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WO2014080512A1 - Light emitting device and method for producing light emitting device - Google Patents

Light emitting device and method for producing light emitting device Download PDF

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Publication number
WO2014080512A1
WO2014080512A1 PCT/JP2012/080437 JP2012080437W WO2014080512A1 WO 2014080512 A1 WO2014080512 A1 WO 2014080512A1 JP 2012080437 W JP2012080437 W JP 2012080437W WO 2014080512 A1 WO2014080512 A1 WO 2014080512A1
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WO
WIPO (PCT)
Prior art keywords
optical path
path changing
layer
region
light
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Ceased
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PCT/JP2012/080437
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French (fr)
Japanese (ja)
Inventor
黒田 和男
秀雄 工藤
浩 大畑
敏治 内田
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Pioneer Corp
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Pioneer Corp
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Priority to PCT/JP2012/080437 priority Critical patent/WO2014080512A1/en
Publication of WO2014080512A1 publication Critical patent/WO2014080512A1/en
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10KORGANIC ELECTRIC SOLID-STATE DEVICES
    • H10K50/00Organic light-emitting devices
    • H10K50/80Constructional details
    • H10K50/85Arrangements for extracting light from the devices
    • H10K50/858Arrangements for extracting light from the devices comprising refractive means, e.g. lenses

Definitions

  • the present invention relates to a light emitting device having an organic light emitting layer and a method for manufacturing the light emitting device.
  • a light emitting device having an organic light emitting layer as one of the light emitting devices.
  • this light emitting device it is desired to improve the ratio of light emitted to the outside (light extraction efficiency) of the light generated in the organic light emitting layer.
  • Patent Document 1 As a technique for improving the light extraction efficiency, there is one described in Patent Document 1.
  • the organic EL element described in Patent Document 1 includes an organic thin film layer, a pair of electrodes, one of which is a transparent electrode, sandwiching the organic thin film layer, a high refractive index layer having a higher refractive index than the organic thin film layer, and a medium And a layer in contact with a high refractive index layer in which microspheres having different refractive indexes are dispersed.
  • Patent Document 1 describes that the light extraction efficiency is improved by providing a periodic structure in which microspheres are dispersed in a medium. Specifically, the microspheres consists SiO 2, the layer in contact with the high refractive index layer, a titanium oxide layer formed by dispersing the microspheres, also made of titanium oxide layer a high refractive index layer.
  • Patent Document 1 The inventor considered that the technique described in Patent Document 1 has the following problems.
  • the technique of Patent Document 1 since microspheres having a refractive index different from that of the medium are dispersed in the medium, the refractive index changes sharply at the interface between the microsphere and the medium. For this reason, if there is no microsphere, light that is originally extracted from the organic EL element may be reflected at the interface between the microsphere and the medium, thereby changing the optical path in a direction different from the extraction direction. There is. Therefore, the technique of Patent Document 1 has room for improvement regarding light extraction efficiency.
  • An example of a problem to be solved by the present invention is to improve the light extraction efficiency of the light emitting device.
  • the invention according to claim 1 is a translucent substrate; A translucent first electrode disposed on one surface side of the translucent substrate; A second electrode disposed on the opposite side of the translucent substrate with respect to the first electrode; An organic functional layer including at least a light-emitting layer and disposed between the first electrode and the second electrode; An optical path changing region that changes an optical path of the light in the process of transmitting light; and a base region other than the optical path changing region, and is disposed between the translucent substrate and the second electrode.
  • An optical path changing layer, With The difference in refractive index between the optical path changing region and the base region is a light emitting device that increases as the distance from the boundary between the optical path changing region and the base region increases inward of the optical path changing region.
  • a step of forming a light-transmitting first electrode on one surface side of the light-transmitting substrate Forming an organic functional layer including at least a light emitting layer on a side opposite to the light-transmitting substrate with respect to the first electrode; Forming a second electrode on the side opposite to the first electrode with respect to the organic functional layer;
  • An optical path changing layer including an optical path changing area for changing an optical path of the light in the process of transmitting light, and a base area other than the optical path changing area, the light-transmitting substrate, the second electrode, Forming between, and
  • a difference in refractive index between the optical path changing area and the base area increases as the distance from the boundary between the optical path changing area and the base area increases inward of the optical path changing area.
  • a method of manufacturing a light emitting device for forming the optical path changing layer is
  • FIG. 9A is a plan view showing the configuration of the light emitting device according to Example 1
  • FIG. 9B is a cross-sectional view taken along the line BB in FIG. 9A. It is sectional drawing which shows the modification 1 of an organic functional layer. It is sectional drawing which shows the modification 2 of an organic functional layer.
  • FIG. 1 is a cross-sectional view illustrating a configuration of a light emitting device 100 according to the embodiment.
  • the light emitting device 100 includes an organic EL (Electro Luminescence) element.
  • the light emitting device 100 can be used as a light source of, for example, a display, a lighting device, or an optical communication device.
  • the light emitting device 100 includes a translucent substrate 110, an optical path changing layer 120, a first electrode 130, an organic functional layer 140, and a second electrode 150.
  • the first electrode 130 is translucent.
  • the second electrode 150 is disposed on the opposite side of the translucent substrate 110 with respect to the first electrode 130.
  • the organic functional layer 140 includes at least a light emitting layer.
  • the organic functional layer 140 is disposed between the first electrode 130 and the second electrode 150.
  • the optical path changing layer 120 includes an optical path changing area 121 and a base area 122.
  • the optical path changing area 121 changes the optical path of the light in the process of transmitting the light.
  • the base region 122 is a region other than the optical path changing region 121 in the optical path changing layer 120.
  • the optical path changing layer 120 is disposed between the translucent substrate 110 and the second electrode 150.
  • the refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward.
  • the translucent substrate 110 is a plate-like member made of a translucent material such as glass or resin.
  • the upper surface of the translucent substrate 110 that is, the surface of the translucent substrate 110 opposite to the organic functional layer 140 is a flat light extraction surface. This light extraction surface is in contact with air (refractive index 1) filling the light emission space.
  • the light extraction film is affixed on the upper surface of the translucent board
  • the first electrode 130 may be a transparent electrode made of a metal oxide conductor such as ITO (Indium Tin Oxide) or IZO (Indium Zinc Oxide). However, the first electrode 130 may be a metal thin film that is thin enough to transmit light.
  • a metal oxide conductor such as ITO (Indium Tin Oxide) or IZO (Indium Zinc Oxide).
  • the first electrode 130 may be a metal thin film that is thin enough to transmit light.
  • the second electrode 150 is a reflective electrode made of a metal film such as Al.
  • the second electrode 150 reflects light traveling from the organic functional layer 140 toward the second electrode 150 toward the translucent substrate 110.
  • the light emitting layer of the organic functional layer 140 When a voltage is applied between the first electrode 130 and the second electrode 150, the light emitting layer of the organic functional layer 140 emits light.
  • the first electrode 130, the base region 122 of the optical path changing layer 120, the optical path changing region 121 of the optical path changing layer 120, the translucent substrate 110, and the organic functional layer 140 all emit light from the organic functional layer 140. Transmits at least part of the light. Part of the light emitted from the light emitting layer is emitted (extracted) from the light extraction surface of the light-transmitting substrate 110 to the outside of the light emitting device 100 (that is, the light emission space).
  • the optical path changing layer 120 all areas other than the optical path changing area 121 are the base area 122.
  • the optical path changing layer 120 may be configured to include other areas of the optical path changing area 121 and the base area 122.
  • the optical path changing layer 120 In the optical path changing layer 120, one optical path changing area 121 exists. Alternatively, the optical path changing layer 120 has a plurality of optical path changing areas 121 in a random arrangement.
  • the refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward. That is, the refractive index of the optical path changing region 121 is reduced or increased as it moves away from the boundary between the optical path changing region 121 and the base region 122 inward of the optical path changing region 121.
  • the refractive index difference monotonously increases as the distance from the boundary between the optical path changing region 121 and the base region 122 increases.
  • an increasing tendency is recognized as a whole in the direction away from the boundary between the optical path changing region 121 and the base region 122, and for example, it may be decreased in a part of the section.
  • the refractive index of the optical path changing area 121 is preferably the same as the refractive index of the base area 122 at the boundary between the optical path changing area 121 and the base area 122.
  • the refractive index difference between the optical path changing area 121 and the base area 122 gradually increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward. That is, it is preferable that there is no portion where the refractive index difference increases discontinuously.
  • the dimension d of the optical path changing region 121 is preferably equal to or longer than the emission wavelength from the light emitting layer of the organic functional layer 140.
  • the peak wavelength of the emission wavelength is, for example, in the visible light region. Therefore, the dimension d is, for example, at least (360 nm / average refractive index of the optical path changing layer 120) or more, and preferably at least (400 nm / average refractive index of the optical path changing layer 120). However, it is preferable that the dimension d is sufficiently larger than the emission wavelength from the light emitting layer.
  • the dimension d is 200 nm or more for blue and 311 nm for green. As mentioned above, it is more preferable to set it as 356 nm or more about red, and 356 nm or more about white.
  • the shape of the optical path changing region 121 is at least a part of a sphere having a diameter equal to or larger than the emission wavelength from the light emitting layer. That is, the outer shape of the optical path changing region 121 includes at least a part of a spherical outer peripheral surface having a diameter equal to or larger than the emission wavelength from the light emitting layer.
  • the outer shape of the optical path changing region 121 includes a curved surface that is convex toward the second electrode 150 side.
  • the optical path changing region 121 includes a spherical lower half having a diameter equal to or larger than the emission wavelength from the light emitting layer, and is directed toward the second electrode 150 (downward in FIG. 1). Includes convex curved surfaces.
  • the optical path changing region 121 is exposed on the end surface (upper surface in FIG. 1) of the optical path changing layer 120 on the light transmitting substrate 110 side, the optical path changing region 121 is on the end surface. It does not have to be exposed. That is, a part of the base region 122 may exist between the end surface of the light path changing layer 120 on the light transmitting substrate 110 side and the light path changing region 121. Further, in FIG. 1, the optical path changing area 121 having a shape in which the upper part of the sphere is missing is illustrated, but the optical path changing area 121 may be spherical (entire).
  • the optical path changing region 121 includes a region having a refractive index smaller than that of the base region 122.
  • the refractive index of the optical path changing area 121 is smaller than the refractive index of the base area 122.
  • the optical path changing layer 120 is disposed between the translucent substrate 110 and the first electrode 130.
  • the refractive index of the layer including the base region 122 and the optical path changing region 121 of the optical path changing layer 120 is preferably not less than the refractive index of the translucent substrate 110 and not more than 2.0, for example. More preferably, the refractive index of the optical path changing layer 120 is equal to the refractive index of the first electrode 130.
  • the refractive index of the layer including the base region 122 and the optical path changing region 121 of the optical path changing layer 120 can be set to be equal to or higher than the refractive index of the organic functional layer 140, for example.
  • the optical path changing layer 120 is made of a dielectric, for example.
  • the material of the optical path changing layer 120 can be the same as the material of the organic functional layer 140, for example.
  • the refractive index of the organic functional layer 140 is, for example, about 1.6 or more and 2.0 or less.
  • the optical path changing area 121 is formed, for example, by heating a part of the optical path changing layer 120 (base area 122). Therefore, as the material of the optical path changing layer 120, for example, a material whose refractive index is lowered by heating can be used. That is, the material of the optical path changing layer 120 can be a material having a refractive index higher than that of the organic functional layer 140 and having a low refractive index when heated. Examples of such materials include organic materials such as phthalocyanine used for DVDs or CDs.
  • one surface (the lower surface in FIG. 1) of the translucent substrate 110 and one surface (the upper surface in FIG. 1) of the optical path changing layer 120 are in contact with each other.
  • the other surface (lower surface in FIG. 1) of the optical path changing layer 120 and one surface (upper surface in FIG. 1) of the first electrode 130 are in contact with each other.
  • the other surface (lower surface in FIG. 1) of the first electrode 130 and one surface (upper surface in FIG. 1) of the organic functional layer 140 are in contact with each other.
  • the other surface (lower surface in FIG. 1) of the organic functional layer 140 and one surface (upper surface in FIG. 1) of the second electrode 150 are in contact with each other.
  • another layer may exist between the translucent substrate 110 and the optical path changing layer 120.
  • another layer may exist between the optical path changing layer 120 and the first electrode 130.
  • another layer may exist between the first electrode 130 and the organic functional layer 140.
  • another layer may exist between the organic functional layer 140 and the second electrode 150.
  • FIG. 2 is a diagram showing an example of the refractive index change characteristic from the optical path changing layer 120 to the translucent substrate 110. That is, FIG. 2 shows an example of the refractive index change characteristic from one end A1 to the other end A2 of the line segment A in FIG.
  • the refractive index is constant regardless of the position (region R1 in FIG. 2).
  • the refractive index of the boundary between the base region 122 and the optical path changing region 121 is the same as the refractive index of the base region 122.
  • the refractive index gradually increases as the distance from the boundary between the optical path changing region 121 and the base region 122 increases, that is, toward the center of the above-described spherical shape (a spherical shape whose diameter is equal to or larger than the emission wavelength from the light emitting layer). Is reduced (region R2 in FIG. 2). Furthermore, the refractive index gradually increases again from the spherical center toward the light transmitting substrate 110 (region R3 in FIG. 2). As described above, the refractive index of the optical path changing region 121 is the same as the refractive index of the base region 122 at the boundary with the base region 122, and gradually decreases as the distance from the boundary increases. In addition, the refractive index of the translucent substrate 110 is smaller than the refractive index of the optical path changing layer 120 (region R4 in FIG. 2).
  • FIG. 3 is a cross-sectional view of a main part illustrating an example of the operation of the light emitting device 100 according to the first embodiment, and illustrates only the translucent substrate 110, the optical path changing layer 120, and the first electrode 130.
  • the refractive index of the optical path changing region 121 decreases as the distance from the base region 122 increases, for example, an operation as described below can be realized.
  • the refractive index of the optical path changing layer 120 is sufficiently large (more than the refractive index of the translucent substrate 110), the light traveling obliquely upward in the first electrode 130 is incident on the optical path changing layer 120 as it is.
  • this light travels in the order of the optical paths L11 and L12 shown in FIG. 3 when the optical path changing area 121 does not exist in the optical path changing layer 120. That is, the light travels obliquely upward in the optical path changing layer 120 (optical path L11), and then reflects at the interface between the optical path changing layer 120 and the translucent substrate 110 and travels diagonally downward (optical path L12).
  • the optical path changing region 121 exists in the optical path changing layer 120, the optical path of this light gradually increases in the process of passing through the optical path changing region 121 as indicated by the optical path L1. Be changed. Thereby, the direction of this light can be changed to less than the critical angle at the interface between the optical path changing layer 120 and the translucent substrate 110, and this light can be incident from the optical path changing region 121 to the translucent substrate 110 side. Further, this light can be emitted from the translucent substrate 110 to the upper side thereof (that is, outside the light emitting device 100).
  • FIG. 4 is a sectional view showing a part of the manufacturing method.
  • This manufacturing method includes the following steps (1) to (4). (1) Step of forming a transparent first electrode 130 on one surface side of the transparent substrate 110 (2) At least light emission on the opposite side of the transparent substrate 110 with respect to the first electrode 130 Step of forming organic functional layer 140 including layers (3) Step of forming second electrode 150 on the side opposite to first electrode 130 with respect to organic functional layer 140 (4) Transmitting light An optical path changing layer 120 including an optical path changing area 121 that changes the optical path of the light in the process and a base area 122 other than the optical path changing area 121 is formed between the translucent substrate 110 and the second electrode 150.
  • Step of forming in between In the step of forming the optical path changing layer 120, the refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward of the optical path changing area 121. Thus, the optical path changing layer 120 is formed.
  • an organic material such as NPB or phthalocyanine is vapor-deposited or applied on the lower surface of the translucent substrate 110 to form a portion that becomes the base region 122 in the optical path changing layer 120 (FIG. 4A).
  • the optical path changing region 121 is formed at an appropriate timing after the base region 122 is formed. The timing and method for forming the optical path changing region 121 will be described later.
  • a light-transmitting conductive film made of a metal oxide conductor such as ITO (Indium Tin Oxide) or IZO (Indium Zinc Oxide) is formed on the lower surface of the optical path changing layer 120 (base region 122) by sputtering or the like.
  • a first electrode 130 is formed by patterning the film by etching.
  • the organic functional layer 140 is formed by applying an organic material to the lower surface of the first electrode 130.
  • a second electrode 150 is formed by depositing a metal material such as Al in a desired pattern on the lower surface of the organic functional layer 140 by vapor deposition using a mask or the like.
  • a bus line and a partition may be formed at an appropriate timing as needed.
  • a sealing layer may be formed on the lower surface of the second electrode 150 as necessary.
  • the optical path changing region 121 is formed by heating a part of the optical path changing layer 120 (base region 122) by irradiating light. Specifically, for example, by irradiating a part of the optical path changing layer 120 with laser light, a part of the optical path changing layer 120 can be heated to form the optical path changing area 121 (FIG. 4B). ). By heating a part of the optical path changing layer 120, the molecular structure of the material constituting the optical path changing layer 120 is changed, or the density distribution of the material constituting the optical path changing layer 120 is changed (in this embodiment, The refractive index of the portion decreases.
  • the intensity distribution of the light (laser light or the like) irradiated by the above-described method is a Gaussian distribution, and the intensity of the central portion of the irradiation spot of the light is increased. For this reason, the closer to the center of the irradiation spot, the greater the influence on the molecular structure and density distribution of the material constituting the optical path changing layer 120. Therefore, for example, the refractive index of the optical path changing region 121 gradually decreases toward the center of the irradiation spot.
  • the timing for forming the optical path changing region 121 can be any timing after the optical path changing layer 120 (base region 122) is formed.
  • the optical path changing region 121 When forming the optical path changing region 121 after forming the optical path changing layer 120 (base region 122) and before forming the first electrode 130, light is irradiated from any surface side of the optical path changing layer 120 (base region 122). You may do it.
  • the optical path changing region 121 is formed after the formation of the first electrode 130 and before the formation of the organic functional layer 140, in order to suppress efficient light irradiation and damage to the first electrode 130 due to concentrated light. Further, light is irradiated from the side of the transparent substrate 110 close to the processing point. In any of these cases, the organic functional layer 140 has not yet been formed. For this reason, since it is not necessary to consider the damage to the organic functional layer 140, either a CW laser (continuous wave oscillation operation laser) or a pulse laser may be used.
  • the optical path changing region 121 may be formed after the sealing is completed and the light emitting device 100 having the panel structure is constructed. In this case, light is irradiated from the translucent substrate 110 side. In this case, in order to use a CW laser or a pulse laser, it is preferable to consider that heat is not applied to the organic functional layer 140 as much as possible. Alternatively, a femtosecond laser or a nanosecond laser may be used.
  • the large-area optical path changing area 121 may be formed by irradiating the laser once, or the small area is irradiated in a plurality of times, and the large-area optical path changing area 121 is formed by a set of these areas. May be. In this case, a discontinuous surface with a refractive index may be formed in the optical path changing region 121.
  • the light irradiation for forming the optical path changing region 121 is not limited to the laser light irradiation.
  • the optical path changing region 121 can also be formed by allowing light having a single wavelength other than the laser to pass through the mask and condensing with a lens and forming an image on a part of the optical path changing layer 120. it can. In this case, it is possible to perform heat treatment on a larger area at a time than when laser light is used.
  • the light emitting device 100 includes the optical path changing layer 120 disposed between the translucent substrate 110 and the second electrode 150.
  • the optical path changing layer 120 includes an optical path changing area 121 and a base area 122. In the process of light passing through the optical path changing area 121, the optical path of the light is changed. Therefore, if the optical path changing area 121 does not exist, the light is not taken out from the light emitting apparatus 100 and is repeatedly reflected and attenuated in the light emitting apparatus 100. It is possible to change the optical path of the light to be taken out from the light emitting device 100. Therefore, the light extraction efficiency can be improved.
  • the refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward.
  • the transmittance in the vicinity of the critical angle suddenly changes when the refractive index gradually changes in two layers having different refractive indexes. That is, when the refractive index changes sharply at the interface, the transmittance just before the critical angle decreases, and the reflectance increases accordingly. Conversely, when the refractive index gradually changes, it is possible to realize a state where the transmittance is high until just before the critical angle.
  • the difference in refractive index between the base region 122 and the optical path changing region 121 is suppressed, and there is no significant interface between the base region 122 and the optical path changing region 121.
  • the occurrence of light reflection at the boundary between the base region 122 and the optical path changing region 121 is suppressed. Therefore, even when the optical path changing region 121 does not exist, the light extracted from the light emitting device 100 can be emitted from the light emitting device 100 after smoothly entering the optical path changing region 121. Thereby, the light extraction efficiency can be further improved.
  • the refractive index of the optical path changing region 121 is the same as the refractive index of the base region 122 at the boundary between the optical path changing region 121 and the base region 122, Reflection can be substantially prevented from occurring. For this reason, the light extraction efficiency can be further improved.
  • the optical path changing area 121 and the base area 122 gradually increases from the boundary between the optical path changing area 121 and the base area 122 toward the inward direction of the optical path changing area 121, the optical path changing area There are no places where the refractive index changes discontinuously in 121. Thereby, the reflection of the light in the optical path changing area 121 can be substantially prevented from occurring. For this reason, the light extraction efficiency can be further improved.
  • the dimension of the optical path changing region 121 is equal to or greater than the emission wavelength from the light emitting layer, the refraction and reflection of light at the boundary between the optical path changing region 121 and the base region 122 can be controlled more reliably (scattering can be suppressed). The light extraction efficiency can be improved.
  • the dimension of the optical path changing area 121 is too small, light only travels straight through the optical path changing area 121 and may not be changed in the optical path changing area 121.
  • the outer shape of the optical path changing region 121 is convex toward the outside of the optical path changing region 121. Includes curved surfaces. For this reason, the external shape of the optical path changing area 121 has various angles. Therefore, for light incident on the optical path changing region 121 at various angles, the direction of the light can be changed to an angle at which light can be extracted from the light emitting device 100.
  • the outer shape of the optical path changing region 121 includes a curved surface convex toward the second electrode 150 side
  • the outer shape of the optical path changing region 121 on the second electrode 150 side has various angles. Therefore, for the light incident on the optical path changing region 121 at various angles from the second electrode 150 side, the direction of the light can be changed to an angle at which light can be extracted from the light emitting device 100.
  • the optical path changing region 121 includes a region having a refractive index smaller than that of the base region 122, for example, as shown in FIG. 3, the direction of light obliquely traveling from the second electrode 150 side to the translucent substrate 110 side is set. Thus, the direction can be easily changed in the direction of taking out from the light emitting device 100.
  • the first electrode 130 may be a transparent electrode made of, for example, ITO.
  • a transparent electrode such as ITO has a high refractive index (for example, about 1.75 to 1.83). Therefore, when the optical path changing layer 120 is disposed between the translucent substrate 110 and the first electrode 130, as described above, the refractive index of the optical path changing layer 120 is set to the refractive index of the translucent substrate 110. It is preferable that the ratio is not less than 2.0 and not more than 2.0. Thereby, light can be easily extracted from the first electrode 130 to the optical path changing layer 120, and light can also be easily extracted from the optical path changing layer 120 to the translucent substrate 110.
  • the optical path changing region 121 is formed by heating a part of the optical path changing layer 120 (base region 122) by irradiating light or the like. Therefore, since the optical path changing region 121 can be easily formed at a desired position in the optical path changing layer 120 with a desired size, the light emitting device 100 having a desired structure can be easily manufactured.
  • the high refractive index layer and the layer in contact with the high refractive index layer are each made of a titanium oxide layer, even if a strong barrier film is additionally formed, The titanium oxide layer may adversely affect the organic light emitting layer.
  • the optical path changing layer 120 is a layer in which the refractive index of a part of the organic layer such as phthalocyanine is changed, adverse effects on the organic functional layer 140 can be suppressed.
  • FIG. 5 is a cross-sectional view showing the configuration of the light emitting device 100 according to the second embodiment.
  • the optical path changing layer 160 having the same configuration as the optical path changing layer 120 in the first embodiment is disposed between the organic functional layer 140 and the second electrode 150.
  • the optical path changing layer 160 includes an optical path changing area 161 similar to the optical path changing area 121 and a base area 162 similar to the base area 122.
  • the material of the optical path changing layer 160 may be the same material as the electron injection layer (described later) of the organic functional layer 140, for example. In this case, the refractive index of the optical path changing layer 160 is about 1.5 or more and 1.8 or less.
  • a high refractive index layer 190 may be arranged instead of the optical path changing layer 120.
  • the high refractive index layer 190 has the same material and optical characteristics as the base region 122 of the optical path changing layer 120.
  • the organic functional layer 140 and the optical path changing layer 160 may be in contact with each other, or another layer may exist between the organic functional layer 140 and the optical path changing layer 160.
  • the optical path changing layer 160 and the second electrode 150 may be in contact with each other, or another layer may exist between the optical path changing layer 160 and the second electrode 150.
  • the translucent substrate 110 and the high refractive index layer 190 may be in contact with each other, or another layer may exist between the translucent substrate 110 and the high refractive index layer 190.
  • the high refractive index layer 190 and the first electrode 130 may be in contact with each other, or another layer may exist between the high refractive index layer 190 and the first electrode 130.
  • the optical path changing layer 160 is disposed between the organic functional layer 140 and the second electrode 150 as in the second embodiment, the light extraction efficiency is improved as in the first embodiment. can do.
  • the organic functional layer 140 may be made of a material having a high refractive index to some extent (for example, about 1.8). For this reason, when the optical path changing layer 160 is disposed between the organic functional layer 140 and the second electrode 150 as in the present embodiment, the refractive index of the optical path changing layer 160 is 1.0 or more, In addition, the refractive index is preferably equal to or lower than the refractive index of the organic functional layer 140. Accordingly, light can be easily extracted from the optical path changing layer 160 to the organic functional layer 140, and the light reflectivity at the interface between the optical path changing layer 160 and the second electrode 150 is increased, and more light is transmitted. It can be directed to the optical substrate 110 side.
  • FIG. 6 is a cross-sectional view illustrating a configuration of a light emitting device 100 according to the third embodiment.
  • the light emitting device 100 according to the third embodiment includes an optical path changing layer 160 disposed between the organic functional layer 140 and the second electrode 150 in addition to the configuration of the first embodiment. . That is, the light emitting device 100 according to the third embodiment includes two optical path changing layers 120 and 160.
  • the configuration of the optical path changing layer 120 is the same as that of the first embodiment, and the configuration of the optical path changing layer 160 is the same as that of the second embodiment.
  • the light extraction efficiency can be improved as in the first embodiment.
  • the optical path changing region 121 is different from the first embodiment in that it is polycrystallized. That is, the optical path changing region 121 is obtained by crystallizing the material of the base region 122 by heating and cooling. NPB or the like becomes a spherical shape while linear crystals grow as a whole by heating and cooling. As a result, the optical path changing region 121 includes a region having a refractive index larger than that of the base region 122. In the present embodiment, since the boundary between the optical path changing region 121 and the base region 122 is the boundary between the polycrystalline sphere and the surrounding base region 122, the optical path is changed at the boundary between the optical path changing region 121 and the base region 122.
  • the refractive index of the change region 121 is the same as the refractive index of the base region 122.
  • the refractive index of the optical path changing region 121 is larger than the refractive index of the base region 122.
  • the refractive index of the optical path changing area 121 increases (for example, gradually) as it moves away from the boundary between the optical path changing area 121 and the base area 122 inward of the optical path changing area 121.
  • the optical path changing region 121 having a refractive index larger than that of the base region 122
  • a material whose refractive index is increased by heating is used as the material of the optical path changing layer 120 (base region 122).
  • the optical path changing layer 120 (base region 122) is configured by heating a part of the optical path changing layer 120 (base region 122) of such material in the same manner as in the first embodiment and then cooling. Crystallization of the material occurs.
  • the refractive index of the portion becomes higher than the refractive index of the surrounding portion (that is, the base region 122), and gradually increases as the refractive index of the portion moves away from the base region 122, for example.
  • NPB N, N-di (naphthalene-1-yl) -N, N-diphenyl-benzidine
  • FIG. 7 is a diagram illustrating an example of a change characteristic of the refractive index from the optical path changing layer 120 to the translucent substrate 110 of the light emitting device 100 according to the fourth embodiment. That is, FIG. 7 shows another example of the change characteristic of the refractive index from one end A1 to the other end A2 of the line segment A in FIG.
  • the refractive index is constant regardless of the position (region R1 in FIG. 7).
  • the refractive index of the boundary between the base region 122 and the optical path changing region 121 (the boundary between the region R1 and the region R2 in FIG. 7) is the same as the refractive index of the base region 122.
  • the refractive index gradually increases as the distance from the boundary between the optical path changing region 121 and the base region 122 increases, that is, toward the center of the above-described spherical shape (a spherical shape whose diameter is equal to or larger than the emission wavelength from the light emitting layer). Has increased (region R2 in FIG. 7). Further, the refractive index gradually decreases again from the spherical center toward the translucent substrate 110 (region R3 in FIG. 7). That is, the refractive index of the optical path changing region 121 is the same as the refractive index of the base region 122 at the boundary with the base region 122, and gradually increases as the distance from the boundary increases.
  • the refractive index of the translucent substrate 110 is smaller than the refractive index of the optical path changing layer 120 (region R4 in FIG. 7). Also in the case of the fourth embodiment, the direction of light is gradually changed in the process of light passing through the optical path changing region 121.
  • the example in which the optical path changing layer 120 is disposed between the translucent substrate 110 and the first electrode 130 has been described.
  • an optical path changing layer having an optical path changing region that is crystallized and has a refractive index larger than that of the base region may be disposed between the organic functional layer 140 and the second electrode 150. That is, the refractive index of the optical path changing region 161 of the optical path changing layer 160 of the second embodiment or the third embodiment may be larger than the refractive index of the base region 162.
  • the material of the optical path changing layer 160 for example, a material having a refractive index lower than the refractive index of the organic functional layer 140 and having a higher refractive index by heating is used.
  • the optical path changing layer 160 is formed between the organic functional layer 140 and the second electrode 150 as in the second embodiment (and the third embodiment), by partially heating and cooling with a laser, It is preferable to form the crystallized optical path changing region 161 as in the fourth embodiment. In this case, since the output (power) of the laser can be suppressed compared to Example 1, damage to the organic functional layer 140 when the optical path changing region 161 is formed can be suppressed.
  • the optical path changing layer 160 is partially heated and cooled by the laser to be crystallized, and then the electrode 150 The film thickness of the electrode 150 is increased until the film thickness is such that light can be reflected.
  • FIG. 8 is a cross-sectional view of an essential part showing an example of the operation of the light emitting device according to the fourth embodiment, and only the organic functional layer 140, the optical path changing layer 160, and the second electrode 150 are illustrated.
  • the optical path changing layer 160 having the optical path changing area 161 similar to the optical path changing area 121 having the refractive index characteristic as described in FIG. 7 is disposed between the organic functional layer 140 and the second electrode 150. Will be described.
  • optical path changing region 161 in the optical path changing layer 160 it is assumed that there is light traveling in the order of the optical paths L11 and L12 shown in FIG. That is, the light travels obliquely downward in the optical path changing layer 160 (optical path L11), and then reflects on the second electrode 150 and travels obliquely upward (optical path L12). Further, this light is then transmitted to the interface between the optical path changing layer 120 and the translucent substrate 110 (when the optical path changing layer 120 exists) or to the interface between the first electrode 130 and the translucent substrate 110 (optical path changing). Suppose the layer 120 is not present) and proceed diagonally downward.
  • the optical path changing region 161 exists in the optical path changing layer 160, the optical path of this light gradually goes downward in the process of passing through the optical path changing region 161 as shown by the optical path L1. Be changed. This light is then reflected by the second electrode 150 and travels as indicated by the optical path L2.
  • the optical path L2 is an interface between the optical path changing layer 120 and the translucent substrate 110 (when the optical path changing layer 120 is present) or an interface between the first electrode 130 and the translucent substrate 110 (optical path changing layer). It is assumed that the angle is less than the critical angle (when 120 does not exist). Therefore, this light can be incident on the light transmitting substrate 110 side from the optical path changing layer 120 or the first electrode 130, and further this light is further transmitted from the light transmitting substrate 110 to the upper side (that is, outside the light emitting device). Can be radiated.
  • Example 1 In Example 1, an example of a more specific configuration of the light emitting device 100 according to the first embodiment will be described.
  • FIG. 9A is a plan view showing the configuration of the light emitting device according to Example 1
  • FIG. 9B is a cross-sectional view taken along the line BB in FIG. 9A. 9B and 9A are upside down from FIG.
  • the first electrode 130 constitutes an anode.
  • the plurality of first electrodes 130 each extend in the Y direction in a strip shape. Adjacent first electrodes 130 are spaced apart from each other at a constant interval in the X direction orthogonal to the Y direction.
  • Each of the first electrodes 130 is made of a metal oxide conductor such as ITO or IZO, for example.
  • the refractive index of the first electrode 130 is approximately the same as that of the optical path changing layer 120 (for example, approximately 1.8).
  • a bus line 170 for supplying a power supply voltage to the first electrode 130 is formed on each surface of the first electrode 130.
  • An insulating film 180 is formed on the optical path changing layer 120 and the first electrode 130.
  • a plurality of stripe-shaped openings each extending in the Y direction are formed.
  • a plurality of banks (partition walls) made of the insulating film 180 are formed.
  • Each of the openings formed in the insulating film 180 reaches the first electrode 130, and the surface of each first electrode 130 is exposed at the bottom of the opening.
  • An organic functional layer 140 is formed on the first electrode 130 in each opening of the insulating film 180.
  • the organic functional layer 140 is configured by stacking a hole injection layer 141, a hole transport layer 142, a light emitting layer 143 (light emitting layers 143R, 143G, 143B), and an electron transport layer 144 in this order.
  • Materials for the hole injection layer 141 and the hole transport layer 142 include aromatic amine derivatives, phthalocyanine derivatives, porphyrin derivatives, oligothiophene derivatives, polythiophene derivatives, benzylphenyl derivatives, compounds in which tertiary amines are linked by fluorene groups, hydrazones. Derivatives, silazane derivatives, silanamine derivatives, phosphamine derivatives, quinacridone derivatives, polyaniline derivatives, polypyrrole derivatives, polyphenylene vinylene derivatives, polythienylene vinylene derivatives, polyquinoline derivatives, polyquinoxaline derivatives, carbon and the like.
  • the light emitting layers 143R, 143G, and 143B are made of a fluorescent organometallic compound that emits red light, green light, and blue light, respectively.
  • the light emitting layers 143R, 143G, and 143B are arranged side by side in a state of being separated from each other by a bank made of the insulating film 180. That is, the organic functional layer 140 forms a plurality of light emitting regions separated by banks.
  • An electron transport layer 144 is formed so as to cover the surfaces of the light emitting layers 143R, 143G, 143B and the insulating film 180.
  • a second electrode 150 is formed so as to cover the surface of the electron transport layer 144.
  • the second electrode 150 constitutes a cathode.
  • the second electrode 150 is formed in a band shape.
  • the second electrode 150 is made of a metal such as Al or an alloy having a low work function and high reflectivity.
  • the refractive index of the organic functional layer 140 is approximately the same as that of the first electrode 130 and the optical path changing layer 120 (for example, a refractive index of approximately 1.8).
  • the light emitting layers 143R, 143G, and 143B that emit red, green, and blue light are repeatedly arranged in stripes, and the red, green, and green light is emitted from the surface of the translucent substrate 110 that serves as a light extraction surface.
  • Blue light is mixed at an arbitrary ratio to emit light that is recognized as a single emission color (for example, white).
  • FIG. 10 is a diagram illustrating a first modification of the layer structure of the organic functional layer 140.
  • the organic functional layer 140 according to Modification 1 has a structure in which a hole injection layer 141, a hole transport layer 142, a light emitting layer 143, an electron transport layer 144, and an electron injection layer 145 are stacked in this order. That is, the organic functional layer 140 is an organic electroluminescence light emitting layer. Note that instead of the hole injection layer 141 and the hole transport layer 142, one layer having the functions of these two layers may be provided. Similarly, instead of the electron transport layer 144 and the electron injection layer 145, a single layer having the functions of these two layers may be provided (see Example 1 (FIG. 9B)).
  • the light emitting layer 143 is, for example, a layer that emits red light, a layer that emits blue light, a layer that emits yellow light, or a layer that emits green light.
  • a region having a light emitting layer 143 that emits red light, a region having a light emitting layer 143 that emits green light, and a region having a light emitting layer 143 that emits blue light are repeatedly provided. (See Example 1 (FIG. 9B)).
  • the light emitting device 100 emits light in a single light emission color such as white.
  • the light emitting layer 143 may be configured to emit light in a single light emission color such as white by mixing materials for emitting a plurality of colors.
  • FIG. 11 is a diagram illustrating a second modification of the layer structure of the organic functional layer 140.
  • the light emitting layer 143 of the organic functional layer 140 according to Modification 2 has a configuration in which light emitting layers 143a, 143b, and 143c are stacked in this order.
  • the light emitting layers 143a, 143b, and 143c emit light of different colors (for example, red, green, and blue).
  • the light emitting layers 143a, 143b, and 143c emit light at the same time, so that the light emitting device 100 emits light in a single light emission color such as white.
  • the shape of the optical path changing region (121, 161) is an example in which the diameter is at least a part of a sphere having a wavelength equal to or greater than the emission wavelength from the light emitting layer, in particular, the outer shape of the optical path changing region is the second electrode 150 side.
  • An example including a convex curved surface has been described.
  • the optical path changing region (121, 161) may be formed in other shapes.
  • the light irradiation for forming the optical path changing region (121, 161) is not limited to spot irradiation, but by intermittently irradiating, an optical path changing region having a structure like a grating (diffraction grating) ( 121, 161) may be formed.
  • the optical path changing region (121, 161) may be a bubble formed in the base region (122, 162).
  • the refractive index of the optical path changing region 121 is the same as the refractive index of the base region 122 at the boundary between the optical path changing region 121 and the base region 122 has been described. It may change continuously. For example, when the base region 122 is irradiated with laser light with stronger energy, a discontinuous surface with a refractive index may be formed at the boundary between the optical path changing region 121 and the base region 122.

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Abstract

This light emitting device (100) comprises an optical-path changing layer (120). The optical-path changing layer (120) includes an optical-path changing region (121) and a base region (122) other than the optical-path changing region (121), and is arranged between a light-transmissive substrate (110) and a second electrode (150). The difference in refractive index between the optical-path changing region (121) and the base region (122) increases with the increase in distance from the boundary between the optical-path changing region (121) and the base region (122) toward the inside of the optical-path changing region (121). The optical-path changing region (121) changes the optical path of light in the course of letting the light pass therethrough.

Description

発光装置及び発光装置の製造方法LIGHT EMITTING DEVICE AND LIGHT EMITTING DEVICE MANUFACTURING METHOD

 本発明は、有機発光層を有する発光装置及び発光装置の製造方法に関する。 The present invention relates to a light emitting device having an organic light emitting layer and a method for manufacturing the light emitting device.

 発光装置の1つに有機発光層を有する発光装置がある。この発光装置においては、有機発光層で発生した光のうち外部に放射される光の割合(光取り出し効率)を向上することが望まれている。 There is a light emitting device having an organic light emitting layer as one of the light emitting devices. In this light emitting device, it is desired to improve the ratio of light emitted to the outside (light extraction efficiency) of the light generated in the organic light emitting layer.

 光取り出し効率の向上を目的とした技術としては、特許文献1に記載のものがある。特許文献1に記載された有機EL素子は、有機薄膜層と、一方が透明電極であり有機薄膜層を挟持する一対の電極と、有機薄膜層よりも屈折率が高い高屈折率層と、媒質中に媒質とは屈折率が異なる微小球を分散させてなる高屈折率層に接している層と、を有する。特許文献1には、媒質中に微小球を分散させた周期構造を設けることにより、光取り出し効率が向上する旨の記載がある。具体的には、微小球はSiOからなり、高屈折率層に接している層は、この微小球を分散した酸化チタン層であり、高屈折率層も酸化チタン層からなる。 As a technique for improving the light extraction efficiency, there is one described in Patent Document 1. The organic EL element described in Patent Document 1 includes an organic thin film layer, a pair of electrodes, one of which is a transparent electrode, sandwiching the organic thin film layer, a high refractive index layer having a higher refractive index than the organic thin film layer, and a medium And a layer in contact with a high refractive index layer in which microspheres having different refractive indexes are dispersed. Patent Document 1 describes that the light extraction efficiency is improved by providing a periodic structure in which microspheres are dispersed in a medium. Specifically, the microspheres consists SiO 2, the layer in contact with the high refractive index layer, a titanium oxide layer formed by dispersing the microspheres, also made of titanium oxide layer a high refractive index layer.

特開2004-14530号公報JP 2004-14530 A

 本発明者は、特許文献1に記載の技術では、以下に説明する問題があると考えた。
 特許文献1の技術では、媒質とは屈折率が異なる微小球を媒質中に分散させているため、微小球と媒質との界面において、屈折率が急峻に変化する。このため、微小球が存在しなければ本来有機EL素子から取り出される光についても、微小球と媒質との界面において反射することによって、取り出し方向とは異なる向きへと光路が変化してしまう可能性がある。よって、特許文献1の技術は、光取り出し効率に関し、改善の余地がある。
The inventor considered that the technique described in Patent Document 1 has the following problems.
In the technique of Patent Document 1, since microspheres having a refractive index different from that of the medium are dispersed in the medium, the refractive index changes sharply at the interface between the microsphere and the medium. For this reason, if there is no microsphere, light that is originally extracted from the organic EL element may be reflected at the interface between the microsphere and the medium, thereby changing the optical path in a direction different from the extraction direction. There is. Therefore, the technique of Patent Document 1 has room for improvement regarding light extraction efficiency.

 本発明が解決しようとする課題としては、発光装置の光取り出し効率を向上することが一例として挙げられる。 An example of a problem to be solved by the present invention is to improve the light extraction efficiency of the light emitting device.

 請求項1に記載の発明は、透光性基板と、
 前記透光性基板の一方の面側に配置された透光性の第1電極と、
 前記第1電極を基準として前記透光性基板とは反対側に配置された第2電極と、
 少なくとも発光層を含んでおり、前記第1電極と前記第2電極との間に配置されている有機機能層と、
 光を透過させる過程で当該光の光路を変更する光路変更領域と、前記光路変更領域以外のベース領域と、を含んでおり、前記透光性基板と前記第2電極との間に配置されている光路変更層と、
 を備え、
 前記光路変更領域と前記ベース領域との屈折率差は、前記光路変更領域と前記ベース領域との境界から前記光路変更領域の内向きに遠ざかるにつれて大きくなっている発光装置である。
The invention according to claim 1 is a translucent substrate;
A translucent first electrode disposed on one surface side of the translucent substrate;
A second electrode disposed on the opposite side of the translucent substrate with respect to the first electrode;
An organic functional layer including at least a light-emitting layer and disposed between the first electrode and the second electrode;
An optical path changing region that changes an optical path of the light in the process of transmitting light; and a base region other than the optical path changing region, and is disposed between the translucent substrate and the second electrode. An optical path changing layer,
With
The difference in refractive index between the optical path changing region and the base region is a light emitting device that increases as the distance from the boundary between the optical path changing region and the base region increases inward of the optical path changing region.

 請求項12に記載の発明は、透光性基板の一方の面側に、透光性の第1電極を形成する工程と、
 前記第1電極を基準として前記透光性基板とは反対側に、少なくとも発光層を含んで構成される有機機能層を形成する工程と、
 前記有機機能層を基準として前記第1電極とは反対側に、第2電極を形成する工程と、
 光を透過させる過程で当該光の光路を変更する光路変更領域と、前記光路変更領域以外のベース領域と、を含んで構成される光路変更層を、前記透光性基板と前記第2電極との間に形成する工程と、
 を備え、
 前記光路変更層を形成する工程では、前記光路変更領域と前記ベース領域との屈折率差が、前記光路変更領域と前記ベース領域との境界から前記光路変更領域の内向きに遠ざかるにつれて大きくなるように、前記光路変更層を形成する発光装置の製造方法である。
According to a twelfth aspect of the present invention, a step of forming a light-transmitting first electrode on one surface side of the light-transmitting substrate;
Forming an organic functional layer including at least a light emitting layer on a side opposite to the light-transmitting substrate with respect to the first electrode;
Forming a second electrode on the side opposite to the first electrode with respect to the organic functional layer;
An optical path changing layer including an optical path changing area for changing an optical path of the light in the process of transmitting light, and a base area other than the optical path changing area, the light-transmitting substrate, the second electrode, Forming between, and
With
In the step of forming the optical path changing layer, a difference in refractive index between the optical path changing area and the base area increases as the distance from the boundary between the optical path changing area and the base area increases inward of the optical path changing area. And a method of manufacturing a light emitting device for forming the optical path changing layer.

 上述した目的、およびその他の目的、特徴および利点は、以下に述べる好適な実施の形態、およびそれに付随する以下の図面によってさらに明らかになる。 The above-described object and other objects, features, and advantages will be further clarified by a preferred embodiment described below and the following drawings attached thereto.

第1の実施形態に係る発光装置の構成を示す断面図である。It is sectional drawing which shows the structure of the light-emitting device which concerns on 1st Embodiment. 光路変更層から透光性基板にかけての屈折率の変化特性の例を示す図である。It is a figure which shows the example of the change characteristic of the refractive index from an optical path change layer to a translucent board | substrate. 第1の実施形態に係る発光装置の動作の例を示す要部断面図である。It is principal part sectional drawing which shows the example of operation | movement of the light-emitting device which concerns on 1st Embodiment. 第1の実施形態に係る発光装置の製造方法の一部の工程を示す断面図である。It is sectional drawing which shows the one part process of the manufacturing method of the light-emitting device which concerns on 1st Embodiment. 第2の実施形態に係る発光装置の構成を示す断面図である。It is sectional drawing which shows the structure of the light-emitting device which concerns on 2nd Embodiment. 第3の実施形態に係る発光装置の構成を示す断面図である。It is sectional drawing which shows the structure of the light-emitting device which concerns on 3rd Embodiment. 第4の実施形態に係る発光装置の光路変更層から透光性基板にかけての屈折率の変化特性の例を示す図である。It is a figure which shows the example of the change characteristic of the refractive index from the optical path change layer of the light-emitting device which concerns on 4th Embodiment to the translucent board | substrate. 第4の実施形態に係る発光装置の動作の例を示す要部断面図である。It is principal part sectional drawing which shows the example of operation | movement of the light-emitting device which concerns on 4th Embodiment. 図9(a)は実施例1に係る発光装置の構成を示す平面図であり、図9(b)は図9(a)におけるB-B線に沿った断面図である。FIG. 9A is a plan view showing the configuration of the light emitting device according to Example 1, and FIG. 9B is a cross-sectional view taken along the line BB in FIG. 9A. 有機機能層の変形例1を示す断面図である。It is sectional drawing which shows the modification 1 of an organic functional layer. 有機機能層の変形例2を示す断面図である。It is sectional drawing which shows the modification 2 of an organic functional layer.

 以下、実施の形態について、図面を用いて説明する。尚、すべての図面において、同様の構成要素には同一の符号を付し、適宜説明を省略する。 Hereinafter, embodiments will be described with reference to the drawings. In all the drawings, the same components are denoted by the same reference numerals, and description thereof will be omitted as appropriate.

 (第1の実施形態)
 図1は実施形態に係る発光装置100の構成を示す断面図である。発光装置100は、有機EL(Electro Luminescence)素子を含んで構成される。この発光装置100は、例えばディスプレイ、照明装置、又は光通信装置の光源として用いることができる。
(First embodiment)
FIG. 1 is a cross-sectional view illustrating a configuration of a light emitting device 100 according to the embodiment. The light emitting device 100 includes an organic EL (Electro Luminescence) element. The light emitting device 100 can be used as a light source of, for example, a display, a lighting device, or an optical communication device.

 本実施形態に係る発光装置100は、透光性基板110と、光路変更層120と、第1電極130と、有機機能層140と、第2電極150と、を有する。第1電極130は透光性である。第2電極150は、第1電極130を基準として透光性基板110とは反対側に配置されている。有機機能層140は、少なくとも発光層を含んで構成されている。有機機能層140は、第1電極130と第2電極150との間に配置されている。光路変更層120は、光路変更領域121と、ベース領域122と、を含んで構成されている。光路変更領域121は、光を透過させる過程で当該光の光路を変更する。ベース領域122は、光路変更層120における光路変更領域121以外の領域である。光路変更層120は、透光性基板110と第2電極150との間に配置されている。光路変更領域121とベース領域122との屈折率差は、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて大きくなっている。 The light emitting device 100 according to the present embodiment includes a translucent substrate 110, an optical path changing layer 120, a first electrode 130, an organic functional layer 140, and a second electrode 150. The first electrode 130 is translucent. The second electrode 150 is disposed on the opposite side of the translucent substrate 110 with respect to the first electrode 130. The organic functional layer 140 includes at least a light emitting layer. The organic functional layer 140 is disposed between the first electrode 130 and the second electrode 150. The optical path changing layer 120 includes an optical path changing area 121 and a base area 122. The optical path changing area 121 changes the optical path of the light in the process of transmitting the light. The base region 122 is a region other than the optical path changing region 121 in the optical path changing layer 120. The optical path changing layer 120 is disposed between the translucent substrate 110 and the second electrode 150. The refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward.

 以下においては、説明を簡単にするため、発光装置100の各構成要素の位置関係(上下関係等)が各図に示す関係であるものとして説明を行う。ただし、この説明における位置関係は、発光装置100の使用時の位置関係とは無関係である。 Hereinafter, in order to simplify the description, description will be made assuming that the positional relationship (vertical relationship, etc.) of each component of the light emitting device 100 is the relationship shown in each drawing. However, the positional relationship in this description is irrelevant to the positional relationship when the light emitting device 100 is used.

 透光性基板110は、ガラスや樹脂などの透光性を有する材料からなる板状部材である。例えば、透光性基板110の上面、すなわち透光性基板110における有機機能層140とは反対側の面は、平坦な光取り出し面となっている。この光取り出し面は、光放出空間を充たす空気(屈折率1)と接している。なお、透光性基板110の上面には、光取り出しフィルムが貼り付けられており、この光取り出しフィルムの上面が、光取り出し面を構成していても良い。 The translucent substrate 110 is a plate-like member made of a translucent material such as glass or resin. For example, the upper surface of the translucent substrate 110, that is, the surface of the translucent substrate 110 opposite to the organic functional layer 140 is a flat light extraction surface. This light extraction surface is in contact with air (refractive index 1) filling the light emission space. In addition, the light extraction film is affixed on the upper surface of the translucent board | substrate 110, and the upper surface of this light extraction film may comprise the light extraction surface.

 第1電極130は、例えばITO(Indium Tin Oxide)やIZO(Indium Zinc Oxide)などの金属酸化物導電体からなる透明電極とすることができる。ただし、第1電極130は、光が透過する程度に薄い金属薄膜であっても良い。 The first electrode 130 may be a transparent electrode made of a metal oxide conductor such as ITO (Indium Tin Oxide) or IZO (Indium Zinc Oxide). However, the first electrode 130 may be a metal thin film that is thin enough to transmit light.

 第2電極150は、例えば、Alなどの金属膜からなる反射電極である。第2電極150は、有機機能層140から第2電極150側に向かう光を、透光性基板110側に向けて反射する。 The second electrode 150 is a reflective electrode made of a metal film such as Al. The second electrode 150 reflects light traveling from the organic functional layer 140 toward the second electrode 150 toward the translucent substrate 110.

 第1電極130と第2電極150との間に電圧が印加されることにより、有機機能層140の発光層が発光する。第1電極130、光路変更層120のベース領域122、光路変更層120の光路変更領域121、透光性基板110、及び、有機機能層140は、いずれも、有機機能層140の発光層が発光した光の少なくとも一部を透過する。発光層が発光した光の一部は、透光性基板110の光取り出し面から、発光装置100の外部(つまり上記光放出空間)に放射される(取り出される)。 When a voltage is applied between the first electrode 130 and the second electrode 150, the light emitting layer of the organic functional layer 140 emits light. The first electrode 130, the base region 122 of the optical path changing layer 120, the optical path changing region 121 of the optical path changing layer 120, the translucent substrate 110, and the organic functional layer 140 all emit light from the organic functional layer 140. Transmits at least part of the light. Part of the light emitted from the light emitting layer is emitted (extracted) from the light extraction surface of the light-transmitting substrate 110 to the outside of the light emitting device 100 (that is, the light emission space).

 例えば、光路変更層120において、光路変更領域121以外の領域は、すべてベース領域122となっている。ただし、光路変更層120は、光路変更領域121及びベース領域122の他の領域を含んで構成されていても良い。 For example, in the optical path changing layer 120, all areas other than the optical path changing area 121 are the base area 122. However, the optical path changing layer 120 may be configured to include other areas of the optical path changing area 121 and the base area 122.

 光路変更層120には、1つの光路変更領域121が存在している。または、光路変更層120には、複数の光路変更領域121が、ランダムな配置で存在している。 In the optical path changing layer 120, one optical path changing area 121 exists. Alternatively, the optical path changing layer 120 has a plurality of optical path changing areas 121 in a random arrangement.

 上記のように、光路変更領域121とベース領域122との屈折率差は、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて大きくなっている。すなわち、光路変更領域121の屈折率は、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて、低減又は増大している。ここで、この屈折率差は、光路変更領域121とベース領域122との境界から遠ざかるにつれて、単調増加していることが好ましい。ただし、光路変更領域121とベース領域122との境界から遠ざかる方向において、全体として増加傾向が認められればよく、例えば、一部区間において減少していても良い。 As described above, the refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward. That is, the refractive index of the optical path changing region 121 is reduced or increased as it moves away from the boundary between the optical path changing region 121 and the base region 122 inward of the optical path changing region 121. Here, it is preferable that the refractive index difference monotonously increases as the distance from the boundary between the optical path changing region 121 and the base region 122 increases. However, it is sufficient that an increasing tendency is recognized as a whole in the direction away from the boundary between the optical path changing region 121 and the base region 122, and for example, it may be decreased in a part of the section.

 光路変更領域121の屈折率は、光路変更領域121とベース領域122との境界においては、ベース領域122の屈折率と同じであることが好ましい。 The refractive index of the optical path changing area 121 is preferably the same as the refractive index of the base area 122 at the boundary between the optical path changing area 121 and the base area 122.

 光路変更領域121とベース領域122との屈折率差は、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて、徐々に大きくなっていることが好ましい。すなわち、この屈折率差が不連続に大きくなる箇所が存在しないことが好ましい。 It is preferable that the refractive index difference between the optical path changing area 121 and the base area 122 gradually increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward. That is, it is preferable that there is no portion where the refractive index difference increases discontinuously.

 光路変更領域121の寸法dは、有機機能層140の発光層からの発光波長以上であることが好ましい。発光波長のピーク波長は、例えば、可視光領域である。このため、寸法dは、例えば、少なくとも(360nm/光路変更層120の平均屈折率)以上、好ましくは、少なくとも(400nm/光路変更層120の平均屈折率)以上である。ただし、寸法dは、発光層からの発光波長よりも十分大きいことが好ましい。このため、例えば、光路変更層120の屈折率を1.8とした場合に、個別の発光色の領域の各々について寸法dを定めるなら、寸法dは、青については200nm以上、緑については311nm以上、赤については356nm以上、白色については356nm以上とすることがより好ましい。 The dimension d of the optical path changing region 121 is preferably equal to or longer than the emission wavelength from the light emitting layer of the organic functional layer 140. The peak wavelength of the emission wavelength is, for example, in the visible light region. Therefore, the dimension d is, for example, at least (360 nm / average refractive index of the optical path changing layer 120) or more, and preferably at least (400 nm / average refractive index of the optical path changing layer 120). However, it is preferable that the dimension d is sufficiently larger than the emission wavelength from the light emitting layer. Therefore, for example, when the refractive index of the optical path changing layer 120 is 1.8, if the dimension d is determined for each of the individual emission color regions, the dimension d is 200 nm or more for blue and 311 nm for green. As mentioned above, it is more preferable to set it as 356 nm or more about red, and 356 nm or more about white.

 例えば、光路変更領域121の形状は、直径が発光層からの発光波長以上の球形の少なくとも一部分である。すなわち、光路変更領域121の外形形状は、直径が発光層からの発光波長以上の球形の外周面の少なくとも一部分を含む。例えば、光路変更領域121の外形は、第2電極150側に向けて凸の曲面を含む。例えば、図1に示すように、光路変更領域121は、直径が発光層からの発光波長以上の球形の下半部を含んでおり、第2電極150側(図1において下側)に向けて凸の曲面を含む。 For example, the shape of the optical path changing region 121 is at least a part of a sphere having a diameter equal to or larger than the emission wavelength from the light emitting layer. That is, the outer shape of the optical path changing region 121 includes at least a part of a spherical outer peripheral surface having a diameter equal to or larger than the emission wavelength from the light emitting layer. For example, the outer shape of the optical path changing region 121 includes a curved surface that is convex toward the second electrode 150 side. For example, as shown in FIG. 1, the optical path changing region 121 includes a spherical lower half having a diameter equal to or larger than the emission wavelength from the light emitting layer, and is directed toward the second electrode 150 (downward in FIG. 1). Includes convex curved surfaces.

 なお、図1では、光路変更領域121が光路変更層120における透光性基板110側の端面(図1の上面)に露出している例を示しているが、当該端面に光路変更領域121が露出していなくても良い。すなわち光路変更層120における透光性基板110側の端面と光路変更領域121との間にベース領域122の一部分が存在していても良い。また、図1では、球形の上部が欠けた形状の光路変更領域121を例示しているが、光路変更領域121が球形(の全体)であっても良い。 1 shows an example in which the optical path changing region 121 is exposed on the end surface (upper surface in FIG. 1) of the optical path changing layer 120 on the light transmitting substrate 110 side, the optical path changing region 121 is on the end surface. It does not have to be exposed. That is, a part of the base region 122 may exist between the end surface of the light path changing layer 120 on the light transmitting substrate 110 side and the light path changing region 121. Further, in FIG. 1, the optical path changing area 121 having a shape in which the upper part of the sphere is missing is illustrated, but the optical path changing area 121 may be spherical (entire).

 本実施形態の場合、例えば、光路変更領域121は、ベース領域122よりも屈折率が小さい領域を含む。例えば、光路変更領域121とベース領域122との境界を除き、光路変更領域121の屈折率は、ベース領域122の屈折率よりも小さい。 In the case of the present embodiment, for example, the optical path changing region 121 includes a region having a refractive index smaller than that of the base region 122. For example, except for the boundary between the optical path changing area 121 and the base area 122, the refractive index of the optical path changing area 121 is smaller than the refractive index of the base area 122.

 本実施形態の場合、光路変更層120は、透光性基板110と第1電極130との間に配置されている。この場合、光路変更層120のベース領域122及び光路変更領域121からなる層の屈折率は、例えば、透光性基板110の屈折率以上で、且つ、2.0以下であることが好ましい。より好ましくは、光路変更層120の屈折率は、第1電極130の屈折率と同等とする。 In the case of this embodiment, the optical path changing layer 120 is disposed between the translucent substrate 110 and the first electrode 130. In this case, the refractive index of the layer including the base region 122 and the optical path changing region 121 of the optical path changing layer 120 is preferably not less than the refractive index of the translucent substrate 110 and not more than 2.0, for example. More preferably, the refractive index of the optical path changing layer 120 is equal to the refractive index of the first electrode 130.

 また、光路変更層120のベース領域122及び光路変更領域121からなる層の屈折率は、例えば、有機機能層140の屈折率以上とすることができる。光路変更層120は、例えば、誘電体からなる。光路変更層120の材料は、例えば、有機機能層140の材料と同じとすることができる。有機機能層140の屈折率は、例えば、1.6以上2.0以下程度である。 In addition, the refractive index of the layer including the base region 122 and the optical path changing region 121 of the optical path changing layer 120 can be set to be equal to or higher than the refractive index of the organic functional layer 140, for example. The optical path changing layer 120 is made of a dielectric, for example. The material of the optical path changing layer 120 can be the same as the material of the organic functional layer 140, for example. The refractive index of the organic functional layer 140 is, for example, about 1.6 or more and 2.0 or less.

 光路変更領域121は、例えば、光路変更層120(ベース領域122)の一部分を加熱することにより形成されている。したがって、光路変更層120の材料としては、例えば、加熱により屈折率が低下するものを用いることができる。すなわち、光路変更層120の材料は、有機機能層140の屈折率以上の屈折率を有し、加熱により低屈折率となる材料とすることができる。このような材料の例としては、DVD又はCDなどに用いられるフタロシアニンなどの有機材料が挙げられる。光路変更層120の一部分を加熱することにより、分子構造が破壊され、加熱された部分の屈折率が低下する。 The optical path changing area 121 is formed, for example, by heating a part of the optical path changing layer 120 (base area 122). Therefore, as the material of the optical path changing layer 120, for example, a material whose refractive index is lowered by heating can be used. That is, the material of the optical path changing layer 120 can be a material having a refractive index higher than that of the organic functional layer 140 and having a low refractive index when heated. Examples of such materials include organic materials such as phthalocyanine used for DVDs or CDs. By heating a part of the optical path changing layer 120, the molecular structure is destroyed and the refractive index of the heated part is lowered.

 例えば、透光性基板110の一方の面(図1における下面)と光路変更層120の一方の面(図1における上面)とが相互に接している。また、光路変更層120の他方の面(図1における下面)と第1電極130の一方の面(図1における上面)とが相互に接している。また、第1電極130の他方の面(図1における下面)と有機機能層140の一方の面(図1における上面)とが相互に接している。また、有機機能層140の他方の面(図1における下面)と第2電極150の一方の面(図1における上面)とが相互に接している。ただし、透光性基板110と光路変更層120との間には他の層が存在していても良い。同様に、光路変更層120と第1電極130との間には他の層が存在していても良い。同様に、第1電極130と有機機能層140との間には他の層が存在していても良い。同様に、有機機能層140と第2電極150との間には他の層が存在していても良い。 For example, one surface (the lower surface in FIG. 1) of the translucent substrate 110 and one surface (the upper surface in FIG. 1) of the optical path changing layer 120 are in contact with each other. Further, the other surface (lower surface in FIG. 1) of the optical path changing layer 120 and one surface (upper surface in FIG. 1) of the first electrode 130 are in contact with each other. Further, the other surface (lower surface in FIG. 1) of the first electrode 130 and one surface (upper surface in FIG. 1) of the organic functional layer 140 are in contact with each other. Further, the other surface (lower surface in FIG. 1) of the organic functional layer 140 and one surface (upper surface in FIG. 1) of the second electrode 150 are in contact with each other. However, another layer may exist between the translucent substrate 110 and the optical path changing layer 120. Similarly, another layer may exist between the optical path changing layer 120 and the first electrode 130. Similarly, another layer may exist between the first electrode 130 and the organic functional layer 140. Similarly, another layer may exist between the organic functional layer 140 and the second electrode 150.

 図2は光路変更層120から透光性基板110にかけての屈折率の変化特性の例を示す図である。すなわち、図2は図1の線分Aの一端A1から他端A2にかけての屈折率の変化特性の例を示す。例えば、ベース領域122内においては、位置にかかわらず屈折率が一定である(図2の領域R1)。ベース領域122と光路変更領域121との境界(図2の領域R1と領域R2との境界)の屈折率は、ベース領域122の屈折率と同じである。光路変更領域121内においては、光路変更領域121とベース領域122との境界から遠ざかるにつれて、すなわち上記の球形(直径が発光層からの発光波長以上の球形)の中心に向かうにつれて、徐々に屈折率が低減している(図2の領域R2)。更に上記の球形の中心から透光性基板110側に向かうにつれて、再び屈折率が徐々に増大している(図2の領域R3)。このように、光路変更領域121の屈折率は、ベース領域122との境界においてはベース領域122の屈折率と同じであり、且つ、当該境界から遠ざかるにつれて徐々に低減している。なお、透光性基板110の屈折率は、光路変更層120の屈折率よりも小さい(図2の領域R4)。 FIG. 2 is a diagram showing an example of the refractive index change characteristic from the optical path changing layer 120 to the translucent substrate 110. That is, FIG. 2 shows an example of the refractive index change characteristic from one end A1 to the other end A2 of the line segment A in FIG. For example, in the base region 122, the refractive index is constant regardless of the position (region R1 in FIG. 2). The refractive index of the boundary between the base region 122 and the optical path changing region 121 (the boundary between the region R1 and the region R2 in FIG. 2) is the same as the refractive index of the base region 122. In the optical path changing region 121, the refractive index gradually increases as the distance from the boundary between the optical path changing region 121 and the base region 122 increases, that is, toward the center of the above-described spherical shape (a spherical shape whose diameter is equal to or larger than the emission wavelength from the light emitting layer). Is reduced (region R2 in FIG. 2). Furthermore, the refractive index gradually increases again from the spherical center toward the light transmitting substrate 110 (region R3 in FIG. 2). As described above, the refractive index of the optical path changing region 121 is the same as the refractive index of the base region 122 at the boundary with the base region 122, and gradually decreases as the distance from the boundary increases. In addition, the refractive index of the translucent substrate 110 is smaller than the refractive index of the optical path changing layer 120 (region R4 in FIG. 2).

 図3は第1の実施形態に係る発光装置100の動作の例を示す要部断面図であり、透光性基板110、光路変更層120及び第1電極130のみを図示している。光路変更領域121の屈折率が、ベース領域122から遠ざかるにつれて低減している場合、例えば、以下に説明するような動作を実現することができる。 FIG. 3 is a cross-sectional view of a main part illustrating an example of the operation of the light emitting device 100 according to the first embodiment, and illustrates only the translucent substrate 110, the optical path changing layer 120, and the first electrode 130. When the refractive index of the optical path changing region 121 decreases as the distance from the base region 122 increases, for example, an operation as described below can be realized.

 光路変更層120の屈折率が十分な大きさ(透光性基板110の屈折率以上)であることにより、第1電極130内を斜め上向きに進む光は、そのまま光路変更層120に入射する。 When the refractive index of the optical path changing layer 120 is sufficiently large (more than the refractive index of the translucent substrate 110), the light traveling obliquely upward in the first electrode 130 is incident on the optical path changing layer 120 as it is.

 この光は、光路変更層120に光路変更領域121が存在しない場合には、図3に示す光路L11、L12の順に進むものとする。すなわち、この光は、光路変更層120内を斜め上向きに進み(光路L11)、その後、光路変更層120と透光性基板110との界面において反射して、斜め下向きに進む(光路L12)ものとする。 Suppose that this light travels in the order of the optical paths L11 and L12 shown in FIG. 3 when the optical path changing area 121 does not exist in the optical path changing layer 120. That is, the light travels obliquely upward in the optical path changing layer 120 (optical path L11), and then reflects at the interface between the optical path changing layer 120 and the translucent substrate 110 and travels diagonally downward (optical path L12). And

 本実施形態の場合、光路変更層120に光路変更領域121が存在することにより、この光の光路は、光路L1で示されるように、光路変更領域121内を通過する過程で、徐々に上向きに変更される。これにより、この光の向きを光路変更層120と透光性基板110との界面における臨界角未満に変更し、この光を光路変更領域121から透光性基板110側へ入射させることができる。更に、この光を透光性基板110から更にその上側(つまり発光装置100の外部)へ放射させることができる。 In the case of the present embodiment, since the optical path changing region 121 exists in the optical path changing layer 120, the optical path of this light gradually increases in the process of passing through the optical path changing region 121 as indicated by the optical path L1. Be changed. Thereby, the direction of this light can be changed to less than the critical angle at the interface between the optical path changing layer 120 and the translucent substrate 110, and this light can be incident from the optical path changing region 121 to the translucent substrate 110 side. Further, this light can be emitted from the translucent substrate 110 to the upper side thereof (that is, outside the light emitting device 100).

 次に、本実施形態に係る発光装置の製造方法の一例を説明する。図4はこの製造方法の一部の工程を示す断面図である。この製造方法は、以下の(1)~(4)の工程を備える。
 (1)透光性基板110の一方の面側に、透光性の第1電極130を形成する工程
 (2)第1電極130を基準として透光性基板110とは反対側に、少なくとも発光層を含んで構成される有機機能層140を形成する工程
 (3)有機機能層140を基準として第1電極130とは反対側に、第2電極150を形成する工程
 (4)光を透過させる過程で当該光の光路を変更する光路変更領域121と、光路変更領域121以外のベース領域122と、を含んで構成される光路変更層120を、透光性基板110と第2電極150との間に形成する工程(図4(a)、図4(b))
 そして、光路変更層120を形成する工程では、光路変更領域121とベース領域122との屈折率差が、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて大きくなるように、光路変更層120を形成する。
Next, an example of a method for manufacturing the light emitting device according to this embodiment will be described. FIG. 4 is a sectional view showing a part of the manufacturing method. This manufacturing method includes the following steps (1) to (4).
(1) Step of forming a transparent first electrode 130 on one surface side of the transparent substrate 110 (2) At least light emission on the opposite side of the transparent substrate 110 with respect to the first electrode 130 Step of forming organic functional layer 140 including layers (3) Step of forming second electrode 150 on the side opposite to first electrode 130 with respect to organic functional layer 140 (4) Transmitting light An optical path changing layer 120 including an optical path changing area 121 that changes the optical path of the light in the process and a base area 122 other than the optical path changing area 121 is formed between the translucent substrate 110 and the second electrode 150. Step of forming in between (FIGS. 4A and 4B)
In the step of forming the optical path changing layer 120, the refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward of the optical path changing area 121. Thus, the optical path changing layer 120 is formed.

 以下、図1及び図4を参照して、製造工程を順に説明する。 Hereinafter, the manufacturing process will be described in order with reference to FIG. 1 and FIG.

 先ず、透光性基板110の下面に、NPBやフタロシアニンなどの有機材料を蒸着又は塗布し、光路変更層120におけるベース領域122となる部分を形成する(図4(a))。なお、ベース領域122の成膜後、適切なタイミングで光路変更領域121を形成する。光路変更領域121を形成するタイミング及びその形成方法については後述する。 First, an organic material such as NPB or phthalocyanine is vapor-deposited or applied on the lower surface of the translucent substrate 110 to form a portion that becomes the base region 122 in the optical path changing layer 120 (FIG. 4A). Note that the optical path changing region 121 is formed at an appropriate timing after the base region 122 is formed. The timing and method for forming the optical path changing region 121 will be described later.

 次に、光路変更層120(ベース領域122)の下面に、スパッタ法などによりITO(Indium Tin Oxide)やIZO(Indium Zinc Oxide)などの金属酸化物導電体からなる透光性の導電膜を成膜し、エッチングによりこれをパターニングして第1電極130を形成する。 Next, a light-transmitting conductive film made of a metal oxide conductor such as ITO (Indium Tin Oxide) or IZO (Indium Zinc Oxide) is formed on the lower surface of the optical path changing layer 120 (base region 122) by sputtering or the like. A first electrode 130 is formed by patterning the film by etching.

 次に、第1電極130の下面に有機材料を塗布することにより有機機能層140を形成する。 Next, the organic functional layer 140 is formed by applying an organic material to the lower surface of the first electrode 130.

 次に、有機機能層140の下面に、マスクを用いた蒸着法などによりAl等の金属材料を所望のパターンに堆積させて、第2電極150を形成する。 Next, a second electrode 150 is formed by depositing a metal material such as Al in a desired pattern on the lower surface of the organic functional layer 140 by vapor deposition using a mask or the like.

 なお、必要に応じてバスラインや隔壁(図9参照)をそれぞれ適切なタイミングで形成しても良い。また、第2電極150の下面には必要に応じて封止層を形成しても良い。 In addition, you may form a bus line and a partition (refer FIG. 9) at an appropriate timing as needed. Further, a sealing layer may be formed on the lower surface of the second electrode 150 as necessary.

 次に、光路変更領域121の形成の仕方について説明する。 Next, how to form the optical path changing region 121 will be described.

 光路変更領域121は、光を照射することによって光路変更層120(ベース領域122)の一部分を加熱することにより形成する。具体的には、例えば、光路変更層120の一部分に対してレーザ光を照射することにより、光路変更層120の一部分を加熱し、光路変更領域121を形成することができる(図4(b))。光路変更層120の一部分を加熱することにより、光路変更層120を構成する材料の分子構造が変化したり、或いは、光路変更層120を構成する材料の粗密分布が変化(本実施形態の場合、密度が低下)したりするので、当該一部分の屈折率が低下する。 The optical path changing region 121 is formed by heating a part of the optical path changing layer 120 (base region 122) by irradiating light. Specifically, for example, by irradiating a part of the optical path changing layer 120 with laser light, a part of the optical path changing layer 120 can be heated to form the optical path changing area 121 (FIG. 4B). ). By heating a part of the optical path changing layer 120, the molecular structure of the material constituting the optical path changing layer 120 is changed, or the density distribution of the material constituting the optical path changing layer 120 is changed (in this embodiment, The refractive index of the portion decreases.

 ここで、上述した方法により照射される光(レーザ光等)の強度分布はガウシアン分布であり、当該光の照射スポットの中心部の強度が高くなる。このため、照射スポットの中央に近いほど、光路変更層120を構成する材料の分子構造や粗密分布に与える影響が大きい。よって、光路変更領域121の屈折率は、例えば、照射スポットの中心に向けて徐々に低減する。 Here, the intensity distribution of the light (laser light or the like) irradiated by the above-described method is a Gaussian distribution, and the intensity of the central portion of the irradiation spot of the light is increased. For this reason, the closer to the center of the irradiation spot, the greater the influence on the molecular structure and density distribution of the material constituting the optical path changing layer 120. Therefore, for example, the refractive index of the optical path changing region 121 gradually decreases toward the center of the irradiation spot.

 光路変更領域121を形成するタイミングは、光路変更層120(ベース領域122)の形成後の任意のタイミングとすることができる。 The timing for forming the optical path changing region 121 can be any timing after the optical path changing layer 120 (base region 122) is formed.

 光路変更層120(ベース領域122)の形成後、第1電極130の形成前に、光路変更領域121を形成する場合は、光路変更層120(ベース領域122)の何れの面側から光を照射しても良い。
 また、第1電極130の形成後、有機機能層140の形成前に、光路変更領域121を形成する場合は、効率的光の照射および、集中した光による第1電極130のダメージを抑制するために、加工するポイントから近い透光性基板110側から光を照射する。
 これらの何れの場合も、未だ有機機能層140が形成されていない。このため、有機機能層140へのダメージを考慮する必要がないので、CWレーザ(連続波発振動作レーザ)とパルスレーザの何れを用いても良い。
When forming the optical path changing region 121 after forming the optical path changing layer 120 (base region 122) and before forming the first electrode 130, light is irradiated from any surface side of the optical path changing layer 120 (base region 122). You may do it.
In addition, when the optical path changing region 121 is formed after the formation of the first electrode 130 and before the formation of the organic functional layer 140, in order to suppress efficient light irradiation and damage to the first electrode 130 due to concentrated light. Further, light is irradiated from the side of the transparent substrate 110 close to the processing point.
In any of these cases, the organic functional layer 140 has not yet been formed. For this reason, since it is not necessary to consider the damage to the organic functional layer 140, either a CW laser (continuous wave oscillation operation laser) or a pulse laser may be used.

 また、有機機能層140及び第2電極150の形成後、封止まで終わってパネル構造の発光装置100を構築した後で、光路変更領域121を形成しても良い。この場合、透光性基板110側から光を照射する。この場合、CWレーザやパルスレーザを用いるには、有機機能層140になるべく熱が加わらないように配慮することが好ましい。或いは、フェムト秒レーザやナノ秒レーザを用いても良い。 Further, after the formation of the organic functional layer 140 and the second electrode 150, the optical path changing region 121 may be formed after the sealing is completed and the light emitting device 100 having the panel structure is constructed. In this case, light is irradiated from the translucent substrate 110 side. In this case, in order to use a CW laser or a pulse laser, it is preferable to consider that heat is not applied to the organic functional layer 140 as much as possible. Alternatively, a femtosecond laser or a nanosecond laser may be used.

 レーザを一回照射することにより大きな領域の光路変更領域121を形成しても良いし、複数回に分けて小さな領域に対する照射を行い、これら領域の集合により大きな領域の光路変更領域121を形成しても良い。この場合、光路変更領域121内において、屈折率の不連続面が形成される場合がある。 The large-area optical path changing area 121 may be formed by irradiating the laser once, or the small area is irradiated in a plurality of times, and the large-area optical path changing area 121 is formed by a set of these areas. May be. In this case, a discontinuous surface with a refractive index may be formed in the optical path changing region 121.

 なお、光路変更領域121を形成するための光の照射は、レーザ光の照射に限らない。例えば、レーザ以外の強力な単一波長の光を、マスクを透過させ、且つ、レンズにより集光して光路変更層120の一部分に結像することによっても、光路変更領域121を形成することができる。この場合、レーザ光を用いる場合よりも広い領域を一度に加熱処理することも可能である。 Note that the light irradiation for forming the optical path changing region 121 is not limited to the laser light irradiation. For example, the optical path changing region 121 can also be formed by allowing light having a single wavelength other than the laser to pass through the mask and condensing with a lens and forming an image on a part of the optical path changing layer 120. it can. In this case, it is possible to perform heat treatment on a larger area at a time than when laser light is used.

 以上、第1の実施形態によれば、発光装置100は、透光性基板110と第2電極150との間に配置されている光路変更層120を備える。この光路変更層120は、光路変更領域121と、ベース領域122と、を含んで構成されている。光が光路変更領域121を透過する過程で、当該光の光路が変更されるので、光路変更領域121が存在しなければ発光装置100から取り出されずに発光装置100内で反射を繰り返して減衰してしまう光の光路を、発光装置100から取り出される向きに変更することができる。よって、光取り出し効率を向上させることができる。 As described above, according to the first embodiment, the light emitting device 100 includes the optical path changing layer 120 disposed between the translucent substrate 110 and the second electrode 150. The optical path changing layer 120 includes an optical path changing area 121 and a base area 122. In the process of light passing through the optical path changing area 121, the optical path of the light is changed. Therefore, if the optical path changing area 121 does not exist, the light is not taken out from the light emitting apparatus 100 and is repeatedly reflected and attenuated in the light emitting apparatus 100. It is possible to change the optical path of the light to be taken out from the light emitting device 100. Therefore, the light extraction efficiency can be improved.

 ここで、光路変更領域121とベース領域122との屈折率差は、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて大きくなっている。一般的に屈折率が互いに異なる2つの層において徐々に屈折率が変わると、臨界角近辺での透過率が急に変わることがシミュレーションで解っている。すなわち屈折率が界面で急峻に変化すると、臨界角直前の透過率が減少し、その分反射率が多くなる。逆に徐々に屈折率が変わると臨界角直前まで、透過率が高い状態が実現可能である。また、ベース領域122と光路変更領域121との屈折率差が抑制された構造を実現でき、ベース領域122と光路変更領域121との間には顕著な界面が存在しないようにできる。これにより、ベース領域122と光路変更領域121との境界における光の反射の発生が抑制される。よって、光路変更領域121が存在していない場合であっても発光装置100から取り出される光についても、スムーズに光路変更領域121内に入射させた後に、発光装置100から放射させることができる。これにより、光取り出し効率を一層向上させることができる。 Here, the refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward. In general, it has been found by simulation that the transmittance in the vicinity of the critical angle suddenly changes when the refractive index gradually changes in two layers having different refractive indexes. That is, when the refractive index changes sharply at the interface, the transmittance just before the critical angle decreases, and the reflectance increases accordingly. Conversely, when the refractive index gradually changes, it is possible to realize a state where the transmittance is high until just before the critical angle. Further, it is possible to realize a structure in which the difference in refractive index between the base region 122 and the optical path changing region 121 is suppressed, and there is no significant interface between the base region 122 and the optical path changing region 121. Thereby, the occurrence of light reflection at the boundary between the base region 122 and the optical path changing region 121 is suppressed. Therefore, even when the optical path changing region 121 does not exist, the light extracted from the light emitting device 100 can be emitted from the light emitting device 100 after smoothly entering the optical path changing region 121. Thereby, the light extraction efficiency can be further improved.

 特に、光路変更領域121の屈折率が、光路変更領域121とベース領域122との境界においてはベース領域122の屈折率と同じである場合、ベース領域122と光路変更領域121との境界において光の反射が実質的に発生しないようにできる。このため、光取り出し効率を一層向上させることができる。 In particular, when the refractive index of the optical path changing region 121 is the same as the refractive index of the base region 122 at the boundary between the optical path changing region 121 and the base region 122, Reflection can be substantially prevented from occurring. For this reason, the light extraction efficiency can be further improved.

 また、光路変更領域121とベース領域122との屈折率差が、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて徐々に大きくなっている場合、光路変更領域121内において屈折率が不連続に変化する箇所が無い。これにより、光路変更領域121内における光の反射が実質的に発生しないようにできる。このため、光取り出し効率を一層向上させることができる。 In addition, when the refractive index difference between the optical path changing area 121 and the base area 122 gradually increases from the boundary between the optical path changing area 121 and the base area 122 toward the inward direction of the optical path changing area 121, the optical path changing area There are no places where the refractive index changes discontinuously in 121. Thereby, the reflection of the light in the optical path changing area 121 can be substantially prevented from occurring. For this reason, the light extraction efficiency can be further improved.

 また、光路変更領域121の寸法が、発光層からの発光波長以上であることにより、光路変更領域121とベース領域122との境界における光の屈折および反射をより確実に制御(散乱を抑制)でき、光取り出し効率を向上させることができる。光路変更領域121の寸法が小さ過ぎる場合は、光が光路変更領域121を直進して透過するのみとなってしまい、光路変更領域121にて光路を変更できない場合が生じる。 Further, when the dimension of the optical path changing region 121 is equal to or greater than the emission wavelength from the light emitting layer, the refraction and reflection of light at the boundary between the optical path changing region 121 and the base region 122 can be controlled more reliably (scattering can be suppressed). The light extraction efficiency can be improved. When the dimension of the optical path changing area 121 is too small, light only travels straight through the optical path changing area 121 and may not be changed in the optical path changing area 121.

 また、光路変更領域121の形状が、直径が発光層からの発光波長以上の球形の少なくとも一部分である場合、光路変更領域121の外形形状は、当該光路変更領域121の外方に向けて凸の曲面を含む。このため、光路変更領域121の外形は、様々な角度を持つ。よって、様々な角度で光路変更領域121に入射する光について、当該光の向きを、発光装置100からの光取り出しが可能な角度に変更することができる。 Further, when the shape of the optical path changing region 121 is at least a part of a sphere having a diameter equal to or larger than the emission wavelength from the light emitting layer, the outer shape of the optical path changing region 121 is convex toward the outside of the optical path changing region 121. Includes curved surfaces. For this reason, the external shape of the optical path changing area 121 has various angles. Therefore, for light incident on the optical path changing region 121 at various angles, the direction of the light can be changed to an angle at which light can be extracted from the light emitting device 100.

 また、光路変更領域121の外形が、第2電極150側に向けて凸の曲面を含む場合、光路変更領域121における第2電極150側の外形は、様々な角度を持つ。よって、第2電極150側から、様々な角度で光路変更領域121に入射する光について、当該光の向きを、発光装置100からの光取り出しが可能な角度に変更することができる。 Further, when the outer shape of the optical path changing region 121 includes a curved surface convex toward the second electrode 150 side, the outer shape of the optical path changing region 121 on the second electrode 150 side has various angles. Therefore, for the light incident on the optical path changing region 121 at various angles from the second electrode 150 side, the direction of the light can be changed to an angle at which light can be extracted from the light emitting device 100.

 また、光路変更領域121は、ベース領域122よりも屈折率が小さい領域を含むので、例えば図3に示すように、第2電極150側から透光性基板110側に斜めに向かう光の向きを、発光装置100から取り出される方向へと容易に変更することができる。 Further, since the optical path changing region 121 includes a region having a refractive index smaller than that of the base region 122, for example, as shown in FIG. 3, the direction of light obliquely traveling from the second electrode 150 side to the translucent substrate 110 side is set. Thus, the direction can be easily changed in the direction of taking out from the light emitting device 100.

 ここで、第1電極130は、例えばITOなどからなる透明電極とすることができる。ITOなどの透明電極は屈折率が高い(例えば、1.75以上1.83以下程度)。このため、光路変更層120が透光性基板110と第1電極130との間に配置されている場合に、上述したように、光路変更層120の屈折率を、透光性基板110の屈折率以上で、且つ、2.0以下とすることが好ましい。これにより、第1電極130から光路変更層120へと光を容易に取り出すことができ、且つ、光路変更層120から透光性基板110へも光を容易に取り出すことができる。 Here, the first electrode 130 may be a transparent electrode made of, for example, ITO. A transparent electrode such as ITO has a high refractive index (for example, about 1.75 to 1.83). Therefore, when the optical path changing layer 120 is disposed between the translucent substrate 110 and the first electrode 130, as described above, the refractive index of the optical path changing layer 120 is set to the refractive index of the translucent substrate 110. It is preferable that the ratio is not less than 2.0 and not more than 2.0. Thereby, light can be easily extracted from the first electrode 130 to the optical path changing layer 120, and light can also be easily extracted from the optical path changing layer 120 to the translucent substrate 110.

 ここで、特許文献1に記載されているように、酸化チタン層などの媒質中にSiOなどの微小球を分散させる場合、微小球を媒質中の任意の位置に配置することが困難である。これに対し、本実施形態では、例えば、光を照射することなどにより光路変更層120(ベース領域122)の一部分を加熱することによって光路変更領域121を形成する。よって、光路変更領域121を、光路変更層120における所望の位置に所望のサイズで容易に形成することができるので、所望の構造の発光装置100を容易に製造することができる。 Here, as described in Patent Document 1, when microspheres such as SiO 2 are dispersed in a medium such as a titanium oxide layer, it is difficult to arrange the microspheres at an arbitrary position in the medium. . On the other hand, in this embodiment, for example, the optical path changing region 121 is formed by heating a part of the optical path changing layer 120 (base region 122) by irradiating light or the like. Therefore, since the optical path changing region 121 can be easily formed at a desired position in the optical path changing layer 120 with a desired size, the light emitting device 100 having a desired structure can be easily manufactured.

 また、特許文献1の技術では、高屈折率層と、高屈折率層に接している層とが、それぞれ酸化チタン層からなるため、仮に強固なバリア膜を追加で形成したとしても、これらの酸化チタン層が有機発光層に悪影響を与える可能性がある。これに対し、本実施形態では、光路変更層120として、フタロシアニンなどの有機層の一部分の屈折率を変化させたものを用いるので、有機機能層140への悪影響を抑制できる。 In the technique of Patent Document 1, since the high refractive index layer and the layer in contact with the high refractive index layer are each made of a titanium oxide layer, even if a strong barrier film is additionally formed, The titanium oxide layer may adversely affect the organic light emitting layer. On the other hand, in this embodiment, since the optical path changing layer 120 is a layer in which the refractive index of a part of the organic layer such as phthalocyanine is changed, adverse effects on the organic functional layer 140 can be suppressed.

 (第2の実施形態)
 図5は第2の実施形態に係る発光装置100の構成を示す断面図である。
(Second Embodiment)
FIG. 5 is a cross-sectional view showing the configuration of the light emitting device 100 according to the second embodiment.

 第2の実施形態の場合、上記の第1の実施形態における光路変更層120と同様の構成の光路変更層160が、有機機能層140と第2電極150との間に配置されている。光路変更層160は、光路変更領域121と同様の光路変更領域161と、ベース領域122と同様のベース領域162と、を含んで構成されている。なお、光路変更層160の材質は、例えば、有機機能層140の電子注入層(後述)と同じ材料としても良い。この場合、光路変更層160の屈折率は、1.5以上1.8以下程度である。 In the case of the second embodiment, the optical path changing layer 160 having the same configuration as the optical path changing layer 120 in the first embodiment is disposed between the organic functional layer 140 and the second electrode 150. The optical path changing layer 160 includes an optical path changing area 161 similar to the optical path changing area 121 and a base area 162 similar to the base area 122. The material of the optical path changing layer 160 may be the same material as the electron injection layer (described later) of the organic functional layer 140, for example. In this case, the refractive index of the optical path changing layer 160 is about 1.5 or more and 1.8 or less.

 第2の実施形態の場合、上記の第1の実施形態において光路変更層120が配置されている領域には、例えば、光路変更層120の代わりに高屈折率層190が配置されていても良い。高屈折率層190は、光路変更層120のベース領域122と同様の材質及び光学的特性のものである。 In the case of the second embodiment, in the region where the optical path changing layer 120 is arranged in the first embodiment, for example, a high refractive index layer 190 may be arranged instead of the optical path changing layer 120. . The high refractive index layer 190 has the same material and optical characteristics as the base region 122 of the optical path changing layer 120.

 なお、有機機能層140と光路変更層160とは相互に接していても良いし、有機機能層140と光路変更層160との間に他の層が存在していても良い。同様に、光路変更層160と第2電極150とは相互に接していても良いし、光路変更層160と第2電極150との間に他の層が存在していても良い。同様に、透光性基板110と高屈折率層190とは相互に接していても良いし、透光性基板110と高屈折率層190との間に他の層が存在していても良い。同様に、高屈折率層190と第1電極130とは相互に接していても良いし、高屈折率層190と第1電極130との間に他の層が存在していても良い。 Note that the organic functional layer 140 and the optical path changing layer 160 may be in contact with each other, or another layer may exist between the organic functional layer 140 and the optical path changing layer 160. Similarly, the optical path changing layer 160 and the second electrode 150 may be in contact with each other, or another layer may exist between the optical path changing layer 160 and the second electrode 150. Similarly, the translucent substrate 110 and the high refractive index layer 190 may be in contact with each other, or another layer may exist between the translucent substrate 110 and the high refractive index layer 190. . Similarly, the high refractive index layer 190 and the first electrode 130 may be in contact with each other, or another layer may exist between the high refractive index layer 190 and the first electrode 130.

 第2の実施形態のように有機機能層140と第2電極150との間に光路変更層160が配置されている場合にも、上記の第1の実施形態と同様に、光取り出し効率を向上することができる。 When the optical path changing layer 160 is disposed between the organic functional layer 140 and the second electrode 150 as in the second embodiment, the light extraction efficiency is improved as in the first embodiment. can do.

 有機機能層140は、ある程度屈折率が高い(例えば1.8程度の)材質からなる場合がある。このため、本実施形態のように光路変更層160が有機機能層140と第2電極150との間に配置されている場合には、光路変更層160の屈折率を、1.0以上で、且つ、有機機能層140の屈折率以下とすることが好ましい。これにより、光路変更層160から有機機能層140へと光を容易に取り出すことができるとともに、光路変更層160と第2電極150との界面における光の反射性を高め、より多くの光を透光性基板110側に向かわせることができる。 The organic functional layer 140 may be made of a material having a high refractive index to some extent (for example, about 1.8). For this reason, when the optical path changing layer 160 is disposed between the organic functional layer 140 and the second electrode 150 as in the present embodiment, the refractive index of the optical path changing layer 160 is 1.0 or more, In addition, the refractive index is preferably equal to or lower than the refractive index of the organic functional layer 140. Accordingly, light can be easily extracted from the optical path changing layer 160 to the organic functional layer 140, and the light reflectivity at the interface between the optical path changing layer 160 and the second electrode 150 is increased, and more light is transmitted. It can be directed to the optical substrate 110 side.

 (第3の実施形態)
 図6は第3の実施形態に係る発光装置100の構成を示す断面図である。
(Third embodiment)
FIG. 6 is a cross-sectional view illustrating a configuration of a light emitting device 100 according to the third embodiment.

 第3の実施形態に係る発光装置100は、上記の第1の実施形態の構成に加えて、有機機能層140と第2電極150との間に配置された光路変更層160を有している。すなわち、第3の実施形態に係る発光装置100は、2層の光路変更層120、160を有している。光路変更層120の構成は上記の第1の実施形態と同様であり、光路変更層160の構成は上記の第2の実施形態と同様である。 The light emitting device 100 according to the third embodiment includes an optical path changing layer 160 disposed between the organic functional layer 140 and the second electrode 150 in addition to the configuration of the first embodiment. . That is, the light emitting device 100 according to the third embodiment includes two optical path changing layers 120 and 160. The configuration of the optical path changing layer 120 is the same as that of the first embodiment, and the configuration of the optical path changing layer 160 is the same as that of the second embodiment.

 第3の実施形態のように2層の光路変更層120、160を有している場合にも、上記の第1の実施形態と同様に、光取り出し効率を向上することができる。 Even in the case of having two optical path changing layers 120 and 160 as in the third embodiment, the light extraction efficiency can be improved as in the first embodiment.

 (第4の実施形態)
 第4の実施形態の場合、光路変更領域121は多結晶化している点で第1の実施形態と相違する。すなわち、光路変更領域121は、ベース領域122の材料を加熱冷却により結晶化したものである。NPBなどは、加熱冷却により、線状の結晶がまるく成長しながら球状の形状になる。その結果、光路変更領域121は、ベース領域122よりも屈折率が大きい領域を含む。本実施形態の場合、光路変更領域121とベース領域122との境界は多結晶の球体とのその周囲のベース領域122との境界なので、光路変更領域121とベース領域122との境界においては、光路変更領域121の屈折率は、ベース領域122の屈折率と同じである。例えば、光路変更領域121とベース領域122との境界を除き、光路変更領域121の屈折率は、ベース領域122の屈折率よりも大きい。光路変更領域121の屈折率は、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて、(例えば徐々に)増大している。
(Fourth embodiment)
In the case of the fourth embodiment, the optical path changing region 121 is different from the first embodiment in that it is polycrystallized. That is, the optical path changing region 121 is obtained by crystallizing the material of the base region 122 by heating and cooling. NPB or the like becomes a spherical shape while linear crystals grow as a whole by heating and cooling. As a result, the optical path changing region 121 includes a region having a refractive index larger than that of the base region 122. In the present embodiment, since the boundary between the optical path changing region 121 and the base region 122 is the boundary between the polycrystalline sphere and the surrounding base region 122, the optical path is changed at the boundary between the optical path changing region 121 and the base region 122. The refractive index of the change region 121 is the same as the refractive index of the base region 122. For example, except for the boundary between the optical path changing region 121 and the base region 122, the refractive index of the optical path changing region 121 is larger than the refractive index of the base region 122. The refractive index of the optical path changing area 121 increases (for example, gradually) as it moves away from the boundary between the optical path changing area 121 and the base area 122 inward of the optical path changing area 121.

 ベース領域122よりも屈折率が大きい光路変更領域121を形成するには、光路変更層120(ベース領域122)の材料として、加熱により屈折率が高くなる材料を用いる。このような材料の光路変更層120(ベース領域122)の一部分を、上記の第1の実施形態と同様の方法で加熱した後、冷却することにより、光路変更層120(ベース領域122)を構成する材料の結晶化が生じる。これにより、当該一部分の屈折率が、その周囲の部分(つまりベース領域122)の屈折率よりも高くなるとともに、例えば、当該一部分の屈折率がベース領域122から遠ざかるにつれて徐々に増大する。光路変更層120の材質としては、例えば、有機機能層140の材料として用いられるNPB(N,N-di(naphthalene-1-yl)-N,N-diphenyl-benzidene)を用いることができる。 In order to form the optical path changing region 121 having a refractive index larger than that of the base region 122, a material whose refractive index is increased by heating is used as the material of the optical path changing layer 120 (base region 122). The optical path changing layer 120 (base region 122) is configured by heating a part of the optical path changing layer 120 (base region 122) of such material in the same manner as in the first embodiment and then cooling. Crystallization of the material occurs. As a result, the refractive index of the portion becomes higher than the refractive index of the surrounding portion (that is, the base region 122), and gradually increases as the refractive index of the portion moves away from the base region 122, for example. As a material of the optical path changing layer 120, for example, NPB (N, N-di (naphthalene-1-yl) -N, N-diphenyl-benzidine) used as a material of the organic functional layer 140 can be used.

 図7は第4の実施形態に係る発光装置100の光路変更層120から透光性基板110にかけての屈折率の変化特性の例を示す図である。すなわち、図7は図1の線分Aの一端A1から他端A2にかけての屈折率の変化特性の他の例を示す。例えば、ベース領域122内においては、位置にかかわらず屈折率が一定である(図7の領域R1)。ベース領域122と光路変更領域121との境界(図7の領域R1と領域R2との境界)の屈折率は、ベース領域122の屈折率と同じである。光路変更領域121内においては、光路変更領域121とベース領域122との境界から遠ざかるにつれて、すなわち上記の球形(直径が発光層からの発光波長以上の球形)の中心に向かうにつれて、徐々に屈折率が増大している(図7の領域R2)。更に上記の球形の中心から透光性基板110側に向かうにつれて、再び屈折率が徐々に低減している(図7の領域R3)。すなわち、光路変更領域121の屈折率は、ベース領域122との境界においてはベース領域122の屈折率と同じであり、且つ、当該境界から遠ざかるにつれて徐々に増大している。なお、透光性基板110の屈折率は、光路変更層120の屈折率よりも小さい(図7の領域R4)。第4の実施形態の場合も、光が光路変更領域121内を通過する過程で、徐々に光の向きが変更される。 FIG. 7 is a diagram illustrating an example of a change characteristic of the refractive index from the optical path changing layer 120 to the translucent substrate 110 of the light emitting device 100 according to the fourth embodiment. That is, FIG. 7 shows another example of the change characteristic of the refractive index from one end A1 to the other end A2 of the line segment A in FIG. For example, in the base region 122, the refractive index is constant regardless of the position (region R1 in FIG. 7). The refractive index of the boundary between the base region 122 and the optical path changing region 121 (the boundary between the region R1 and the region R2 in FIG. 7) is the same as the refractive index of the base region 122. In the optical path changing region 121, the refractive index gradually increases as the distance from the boundary between the optical path changing region 121 and the base region 122 increases, that is, toward the center of the above-described spherical shape (a spherical shape whose diameter is equal to or larger than the emission wavelength from the light emitting layer). Has increased (region R2 in FIG. 7). Further, the refractive index gradually decreases again from the spherical center toward the translucent substrate 110 (region R3 in FIG. 7). That is, the refractive index of the optical path changing region 121 is the same as the refractive index of the base region 122 at the boundary with the base region 122, and gradually increases as the distance from the boundary increases. In addition, the refractive index of the translucent substrate 110 is smaller than the refractive index of the optical path changing layer 120 (region R4 in FIG. 7). Also in the case of the fourth embodiment, the direction of light is gradually changed in the process of light passing through the optical path changing region 121.

 なお、上記においては、第4の実施形態において、光路変更層120を透光性基板110と第1電極130との間に配置した例を説明した。ただし、結晶化し、且つ、ベース領域よりも屈折率が大きい光路変更領域を有する光路変更層を、有機機能層140と第2電極150との間に配置しても良い。すなわち、上記の第2の実施形態又は第3の実施形態の光路変更層160の光路変更領域161の屈折率を、ベース領域162の屈折率よりも大きくしても良い。この場合、光路変更層160の材質としては、例えば、有機機能層140の屈折率未満の屈折率を有し、且つ、加熱により屈折率が高くなる材質を用いる。 In the above description, in the fourth embodiment, the example in which the optical path changing layer 120 is disposed between the translucent substrate 110 and the first electrode 130 has been described. However, an optical path changing layer having an optical path changing region that is crystallized and has a refractive index larger than that of the base region may be disposed between the organic functional layer 140 and the second electrode 150. That is, the refractive index of the optical path changing region 161 of the optical path changing layer 160 of the second embodiment or the third embodiment may be larger than the refractive index of the base region 162. In this case, as the material of the optical path changing layer 160, for example, a material having a refractive index lower than the refractive index of the organic functional layer 140 and having a higher refractive index by heating is used.

 第2の実施形態(及び第3の実施形態)のように有機機能層140と第2電極150との間に光路変更層160を形成する場合、レーザにより部分的に加熱冷却することによって、第4の実施形態のように結晶化した光路変更領域161を形成することが好ましい。この場合実施例1に比べレーザの出力(パワー)を抑制できるので、光路変更領域161の形成の際の有機機能層140へのダメージを抑制することができる。より大きな出力で材料にレーザを照射する時は、レーザが透過できる程度の膜厚の電極150を形成した後、レーザで部分的に光路変更層160を加熱冷却し結晶化したあと、電極150により光を反射できる程度の膜厚となるまで電極150の膜厚を厚くする。 When the optical path changing layer 160 is formed between the organic functional layer 140 and the second electrode 150 as in the second embodiment (and the third embodiment), by partially heating and cooling with a laser, It is preferable to form the crystallized optical path changing region 161 as in the fourth embodiment. In this case, since the output (power) of the laser can be suppressed compared to Example 1, damage to the organic functional layer 140 when the optical path changing region 161 is formed can be suppressed. When irradiating a material with a laser with a larger output, after forming an electrode 150 having a film thickness that allows laser transmission, the optical path changing layer 160 is partially heated and cooled by the laser to be crystallized, and then the electrode 150 The film thickness of the electrode 150 is increased until the film thickness is such that light can be reflected.

 図8は第4の実施形態に係る発光装置の動作の例を示す要部断面図であり、有機機能層140、光路変更層160及び第2電極150のみを図示している。ここでは、図7で説明したような屈折率特性の光路変更領域121と同様の光路変更領域161を有する光路変更層160が有機機能層140と第2電極150との間に配置されている場合について説明する。 FIG. 8 is a cross-sectional view of an essential part showing an example of the operation of the light emitting device according to the fourth embodiment, and only the organic functional layer 140, the optical path changing layer 160, and the second electrode 150 are illustrated. Here, when the optical path changing layer 160 having the optical path changing area 161 similar to the optical path changing area 121 having the refractive index characteristic as described in FIG. 7 is disposed between the organic functional layer 140 and the second electrode 150. Will be described.

 光路変更層160に光路変更領域161が存在しない場合には、図8に示す光路L11、L12の順に進む光があるとする。すなわち、この光は、光路変更層160内を斜め下向きに進み(光路L11)、その後、第2電極150にて反射して、斜め上向きに進む(光路L12)ものとする。更に、この光は、その後、光路変更層120と透光性基板110との界面(光路変更層120が存在する場合)、又は、第1電極130と透光性基板110との界面(光路変更層120が存在しない場合)にて反射して、斜め下向きに進むものとする。 If there is no optical path changing region 161 in the optical path changing layer 160, it is assumed that there is light traveling in the order of the optical paths L11 and L12 shown in FIG. That is, the light travels obliquely downward in the optical path changing layer 160 (optical path L11), and then reflects on the second electrode 150 and travels obliquely upward (optical path L12). Further, this light is then transmitted to the interface between the optical path changing layer 120 and the translucent substrate 110 (when the optical path changing layer 120 exists) or to the interface between the first electrode 130 and the translucent substrate 110 (optical path changing). Suppose the layer 120 is not present) and proceed diagonally downward.

 本実施形態の場合、光路変更層160に光路変更領域161が存在することにより、この光の光路は、光路L1で示されるように、光路変更領域161内を通過する過程で、徐々に下向きに変更される。この光は、その後、第2電極150にて反射し、光路L2で示されるように進む。ここで、光路L2は、光路変更層120と透光性基板110との界面(光路変更層120が存在する場合)、又は、第1電極130と透光性基板110との界面(光路変更層120が存在しない場合)における臨界角未満となっているものとする。よって、この光を、光路変更層120又は第1電極130から透光性基板110側へ入射させることができ、更にこの光を透光性基板110から更にその上側(つまり発光装置の外部)へ放射させることができる。 In the case of the present embodiment, since the optical path changing region 161 exists in the optical path changing layer 160, the optical path of this light gradually goes downward in the process of passing through the optical path changing region 161 as shown by the optical path L1. Be changed. This light is then reflected by the second electrode 150 and travels as indicated by the optical path L2. Here, the optical path L2 is an interface between the optical path changing layer 120 and the translucent substrate 110 (when the optical path changing layer 120 is present) or an interface between the first electrode 130 and the translucent substrate 110 (optical path changing layer). It is assumed that the angle is less than the critical angle (when 120 does not exist). Therefore, this light can be incident on the light transmitting substrate 110 side from the optical path changing layer 120 or the first electrode 130, and further this light is further transmitted from the light transmitting substrate 110 to the upper side (that is, outside the light emitting device). Can be radiated.

 このように、第4の実施形態によっても、第1の実施形態と同様の効果が得られる。 Thus, according to the fourth embodiment, the same effect as that of the first embodiment can be obtained.

 (実施例1)
 実施例1では、第1の実施形態に係る発光装置100のより具体的な構成の例を説明する。図9(a)は実施例1に係る発光装置の構成を示す平面図であり、図9(b)は図9(a)におけるB-B線に沿った断面図である。なお、図9(b)及び図9(a)においては、図1とは上下が反転している。
(Example 1)
In Example 1, an example of a more specific configuration of the light emitting device 100 according to the first embodiment will be described. FIG. 9A is a plan view showing the configuration of the light emitting device according to Example 1, and FIG. 9B is a cross-sectional view taken along the line BB in FIG. 9A. 9B and 9A are upside down from FIG.

 第1電極130は、陽極を構成する。複数の第1電極130が、それぞれ帯状にY方向に延在している。隣り合う第1電極130同士は、Y方向に対して直交するX方向において一定間隔ずつ離間している。第1電極130の各々は、例えばITOやIZO等の金属酸化物導電体等からなる。第1電極130の屈折率は光路変更層120と同程度(例えば屈折率1.8程度)とされる。第1電極130の各々の表面には、第1電極130に電源電圧を供給するためのバスライン170が形成されている。光路変更層120及び第1電極130上には絶縁膜180が形成されている。絶縁膜180には、それぞれY方向に延在するストライプ状の開口部が複数形成されている。これにより、絶縁膜180からなる複数のバンク(隔壁)が形成されている。絶縁膜180に形成された開口部の各々は、第1電極130に達しており、開口部の底部において各第1電極130の表面が露出している。絶縁膜180の各開口部内において、第1電極130上には、有機機能層140が形成されている。有機機能層140は、正孔注入層141、正孔輸送層142、発光層143(発光層143R、143G、143B)、電子輸送層144がこの順序で積層されることにより構成されている。正孔注入層141及び正孔輸送層142の材料としては、芳香族アミン誘導体、フタロシアニン誘導体、ポルフィリン誘導体、オリゴチオフェン誘導体、ポリチオフェン誘導体、ベンジルフェニル誘導体、フルオレン基で3級アミンを連結した化合物、ヒドラゾン誘導体、シラザン誘導体、シラナミン誘導体、ホスファミン誘導体、キナクリドン誘導体、ポリアニリン誘導体、ポリピロール誘導体、ポリフェニレンビニレン誘導体、ポリチエニレンビニレン誘導体、ポリキノリン誘導体、ポリキノキサリン誘導体、カーボン等が挙げられる。発光層143R、143G、143Bは、それぞれ、赤色発光、緑色発光、青色発光を行う蛍光性有機金属化合物等からなる。発光層143R、143G、143Bは、絶縁膜180からなるバンクによって互いに隔てられた状態で並んで配置されている。すなわち、有機機能層140は、バンクによって隔てられた複数の発光領域を形成している。発光層143R、143G、143Bおよび絶縁膜180の表面を覆うように電子輸送層144が形成されている。電子輸送層144の表面を覆うように第2電極150が形成されている。第2電極150は、陰極を構成する。第2電極150は、帯状に形成されている。第2電極150は、仕事関数が低く且つ高反射率を有するAlなどの金属または合金等からなる。尚、有機機能層140の屈折率は、第1電極130および光路変更層120と同程度(例えば屈折率1.8程度)とされる。 The first electrode 130 constitutes an anode. The plurality of first electrodes 130 each extend in the Y direction in a strip shape. Adjacent first electrodes 130 are spaced apart from each other at a constant interval in the X direction orthogonal to the Y direction. Each of the first electrodes 130 is made of a metal oxide conductor such as ITO or IZO, for example. The refractive index of the first electrode 130 is approximately the same as that of the optical path changing layer 120 (for example, approximately 1.8). A bus line 170 for supplying a power supply voltage to the first electrode 130 is formed on each surface of the first electrode 130. An insulating film 180 is formed on the optical path changing layer 120 and the first electrode 130. In the insulating film 180, a plurality of stripe-shaped openings each extending in the Y direction are formed. Thus, a plurality of banks (partition walls) made of the insulating film 180 are formed. Each of the openings formed in the insulating film 180 reaches the first electrode 130, and the surface of each first electrode 130 is exposed at the bottom of the opening. An organic functional layer 140 is formed on the first electrode 130 in each opening of the insulating film 180. The organic functional layer 140 is configured by stacking a hole injection layer 141, a hole transport layer 142, a light emitting layer 143 (light emitting layers 143R, 143G, 143B), and an electron transport layer 144 in this order. Materials for the hole injection layer 141 and the hole transport layer 142 include aromatic amine derivatives, phthalocyanine derivatives, porphyrin derivatives, oligothiophene derivatives, polythiophene derivatives, benzylphenyl derivatives, compounds in which tertiary amines are linked by fluorene groups, hydrazones. Derivatives, silazane derivatives, silanamine derivatives, phosphamine derivatives, quinacridone derivatives, polyaniline derivatives, polypyrrole derivatives, polyphenylene vinylene derivatives, polythienylene vinylene derivatives, polyquinoline derivatives, polyquinoxaline derivatives, carbon and the like. The light emitting layers 143R, 143G, and 143B are made of a fluorescent organometallic compound that emits red light, green light, and blue light, respectively. The light emitting layers 143R, 143G, and 143B are arranged side by side in a state of being separated from each other by a bank made of the insulating film 180. That is, the organic functional layer 140 forms a plurality of light emitting regions separated by banks. An electron transport layer 144 is formed so as to cover the surfaces of the light emitting layers 143R, 143G, 143B and the insulating film 180. A second electrode 150 is formed so as to cover the surface of the electron transport layer 144. The second electrode 150 constitutes a cathode. The second electrode 150 is formed in a band shape. The second electrode 150 is made of a metal such as Al or an alloy having a low work function and high reflectivity. The refractive index of the organic functional layer 140 is approximately the same as that of the first electrode 130 and the optical path changing layer 120 (for example, a refractive index of approximately 1.8).

 このように、赤、緑、青の光をそれぞれ発する発光層143R、143G、143Bは、ストライプ状に繰り返し配置されており、光取り出し面となる透光性基板110の表面からは、赤、緑、青の光が任意の割合で混色されて単一の発光色(例えば白色)として認識される光が放出される。 In this manner, the light emitting layers 143R, 143G, and 143B that emit red, green, and blue light are repeatedly arranged in stripes, and the red, green, and green light is emitted from the surface of the translucent substrate 110 that serves as a light extraction surface. , Blue light is mixed at an arbitrary ratio to emit light that is recognized as a single emission color (for example, white).

 (有機機能層の変形例1)
 図10は、有機機能層140の層構造の変形例1を示す図である。変形例1に係る有機機能層140は、正孔注入層141、正孔輸送層142、発光層143、電子輸送層144、及び電子注入層145をこの順に積層した構造を有している。すなわち有機機能層140は、有機エレクトロルミネッセンス発光層である。なお、正孔注入層141及び正孔輸送層142の代わりに、これら2つの層の機能を有する一つの層を設けてもよい。同様に、電子輸送層144及び電子注入層145の代わりに、これら2つの層の機能を有する一つの層を設けてもよい(実施例1(図9(b))参照)。
(Modification 1 of organic functional layer)
FIG. 10 is a diagram illustrating a first modification of the layer structure of the organic functional layer 140. The organic functional layer 140 according to Modification 1 has a structure in which a hole injection layer 141, a hole transport layer 142, a light emitting layer 143, an electron transport layer 144, and an electron injection layer 145 are stacked in this order. That is, the organic functional layer 140 is an organic electroluminescence light emitting layer. Note that instead of the hole injection layer 141 and the hole transport layer 142, one layer having the functions of these two layers may be provided. Similarly, instead of the electron transport layer 144 and the electron injection layer 145, a single layer having the functions of these two layers may be provided (see Example 1 (FIG. 9B)).

 有機機能層の変形例1において、発光層143は、例えば赤色の光を発光する層、青色の光を発光する層、黄色の光を発光する層、又は緑色の光を発光する層である。この場合、平面視において、赤色の光を発光する発光層143を有する領域、緑色の光を発光する発光層143を有する領域、及び青色の光を発光する発光層143を有する領域が繰り返し設けられていても良い(実施例1(図9(b))参照)。この場合、各領域を同時に発光させると、発光装置100は白色等の単一の発光色で発光する。 In the first modification of the organic functional layer, the light emitting layer 143 is, for example, a layer that emits red light, a layer that emits blue light, a layer that emits yellow light, or a layer that emits green light. In this case, in a plan view, a region having a light emitting layer 143 that emits red light, a region having a light emitting layer 143 that emits green light, and a region having a light emitting layer 143 that emits blue light are repeatedly provided. (See Example 1 (FIG. 9B)). In this case, when each region emits light simultaneously, the light emitting device 100 emits light in a single light emission color such as white.

 なお、発光層143は、複数の色を発光するための材料を混ぜることにより、白色等の単一の発光色で発光するように構成されていても良い。 Note that the light emitting layer 143 may be configured to emit light in a single light emission color such as white by mixing materials for emitting a plurality of colors.

 (有機機能層の変形例2)
 図11は、有機機能層140の層構造の変形例2を示す図である。変形例2に係る有機機能層140の発光層143は、発光層143a,143b,143cをこの順に積層した構成を有している。発光層143a,143b,143cは、互いに異なる色の光(例えば赤、緑、及び青)を発光する。そして発光層143a,143b,143cが同時に発光することにより、発光装置100は白色等の単一の発光色で発光する。
(Variation 2 of the organic functional layer)
FIG. 11 is a diagram illustrating a second modification of the layer structure of the organic functional layer 140. The light emitting layer 143 of the organic functional layer 140 according to Modification 2 has a configuration in which light emitting layers 143a, 143b, and 143c are stacked in this order. The light emitting layers 143a, 143b, and 143c emit light of different colors (for example, red, green, and blue). The light emitting layers 143a, 143b, and 143c emit light at the same time, so that the light emitting device 100 emits light in a single light emission color such as white.

 以上、図面を参照して実施形態及び実施例について述べたが、これらは本発明の例示であり、上記以外の様々な構成を採用することもできる。 As mentioned above, although embodiment and the Example were described with reference to drawings, these are the illustrations of this invention, Various structures other than the above are also employable.

 例えば、上記においては、光路変更領域(121、161)の形状として、直径が前記発光層からの発光波長以上の球形の少なくとも一部分である例、特に、光路変更領域の外形が第2電極150側に向けて凸の曲面を含む例を説明した。ただし、光路変更領域(121、161)は、その他の形状に形成されていても良い。 For example, in the above example, the shape of the optical path changing region (121, 161) is an example in which the diameter is at least a part of a sphere having a wavelength equal to or greater than the emission wavelength from the light emitting layer, in particular, the outer shape of the optical path changing region is the second electrode 150 side. An example including a convex curved surface has been described. However, the optical path changing region (121, 161) may be formed in other shapes.

 また、光路変更領域(121、161)を形成するための光の照射は、スポット的な照射に限らず、断続的に照射することにより、グレーティング(回折格子)のような構造の光路変更領域(121、161)を形成しても良い。 In addition, the light irradiation for forming the optical path changing region (121, 161) is not limited to spot irradiation, but by intermittently irradiating, an optical path changing region having a structure like a grating (diffraction grating) ( 121, 161) may be formed.

 また、光路変更領域(121、161)として、光路変更領域121とベース領域122との境界から光路変更領域121の内向きに遠ざかるにつれて、光路変更領域121とベース領域122との屈折率差が大きくなるものを例示したが、光路変更領域(121、161)は、ベース領域(122、162)に形成された気泡であっても良い。 Further, as the optical path changing area (121, 161), the refractive index difference between the optical path changing area 121 and the base area 122 increases as the distance from the boundary between the optical path changing area 121 and the base area 122 increases inward. However, the optical path changing region (121, 161) may be a bubble formed in the base region (122, 162).

 また、光路変更領域121の屈折率が、光路変更領域121とベース領域122との境界においては、ベース領域122の屈折率と同じである例を説明したが、これらの境界において、屈折率が不連続に変化していても良い。例えば、より強力なエネルギーでレーザ光をベース領域122に照射した場合などに、光路変更領域121とベース領域122との境界に屈折率の不連続面が形成される場合がある。 Further, the example in which the refractive index of the optical path changing region 121 is the same as the refractive index of the base region 122 at the boundary between the optical path changing region 121 and the base region 122 has been described. It may change continuously. For example, when the base region 122 is irradiated with laser light with stronger energy, a discontinuous surface with a refractive index may be formed at the boundary between the optical path changing region 121 and the base region 122.

Claims (12)

 透光性基板と、
 前記透光性基板の一方の面側に配置された透光性の第1電極と、
 前記第1電極を基準として前記透光性基板とは反対側に配置された第2電極と、
 少なくとも発光層を含んでおり、前記第1電極と前記第2電極との間に配置されている有機機能層と、
 光を透過させる過程で当該光の光路を変更する光路変更領域と、前記光路変更領域以外のベース領域と、を含んでおり、前記透光性基板と前記第2電極との間に配置されている光路変更層と、
 を備え、
 前記光路変更領域と前記ベース領域との屈折率差は、前記光路変更領域と前記ベース領域との境界から前記光路変更領域の内向きに遠ざかるにつれて大きくなっている発光装置。
A translucent substrate;
A translucent first electrode disposed on one surface side of the translucent substrate;
A second electrode disposed on the opposite side of the translucent substrate with respect to the first electrode;
An organic functional layer including at least a light-emitting layer and disposed between the first electrode and the second electrode;
An optical path changing region that changes an optical path of the light in the process of transmitting light; and a base region other than the optical path changing region, and is disposed between the translucent substrate and the second electrode. An optical path changing layer,
With
The light emitting device, wherein a difference in refractive index between the optical path changing region and the base region increases as the distance from the boundary between the optical path changing region and the base region increases inward of the optical path changing region.
 前記光路変更領域の屈折率は、前記境界においては前記ベース領域の屈折率と同じである請求項1に記載の発光装置。 The light emitting device according to claim 1, wherein a refractive index of the optical path changing region is the same as a refractive index of the base region at the boundary.  前記屈折率差は、前記境界から前記光路変更領域の内向きに遠ざかるにつれて徐々に大きくなっている請求項1又は2に記載の発光装置 3. The light emitting device according to claim 1, wherein the refractive index difference gradually increases as the distance from the boundary increases inward of the optical path changing region.  前記光路変更領域の寸法は、前記発光層からの発光波長以上である請求項1又は2に記載の発光装置。 The light emitting device according to claim 1 or 2, wherein the dimension of the optical path changing region is equal to or greater than a light emission wavelength from the light emitting layer.  前記光路変更領域の形状は、直径が前記発光層からの発光波長以上の球形の少なくとも一部分である請求項4に記載の発光装置。 The light-emitting device according to claim 4, wherein the shape of the optical path changing region is at least a part of a sphere having a diameter equal to or greater than the emission wavelength from the light-emitting layer.  前記光路変更領域の外形は、前記第2電極側に向けて凸の曲面を含む請求項1又は2に記載の発光装置。 The light emitting device according to claim 1 or 2, wherein an outer shape of the optical path changing region includes a curved surface that is convex toward the second electrode side.  前記光路変更領域は、前記ベース領域よりも屈折率が小さい領域を含む請求項1又は2に記載の発光装置。 3. The light emitting device according to claim 1, wherein the optical path changing region includes a region having a refractive index smaller than that of the base region.  前記光路変更領域は、結晶化しており、
 前記光路変更領域は、前記ベース領域よりも屈折率が大きい領域を含む請求項1又は2に記載の発光装置。
The optical path changing region is crystallized,
The light emitting device according to claim 1, wherein the optical path changing region includes a region having a refractive index larger than that of the base region.
 前記光路変更層は、前記透光性基板と前記第1電極との間に配置され、
 前記光路変更層の屈折率は、前記透光性基板の屈折率以上で、且つ、2.0以下である請求項7に記載の発光装置。
The optical path changing layer is disposed between the translucent substrate and the first electrode,
The light emitting device according to claim 7, wherein a refractive index of the optical path changing layer is not less than a refractive index of the translucent substrate and not more than 2.0.
 前記光路変更層は、前記有機機能層と前記第2電極との間に配置され、
 前記光路変更層の屈折率は、1.0以上で、且つ、前記有機機能層の屈折率以下である請求項7に記載の発光装置。
The optical path changing layer is disposed between the organic functional layer and the second electrode,
The light-emitting device according to claim 7, wherein a refractive index of the optical path changing layer is 1.0 or more and not more than a refractive index of the organic functional layer.
 前記光路変更領域は、前記ベース領域の一部分を加熱することにより形成されている請求項1又は2の何れか一項に記載の発光装置。 3. The light emitting device according to claim 1, wherein the optical path changing region is formed by heating a part of the base region.  透光性基板の一方の面側に、透光性の第1電極を形成する工程と、
 前記第1電極を基準として前記透光性基板とは反対側に、少なくとも発光層を含んで構成される有機機能層を形成する工程と、
 前記有機機能層を基準として前記第1電極とは反対側に、第2電極を形成する工程と、
 光を透過させる過程で当該光の光路を変更する光路変更領域と、前記光路変更領域以外のベース領域と、を含んで構成される光路変更層を、前記透光性基板と前記第2電極との間に形成する工程と、
 を備え、
 前記光路変更層を形成する工程では、前記光路変更領域と前記ベース領域との屈折率差が、前記光路変更領域と前記ベース領域との境界から前記光路変更領域の内向きに遠ざかるにつれて大きくなるように、前記光路変更層を形成する発光装置の製造方法。
Forming a translucent first electrode on one surface side of the translucent substrate;
Forming an organic functional layer including at least a light emitting layer on a side opposite to the light-transmitting substrate with respect to the first electrode;
Forming a second electrode on the side opposite to the first electrode with respect to the organic functional layer;
An optical path changing layer including an optical path changing area for changing an optical path of the light in the process of transmitting light, and a base area other than the optical path changing area, the light-transmitting substrate, the second electrode, Forming between, and
With
In the step of forming the optical path changing layer, a difference in refractive index between the optical path changing area and the base area increases as the distance from the boundary between the optical path changing area and the base area increases inward of the optical path changing area. And a method of manufacturing a light emitting device for forming the optical path changing layer.
PCT/JP2012/080437 2012-11-26 2012-11-26 Light emitting device and method for producing light emitting device Ceased WO2014080512A1 (en)

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JP2003160731A (en) * 2001-11-26 2003-06-06 Nitto Denko Corp Plastic material for laser processing and plastic optical element processed with the material
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