Patent Application
20090039755
1. Field of the invention
The present invention relates to an electron-emitting device applied to a flat type image display apparatus and an image display apparatus fabricated by using the electron-emitting device.
2. Description of the Related Art
A surface conduction electron-emitting device uses a phenomenon in which electrons are emitted by passing a current through a small-area conductive film formed on a substrate in parallel to the film surface and such a conductive film generally has an electron-emitting portion formed by energization (forming) in advance. That is, a DC voltage or a very slowly rising voltage of about 1 V/min is applied to both ends of the conductive film to locally break, deform, or degenerate the conductive film, and thereby form an electron-emitting portion in an electrically high-resistance state. The electron-emitting portion has a crack produced in part of the conductive film and electrons are emitted from around the crack.
The surface conduction electron-emitting device has a simple structure and is easy to manufacture and therefore, a large number of devices can advantageously be arranged in a large area. Thus, various applications making use of this feature are now under study. The applicant concerned has proposed, as a manufacturing method of a surface conduction electron-emitting device advantageous for a large area, a method of forming a conductive film without relying on the sputtering method or evaporation method using a vacuum. An example thereof is a method by which a solution containing organic metal is applied onto a substrate by a spinner and then, the solution is patterned to a desired shape and the organic metal is pyrolytically decomposed to obtain a conductive film made of fine particles. Further, the applicant concerned has proposed in Japanese Patent Application Laid-Open No. 8-171850 a method by which a conductive film of a desired shape is formed by applying droplets of a solution containing organic metal onto a substrate by the inkjet method such as the bubblejet (registered trademark) method and the piezojet method.
A conductive film formed according to one of the above methods is a film made of fine particles of metal or metallic oxide or a highly continuous film. The conductive film is controlled to a desired range of resistance as an electron-emitting device by controlling component materials and a thickness thereof, but is required to be a thin film of several nm to several tens of nm from the viewpoint of the forming process and electron emission efficiency. Fluctuations in resistance of a conductive film need to be suppressed, though the film is thin, from the viewpoint of stability of electron emission characteristics and suppression of fluctuations. In addition, the conductive film is required to have high resistance of about 10 kΩ/sq to several hundreds of kΩ/sq as sheet resistance.
However, a conductive film formed according to one of the above methods and having metal as a main component cannot be used because, if the thickness thereof is several nm or less, resistance thereof fluctuates wildly. If the conductive film has a thickness of several nm or more showing stable resistance, only a low-resistance film of several kΩ/sq or less as sheet resistance can be obtained. If a conductive film is mainly made of metallic oxide and has a thickness of several nm or less, such a thin film cannot be used either because resistance thereof fluctuates wildly. Further, if the conductive film has a thickness of several nm or more showing stable resistance, resistance thereof fluctuates wildly depending on whether moisture or the like is adsorbed on the surface. Even if stabilizing treatment such as vacuum baking is performed, a portion of the film is reduced. Thus, a conductive film of high resistance of about 10 kΩ/sq to several hundreds of kΩ/sq as sheet resistance with stability could not be obtained. Therefore, a problem sometimes arises that electron emission characteristics fluctuate significantly when an electron source in which a plurality of the electron-emitting devices is arranged is used. Also in an image display apparatus constructed by arranging the electron source and an image-forming member such as a phosphor opposite to each other, fluctuations in electron emission characteristics sometimes leads to degradation in image quality, causing a problem.
The present invention has been developed to solve the above problems and an object thereof is to provide an electron-emitting device having a conductive film that has a thickness of several nm to several tens of nm and high resistance of 10 kΩ/sq to several hundreds of kΩ/sq as sheet resistance and shows minor fluctuations in resistance.
Further, another object of the present invention is to provide an image display apparatus having excellent display quality using the electron-emitting device.
An aspect of the present invention is an electron-emitting device having a pair of device electrodes formed on an insulating substrate and a conductive film formed to connect the device electrodes and having an electron-emitting portion, wherein the conductive film has a thickness of 3 nm to 50 nm and is made of precious metal and oxide of base metal, a percentage of the base metal among metals contained in the conductive film is 30 mol % or more, and the conductive film has a concentration gradient of oxide of the base metal in a thickness direction.
Another aspect of the present invention is an image display apparatus including a first plate on which a plurality of the electron-emitting devices are arranged and a second plate on which an image display member irradiated with electrons emitted from the electron-emitting devices is arranged and which is arranged opposite to the electron-emitting devices.
Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.
A first embodiment of the present invention is an electron-emitting device including a pair of device electrodes formed on an insulating substrate and a conductive film formed to connect the device electrodes and having an electron-emitting portion, wherein the conductive film has a thickness of 3 nm to 50 nm and is made of precious metal and oxide of base metal (base metal oxide), a percentage of the base metal among metals contained in the conductive film is 30 mol % or more, and there is a concentration gradient of the base metal oxide in a thickness (or depth) direction.
A second embodiment of the present invention is an image display apparatus including a first plate on which a plurality of the electron-emitting devices are arranged and a second plate on which an image display member irradiated with electrons emitted from the electron-emitting devices is arranged and which is arranged opposite to the electron-emitting devices.
According to the present invention, an electron-emitting device including a conductive film having a thickness of 3 nm to 50 nm and uniform sheet resistance of 10 kΩ/sq to several hundreds of kΩ/sq can be formed so that an electron-emitting device having less fluctuations in electric properties and better electric properties can be obtained. As a result, an image display apparatus with less fluctuations and higher quality can be obtained.
Preferable embodiments of the present invention will exemplarily be described below in detail with reference to drawings. However, dimensions, material, shapes, relative configurations and the like of the following embodiments are not intended to limit the scope of the present invention to these values.
An electron-emitting device in the present invention basically has a pair of device electrodes on an insulating substrate and a conductive film formed to connect the device electrodes and an electron-emitting portion is formed in the conductive film.
The substrate 1 includes, for example, quartz glass, glass in which impurity content such as Na is reduced, soda-lime glass, a glass substrate with SiO2 formed on the surface thereof, and a ceramic substrate such as alumina. If necessary, after the substrate being sufficiently cleaned, a silane coupling agent is used to make the surface of the substrate hydrophobic.
Materials of the device electrodes 2, 3 include metals such as Pd, Pt, Ru, Ag, Au, Ti, In, Cu, Cr, Fe, Zn, Sn, Ta, W, and Pb, and oxides such as PdO, SnO2, In2O3, PbO, and Sb2O3. Also, borides such as HfB2, ZrB2, LaB6, CeB6, YB4, and GdB4, carbides such as TiC, ZrC, HfC, TaC, SiC, and WC, nitrides such as TiN, ZrN, and HfN, semiconductors such as Si and Ge, and carbon are also included.
A distance L between the device electrodes 2, 3 is several hundreds of A to several hundreds of μm. The voltage applied between the device electrodes 2, 3 is preferably low and fabrication with reproducibility is required and thus, the preferable distance L is several hundreds of Å to several μm.
The conductive film 4 according to the present invention is made of precious metal and base metal oxide and is characterized in that the percentage of the base metal among metals contained in the conductive film 4 is 30 atomic % or more and there is a concentration gradient of the base metal oxide in a thickness direction. At least one selected from Pt, Pd, Ir, and Rh is preferably used as the precious metal and at least one selected from V, Cr, Ti, Mg, Mo, Ca, Ba, Y, and In is preferably used as the base metal.
As described above, the conductive film 4 of an electron-emitting device is required to have a thickness of several nm to several tens of nm from the viewpoint of the forming process and electron emission efficiency regardless of which method is used. From the viewpoint of stability of electron emission characteristics and suppression of fluctuations of electron emission characteristics, a conductive film having high resistance of 10 kΩ/sq to several hundreds of kΩ/sq as sheet resistance and showing minor fluctuations in resistance is required. A bulk metal normally has volume resistivity of about 1×10−7 Ωm and sheet resistance of a film simply calculated from a film thickness of 3 nm to 50 nm is 2 Ω/sq to 30 Ω/sq. It is well known that a metal film produced by a common method of manufacture such as a sputtered film, an evaporated film, and a film produced by spinning/burning has resistance increased by several times to several tens of times due to a thin film effect or the like. That is, only films of several tens of Ω/sq to several kΩ/sq are actually obtained. High-resistance films of 1 kΩ/sq or more are in a very thin state of several nm and thus, when many films are formed, such films will have great fluctuations.
As a result of an intensive research, the inventors found that thin films made of precious metal and base metal oxide have minor resistance fluctuations and that conductive films whose ratio of specific resistance to a metal bulk is 100 times to 100,000 times are obtained. That is, if the precious metal used has volume resistivity of about 1×10−7 Ωm and the thickness of films is 3 nm to 50 nm, sheet resistance of several kΩ/sq to several hundreds of kΩ/sq with stability could be obtained and fluctuations could be reduced even when a plurality of films are produced.
Generally, when metal oxide with high resistance is gradually added to a metal, resistance of a mixture of the metal and metal oxide increases, but it is difficult to control resistance and at the same time to reduce fluctuations. In a conductive film according to the present invention, the percentage of the base metal among metals contained in the conductive film is 30 mol % or more and a concentration gradient of the base metal oxide arises in the thickness direction and therefore, the resistance will not increase too much. Thus, when the thickness of a conductive film is changed, the rate of change of thickness becomes larger than that of resistance. As a result, excellent results of minor fluctuations can conceivably be obtained in accordance with the thickness when the ratio of specific resistance to a precious metal bulk is within a range of 100 times to 100,000 times. The concentration gradient of such base metal oxide is confirmed from XPS analysis in the depth direction.
As a method of manufacture of a conductive film according to the present invention, for example, a solution containing a complex of precious metal and base metal is prepared, the solution is applied onto a substrate by spin coating or the inkjet method, and the substrate is heated and burned. By adjusting the amount of precious metal complex and that of base metal complex to a ratio necessary as a conductive film when preparing the solution, a conductive film of that ratio can be produced. When applying the solution onto the substrate by the inkjet method, the abundance of metal can be adjusted by the metal concentration of the solution and the number of times of applying droplets. A commonly used heating means may be used in a burning process and the burning temperature is 250° C. to 500° C. It is also preferable to perform UV irradiation during burning. The state of a film obtained in this manner is confirmed based on results of XPS analysis and X ray diffraction.
The forming process to form the electron-emitting portion 5 is performed to the conductive film 4 obtained as described above.
Specifically, when voltage is applied between the device electrodes 2, 3 from a power supply (not shown) under a predetermined degree of vacuum, a gap (crack) with a changed structure is formed in the conductive film 4. This gap area constitutes the electron-emitting portion 5. While electrons are emitted from the vicinity of the gap formed by the forming process under a predetermined voltage, electron emission efficiency under this condition is very low.
First, a case in which the pulse wave peak is a constant voltage will be described with reference to
Next, a case in which voltage pulses are applied while increasing the pulse wave peak will be described with reference to
Energization forming can be completed when resistance is determined by measuring the current passing through a device to which the pulse voltage is being applied and the determined resistance is, for example, 1 m or more.
However, electron emission efficiency in this state is very low and it is preferable to perform activation described below to increase the electron emission efficiency.
Activation is a process in which a pulse voltage is repeatedly applied between the device electrodes 2, 3 under an appropriate degree of vacuum in which a gas containing carbon atoms is present to cause carbon or carbon compounds derived from the gas to deposit as a carbon film near the gap (crack).
In the present process, for example, tolunitrile is used as a carbon source and is introduced into vacuum space through a slow leak valve to maintain the vacuum at about 1.3×10−4 Pa. The pressure of tolunitrile to be introduced is somewhat influenced by the shape of a vacuum device and members used in the vacuum device, but is preferably 1×10−5 Pa to 1×10−2 Pa.
In
In the activation, voltage application is stopped when an emission current Ie is almost saturated and then, the slow leak valve is closed to end the activation.
By performing the above process, an electron-emitting device as shown in
Basic features of the electron-emitting device produced with the device configuration and the manufacturing method described above will be described using
For measurement of the device current If passing through the device electrodes 2, 3 of the electron-emitting device and the emission current Ie to the anode, the power supply 41 and the ammeter 40 are connected to the device electrodes 2, 3 and the anode electrode 44 to which the power supply 43 and the ammeter 42 are connected is arranged above the electron-emitting device.
The electron-emitting device and the anode electrode 44 are set up in a vacuum device 45 and the vacuum device is equipped with a vacuum pump 46 and devices such as a vacuum gauge required for the vacuum device so that measurement evaluation can be performed in a desired vacuum. Measurements are made by setting the voltage of the anode electrode 44 to 1 kV to 10 kV and a distance H between the anode electrode and the electron-emitting device to 2 mm to 8 mm.
The electron-emitting device has three features for the emission current Ie.
First, as is evident from
Second, the emission current Ie is dependent on the device voltage Vf and thus, the emission current Ie can be controlled by the device voltage Vf.
Third, emission charges captured by an anode electrode 54 are dependent on the time during which the device voltage Vf is applied. That is, the charge quantity captured by the anode electrode 54 can be controlled by the time during which the device voltage Vf is applied.
Next, an image display apparatus in the present invention will be described.
The image display apparatus in the present invention has a first plate on which a plurality of the electron-emitting devices in the present invention is arranged and a second plate on which an image display member irradiated with electrons emitted from the electron-emitting devices is arranged and which is arranged opposite to the electron-emitting devices.
As shown in
Also in
By setting up a supporting member (not shown) called a spacer between the face plate 73 and the rear plate 71, the envelope 77 having sufficient strength against atmospheric pressure for a large-area panel may be formed.
The metal back 75 is usually provided on the inside surface of the phosphor film 74. The metal back is provided in order to improve brightness by specular reflection, among emissions of light by phosphors, of light to the inside surface side to the face plate 73 side, to act as an anode electrode to which an electron beam acceleration voltage is applied, and the like. The metal back 75 can be produced by, after a phosphor film being produced, performing smoothing (usually called filming) of the surface on the inside of the phosphor film and then depositing Al by vacuum deposition or the like.
When the envelope 77 is sealed, phosphors of each color and electron-emitting devices must be matched for a color phosphor film and thus, adequate positioning by bumping upper and lower plates against each other or the like is needed.
In order to maintain a degree of vacuum after the envelope 77 being sealed, in addition to the degree of vacuum of about 10−5 Pa being needed for sealing, getter treatment may be performed. This is a treatment to form an evaporated film by heating a getter arranged at a predetermined position (not shown) inside the envelope immediately before or after the envelope 77 being sealed by a heating method of resistance heating, high-frequency heating and the like. The getter usually has Ba as a main component and maintains the degree of vacuum by adsorption of the evaporated film.
According to the basic features of the electron-emitting device in the present invention, emission electrons from the electron-emitting portion are controlled by the wave height and width of a pulse voltage applied between electrodes facing each other when the applied voltage is the threshold voltage or more. The current amount is controlled also by a mean value thereof and thus, a halftone display is enabled.
When a large number of electron-emitting devices are arranged, a voltage can be applied to any device as needed by determining an selection line by a scanning line signal and applying the pulse voltage to individual devices through each information signal line as needed so that each device can be turned on.
Methods of modulating an electron-emitting device in accordance with an input signal having halftones include the voltage modulation method and the pulse width modulation method.
A specific driving device will be described below.
In
The scanning circuit 92 as an X driver applying a scanning line signal is connected to the X-direction wiring of the image display panel 91 using the electron source substrate and the information signal generator 97 as the Y driver applying an information signal is connected to the Y-direction wiring.
To apply the pulse height modulation method, a circuit that generates fixed width voltage pulses and modulates the wave height of pulses as needed in accordance with input data is used as the information signal generator 97. To apply the pulse width modulation method, a circuit that generates fixed height voltage pulses and modulates the width of voltage pulses as needed in accordance with input data is used as the information signal generator 97.
The control circuit 93 generates each control signal of Tscan, Tsft, and Tmry to each component based on a synchronous signal Tsync sent from the synchronous signal separation circuit 96.
The synchronous signal separation circuit 96 is a circuit for separating an NTSC TV signal input from outside into a synchronous signal component and a luminance signal component. The luminance signal component is input into the shift register 94 in synchronization with the synchronous signal.
The shift register 94 performs serial/parallel conversion of the luminance signal input in serial and time series for each line of image and operates based on a shift clock Tsft sent from the control circuit 93. Serial/parallel converted data of one line of image (corresponding to drive data for n electron-emitting devices) is output from the shift register 94 as n parallel signals.
The line memory 95 is a storage device for storing data of one line of image for a required time and stored content is input into the information signal generator 97.
The information signal generator 97 is a signal source for suitably driving each electron-emitting device in accordance with each luminance signal. An output signal thereof enters the display panel 91 through the Y-direction wiring and is applied to each electron-emitting device present at intersections with the X-direction wiring being selected by the scanning circuit 92.
By scanning the X-direction wiring successively, it becomes possible to drive electron-emitting devices on the whole panel.
In the image display apparatus according to the present invention, as described above, each electron-emitting device is caused to emit electrons by applying a voltage through the X— and Y-direction wirings. On the other hand, a high voltage is applied to the metal back 75, which is an anode electrode, through a high-voltage terminal Hv connected to the DC voltage source Va to accelerate a generated electron beam. An image can be formed by collision of the electron beam against the phosphor film 74.
The configuration of the image display apparatus described here is an example of the image display apparatus in the present invention and various modifications can be made based on technical ideas of the present invention. NTSC input signals are described above, but input signals are not limited to NTSC input signals and the present invention can be applied also to PAL, HDTV and the like.
The process of producing an electron-emitting device in the configuration shown in
2.8 mm thick glass of PD-200 (trade name, manufactured by Asahi Glass Co., Ltd.) having less alkali components was used as the substrate 1 with further 100 nm of SiO2 film applied and burned as a sodium block layer thereon.
Next, a film of titanium Ti as an undercoating layer was formed by the sputtering method on the glass substrate 1 to a thickness of 5 nm and a film of platinum Pt to a thickness of 40 nm. Then, a photo resist was applied and a series of photolithographic processes of exposure, development, and etching was applied for patterning to form the device electrodes 2, 3.
In the present example, the distance L of the device electrodes was set to 10 μm and the width W to 100 μm.
After the substrate being sufficiently cleaned, the substrate was put into a vessel in which vapor of diacetoxy dimethyl silane was saturated and left at room temperature (about 25° C.) for 30 min. Then, the substrate was taken out of the vessel, heated at 120° C. for 15 min, and a silane coupling agent was used to treat the surface of the substrate.
Next, 0.624 g of palladium-proline complex, 0.286 g of chrome EDTA complex, 0.1 g of 88% saponified polyvinyl alcohol (average polymerization degree: 500), 2 g of ethylene glycol, and 15 g of 2-propanol were dissolved in water to make a solution of 100 g. The solution was filtered by a membrane filter of pore size 0.25 μm after dissolution to make a palladium/chrome compound solution (a solution in which the molar ratio of Pd metal and Cr metal is 70:30). The solution was attached between the device electrodes 2, 3 by using an inkjet injection system using a piezo element and adjusting the dot diameter to 60 μm. A substrate was prepared, on which the solution was applied with changing the number of dots (droplets). Pd and Cr oxide were formed between the device electrodes 2, 3 by heating the substrate in an oven in the atmosphere at 350° C. for 30 min.
The substrate was put into a vacuum chamber and baked at substrate temperature of 300° C. and 1×10−5 Pa or less for 10 hours. The length of obtained device of conductive films made of Pd and Cr oxide was observed under an optical microscope and measured, yielding the dot diameter of 60 μm. Measurement of sheet resistance of the conductive films showed 2.60 kΩ/sq in 4-dot case, 2.94 kΩ/sq in 3-dot case, and 4.80 kΩ/sq in 2-dot case.
Quantitative analysis of each conductive film by an X ray microanalyzer (EPMA) was performed to determine the abundance of Pd and Cr metals. Abundances of elements were: 60.3×1015 atoms/cm2 in 4-dot case, 43.3×1015 atoms/cm2 in 3-dot case, and 28.6×1015 atoms/cm2 in 2-dot case.
The above result was used for plotting with the horizontal axis set as the abundance of elements and the vertical axis set as an inverse of sheet resistance to determine an approximated straight line (hereinafter referred to as a conductance curve).
A conductance curve shows a relationship between a metal abundance and an inverse of resistance. If the metal abundance increases, resistance decreases and an inverse of resistance increases. If the metal abundance decreases, resistance increases. If the abundance is 0, resistance is infinite and an inverse thereof is 0. In an ideal system, the conductance curve is a straight line passing through the origin. Generally, resistance increases before the metal abundance decreases to 0, and the y-intercept becomes a negative value. A point of intersection with the x axis is a dead layer where resistance becomes infinite even if metal is present. A material of the present invention is a material that presents no dead layer even if the metal abundance decreases in the range of two to four dots. A material of the present invention has a positive-valued dead layer.
In the present example, the y-intercept of an approximated curve was a positive value. Also, XPS analysis of the film state showed that the abundance of Cr decreased in the depth direction.
0.491 g of palladium-proline complex 0.579 g of chrome EDTA complex, 0.1 g of 88% saponified polyvinyl alcohol (average polymerization degree: 500), 2 g of ethylene glycol, and 15 g of 2-propanol were dissolved in water to make a solution of 100 g. The solution was filtered by a membrane filter of pore size 0.25 μm after dissolution to make a palladium/chrome compound solution (a solution in which the molar ratio of Pd metal and Cr metal is 65:35) and applied to the substrate by changing the number of dots according to a method similar to that in Example 1. After being burnt at 350° C., the substrate was baked at 330° C. for 10 hours in a vacuum chamber. Then, resistance was measured. Sheet resistance of obtained conductive films was 13.5 kΩ/sq in 2-dot case, 8.87 kΩ/sq in 3-dot case, and 7.20 kΩ/sq in 4-dot case. The metal abundance was determined by EPMA to also determine the abundance of elements. The result was 38.6×1015 atoms/cm2 in 2-dot case, 56.8×1015 atoms/cm2 in 3-dot case, and 75.9×1015 atoms/cm2 in 4-dot case.
Similarly to Example 1, the above result was used for plotting with the horizontal axis set as the abundance of elements and the vertical axis set as an inverse of sheet resistance to determine a conductance curve thereof. As a result, the y-intercept of an approximated curve was a positive value. Also, XPS analysis of the film state showed that the abundance of Cr decreased in the depth direction.
0.453 g of palladium-proline complex, 0.662 g of chrome EDTA complex, 0.1 g of 88% saponified polyvinyl alcohol (average polymerization degree: 500), 2 g of ethylene glycol, and 15 g of 2-propanol were dissolved in water to make a solution of 100 g. The solution was filtered by a membrane filter of pore size 0.25 μm after dissolution to make a palladium/chrome compound solution (a solution in which the molar ratio of Pd metal and Cr metal is 60:40) and applied to the substrate by changing the number of dots according to a method similar to that in Example 1. After being burnt at 350° C. while being irradiated with UV, the substrate was baked at 350° C. for 10 hours in a vacuum chamber. Then, resistance was measured. Sheet resistance of obtained conductive films was 46.1 kΩ/sq in 2-dot case, 31.5 kΩ/sq in 3-dot case, and 24.4 kΩ/sq in 4-dot case. The metal abundance was determined by EPMA to also determine the abundance of elements. The result was 45.2×1015 atoms/cm2 in 2-dot case, 64.1×1015 atoms/cm2 in 3-dot case, and 87.4×1015 atoms/cm2 in 4-dot case.
Similarly to Example 1, the above result was used for plotting with the horizontal axis set as the abundance of elements and the vertical axis set as an inverse of sheet resistance to determine a conductance curve thereof. As a result, the y-intercept of an approximated curve was a positive value. Also, XPS analysis of the film state showed that the abundance of Cr decreased in the depth direction.
0.507 g of palladium-proline complex, 0.543 g of chrome EDTA complex, 0.1 g of 88% saponified polyvinyl alcohol (average polymerization degree: 500), 2 g of ethylene glycol, and 15 g of 2-propanol were dissolved in water to make a solution of 100 g. The solution was filtered by a membrane filter of pore size 0.25 μn after dissolution to make a palladium/chrome compound solution (a solution in which the molar ratio of Pd metal and Cr metal is 50:50) and applied to the substrate by changing the number of dots according to a method similar to that in Example 1. After being burnt at 350° C. while being irradiated with UV, the substrate was baked at 330° C. for 10 hours in a vacuum chamber. Then, resistance was measured. Sheet resistance of obtained conductive films was 280 kΩ/sq in 2-dot case, 205 kΩ/sq in 3-dot case, and 162 kΩ/sq in 4-dot case. The metal abundance was determined by EPMA to also determine the abundance of elements. The result was 44.2×1015 atoms/cm2 in 2-dot Case, 66.4×1015 atoms/cm2 in 3-dot case, and 86.5×1015 atoms/cm2 in 4-dot case.
Similarly to Example 1, the above result was used for plotting with the horizontal axis set as the abundance of elements and the vertical axis set as an inverse of sheet resistance to determine a conductance curve thereof. As a result, the y-intercept of an approximated curve was a positive value. Also, XPS analysis of the film state showed that the abundance of Cr decreased in the depth direction.
An experiment similar to that in Example 1 was performed by replacing a palladium/chrome compound solution applied by an inkjet injection system with a platinum/chrome compound solution shown below.
0.412 g of platinum acetate monoethanol complex, 0.662 g of chrome EDTA, 0.1 g of 88% saponified polyvinyl alcohol (average polymerization degree: 500), 2 g of ethylene glycol, and 15 g of 2-propanol were dissolved in water to make a solution of 100 g. The solution was filtered by a membrane filter of pore size 0.25 μm after dissolution to make a platinum/chrome compound solution (a solution in which the molar ratio of Pt metal and Cr metal is 60:40) and applied to the substrate by changing the number of dots according to a method similar to that in Example 1. The substrate was burned in the atmosphere at 350° C. Measurement of sheet resistance resulted in 44.3 kΩ/sq in 2-dot case, 24.1 kΩ/sq in 3-dot case, and 19.0 kΩ/sq in 4-dot case. The metal abundance was determined by EPMA to also determine the abundance of elements. The result was 20.0×1015 atoms/cm2 in 2-dot case, 32.5×1015 atoms/cm2 in 3-dot case, and 45.0×1015 atoms/cm2 in 4-dot case.
Similarly to Example 1, the above result was used for plotting sheet resistance and the abundance of elements with the horizontal axis set as the abundance of elements and the vertical axis set as an inverse of sheet resistance to determine a conductance curve thereof. As a result, the y-intercept of an approximated curve was a positive value. Also, XPS analysis of the film state showed that the abundance of Cr decreased in the depth direction.
Similarly, with respect to metals of V, Cr, Ti, Mg, Mo, Ca, Ba, Y, and In, solution was prepared by mixing palladium-proline complex and EDTA complex of the metal in the ratio of 70:30. The solution was applied as two dots, three dots, and four dots by an inkjet injection system to the substrate. After being burnt at 350° C., the substrate was put into a vacuum chamber and baked at 300° C. for 10 hours. Then, sheet resistance of obtained conductive films was measured. Similarly to Example 1, the above result was used for plotting with the horizontal axis set as the abundance of elements and the vertical axis set as an inverse of sheet resistance to determine a conductance curve thereof. As a result, the y-intercept of an approximated curve was a positive value.
In a conductive film according to the present invention, as described above, the y-intercept of a conductance curve is a positive value and the rate of change of thickness was larger than that of resistance.
As shown in
A paste material (NP-4035C manufactured by Noritake Co., Limited) was printed on the substrate using a technique of screen printing and the substrate was burned at 450° C. to form a Y-direction wiring 63 having a thickness of 10 μm as shown in
A paste material (NP-7710 manufactured by Noritake Co., Limited) was printed on the substrate using a technique of screen printing and the substrate was burned at 570° C. to form an insulating film 102 having a thickness of 20 μm as shown in
A paste material (NP-4035C manufactured by Noritake Co., Limited) was printed on the substrate using a technique of screen printing and the substrate was burned at 450° C. to form an X-direction wiring 62 having a thickness of 10 μm as shown in
After the substrate on which the device electrodes 2, 3 and the wirings 62, 63 prepared as described above being cleaned, the surface thereof was treated. The surface treatment process is performed in order to stabilize and make uniform the shape of droplets in a conductive film production process by an inkjet injection system described later. Specifically, the surface treatment process was performed by leaving the substrate in a vessel filled with saturated vapor of dimethyl dimethoxysilane at room temperature (about 25° C.) for 30 min.
After the surface treatment, four droplets of palladium/chrome compound solution used in Example 3 were applied at a time between the device electrodes 2, 3 on the substrate. Droplets applied at this point formed attached droplets by extending to a round shape of 60 μm in diameter on the substrate, each overlapping ends of the device electrodes 2, 3.
After attachment of droplets, the substrate was heated in an oven in the atmosphere at 350° C. for 30 min and then maintained in a vacuum chamber at 330° C. for 10 hours, and the temperature was dropped to the room temperature. The conductive film 4 made of palladium and chrome oxide was formed in an area linking the device electrodes 2, 3 (
The substrate was taken out of the chamber and connection between the device electrodes 2, 3 and the wirings 62, 63 was treated by laser. Then, measurement of sheet resistance of each of 20 lines of devices (2000 devices) yielded 24.4±1 kΩ/sq and fluctuations in resistance were ±4%.
Similarly to Example 6, the device electrodes 2, 3 and the wirings 62, 63 were formed on the glass substrate 101 and four droplets of palladium/chrome compound solution used in Example 3 were applied at a time between the device electrodes 2, 3 using an inkjet injection system.
Next, the substrate was heated in an oven in the atmosphere at 350° C. for 30 min while being irradiated with UV. The substrate formed in this manner was maintained in a vacuum chamber. The X-direction wiring 62 and the Y-direction wiring 63 were respectively connected to a group of probes in the chamber so that energization and resistance measurement could be performed from outside the chamber. Air was exhausted from inside the chamber using a turbo molecular pump and a scroll pump until pressure inside the chamber reached 1×10−6 Pa or less. Subsequently, the temperature of the stage was increased to heat the substrate. The temperature was increased from the room temperature to 300° C. in three hours and kept at 300° C. for 10 hours. Then, the temperature was decreased to finish the heating. Palladium oxide was reduced by the heating process in a vacuum and the conductive film 4 made of palladium and chrome oxide was formed.
Subsequently, the electron-emitting portion 5 was formed in the conductive film 4 by the following forming process while keeping a vacuum state inside the chamber.
The voltage applied to each device had rectangular waveforms. Pulses with the pulse width of 0.1 ms and pulse interval of 50 ms were applied. Voltage application started with 1 V and was increased by 0.1 V every five seconds until the voltage reached 20 V when the voltage application was finished. When the voltage of about 13 to 15 V was applied in the course of increasing the voltage, a forming gap was formed in the conductive film 4 due to an influence of Joule heat resulting from energization and when the voltage application was finished, resistance of the conductive film 4 rose to 1 MΩ or more in all lines. In this manner, as shown in
Subsequently, tolunitrile vapor was introduced into the chamber at the partial pressure of 1.3×10−4 Pa and a pulse voltage was applied to the conductive film 4 for 30 min for activation. Rectangular pulses of 18 V and 1 ms and those of −18 V and 1 ms were alternately applied at 100 Hz. This treatment was to cause carbon to deposit near the electron-emitting portion 5 formed on the substrate to increase the amount of electron emission. Observation of a device current during the activation process showed a uniform increase in current in the whole conductive film 4.
With the above processes, a surface conduction electron source substrate having no non-uniform electron emission efficiency of individual electron-emitting devices on the substrate could be formed.
Further, using the electron source substrate, an image display apparatus as shown in
As a result, it was observed that a uniform display without non-uniformity was achieved over the whole display screen.
While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2007-207347, filed on Aug. 9, 2007, which is hereby incorporated by reference in its entirety.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2007-207347 | Aug 2007 | JP | national |
