LED-based planar light source

Details LED-based planar light source LED-based planar light source

2002-07-19

2004-10-05

Cariaso, Alan (Department: 2875)

Illumination

Plural light sources

With modifier

C362S231000, C362S800000, C313S501000, C313S504000

Reexamination Certificate

active

06799865

ABSTRACT:

TECHNICAL FIELD
The invention relates to an LED-based planar light source in accordance with the preamble of claim
1
. In particular, this is a planar light source for LCD backlighting, or else for other applications, which is, in particular, fully colour-capable and, moreover, has a high luminance.
BACKGROUND ART
JP-A 7-176794 has already disclosed an LED-based planar light source in the case of which a blue LED produces white light on a planar surface by means of partial conversion by a yellow-orange phosphor. However, this simple complementary mixing does not permit good colour rendering.
A more complicated concept with better colour rendering is three colour mixing. In this case, the primary colours red-green-blue (RGB) are used to produce white by mixing. Use can be made here either of a blue LED for the partial conversion of two phosphors which emit red and green (WO 00/33390), or of a UV-emitting LED which excites three phosphors which respectively have their emission in the red, green and blue—see WO 97/48138. Examples are line emitters such as YOB:Ce,Tb (green) and YOS:Eu (red). However, this requires a relatively shortwave emission (UV region <370 nm) in order to be able to achieve high quantum yields. This conditions the use of sapphire substrates for the UV-LEDs which are very expensive. On the other hand, if use is made of a UV-LED based on the cheaper SiC substrates, it is necessary to accept an emission in the region of 380 to 420 nm, and this renders difficult or impossible the use of line emitters in the green and red. This leads to absorption problems in the case of blue phosphors.
A specific problem here is, moreover, the additional absorption loss of blue radiation owing to the broadband nature of the absorption of the red- and green-emitting phosphors. Taken altogether, this leads to clear restrictions in the setting of the light colour and/or the luminance efficiency.
DISCLOSURE OF THE INVENTION
It is an object of the present invention to provide a fully colour-capable planar light source utilizing the colour mixing principle, the radiation from UV-emitting diodes arranged in a planar fashion being converted into light of longer wavelength by means of conversion by at least one UV-absorbing phosphor, and this light being mixed with a blue component, which achieves a high luminance efficiency and yet is economical.
This object is achieved by means of the following features: the radiation of the UV diodes is absorbed by the at least one phosphor while the blue component is provided by at least one blue-emitting LED.
Particularly advantageous refinements are to be found in the dependent claims.
Planar light sources as described in outline in U.S. Pat. No. 5,619,351, for example, are frequently used for backlighting of LCDs. In this case, a compact fluorescent lamp has predominantly been used to date as light source. This requires a high supply voltage and creates problems with electromagnetic compatibility, for which reason it is worth attempting to replace the lamps by LEDs.
According to the invention, a planar light source which is fully colour-capable is provided by utilizing the RGB principle, the radiation of a multiplicity of UV diodes arranged in a planar fashion being converted into light of longer wavelength by means of conversion by phosphors. Here, the term UV means the region of 300 to 420 nm. The radiation of the UV diodes is absorbed solely by green-emitting phosphors (preferably with a peak emission wavelength between 510 and 560 nm, for example SrAl
2
O
4
:Eu
2+
or Eu
2+
-based thiogallates) and red-emitting phosphors (preferably with a peak emission wavelength of more than 590 nm up to 690 nm, for example Sr
2
Si
5
NB:Eu
2+
) while the blue component (preferably with a peak emission wavelength between 430 and 490 nm) is provided by blue-emitting LEDs. This principle is surprising per se, because at first glance it appears substantially more complicated than the known solutions, since more LEDs are used, and the latter must be driven in a fashion separated at least into two groups (UV-LEDs and blue LEDs).
However, it is to be borne in mind in this case that the price of blue LEDs is more favourable than the price of UV-LEDs, and that, on the other hand, it is possible to economize on a few UV-LEDs. Moreover, a spatial separation of the blue LEDs from the red and green phosphors provides an elegant possibility of avoiding partial absorption of the blue radiation of the LEDs by these RG phosphors. Consequently, a more efficient light source can be created at lower cost. Finally, particular advantages are associated with the fact that instead of an expensive UV-LED on a sapphire substrate with an emission peak below 380 nm it is possible to use as UV-LED a cheap GaN-based LED (preferably doped with In and/or Al) on an SiC substrate with an emission peak between 380 and 420 nm. The point is that a slight overlap between the emission spectrum of the UV-LED and an absorption spectrum of, for example, a blue-emitting phosphor plays no role at all in the concept according to the invention, while it yields poorer results in the case of the conversion of UV into blue (>380 nm). This energy spacing (overlap) between excitation source and absorption curve of the phosphor no longer plays an important role with reference to the red- or green-emitting phosphor which, in some circumstances, both use the same activator, in particular Eu. In general, it emerges that the absorption problem no longer plays a role in the case of broadband-emitting phosphors, in particular starting from approximately 490 nm peak emission. The concept of the present invention can therefore not only be applied in the case of RGB mixtures, but also includes the application of additional phosphors. A further application is, finally, the production of a white light source on the simpler principle of blue-yellow mixing, in accordance with the first white-emitting LEDs of the prior art. In this case, the blue component is provided here by the primary emission of a number of blue LEDs, and the yellow component is provided by the yellow emission of a suitable phosphor excited by a number of UV-LEDs. A further application is, moreover, the provision of a planar light source of specific colour, it being possible for this special colour to be produced by mixing a blue and a further component. In this case, the blue component is again provided by the primary emission of a number of blue LEDs, and the further components are provided by the emission of a (or else a plurality of further) suitable phosphor excited by a number of UV-LEDs, the desired colour resulting from the mixing of the emissions. Concrete examples for such phosphors have, for example, peak emissions in the blue-green (for example Sr
6
BP
5
O
20
:Eu
2+
, Sr
4
Al
14
O
25
:EU
2+
) or green-yellow or yellow (for example Sr
2
Si
5
N
8
:Ce
3+
, (Sr,Ba)SiO
4
:Eu
2+
) or yellow-orange (for example Ca
2
Si
5
N
8
:EU
2+
, Ca
1.5
Al
3
Si
9
N
16
:Eu
2+
).
In principle, the RG phosphors can be placed directly on the individual UV-LEDs. It is advantageous for the red- and green-emitting phosphors to be applied to, or implemented inside, on an optical conductor fitted at a spacing from the UV diodes, or on a transparent plate acting like an optical conductor, because the spacing yields a better uniformity of the planar emission. The number of the blue-emitting LEDs per assembly is at most equal to the number of the UV diodes. In the case when the blue-emitting LEDs are arranged in a planar fashion, it corresponds approximately to the number of the UV diodes (50 to 100%, correspondingly).
A substantial reduction in the number of the blue-emitting LEDs (typically by 10 to 40%) can be achieved when the blue-emitting LEDs are arranged in rows at the edge of the surface fitted with the UV-LEDs. They are then launched into the forward emission of the surface by means of suitable techniques known per se. In the simplest case, a single row is arranged laterally at an edge strip next to an array of

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