EP0912991A2

EP0912991A2 - Flat fluorescent light for background lighting and liquid crystal display device fitted with said flat fluorescent light

Info

Publication number: EP0912991A2
Application number: EP98925418A
Authority: EP
Inventors: Frank Vollkommer; Lothar Hitzschke
Original assignee: Patent Treuhand Gesellschaft fuer Elektrische Gluehlampen mbH
Current assignee: HITZSCHKE, LOTHAR, DR.; VOLLKOMMER, FRANK, DR.; Osram GmbH
Priority date: 1997-03-21
Filing date: 1998-03-20
Publication date: 1999-05-06
Anticipated expiration: 2018-03-20
Also published as: JP3264938B2; TW412770B; HU224147B1; HUP0000863A3; WO1998043277A3; JP2000503801A; HUP0000863A2; CN1220771A; US6034470A; CN1267967C; CA2256346A1; ATE261188T1; US6853124B1; CA2256346C; KR100375615B1; DE59810890D1; EP0912991B1; WO1998043277A2; KR20000015788A

Abstract

The invention relates to a flat fluorescent light (1) having a discharge vessel (2) comprising a base plate (7), a cover plate (8) and a frame (9) forming a gastight soldered connection. Structures resembling strip connectors act as electrodes (3-6) inside the discharge vessel. Said structures also act as conductors in the conductor area and as external electricity inlets (13; 14) on the outside. This configuration enables simple and easily automated manufacturing of flat lights in different sizes. Moreover, an almost infinite variety of electrode shapes can be made, specially with regard to creating a homogenous and optimized light density with reduced density loss on the edges of said light. At least the anodes (5, 6) are covered by a dielectric coating (15). Preferably, the light (1) is operated by pulse voltage source and is used for background lighting of LCD's, e.g. in monitors or diver information displays.

Description

Flat fluorescent lamp for backlighting and liquid crystal display device with this flat fluorescent lamp

Technical field

The invention relates to a flat fluorescent lamp for background lighting according to the preamble of claim 1. The invention also relates to a lighting system according to the preamble of claim 18 with this flat fluorescent lamp. Furthermore, the invention relates to a liquid crystal display device according to the preamble of claim 19 with this lighting system.

The term "flat fluorescent lamp" here means fluorescent lamps with a flat geometry that emit white light. They are primarily designed for the backlighting of liquid crystal displays, also known as LCDs (Liquid Crystal Displays).

Furthermore, these are flat lamps with strip-like electrodes, in which either the electrodes of one polarity or all electrodes, i.e. both polarities, are separated from the discharge by means of a dielectric layer (one-sided or two-sided dielectric barrier discharge). Such electrodes are also referred to in the following as "dielectric electrodes".

Under the term "strip-like electrode" - also called "electrode strip" for short - here and in the following an elongated, in Compared to its length, a very thin and narrow structure can be understood which is able to act as an electrode. The edges of this structure need not necessarily be parallel to one another. In particular, substructures should also be included along the long sides of the strips.

The dielectric layer can be formed by the wall of the discharge vessel itself, in that the electrodes are arranged outside the discharge vessel, for example on the outer wall. An advantage of this design with external electrodes is that no gas-tight leadthrough has to be passed through the wall of the discharge vessel. However, the thickness of the dielectric layer - an important parameter that influences, among other things, the ignition and the operating voltage of the discharge - is essentially determined by the requirements placed on the discharge vessel, in particular its mechanical strength.

On the other hand, the dielectric layer can also be implemented in the form of an at least partial covering or layer of at least the anodic part of the electrodes arranged within the discharge vessel. This has the advantage that the thickness of the dielectric layer can be optimized for the discharge properties. However, internal electrodes require gas-tight leadthroughs. As a result, additional manufacturing steps are required, which generally makes the manufacturing more expensive.

Liquid crystal display devices have recently been used in particular in portable computers (laptops, notebooks, palmtop or the like), but also for stationary computer monitors. Further areas of application are information displays in control rooms of industrial plants or flight monitoring devices, displays of cash register systems and automatic cash dispensing systems and television sets, to name just a few. Liquid crystal display devices are also increasingly being used in automotive Mobile technology used for so-called driver information systems. Liquid crystal display devices require a backlight which illuminates the entire liquid crystal display as brightly and evenly as possible.

State of the art

WO 94/23442 discloses a method for operating an incoherently emitting radiation source, in particular a discharge lamp, by means of dielectrically impeded discharge. The operating method provides a sequence of active power pulses, the individual active power pulses being separated from one another by dead times. As a result, a plurality of similar discharges, similar to delta-like (Δ), burn in the plan view, that is perpendicular to the plane in which the electrodes are arranged, between adjacent electrodes of different polarity. These individual discharges are lined up along the electrodes, each widening in the direction of the (current) anode. In the case of alternating polarity of the voltage pulses of a bilaterally dielectric discharge, a superimposition of two delta-shaped structures appears visually. Since these discharge structures are preferably generated with repetition frequencies in the kHz range, the viewer perceives only a "medium" discharge structure corresponding to the temporal resolution of the human eye, for example in the form of an hourglass. The number of individual discharge structures can be influenced, inter alia, by the electrical power that is coupled in. Another advantage of this pulsed mode of operation is the high efficiency of the radiation generation. This mode of operation is also suitable for flat lamps of the type described at the outset, as has already been demonstrated in WO 94/04625. A flat radiator is known from WO 94/04625, which is operated in accordance with the operating method of WO 94/23442. Due to the very efficient mode of operation, the flat radiator produces relatively little heat loss. In the exemplary embodiments, strip-shaped electrodes are arranged on the outer wall of the discharge vessel with the disadvantages described at the outset. Another disadvantage of this solution is that the surface luminance drops significantly towards the edge. The reason for this is, among other things, the radiation contribution from the neighboring areas outside of the discharge vessel which is missing at the edge. In addition, the individual discharges preferably form between the anodes and only one of the two immediately adjacent cathodes. Apparently, individual discharges do not form simultaneously on both sides of the anode strips. Rather, it cannot be predicted from which of the two adjacent cathodes the discharges will form in each case. In relation to the flat radiator as a whole, this results in an irregular discharge structure and, consequently, in a temporally and spatially non-uniform surface luminance.

A uniform surface luminance is desirable for numerous applications of such spotlights. For example, backlighting LCDs requires visual uniformity, the modulation depth of which does not exceed 15%.

DE 19548 003 AI specifies a circuit arrangement with the aid of which unipolar pulse voltage sequences can be generated, such as are required in particular for the efficient operation of discharges which are dielectrically impeded on one side. Smooth impulses with low circuit losses are also achieved on predominantly capacitive loads - such as dielectrically disabled discharge arrangements. EP 0 363 832 discloses, among other things, a UV high-power radiator with strip-shaped electrodes which are arranged on the inner wall of the base plate of the discharge vessel. However, no information is provided on current feedthroughs for connecting the inner electrodes to a voltage source. The UV high-performance lamp is operated with sinusoidal AC voltage. As is known, the achievable UV yields in AC operation are limited to less than approximately 15%. However, higher yields are required for efficient backlighting of LCD systems. In addition, an exemplary embodiment with cooling channels integrated in the base plate is also given, which is impractical for many applications, in particular in the office area and in mobile use.

A liquid crystal display with a surface lighting device is known from EP 0 607453. The area lighting device essentially consists of a plate-shaped light guide and at least one curved rod-shaped fluorescent lamp. The fluorescent lamp is arranged according to the bend on two or more abutting edges of the light guide plate. As a result, the light from a fluorescent lamp is already coupled into the light guide plate at the at least two edges and is scattered by the plate surface facing the liquid crystal display. This measure is intended to achieve good illumination without a correspondingly large number of lamps being required. The disadvantage of this solution is that an optical fiber plate cannot be dispensed with. Furthermore, external reflectors are additionally provided along the lamps, which laterally reflect part of the lamp light into the light guide plate. Nevertheless, in the redistribution from the linear (rod-shaped fluorescent lamp) to the planar (light guide plate) light source, inevitable coupling and scattering losses occur, which reduce the achievable surface luminance. In addition, the lifespan of the Area lighting device limited by the fluorescent lamps. When using multiple fluorescent lamps, the error rate of the entire device increases.

Further disadvantages in the case of fluorescent lamps based on mercury low-pressure discharges result from the properties of the mercury itself. On the one hand, the mercury must first reach its operating vapor pressure, i.e. Fluorescent lamps of this type show a pronounced start-up behavior, which makes switching off a PC monitor equipped with it appear to be inadvisable during a work break. In addition, mercury is harmful to health and must therefore be disposed of as special waste.

Presentation of the invention

It is an object of the present invention to provide a flat fluorescent lamp with strip-like inner electrodes according to the preamble of claim 1, which has an electrode structure and current feedthroughs such that the flat radiator - largely independent of the size and thus the number of electrodes - in relatively few Manufacturing steps and consequently inexpensive to manufacture. Another aspect is the simple design of the electrode structures in terms of production technology, which enables low-cost implementation of flat fluorescent lamps with increased and uniform surface luminance.

This object is achieved by the characterizing features of claim 1. Particularly advantageous refinements can be found in the claims dependent thereon.

Another object of the present invention is to provide a lighting system according to the preamble of claim 18. This Object is solved by the characterizing features of claim 18.

Finally, it is an object of the present invention to provide a liquid crystal display device according to the preamble of claim 19. This object is achieved by the characterizing features of claim 19.

The basic idea of the first part of the invention is to design the inner electrodes, including bushings and outer current leads, as three functionally different sections, each of a single, interconnected, conductor-like structure on the cathode or anode side.

With this concept, the three functionally different parts mentioned - inner electrodes, bushings and outer power supplies - can be produced almost simultaneously in a common manufacturing step, preferably using printing technology. Compared to the prior art, the number of handling and manufacturing steps is significantly reduced. In addition, connections by means of soldering or the like are omitted. between the individual components.

The two structures also offer the advantage of almost any formability. As a result, the shapes of the electrodes, which are optimized to a uniform surface luminance up to the edges, can be implemented in a technically simple and cost-effective manner. For this, for example, only a structured pressure screen has to be designed accordingly. Another advantage of the invention is that the constructive concept enables the cost-effective production of flat fluorescent lamps of almost any size, since all production steps can always be carried out in the same way practically regardless of the size of the spotlight. It can be used to economically implement transmit flat lamps for the backlighting of different sized liquid crystal displays. Further advantages are the high luminance and the high luminous efficacy, a typical specific luminous intensity is approx. 8 cd / W for a lamp including optical diffuser. A number of other advantages of flat lamps in connection with the pulsed operating mode are listed below. Since pulsed, dielectrically impeded discharges have a positive current-voltage characteristic, any number of individual discharges can be arranged next to one another, so that, in principle, flat lamps of almost any size can be realized. In addition, these flat lamps can be operated with only one electrical ballast. Since the filling of the lamp contains no mercury, there is no risk of poisonous mercury vapors and the disposal problem is eliminated. Another advantage of the mercury-free filling is the immediate start of the lamp without starting. Due to the layered electrode structure without filigree individual parts, the lamp is also extremely robust and has a long service life.

According to the invention, the discharge vessel is constructed from a base plate and a cover plate, which are separated by a frame and by means of solder, e.g. Glass solder, are connected to each other to form a closed discharge vessel. On the inner wall of the discharge vessel, gas-tight, strip-like electrodes are applied directly to the base and / or ceiling plate - similar to conductor tracks on an electrical circuit board, e.g. by vapor deposition, screen printing with subsequent baking or similar techniques.

One end of the electrode strips is guided gas-tight to the outside through the solder. The seal between the bushing and frame as well as between the frame and the floor or ceiling plate takes over. In order to keep stresses from different thermal expansions low and to ensure gas tightness even in continuous operation, the materials for solder and frame as well as the floor and ceiling slab are coordinated. In addition, the thicknesses of the preferably metallic electrode strips are chosen to be so thin that on the one hand the thermal stresses remain low and on the other hand the current intensities required during operation can be achieved.

A sufficiently high current carrying capacity of the conductor tracks is of particular importance insofar as the high luminous intensities sought for such flat lamps ultimately require high current intensities. In the case of flat fluorescent lamps for the backlighting of liquid crystal displays (LCD), a particularly high light intensity is essential because of the low transmission of such displays of typically 6%. This problem is exacerbated again in the preferred pulsed operating mode of the discharge, since particularly high currents flow in the conductor tracks during the relatively short duration of the repetitive active power coupling. Only in this way is it possible to couple in sufficiently high average active powers and thereby achieve the desired high light intensity on average.

In order to ensure the aforementioned high current carrying capacity, relatively thick conductor tracks are used. Too small conductor thicknesses harbor the risk of cracks due to local overheating of the conductor paths. The heating of the conductor tracks by the ohmic portion of the conductor rail current is higher, the smaller the cross-sectional area of the conductor tracks. However, there are limits to the width of the conductor tracks, among other things because the shading of the illuminated surface of the flat radiator by the conductor tracks also increases with increasing width. For this reason, rather narrow, but as thick as possible conductor tracks are sought to avoid the problem of cracking due to the development of heat to solve by high current densities in the conductor tracks. Typical thicknesses for conductive silver strips are in the range from 5 μm to 50 μm, preferably in the range from 5.5 μm to 30 μm, particularly preferably in the range from 6 μm to 15 μm.

However, such thick conductor tracks on relatively extensive flat carrier materials, such as are used in flat lamps, lead to the formation of cracks due to material stresses, which can result, for example, from the bending stresses when the discharge vessel is evacuated during the manufacturing process. The reason for the growing risk of crack formation is the dependence of the elongation limit ε of a layer on its thickness d according to ε ° l / Vcf. Accordingly, the stretch limit is lower the greater the layer thickness. In addition, the likelihood of discontinuities within the layer increases dramatically with increasing layer thickness. These discontinuities lead to locally increased tensile stresses within the layer. This ultimately results in the risk of the layer becoming detached from the carrier material.

Surprisingly, it has been shown that flat lamps with such thick conductor tracks can nevertheless be produced in a gas-tight manner and that the service life can also be quite a few thousand hours.

Support points, for example in the form of glass spheres, which are arranged at a suitable distance from one another between the floor and ceiling panels, may also contribute to this, which give the flat radiator sufficient bending stability without causing unacceptably strong shading.

According to the current state of knowledge, among other things, the two parameters d _st - d _E1 and P ₂ = d _St / d _P1 as relevant for life Duration of the flat radiator viewed, where d _st the distance between the support points to each other or to the delimiting side wall, d _E1 the thickness of the electrode tracks and d _P1 the smaller of the two thicknesses of the floor or ceiling plate. Typical values for P _: are in the range from 50 mm μm to 680 mm μm, preferably in the range from 100 mm μm to 500 mm μm, particularly preferably from 200 mm μm to 400 mm μm. Typical values for P ₂ are in the range from 8 to 20, preferably in the range from 9 to 18, particularly preferably from 10 to 15.

Good experiences have been made, for example, with 10 μm thick printed silver layers and glass balls fitted between each 2.5 mm thick floor and ceiling plate at a mutual distance of approx. 34 mm using glass solder. These values result in T. = 340 mm μm and P ₂ = 13.6.

As already mentioned, against the background of the risk of crack formation, it is in principle advantageous to realize the large cross-sectional areas of the conductor tracks, which are also required because of the high load-bearing capacity required, instead of mainly using a large thickness, by means of a corresponding width of the conductor tracks. Especially when electrodes are on both the bottom and the top plate, i.e. are consequently also arranged on the inside of the primary luminous surface of the flat spotlight, the problem of shadowing by the conductor tracks themselves can at least be alleviated as follows.

For this purpose, the anodes and / or cathodes are each composed of two electrically conductive components coupled to one another. The first component is designed as a relatively narrow strip, but it is made of a material capable of withstanding high currents, preferably of metal, for example gold or silver. The second component is designed as a wider strip than the first component. For that he is targeted from one material essentially transparent for visible radiation, for example made of indium tin oxide (ITO). Because of the larger width of the strip that is possible as a result, despite the possibly lower electrical conductivity, the overall current carrying capacity of the second component is also sufficient. Both components are in electrical contact with each other. In this way, a sufficiently large electrode area - an important parameter for the dielectric barrier discharge - is also realized.

In one variant, the two components are galvanically separated from one another by a dielectric. The coupling between the two components is capacitive. The second component is preferably arranged closer to the inside of the discharge vessel than the first component. In addition, only the first component is continued as a feedthrough and power supply to the outside. In this case, the second component merely serves to enlarge the effective electrode area within the discharge vessel.

At least the inner wall of the ceiling panel is coated with a mixture of phosphors, which converts the UV / VUV radiation from the gas discharge into white light during operation. To be able to convert as much of the UV / VUV radiation as possible, i.e. In order to maximize the luminous flux, the inner wall of the discharge vessel is complete, i.e. Ceiling plate, frame and base plate coated with the phosphor mixture.

The outer power supply lines are arranged on an outer edge of the floor and / or ceiling plate and / or the frame. For this purpose, the base plate or the ceiling plate is or are extended beyond the frame, at least on the sides of the flat lamp on which the bushings lead from the inside of the discharge vessel to the outside. Outside the discharge vessel, the electrode strips end after the lead-through area in a number of external current leads corresponding to the number of electrode strips. Viewed individually, each electrode strip is thus designed as a structure similar to a conductor track, which in each case comprises the three following, functionally different partial areas: inner electrode area, lead-through area and outer current supply area.

The connection of the power supply lines of the same polarity to the two poles of a pulse voltage source takes place, for example, with the aid of a suitable plug-cable combination.

In addition, the electrode strips of the same polarity can merge into a common, bus-like external power supply. In operation, these two external power supplies can be connected directly to one pole of the voltage source. In this case, there is no need for a special plug-cable combination.

In a first embodiment, the strip-like electrodes are arranged next to one another on the base plate (case I). This results in an essentially flat discharge structure during operation. The advantage is that shadowing from the electrodes on the illuminated ceiling panel is avoided. Between the cathode strips are two parallel anode strips, i.e. an anode pair, instead of a single anode strip previously arranged. This solves the problem described at the outset that, in the cited prior art, individual discharges burn from only one of two adjacent cathode strips in the direction of the individual anode strip lying between them.

In a variant, the two anode strips of each anode pair are widened in the direction of their respective two narrow sides. Along the broadening, an increasing electrical current density and consequently also an increasing luminance of the individual discharges is achieved. The advantage is a relatively uniform luminance distribution up to the edges of the flat lamp.

The anode strips are widened asymmetrically with respect to their longitudinal axis in the direction of the respective anodic partner strip. As a result of this measure, the respective distance from the adjacent cathode remains constant despite the widening of the anode strips. Consequently, the ignition conditions for all individual discharges along the electrode strips are the same during operation. This ensures that the individual discharges are lined up along the entire length of the electrode (provided there is sufficient electrical input power).

The anode strips can also be widened in the direction of the respective adjacent cathode without the advantageous effect of the widening being lost in principle. In this case, however, the broadening is only relatively weak. This prevents the discharges from occurring only at the location of the greatest width of the anode strip, i.e. at the location of the shortest stroke distance in this case. The broadening is significantly smaller than the stroke distance, typically about a tenth of the stroke distance. Furthermore, both types of distribution can also be combined, i.e. the widening is then both in the direction of the respective anode partner and also to the adjacent cathode.

The electrode structure for a bilaterally disabled discharge is preferably of symmetrical design, since in this case the polarity of the electrodes changes. As a result, each electrode acts alternately as an anode or cathode. The basic relationships of the structure are shown schematically in FIG. 1. The entire conductor track-like structure 100 consists of a first part 101 and a second part 102. Both parts 101, 102 have the double anode strips 103a and 103b or 104a and 104b already described, the double anode strips 103a, b of the first part 101 and the double anode strips 104a, b of the second part 102 of the structure being arranged alternately next to one another. Both parts 101, 102 of the electrode structure are covered with a dielectric layer (not shown). At their mutually opposite ends the double anode strips 103a, b; or 104a, b into bus-like external power supply lines 105; 106 a. In operation, the two outer power supply lines 105; 106 each connected to one pole of the voltage source (not shown).

In a variant for a unilaterally or bilaterally disabled discharge with unipolar voltage pulses, the cathode strips specifically have spatially preferred starting points for the individual discharges. To clarify the basic relationships, the electrode structure for a flat lamp with a diagonal of 6.8 "is shown schematically in FIG. 2. The anode-side structure 107 has the double anode strips 108a and 108b already mentioned several times. The anode-side structure 107 is terminated on both sides a single anode strip 109 and 110. In the case of the cathode strips 111 of the structure 112 on the cathode side, the preferred starting points are realized by nose-like extensions 113 facing the respectively adjacent anode strip. They cause locally limited amplifications of the electric field and consequently that the delta-shaped individual discharges (not ignite) only at these points 113. This enables a uniform distribution of the individual discharges within the flat discharge vessel to be forced during operation, without the extensions the individual discharges would occur during the vertical B Due to convection, it is increasingly moving into the upper area of the flat lamp. The extensions to the respective two narrow sides of the strip-like cathodes are preferably spatially arranged more densely (not shown; see FIG. 3a). The advantage is again a relatively uniform luminance distribution up to the edges of the flat lamp, ie the disadvantage of the drop in the luminance in the prior art mentioned at the outset is effectively eliminated. The anode 109a, b and cathode strips 111 open at their mutually opposite ends into an anode-side 114 and cathode-side 115 bus-like external power supply. In operation, the anode-side power supply 114 is connected to the positive pole (+) and the cathode-side power supply 115 to the negative pole (-) of a voltage source (not shown) supplying unipolar voltage pulses.

In addition, in one embodiment the feature of widening the double anode strips can also be combined with the feature of the compression of the cathode processes.

In a further embodiment, anode and cathode strips are arranged on different plates (case II). In operation, the discharges consequently burn from the electrodes of one plate through the discharge space to the electrodes of the other plate. Two anode strips are assigned to each cathode strip in such a way that, when viewed in cross-section with respect to the electrodes, the imaginary connection of cathode strips and corresponding anode strips results in the shape of a “V” It has been shown that this arrangement can achieve higher UV yields than if anodes and cathodes are arranged alternately next to one another on the basis of the current state of knowledge, this positive effect is attributed to reduced wall losses the double anode strips are arranged on the ceiling plate, which primarily serves to decouple light, and the cathode strips are arranged on the base plate. The advantage is the low shadowing of the ceiling plate Useful light, since the anode strips are narrower than the cathode strips.

In the case of the type II flat lamp, the two-part electrodes explained above can be used with particular advantage to reduce the shading effect. For this purpose, at least the anode strips are advantageously each composed of a narrow, high-current-carrying and a wide transparent component.

In addition, it is also advantageous for case II if the cathode strips have extensions, as in case I. To minimize the edge drop in the luminance, there is also a compression of these extensions and / or

Widening of the anode strips to the edge of the flat lamp advantageous.

Furthermore, it is advantageous to apply a light-reflecting layer, for example Al ₂ O _a and / or Ti0 ₂ , to the base plate. This prevents part of the white light which is emitted by the phosphor layer by converting the UV / VUV radiation from being transmitted through the base plate and being lost through the base plate for the direction of use.

Inside the discharge vessel there is an inert gas, preferably xenon and possibly one or more buffer gases, e.g. Argon or neon. The internal pressure is typically approx. 10 kPa to approx. 100 kPa.

In particular for relatively large flat lamps, it may be appropriate to insert balls made of an electrically insulating material, for example glass, as spacers or support points between the floor and ceiling panels. This increases the mechanical stability and reduces the risk of implosion due to the pressure difference between inside and outside. It is advisable to fix the balls with solder. It is also advantageous to provide the support points with a reflection and a light to provide a layer of fabric to maximize the luminance of the flat lamp.

Protection is also claimed for a lighting system which consists of the aforementioned new flat lamp and a pulse voltage source.

The lighting system according to the invention is completed by a pulse voltage source, the output poles of which are connected to the external power supply lines of the electrodes of the discharge vessel and which supplies a sequence of voltage pulses during operation. A suitable circuit arrangement for generating unipolar pulse voltage sequences is described in German patent application P 195 48 003.1. The lighting system can also be operated with unipolar and bipolar pulse voltages, e.g. are generated by the circuit disclosed in WO96 / 05653.

Protection is also claimed for a liquid crystal display device which uses the aforementioned lighting system as background lighting for the liquid crystal display.

The liquid crystal display device according to the invention in turn uses this lighting system as backlighting for the liquid crystal display. For this purpose, the device contains a receptacle in which the liquid crystal display including control electronics for controlling the liquid crystal display and the lighting system are arranged. The lighting system and the liquid crystal display are oriented to one another in such a way that the ceiling plate of the flat lamp of the lighting system illuminates the rear of the liquid crystal display. An optical diffuser is optionally arranged between the flat lamp and the liquid crystal display. It serves to smooth the luminance of the flat lamp. This is particularly advantageous in the case of large-area displays in order to compensate for shadowing caused by the glass spheres which act as support points. Furthermore, so-called light reinforcement films, also known as BEF (Brightness Enhancement Film), are optionally arranged between the flat lamp and the liquid crystal display or, if appropriate, between the diffuser and the liquid crystal display. They serve to concentrate the light from the backlight in a narrower solid angle and consequently to increase the brightness within the viewing angle range. The mercury-free filling of the flat lamp enables an immediate start without start-up behavior. This makes it possible to switch off the flat lamp even when the display device is not used for a short time, for example during a work break, and consequently to save electrical energy. It is also advantageous that the proposed liquid crystal display device manages without external reflectors and light guiding devices, which reduces the number of components and consequently the system costs.

Description of the drawings

In the following, the invention will be explained in more detail using an exemplary embodiment. Show it:

FIG. 1 shows the principle of an electrode structure according to the invention for a bilaterally disabled discharge,

FIG. 2 shows the basic relationships of the electrode structure for a flat lamp with a diagonal of 6.8 ", preferably to be operated with unipolar voltage pulses, FIG. 3a shows a schematic representation of a partially broken top view of a flat lamp according to the invention with electrodes arranged on the base plate,

Figure 3b is a schematic representation of a side view of the flat lamp from Figure 3a.

FIG. 4 shows the sectional view of the implementation of a double anode,

FIG. 5 a flat lamp with a pulse voltage source,

FIG. 6a shows a schematic illustration of a side view of a flat lamp with electrodes arranged on both the base plate and the cover plate,

FIG. 6b shows a partial sectional view of some bushings of the flat lamp from FIG. 6a,

Figure 7 shows a liquid crystal display device according to the invention including a flat lamp.

FIG. 8a shows a schematic representation of a partially broken top view of a further flat lamp according to the invention with electrodes arranged on the base plate,

FIG. 8b shows a schematic illustration of a side view of the flat lamp from FIG. 8a,

Figure 9 is a partial sectional view of a flat lamp with two-part anodes.

FIGS. 3a, 3b show a schematic representation of a top view and side view of a flat fluorescent lamp that emits white light during operation emitted. It is designed as a backlight for an LCD (Liquid Crystal Display).

The flat lamp 1 consists of a flat discharge vessel 2 with a rectangular base area, four strip-like metallic cathodes 3, 4 (-) and dielectric anodes (+), three of which are designed as elongated double anodes 5 and two as individual strip-like anodes 6. The discharge vessel 2 in turn consists of a base plate 7, a cover plate 8 and a frame 9. Base plate 7 and cover plate 8 are each gas-tightly connected to the frame 9 by means of glass solder 10 such that the interior 11 of the discharge vessel 2 is cuboid. The base plate 7 is larger than the cover plate 8 in such a way that the discharge vessel 2 has a peripheral free-standing edge. The inner wall of the ceiling panel 8 is coated with a phosphor mixture (not visible in the illustration), which converts the UV / VUV radiation generated by the discharge into visible white light. It is a three-band phosphor with the blue component BAM (BaMgAlιoOi7- Eu ²⁺ ), the green component LAP (LaPO ^ [Tb ³⁺ , Ce ³⁺ ]) and the red component YOB ([Y, Gd] Bθ3: Eu ³⁺ ). The breakthrough in the ceiling plate 8 is only for illustrative purposes and provides a view of a part of the cathodes 3, 4 and anodes 5, 6.

The cathodes 3, 4 and anodes 5, 6 are arranged alternately and in parallel on the inner wall of the base plate 7. The anodes 6, 5 and cathodes 3, 4 are each extended at one end and guided on the bottom plate 7 from the inside 11 of the discharge vessel 2 on both sides in such a way that the associated anodic 12 or cathodic bushings on opposite sides the bottom plate 7 are arranged. On the edge of the base plate 7, the electrode strips 3, 4, 5, 6 merge into 13 and 14 anode-side external power supply. The outer power supply lines 13, 14 serve as contacts for connection to preferably an electrical pulse voltage source (not shown). The connection to the two poles of a voltage source usually takes place as follows. First of all, the individual anodic and cathodic power supply lines are each connected to one another, for example by means of a suitable plug connector (not shown) including connecting lines. Finally, the two common anodic or cathodic connecting lines are connected to the associated two poles of the voltage source.

In the interior 11 of the discharge vessel 2, the anodes 5, 6 are completely covered with a glass layer 15, the thickness of which is approximately 250 μm.

The two anode strips 5a, 5b of each anode pair 5 are widened in the direction of the two edges 16, 17 of the flat lamp 1, which are oriented perpendicular to the electrode strips 3-6, and asymmetrically only in the direction of the respective partner strips 5b and 5a . The mutual greatest distance between the two strips of each anode pair 5 is approximately 4 mm, the smallest distance is approximately 3 mm. The two individual anode strips 6 are each arranged in the immediate vicinity of the two edges 18, 19 of the flat lamp 1 which are parallel to the electrode strips 3-6.

The cathode strips 3; 4 have nose-like semicircular projections 20 facing the respectively adjacent anode 5; 6. They cause locally limited amplifications of the electric field and consequently that the delta-shaped individual discharges (not shown) ignite and burn only at these points. The extensions 20 of the two cathodes 4, which are immediately adjacent to the edges 18, 19 of the flat lamp 1 parallel to the electrode strips 3-6, are on the sides facing these edges 18, 19 and towards the narrow sides of the electrode strips 4, 5 arranged closer than on the center of the flat lamp 1 turned side. The distance between the extensions 20 and the respective directly adjacent anode strip is approximately 6 mm. The radius of the semicircular extensions 20 is approximately 2 mm.

The individual electrodes 3-6, including feedthroughs and external power supply lines 13, 14, are each designed as functionally different sections of interconnected silver-like structures. The structures have a thickness of approx. 10 μm and are applied directly to the base plate 7 by means of screen printing technology and subsequent baking.

Inside the flat lamp 1 there is a gas filling made of xenon with a filling pressure of 10 kPa.

In a variant (not shown; the design corresponds qualitatively to the illustration in FIG. 2) for the backlighting of a 15 "monitor, 14 ^' double anode strips and 15 cathodes are alternately arranged on the base plate of a flat fluorescent lamp. The two ends of the electrode arrangement form one each The cathodes have 32 semicircular projections offset from one another along their two long sides. The outer dimensions of the lamp are approximately 315 mm • 239 mm • 10 mm (length • width • height). The wall thickness of the base and ceiling plate The frame is made of a glass tube with a diameter of approximately 5 mm. 48 precision glass balls with a diameter of 5 mm are arranged equidistantly between the base and ceiling plate. The anode and cathode strips open at their mutually opposite ends in an anod bus-side external power supply on the side or cathode side (cf. also Figure 2). In operation, the anode-side power supply with the plus pole (+) and the cathode-side power supply connected to the negative pole (-) of a unipolar voltage source supplying voltage pulses.

FIG. 4 schematically shows part of a sectional view along the line AA (see FIG. 3a). The same features are provided with the same reference numbers. The part shown includes, for example, the feedthrough 12 of a double anode 5. In principle, the structure of the remaining electrodes is similar. The two lead-through strips 12a, 12b are applied directly to the base plate 7 and are also completely covered with the glass layer 15. The base plate 7 with the feedthrough 12 including the glass layer 15 are in turn connected gas-tight to the frame 9 by means of glass solder 10. Likewise, the ceiling plate 8 is connected gas-tight to the frame 9 to the discharge vessel 2 by means of glass solder 10.

To operate the flat lamp 1, the cathodes 3, 4 and anodes 5, 6 in FIG. 5 are each connected to a pole 21, 22 of a pulse voltage source 23 via the current leads 13 and 14, respectively. During operation, the pulse voltage source supplies unipolar voltage pulses, which are separated from one another by pauses. A suitable pulse voltage source for this is described in German patent application P19548003.1. A large number of individual discharges (not shown) are formed, which burn between the extensions 20 of the respective cathode 3, 4 and the corresponding immediately adjacent anode strip 5, 6.

FIGS. 6a and 6b schematically show a side view or a partial section perpendicular to the electrodes of a further variant of the flat fluorescent lamp from FIG. 3a. Here the cathodes 24 are applied to the inner wall of the ceiling plate 8. Each cathode 24 is assigned an anode pair 25a, 25b in such a way that, in the cross section of FIG. 6b, the imaginary connection of cathodes 24 and corresponding anodes 25a, 25b is in the form of an upside-down “V” results. The approximate distances between the cathodes 24, between the individual anodes 25a, 25b of the corresponding anode pairs with one another and between the adjacent corresponding anode pairs are 22 mm, 18 mm and 4 mm, respectively. The cathodes 24 each have nose-like semicircular extensions 26a, 26b along their two longitudinal sides and at a mutual spacing of approximately 10 mm. In operation, individual discharges start at these extensions 26a, 26b and burn to their associated anode strips 25a and 25b, respectively. The part shown comprises, by way of example, only two cathodes 24 with their respective anode pair 25a, 25b. The structure and basic arrangement of the remaining electrodes are the same. Cathodes 24 and anodes 25a, 25b are led to the outside on the same narrow side of the fluorescent lamp and pass on the corresponding edge of the top plate 8 or bottom plate 7 into the cathode-side 27 or anode-side 14 outer power supply. As can be seen in the sectional illustration (FIG. 6b), both the anodes 25a, 25b and the cathodes 24 are completely covered with a dielectric layer 28 and 29 (discharge that is dielectrically impeded on both sides), which extends over the entire inner wall of the bottom 7 or cover plate 8 extends. A light-reflecting layer 30 made of A1 ₂ 0 ₃ or TiO _{2 is} applied to the dielectric layer 28 of the base plate 7. The last layer is followed by and also on the dielectric layer 29 of the ceiling plate 8, a phosphor layer 31 or 32 made of a BAM, LAP, YOB mixture.

In Figure 7, a side view, partially in section, of a liquid crystal display device 33 is shown schematically, with the flat fluorescent lamp 1 corresponding to Figure la as background lighting for a liquid crystal display 35 known per se. Between the flat fluorescent lamp 1 and the liquid crystal display 35 is a diffuser 36 as optical diffuser arranged. Between the lens 36 and the liquid crystal display 35 two light amplification foils (BEF) 37, 38 from 3M are arranged. The fluorescent lamp 1, the diffusing screen 36, the two light intensifying foils 37, 38 and the liquid crystal display 35 are arranged in a housing and are held by the frame 39 of the housing. A heat sink 41 is arranged on the outside of the rear wall 40 of the housing. In addition, on the outside of the housing rear wall 40, the circuit arrangement 23 connected to the flat fluorescent lamp 34 corresponding to FIG. 5 and a control electronics 42 known per se and connected to the liquid crystal display 35 are arranged. For further details on a suitable liquid crystal display 35 with control electronics 42, reference is made to EP 0 607453.

The flat lamp 1 ′ shown schematically in plan view and side view in FIGS. 8a-8b differs from flat lamp 1 (FIGS. 3a and 3b) only in the design of the external power supply 12; 13. The feedthroughs 10; 11 of each electrode strip 3; 4 are initially continued on the edge of the base plate 5 and open into a bus-like conductor track on the cathode-side 12 or anode-side 13. The ends (+, -) of these conductor tracks 12; 13 serve as external contacts for the connection to an electrical voltage source (not shown).

FIG. 9 shows a schematic partial sectional illustration of a further variant of the flat lamp. It differs from that shown in FIG. 6b essentially in that the anodes 25a and 25b of each anode pair 25 are made in two parts. They each consist of a narrow silver strip 25 'and a wider transparent indium tin oxide strip 25 ", the silver strip 25' being embedded in the indium tin oxide strip 25". In this way, shading is reduced by the anodes on the ceiling plate, ie their effective transparency for the useful light is increased. The invention is not restricted by the exemplary embodiments specified. Features of different exemplary embodiments can also be combined.

Claims

claims

1. Flat fluorescent lamp (1) for the backlight with an at least partially transparent and filled with a gas filled flat discharge vessel (2) made of electrically non-conductive material, the discharge vessel (2) on its inner wall at least partially a layer of a phosphor or

Has phosphor mixture, and with strip-like electrodes (3-6) arranged on the inner wall of the discharge vessel (2), at least the anodes (5,6) each being covered with a dielectric layer (15), characterized in that

• The discharge vessel (2) consists of a base plate (7), a cover plate (8) and a frame (9), the base plate (7), the cover plate (8) and the frame (9) being gas-tight by means of solder (10) are interconnected

• The strip-like electrodes (3-6) additionally pass through (12) and these into current leads (13, 14) such that the electrodes (3-6), lead-throughs (12) and outer current leads (13, 14) are constructed as structures similar to conductor tracks (3, 4, 13; 5, 6, 14), the leadthroughs being guided to the outside in a gas-tight manner covered by the solder (10) and the immediately adjacent external power supply lines (13, 14) for connection serve an electrical supply source.

2. Flat fluorescent lamp according to claim 1, characterized in that the thickness of the structures in the range between 5 microns and 50 microns, preferably in the range of 5.5 microns to 30 microns, particularly preferably in the range of. 6 μm to 15 μm.

3. Flat fluorescent lamp according to claim 1 or 2, characterized in that spacers are arranged between the floor and the ceiling plate.

4. Flat fluorescent lamp according to claim 3, characterized in that the spacers are realized by glass balls.

5. Flat radiator according to claim 3 or 4, characterized in that the parameter d _St • d _{E1 is} in the range from 50 mm μm to 680 mm μm, preferably in the range from 100 mm μm to 500 mm μm, particularly preferably in the range from 200 mm μm to 400 mm μm, where d _{st is} the distance between the support points or to the delimiting side wall and d _E1 denote the thickness of the electrode tracks.

6. Flat radiator according to one of claims 3 to 5, characterized in that the parameter P ₂ = d _St / dpj is in the range from 8 to 20, preferably in the range from 9 to 18, particularly preferably in the range from 10 to 15, where d _St the distance between the support points to each other or to the delimiting side wall and d _pl the smaller of the two thicknesses of the floor or ceiling slab.

7. Flat fluorescent lamp according to one of claims 1 to 6, characterized in that the strip-like cathodes (3, 4) have nose-like extensions (20) along their long sides.

8. Flat fluorescent lamp according to claim 7, characterized in that the extensions (20) in the direction of the respective two narrow sides of the strip-like cathodes (4) are arranged spatially increasingly densely.

9. Flat fluorescent lamp according to one of the preceding claims, characterized in that the strip-like electrodes (3-6) next to one another on the inner wall of the base plate (7) of the discharge vessel (2), two anode strips (5a, 5b), ie one pair of anodes (5), being arranged between adjacent cathode strips (3,3 and 3,4).

10. Flat fluorescent lamp according to claim 9, characterized in that the two anode strips (5a; 5b) of each anode pair (5) are widened in the direction of their respective two narrow sides.

11. Flat fluorescent lamp according to claim 10, characterized in that the widenings with respect to the respective longitudinal axis of the strips (5a; 5b) are asymmetrical and exclusively in the direction of the respective partner strip (5b or 5a), so that the respective distance between Anode strips (5a, 5b) and adjacent cathode strips (3) and (4) are constant throughout.

12. Flat fluorescent lamp according to one or more of the preceding claims, characterized in that the cathodes (24) and anodes (25) are arranged on different plates, preferably the anodes (25) on the ceiling plate (8) and the cathodes (24) the bottom plate (7), with each cathode (24) being assigned two anodes (25a, 25b) in such a way that the imaginary connection of the cathode (24) and corresponding anodes (25a, 25b) is viewed in cross-section with respect to the electrodes Form of a possibly upside down "V" results.

13. Flat fluorescent lamp according to one or more of the preceding claims, characterized in that the anodes and / or cathodes each consist of two electrically conductive coupled

Components (25 ', 25 ") exist, the first component (25') being a narrow, high-current-carrying strip and the second component te (25 ") as compared to the first component (25 ') wider, substantially transparent for visible radiation strips.

14. Flat fluorescent lamp according to claim 13, characterized in that there is a dielectric between the first and second components and consequently the coupling between the two components is capacitive.

15. Flat fluorescent lamp according to claim 13 or 14, characterized in that in each case only the first component is continued as a feedthrough and current supply to the outside and the second component is only used to enlarge the effective electrode area within the discharge vessel.

16. Flat fluorescent lamp one or more of the preceding claims, characterized in that on the inner wall of the base plate (7), the frame (9) and the spacers, a reflection layer for light is applied.

17. Flat fluorescent lamp according to one or more of the preceding claims, wherein the outer power supply lines are designed such that the leadthroughs (12) of the cathodes (3,4) and anodes (5,6) in a cathode or anode-side bus-like conductor track (13; 14) open.

18. Lighting system with a flat fluorescent lamp (1) and with an electrically conductively connected electrical voltage source (23) connected to the flat fluorescent lamp (1), which is suitable for coupling active power pulses separated from one another into the flat fluorescent lamp (1) during breaks, characterized in that that the flat fluorescent lamp (1) has features of one or more of claims 1 to 17.

19. Liquid crystal display device (33) with a liquid crystal display (35), control electronics (42) for driving the liquid crystal display (35), a lighting system as backlight for the liquid crystal display (35) and a receptacle (39) in which the liquid crystal display ( 35) with the control electronics (42) and the lighting system, characterized by the lighting system according to claim 18.

20. Liquid crystal display device according to claim 19, characterized in that at least one optical diffuser (36) is arranged between the flat lamp (1) and liquid crystal display (35).

21. Liquid crystal display device according to claim 19 or 20, characterized in that between the flat lamp (1) and liquid crystal display (35) at least one light reinforcing film (37, 38) BEF (Brightness Enhancement Film) is arranged.

22. A liquid crystal display device according to claim 19 to 21, characterized in that a first optical diffuser, then a light reinforcement film and finally a second optical diffuser are arranged between the flat lamp and the liquid crystal display.