,通过光学显微镜图观察本发明第一优选实施例的制备电子发射层前的带有栅控作用的场发射阴极阵列结构,如附图5所示;
(S134) Photoresist stripping. The substrate coated with SiO2 dielectric film is soaked in the acetone solution, the photoresist covering the
(S14)电子发射层212的制作。带栅控作用的场发射阴极阵列中的电子发射源可包含碳纳米管、氧化锌、氧化锡、氧化镁、氧化铋中的一种或者两种及其以上的组合;可采用电泳沉积、丝网印刷或光刻技术在未被介质层213所覆盖的阴极电极211上制备表面具有场致电子发射性能的电子发射层212。本实施例优先选用电泳沉积制备碳纳米管电子发射源,具体实现过程如下:
(S14) Fabrication of the
(S141)碳纳米管有机浆料的制备。电泳前,将碳纳米管原始粉末放置于100℃的1:1的浓硫酸和浓硝酸中3h;将100 ml松油醇、1 g乙基纤维素混合在95℃水浴条件下搅拌分散均匀,待乙基纤维素混合完全溶解后加入酸化后的5 g碳纳米管粉末,搅拌均匀;最后,在三维球磨机中进行充分球磨24 h,使碳纳米管均匀分散; (S141) Preparation of carbon nanotube organic slurry. Before electrophoresis, the original powder of carbon nanotubes was placed in 1:1 concentrated sulfuric acid and concentrated nitric acid at 100 ° C for 3 h; 100 ml terpineol and 1 g ethyl cellulose were mixed and dispersed evenly in a water bath at 95 ° C. After the ethyl cellulose is mixed and completely dissolved, add 5 g of acidified carbon nanotube powder and stir evenly; finally, fully ball mill for 24 h in a three-dimensional ball mill to make the carbon nanotubes evenly dispersed;
(S142)电泳液配制。取1-5g 碳纳米管有机浆料、500 ml异丙醇、100-500 mg 硝酸镁(Mg(NO3)2·6H2O)混合,在室温下在超声波的作用下分散5h,提高碳纳米管在溶液中的分散性,最后形成稳定的碳纳米管悬浊液,自然冷却至室温或用冷水浴加速冷却至更低温度; (S142) Electrophoresis solution preparation. Mix 1-5g of carbon nanotube organic slurry, 500 ml of isopropanol, and 100-500 mg of magnesium nitrate (Mg(NO 3 ) 2· 6H 2 O), and disperse for 5 hours under the action of ultrasonic waves at room temperature to increase carbon The dispersibility of nanotubes in the solution, finally forming a stable suspension of carbon nanotubes, cooling to room temperature naturally or accelerated cooling to a lower temperature with a cold water bath;
(S143)电泳沉积碳纳米管电子发射层。在电泳过程中,采用栅极220作为电泳阳极,采用阴极电极211作为电泳阴极,通过改变电泳时电压来改变电场大小,采用电泳电压为2-20 V,电泳时间为5-30 min使得碳纳米管电子发射层212均匀地沉积在未被介质层213所覆盖的阴极电极211表面上,从而形成图形化的电子发射层212;
(S143) Electrophoretic deposition of the carbon nanotube electron emission layer. In the electrophoresis process, the
(S144)碳纳米管烧结。电泳后的基片在氮气的保护下经过350℃保温20min后,即可在未被介质层213所覆盖的阴极电极211表面附着一层厚度均匀 的碳纳米管薄膜,通过光学显微镜研究电子发射层制备的情况,如附图6所示。本发明采用场发射阴极阵列中的栅极220作为电泳阳极,采用阴极电极211作为电泳阴极,制备的电子发射层均匀图形化地分布在未被介质层213所覆盖的阴极电极211,而且操作简单,成本低,同时可以实现大面积阴极阵列的制备。
(S144) Carbon nanotube sintering. After the substrate after electrophoresis is kept at 350°C for 20 minutes under the protection of nitrogen, a layer of carbon nanotube film with uniform thickness can be attached to the surface of the
至此,本发明第一优选实施例的带有栅控作用的场发射阴极阵列的制作完成,为了进一步研究带有栅控作用的场发射阴极阵列的场发射性能,将带有栅控作用的场发射阴极阵列与阳极荧光屏配合,在真空中测试了场发射阴极阵列的电子发射情况,从附图7阳极荧光屏发光图来看,带有栅控作用的场发射阴极阵列的场致发射的均匀性好。 So far, the fabrication of the field emission cathode array with grid control function in the first preferred embodiment of the present invention is completed. In order to further study the field emission performance of the field emission cathode array with grid control function, the field emission cathode array with grid control function The emission cathode array cooperates with the anode fluorescent screen, and the electron emission of the field emission cathode array is tested in vacuum. From the luminescence diagram of the anode fluorescent screen in the accompanying drawing 7, the field emission uniformity of the field emission cathode array with grid control effect good.
为了减少成本,对本发明第一优选实施例进行改良,将条状的介质层213改为阵列分布的介质层213,本发明第二优选实施例的带栅控作用的场发射阴极阵列如图7、8、9所示,包括玻璃基板200,设置于玻璃基板200上的阴极210和栅极220,所述的阴极210和栅极220设置在玻璃基板200同一平面上,阴极210是由多列相互平行的条状阴极电极211以及在各列的条状阴极电极211上交替设置电子发射层212和介质层213构成,所述的介质层213是等间距地设置在阴极电极211上,介质层是覆盖在阴极电极上的矩形状介质层,介质层厚度为10nm-100nm,构成介质层材料包含SiO2、Ta2O5、AlN、Al2O3、Si3N4、BN、TiO2中的一种或者两种及其以上的组合。所述的电子发射层212是等间距地设置在未被介质层213所覆盖的阴极电极211上,所述的栅极220是由多列相互平行的栅极电极构成,所述各列的栅极电极由纵向电极221和数个横向带222构成,所述的栅极电极和阴极电极211交替设置在玻璃基板200上,所述的位于各列阴极电极211的电子发射层212与相邻栅极电极的横向带222平行相对。每列栅极电极的横向带222可以等间距对称地设置在栅极电极的纵向电极221两侧,横向带222垂直于纵向电极221,横向带222的宽度为1μm-1mm,横向带222的长度为100μm-2mm,各列栅极电极上的相邻横向带222之间的距离100μm-2mm。
In order to reduce the cost, the first preferred embodiment of the present invention is improved, and the strip-shaped
该带栅控作用的场发射阴极阵列的制造方法,包括下列步骤: The manufacturing method of the field emission cathode array with gate control function comprises the following steps:
(S21)玻璃基板200的准备:对整个玻璃进行划片,清洗; (S21) Preparation of the glass substrate 200: scribing and cleaning the entire glass;
(S22)阴极电极211和栅极220的制作。在基板200表面形成阴极电极211和栅极220,其所用材料可以选用Cu,W,Co,Ni,Ta,TaN,Ti,Zn,Al,Cr,感光银浆中的一种金属电极或者两种及其以上的组合的复合金属电极。本实施例优选采用印刷、光刻和烧结技术制备厚膜银浆导电电极。具体过程包括:
( S22 ) Fabrication of the
(S221)感光银浆印刷。利用250目网版将感光银浆印刷至玻璃基片200表面,并在110℃保温20 min。
(S221) Photosensitive silver paste printing. Use a 250-mesh screen to print photosensitive silver paste onto the surface of the
(S222)曝光。预烘干的感光银浆膜层自然冷却至室温后进行曝光,将阴极图形的掩膜版遮盖在感光银浆膜层上,感光银浆的光敏剂呈负性,所以受紫外光照的图形被光固化,不受紫外光照的图形保持不变。 (S222) exposure. The pre-dried photosensitive silver paste film layer is naturally cooled to room temperature before exposure, and the mask plate of the cathode pattern is covered on the photosensitive silver paste film layer. The photosensitizer of the photosensitive silver paste is negative, so the pattern subjected to ultraviolet light is exposed Light curing, graphics that are not exposed to UV light remain unchanged.
(S223)显影。用浓度为0.4%的Na2CO3溶液显影,未被光固化的感光银浆被Na2CO3溶液除去,留下所需的图形。 (S223) Developing. Develop with a Na 2 CO 3 solution with a concentration of 0.4%, and the photosensitive silver paste that has not been cured by light is removed by the Na 2 CO 3 solution, leaving the desired pattern.
(S224)高温烧结。显影后的图形在氮气的保护下530℃的温度下烧结30min后形成阴极电极211和栅极220。
(S224) High temperature sintering. The developed pattern is sintered at 530° C. for 30 minutes under the protection of nitrogen to form the
(S23)介质层213的制作。带栅控作用的场发射阴极阵列中的介质层213既可以是覆盖阴极电极211、玻璃基板200和栅极220上的纵向电极221的条状介质层,也可以是覆盖在阴极电极211上矩形介质层,其成分可为SiO2、Ta2O5、AlN、Al2O3、Si3N4、BN、TiO2。本实施例优先选用SiO2矩形介质层。具体实现过程与实施例一中的步骤二基本相似,所不同之处在于介质层213只覆盖与栅极电极上的纵向电极221平行相对的阴极电极211上,形成矩形状介质层213,具体实现过程如下:
( S23 ) Fabrication of the
(S231)光刻胶旋涂。利用旋涂工艺将RZJ-304光刻胶转移至带有阴极电极211和栅极220的玻璃基片上,在烘箱中进行烘烤,烘烤温度110℃,保温时间25min;
(S231) Photoresist spin coating. Transfer the RZJ-304 photoresist to the glass substrate with the
(S232)曝光显影。预烘干的光刻胶膜层自然冷却至室温后进行曝光,将制备好的掩模版盖在光刻胶膜层上,在光强为4.4mW/cm2光刻机上曝光11秒,用浓度为3%的RZX-3038溶液显影,被光固化的、与栅极电极上的纵向电极221平行相对的阴极电极211上的光刻胶被RZX-3038溶液除去;
(S232) Exposure and development. The pre-dried photoresist film layer was naturally cooled to room temperature and then exposed. The prepared mask was covered on the photoresist film layer and exposed for 11 seconds on a photolithography machine with a light intensity of 4.4mW/ cm2 . For the development of 3% RZX-3038 solution, the photoresist on the
(S233)SiO2介质薄膜镀制。利用溅射或电子束蒸发在上述所制的玻璃基片上沉积一层厚度为10nm-100nm的SiO2介质薄膜; (S233) SiO 2 dielectric thin film plating. Utilizing sputtering or electron beam evaporation to deposit a layer of SiO with a thickness of 10nm-100nm on the above-mentioned prepared glass substrate Dielectric film;
(S234)光刻胶剥离。将镀有SiO2介质薄膜基片浸泡在丙酮溶液中,覆盖在栅极电极、与栅极电极上的横向带222平行相对的阴极电极211及无电极处的光刻胶会被丙酮溶解而除去其表面上的介质层,留下与栅极电极上的纵向电极221平行相对的阴极电极211上的矩形状介质层213。
(S234) The photoresist is stripped. Soak the substrate coated with SiO2 dielectric film in the acetone solution, and the photoresist covering the grid electrode, the
(S24)电子发射源的制作。为了提高电子发射层212中的发射材料和衬底的结合力,提高电子发射层的场致电子发射能力,也可在电子发射层212掺杂纳米银颗粒、纳米金颗粒、纳米铜颗粒、纳米锡颗粒、纳米氧化锌颗粒、纳米镍颗粒,颗粒直径为0.1 nm-10μm,结合本优选实施例1中的电泳沉积法制备电子发射层212,可将纳米银金属颗粒添加入到电泳液中,通过电泳沉积工艺沉积到未被介质层213所覆盖的阴极电极211上。具体实现过程如下:
(S24) Fabrication of an electron emission source. In order to improve the binding force between the emission material and the substrate in the
(S241)纳米银/碳纳米管有机浆料的制备。电泳前,将碳纳米管原始粉末放置于100℃的1:1的浓硫酸和浓硝酸中3h;将100 ml松油醇、1g乙基纤维素混合在95℃水浴条件下搅拌分散均匀,待乙基纤维素混合完全溶解后加入酸化后的5 g碳纳米管粉末和5 g纳米银颗粒,搅拌均匀。最后,在三维球磨机中进行充分球磨24 h,使碳纳米管均匀分散; (S241) Preparation of nano-silver/carbon nanotube organic paste. Before electrophoresis, the original powder of carbon nanotubes was placed in 1:1 concentrated sulfuric acid and concentrated nitric acid at 100°C for 3 hours; 100 ml of terpineol and 1 g of ethyl cellulose were mixed and dispersed evenly in a water bath at 95°C. Add 5 g carbon nanotube powder and 5 g nano-silver particles after the acidification after ethyl cellulose is mixed and completely dissolved, and stir evenly. Finally, full ball milling was carried out in a three-dimensional ball mill for 24 h to disperse the carbon nanotubes evenly;
(S242)电泳液配制。取1-5 g纳米银/碳纳米管有机浆料、500 ml异丙醇、100-500 mg硝酸镁(Mg(NO3)2·6H2O)混合,在室温下在超声波的作用下分散5h,提高碳纳米管在溶液中的分散性,最后形成稳定的碳纳米管悬浊液,自然冷却至室温或用冷水浴加速冷却至更低温度; (S242) Electrophoresis solution preparation. Take 1-5 g of nano-silver/carbon nanotube organic slurry, 500 ml of isopropanol, 100-500 mg of magnesium nitrate (Mg(NO 3 ) 2· 6H 2 O), mix them, and disperse under the action of ultrasonic waves at room temperature 5h, improve the dispersion of carbon nanotubes in the solution, and finally form a stable suspension of carbon nanotubes, naturally cool to room temperature or use a cold water bath to accelerate cooling to a lower temperature;
(S243)电泳沉积纳米银/碳纳米管复合材料。在电泳过程中,采用栅极220作为电泳阳极,采用阴极电极211作为电泳阴极,通过改变电泳时电压来改变电场大小,采用电泳电压为2-20 V,电泳时间为5-30 min使得碳纳米管电子发射层212均匀地沉积在未被介质层213所覆盖的阴极电极211表面上,从而形成图形化的纳米银/碳纳米管电子发射层212;
(S243) Electrophoretic deposition of nano-silver/carbon nanotube composite materials. In the electrophoresis process, the
(S244)纳米银/碳纳米管烧结。电泳沉积后的基片在氮气的保护下经过350℃保温20min后,即可在未被介质层所覆盖的阴极电极211表面附着一层厚度均匀的纳米银/碳纳米管电子发射层212。
(S244) Nanosilver/carbon nanotube sintering. After the electrophoretic deposition substrate is kept at 350° C. for 20 minutes under the protection of nitrogen, a layer of nano-silver/carbon nanotube
综上所述,本发明公开的带有栅控作用的场发射阴极阵列可以实现低压调控,降低场发射阴极阵列的开启电场,提高电子发射的均匀性和电子发射效率,而且结构简单、制造工艺容易、成本低廉、制作过程稳定可靠的优点。 In summary, the field emission cathode array with gate control function disclosed by the present invention can realize low-voltage regulation, reduce the open electric field of the field emission cathode array, improve the uniformity and efficiency of electron emission, and has a simple structure and a manufacturing process Easy, low cost, stable and reliable manufacturing process.
本发明提供优选实施例,但不应该认为仅限于在此阐述的实施例。在附图3-10中,为了清除放大了层和区域的厚度,但作为示意图不应该认为严格反映了几何尺寸的比例关系。附图为本发明的理想化实施例的示意图,本发明所示的实施例不应该被认为仅限于图中所示的区域的特定形状,而是包括所得到的形状,比如制造引起的偏差。在本实施例中均以矩形表示,附图中的表示是示意性的,但这不应该被认为限制本发明的范围。 The present invention provides preferred embodiments, but should not be considered limited to the embodiments set forth herein. In accompanying drawings 3-10, the thicknesses of layers and regions are exaggerated for clarity, but as schematic diagrams, it should not be regarded as strictly reflecting the proportional relationship of geometric dimensions. The drawings are schematic illustrations of idealized embodiments of the invention. The illustrated embodiments of the invention should not be construed as limited to the particular shapes of regions illustrated in the drawings but are to include resulting shapes such as manufacturing-induced deviations. In this embodiment, they are all represented by rectangles, and the representations in the drawings are schematic, but this should not be considered as limiting the scope of the present invention.
以上例子主要说明了本发明的一种带栅控作用的场发射阴极制备方法。尽管只对其中一些本发明的实施方式进行了描述,但是本领域普通技术人员应当了解,本发明可以在不偏离其主旨与范围内以许多其他的形式实施。因此,所展示的例子与实施例方式被视为示意性的而非限制性的,在不脱离如所附各权利要求所定义的本发明精神及范围的情况下,本发明可能涵盖各种的修改与替换。以上所述仅为本发明的较佳实施例,凡依本发明申请专利范围所做的均等变化与修饰,皆应属本发明的涵盖范围。 The above example mainly illustrates the preparation method of a field emission cathode with gate control function of the present invention. Although only some of the embodiments of the present invention have been described, those skilled in the art should appreciate that the present invention can be implemented in many other forms without departing from the spirit and scope thereof. Accordingly, the examples and embodiments shown are to be regarded as illustrative and not restrictive, and the invention may cover various aspects without departing from the spirit and scope of the invention as defined in the appended claims. Modify and replace. The above descriptions are only preferred embodiments of the present invention, and all equivalent changes and modifications made according to the scope of the patent application of the present invention shall fall within the scope of the present invention.
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