Electric lamp and discharge devices – With luminescent solid or liquid material – Vacuum-type tube
Reexamination Certificate
2001-02-22
2004-11-16
Cariaso, Alan (Department: 2875)
Electric lamp and discharge devices
With luminescent solid or liquid material
Vacuum-type tube
C252S30140H, C252S30140R
Reexamination Certificate
active
06819041
ABSTRACT:
BACKGROUND OF THE INVENTION AND RELATED ART STATEMENT
The present invention relates to a luminescence crystal particle which emits light upon irradiation with an energy beam, a luminescence crystal particle composition, a display panel constituted of such luminescence crystal particles and a flat-panel display having such a display panel.
As an image display device that can be substituted for a currently mainstream cathode ray tube (CRT), flat-screen (flat-panel) displays are studied in various ways. Such fat-panel displays include a liquid crystal display (LCD), an electroluminescence display (ELD) and a plasma display (PDP). There has been also proposed a cold cathode field emission display capable of emitting electrons into a vacuum from a solid without relying on thermal excitation, a so-called field emission display (FED), and it attracts attention from the viewpoint of the brightness of a display screen and low power consumption.
FIG. 1
 shows a typical constitution of the cold cathode field emission display. In this display, a display panel 
20
 and a back panel 
10
 are placed so as to face each other, and these two panels 
10
 and 
20
 are bonded to each other through a frame (not shown) in their circumferential portions. A space closed with these two panels forms a vacuum space. The back panel 
10
 has cold cathode field emission devices (to be referred to as “field emission devices” hereinafter) as electron-emitting elements. One example shown in 
FIG. 1
 is a so-called Spindt-type field emission device having a conical electron-emitting portion 
16
. The Spindt-type field emission device comprises a stripe-shaped cathode electrode 
12
 formed on a substrate 
11
; an insulating layer 
13
 formed on the cathode electrode 
12
 and the substrate 
11
; a stripe-shaped gate electrode 
14
 formed on the insulating layer 
13
; and a conical electron-emitting portion 
16
 formed in an opening portion 
15
 formed in the gate electrode 
14
 and the insulating layer 
13
. The electron-emitting portion 
16
 is formed on a portion of the cathode electrode 
12
 which portion is positioned in a bottom portion of the opening portion 
15
. Generally, a number of such electron-emitting portions 
16
 are formed to correspond to one of phosphor layers 
22
 to be described later. A relatively negative voltage (video signal) is applied to the electron-emitting portion 
16
 from a cathode electrode driving circuit 
31
 through the cathode electrode 
12
, and a negatively positive voltage (scanning signal) is applied to the gate electrode 
14
 from a gate electrode driving circuit 
32
. An electric field is generated due to the application of these voltages, and due to the electric field, electrons are emitted from the top end of the electron-emitting portion 
16
 on the basis of a quantum tunnel effect. The electron-emitting element shall not be limited to the above Spindt-type field emission device, and field emission devices of other types such as edge-type, flat-type or crown-type field emission devices are used in some cases. Further, reversibly, the scanning signal may be inputted to the cathode electrode 
12
, and the video signal may be inputted to the gate electrode 
14
.
The display panel 
20
 has a plurality of phosphor layers 
22
 which are formed on a support member 
21
 made of glass or the like and have the form of dots or stripes, and an anode electrode 
24
 made of an electrically conductive reflection film formed on the phosphor layers 
22
 and the support member 
21
. A positive voltage higher than the positive voltage applied to the gate electrode 
14
 is applied to the anode electrode 
24
 from an accelerating power source (anode electrode driving circuit) 
33
, and it works to guide electrons emitted from the electron-emitting portion 
16
 to the vacuum space toward the phosphor layer 
22
. Further, the anode electrode 
24
 functions to protect the phosphor particles constituting the phosphor layer 
22
 from sputtering by particles such as ions, functions to reflect light emitted from the phosphor layers 
22
 on the basis of electron excitation to the side of the support member 
21
 to improve the brightness of a display screen observed from an outside of the support member 
21
, and functions to prevent excess charge to stabilize the potential of the display panel 
20
. That is, the anode electrode 
24
 not only carries out its function as an anode electrode but also carries out the function of a member known as a metal back layer in the field of a cathode ray tube (CRT). The anode electrode 
24
 is generally constituted of a thin aluminum film. A black matrix 
23
 is formed between one phosphor layer 
22
 and another phosphor layer 
22
.
FIG. 2A
 shows a schematic plan view of the display panel having phosphor layers 
22
R, 
22
G and 
22
B formed in the form of dots, and 
FIG. 2B
 shows a schematic partial cross-sectional view taken along a line X—X in 
FIG. 2A. A
 region where the phosphor layers 
22
R, 
22
G and 
22
B are arranged is an effective field which carries out a practical function, and a region where the anode electrode is formed is nearly in agreement with the effective field. For clear showing in 
FIG. 2A
, the region where the anode electrode is formed is provided with slanting lines. A circumferential region to the effective field is an ineffective field for supporting the function of the effective field, where peripheral circuits are formed and a display screen is mechanically supported.
In the cold cathode field emission display, the anode electrode is not necessarily required to be constituted of the anode electrode 
24
 made of an electrically conductive reflection film. It may be constituted of an anode electrode 
25
 made of a transparent electrically conductive film formed on the support member 
21
, as is shown in 
FIG. 2C
 which is a schematic partial cross-sectional view similarly taken along a line X—X in FIG. 
2
A. On the support member 
21
, each of the anode electrodes 
24
 and 
25
 is formed nearly on the entire surface of the effective field.
FIG. 3A
 shows a schematic plan view of the display panel having the phosphor layers 
22
R, 
22
G and 
22
B formed in the form of stripes, and 
FIGS. 3B and 3C
 show schematic partial cross-sectional views taken along a line X—X in FIG. 
3
A. In 
FIGS. 3A
, 
3
B and 
3
C, the same portions as those in 
FIGS. 2A
, 
2
B and 
2
C are shown by the same reference numerals, and detailed explanations of the same portions are omitted. 
FIG. 3B
 shows a constitution in which the anode electrode 
24
 is made of an electrically conductive reflection film, and 
FIG. 3C
 shows a constitution in which the anode electrode 
25
 is made of a transparent electrically conductive film. Each of the anode electrodes 
24
 and 
25
 is formed nearly on the entire surface of the effective field of the display panel.
In the cold cathode field emission display that is a flat-panel display, the flying distance of electrons is far smaller than the counterpart in a cathode ray tube, so that it is difficult to increase an electron-accelerating voltage to the level of an electron-accelerating voltage in the cathode ray tube. In the cold cathode field emission display, if the electron-accelerating voltage is too high, spark discharge is liable to take place between the electron-emitting portion in the back panel and the film which functions as an anode electrode in the display panel, and the display quality of the cold cathode field emission display may be impaired to a great extent. The accelerating voltage is therefore controlled to be approximately 10 kilovolts or lower.
In addition to the above problem, the cold cathode field emission display for which it is required to select the above low electron-accelerating voltage involves characteristic problems from which the cathode ray tube is free. In a cathode ray tube permitting the acceleration at a high voltage, electrons enter the phosphor layers deep, so that the electron energy is received in a relatively broad region inside the phosphor layers to excite a relatively large 
Cariaso Alan
Dong Dalei
Kananen Ronald P.
Rader & Fishman & Grauer, PLLC
Sony Corporation
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