Phosphor layer for micro-LED applications

Abstract

Embodiments include a device having a micro-LED that includes at least two, individually addressable light emitting diodes on a same substrate; a phosphor converter layer disposed on the micro-LED, the phosphor converter layer including phosphor particles having a D50 of greater than 1 μm and less than 10 μm.

Claims

1. A device comprising: a micro-LED comprising at least two individually addressable light emitting diodes on a same substrate; and a phosphor converter layer disposed on the micro-LED and extending over the at least two light emitting diodes and across a gap therebetween, the phosphor converter layer comprising a plurality of phosphor particles having an average particle size or median diameter (D50) of greater than 1 μm and less than 10 μm, wherein a thickness of the phosphor converter layer is greater than 4 μm and less than 20 μm, wherein the phosphor converter layer further comprises a thin layer of non-luminescent material coating on the phosphor particles, and wherein the thin layer has a thickness of less than 200 nm, the at least two light emitting diodes exhibiting a contrast ratio greater than 1:18, said contrast ratio resulting at least in part from the D50 of the phosphor particles and the thickness of the phosphor converter layer.

2. The device of claim 1, wherein the plurality of phosphor particles has a D50 of greater than 2 μm and less than 7 μm.

3. The device of claim 2, wherein the plurality of phosphor particles has a D50 of greater than 3 μm and less than 5 μm.

4. The device of claim 1, wherein the thickness of the phosphor converter layer is greater than 8 μm and less than 15 μm.

5. The device of claim 1, wherein the thickness of the phosphor converter layer is greater than 10 μm and less than 13 μm.

6. The device of claim 1, wherein the phosphor converter layer further comprises a matrix, and the matrix has a refractive index of 1 or greater and less than or equal to 1.5.

7. The device of claim 6, wherein the matrix has a refractive index of 1 or greater and less than 1.4.

8. The device of claim 7, wherein the matrix has a refractive index of 1 or greater and less than 1.2.

9. The device of claim 1, wherein the thin layer comprises a metal oxide.

10. The device of claim 9, wherein the thin layer comprises at least one of Al.sub.2O.sub.3, HfO.sub.2, Ta.sub.2O.sub.5, ZrO.sub.2, TiO.sub.2, and SiO.sub.2.

11. The device of claim 1, wherein the thin layer has a thickness between 40-150 nm.

12. The device of claim 1, the contrast ratio being greater than 1:100.

13. A method for making the device of claim 1, the method comprising: depositing the plurality of phosphor particles in a layer that extends over the at least two light emitting diodes on the substrate and across the gap between the at least two light emitting diodes; and forming the thin layer of non-luminescent material so as to coat the phosphor particles.

14. The method of claim 13, wherein the phosphor converter layer is deposited by spray coating or sedimentation.

15. The method of claim 13, wherein the thin layer is formed by atomic layer deposition.

16. The method of claim 13, wherein the thin layer comprises a metal oxide.

17. The method of claim 16, wherein the thin layer comprises at least one of Al.sub.2O.sub.3, HfO.sub.2, Ta.sub.2O.sub.5, ZrO.sub.2, TiO.sub.2, and SiO.sub.2.

18. The method of claim 13, wherein the plurality of phosphor particles has a D50 of greater than 2 μm and less than 7 μm.

19. The method of claim 13, wherein the thickness of the phosphor converter layer is greater than 8 μm and less than 15 μm.

20. The method of claim 13, wherein the phosphor converter layer further comprises a matrix, and the matrix has a refractive index of 1 or greater and less than or equal to 1.5.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) FIG. 1a illustrates a plan view of a portion of one type of micro-LED device.

(2) FIG. 1b illustrates a side view of a portion of one type of micro-LED device through line AA of FIG. 1a.

(3) FIG. 2 shows a measured particle size distribution of a garnet phosphor powder.

(4) FIG. 3a shows optical resolution of a simulated micro-LED with a single line of pixels in the on state and neighboring pixels in the off state.

(5) FIG. 3b shows color over source variation of a simulated micro-LED with a single line of pixels in the on state and neighboring pixels in the off state.

(6) FIG. 3c shows a radiation pattern of a simulated micro-LED with a single line of pixels in the on state and neighboring pixels in the off state.

(7) FIG. 4a, FIG. 4b and FIG. 4c show the results for the simulation when everything was held the same as in FIGS. 3a, 3b, and 3c, except that the refractive index of the matrix material was set to equal 1.

(8) FIG. 5a and FIG. 5b show a simulation data for the same micro-LED as in FIGS. 3a-3c, and 4a-4c, except the simulation was performed for six different particle size values and six different phosphor converter layer thicknesses.

(9) FIG. 6a and FIG. 6b illustrate a method of forming a high optical contrast phosphor converter.

(10) FIG. 7a, FIG. 7b and FIG. 7c show the results for the simulation when everything was held the same as in FIGS. 4a, 4b, and 4c, except that the thickness of the phosphor converter layer and the particle size are reduced.

(11) FIG. 8 show the relative flux as a function of Al.sub.2O.sub.3 layer thickness in a phosphor converter.

(12) FIG. 9 is a diagram of the experimental setup for the optical contrast measurement of the example phosphor converter.

(13) FIG. 10 is an image of the line of blue light through the example phosphor converter layer.

(14) FIG. 11 shows the measured line profile, perpendicular to the open line in the Al layer on the example phosphor converter layer.

(15) FIG. 12 shows an SEM (scanning electron microscope) image of the interface of a cross-section of a phosphor converter layer on a substrate with the thin layer of Al.sub.2O.sub.3 coating the phosphor material particles.

DETAILED DESCRIPTION

(16) Micro-LEDs, also referred to as μLEDs, are arrays of a large number of individually addressable LED devices on one chip. Micro-LED arrays have application in lighting, for instance automotive lighting, and displays. As the individual LEDs, or pixels, are individually addressable, light patterns can be displayed on the micro-LED.

(17) FIG. 1a illustrates a plan view of a portion of one type of micro-LED device. In FIG. 1a, each square 110 represents a single LED device, or pixel, of which there may be in the range of 20000 per micro-LED. FIG. 1a shows only a portion of such a micro-LED for illustration purposes. Between each individual LED there is a gap 105, which may be, for example, a metal wall (e.g., Cu), that coats each side of an LED die 110. Dimensions for an individual pixel may be, for example, 40×40 μm.sup.2 and dimensions for gap 105 may be, for example 8 μm.

(18) One method for forming a micro-LED is to use epitaxial growth to form the multiple individual LEDs 110 on a die in a flip-chip construction as is known in the art. FIG. 1b illustrates a side view of a portion of one type of micro-LED device taken through line AA of FIG. 1a. FIG. 1b shows LED dies 110.

(19) A phosphor converter 163 is on LED dies 110. The phosphor converter 163 may be formed of phosphor particles contained in a matrix, for example, garnet particles contained in silicone. Alternatively, or in addition, the phosphor converter 163 contains a densely sintered phosphor ceramic, such as Lumiramic™. In one example, the individual LEDs produce a blue light and the phosphor converter converts the blue light to a white light to produce a micro-LED that is monochrome white at a CCT of about 5700K.

(20) The phosphor converter 163 can be defined by three parameters: (a) its thickness, (b) the refractive index of the matrix, and (c) the particle size and the refractive index of the phosphor material. The thickness, or width, of phosphor converter 163 is represented by W in FIG. 1b. The refractive index of the matrix is determined by the material chosen for the matrix, which is often silicone, with a refractive index of 1.5. The phosphor materials in the phosphor converter 163 have a particle size given by D50. Here, D represents the diameter of powder particles, and D50 means a cumulative 50% point of volume (or 50% pass particle size) and may be referred to as an average particle size or median diameter. D50 values for particles may be provided by the supplier of the powder particle material or may be measured. For example, FIG. 2 shows a measured particle size distribution of a garnet phosphor powder analyzed using a PA-950 laser particle size analyzer from Horiba Company, with a measuring range of 0.01 μm to 3000 μm. The measurement principle is based on the measurement of the pattern of scattered light in a wide angular range. This distribution of scattered light is used to calculate the particle size distribution using Mie's theory, as is understood by a person of ordinary skill in the art. In the data shown in FIG. 4, D(v, 0.1)=3.10017 (μm), D(v,0.5), which is D50, =5.26114 (μm), and D(v,0.9)=8.17130 (μm), where D(v, x.x) defines the particle sizes for the cumulative particle volumes of 10%, 50% and 90% of the distribution.

(21) A problem encountered with micro-LEDs is that there can be very low optical contrast between neighboring pixels when one pixel is on and a neighboring pixel is off. Thus, for instance, if the pixels in row 120 of FIG. 1a are in the on state, and pixels in rows 130 and 140 are in the off state, light emitted from the pixels in row 120 extends across the adjacent trench and over the pixels and trench areas on each side of the row 120, so that rows 130 and 140 (and the equivalent rows on the opposite side of row 120) do not appear dark, or off. This problem is illustrated in FIGS. 3a, 3b, and 3c, which show a simulation for a single line of pixels (row 120 in FIG. 1a) in the on state and neighboring pixels (rows 130 and 140 of FIG. 1a) in the off state. In FIGS. 3a-3c, the x-coordinate is perpendicular to the lines of pixels. The simulation was performed by using a Monte-Carlo ray-tracing algorithm. Blue LED photons are partially absorbed in a scattering phosphor layer. Probabilities for scattering and absorption are derived from single particle Mie coefficients.

(22) FIG. 3a shows the optical resolution of the micro-LED. In FIG. 3a, pixels in rows 120, 130 and 140 are represented by 320, 330 and 340 along the x-coordinate, respectively. For the simulation, each pixel was given a width of 35 μm, and each pixels were separated by 5 μm. The phosphor converter layer, i.e. 163 in FIG. 1b, was given a width (represented by W in FIG. 1b) of 30 μm. Phosphor converter layer 163 was assumed to have phosphor pixels with a size D50 of 13 μm in a matrix with a refractive index of 1.5. Pixel row 320 is in the on state and pixels rows 330 and 340 in the off state. Plot 384 represents the emitted green/yellow light and plot 386 represents the emitted blue light. Plots 384 and 386 show that the light emitted by pixel row 320 extends over the adjacent pixels and the optical resolution is poor. In particular, the optical contrast ratio, which is the integrated flux over the second off-line (340) to the on-line (320), is 1:3.

(23) FIG. 3b shows the color over source variation as the v′ color coordinate value along the x-coordinate, and FIG. 3c shows the radiation pattern indicating the amount (flux) of emitted radiation as a function of the polar angle towards the direction of normal emission, for the simulated micro-LED with the single line of pixels in the on state and neighboring pixels in the off state. FIG. 3b shows the calculated emission from the phosphor (384) compared to a cosine distribution (350).

(24) To increase the contrast between on state pixels and off state pixels, and hence improve the optical resolution, parameters that define the phosphor converter 163 were modified.

(25) Lowering the refractive index of the matrix for the phosphor converter 163 increases scattering and thus the optical contrast. FIGS. 4a, 4b, and 4c shows the results for the simulation when everything was held the same as in FIGS. 3a, 3b, and 3c, except that the refractive index of the matrix material was set to equal 1, i.e., the refractive index of air. As can be seen in FIGS. 4a, 4b, and 4c, the optical resolution, color over source variation, and radiation pattern all improve with the removal of the matrix, i.e., setting the refractive index value to =1. Viewing for example, FIG. 4a, the emitted green/yellow light plot 484 and the emitted blue light plot 486 both narrow closer to line 320 as compared to the corresponding plots 384 and 385 in FIG. 3a. Viewing, for example, FIG. 4b, the color over source variation 442 is improved as compared to the corresponding 342 in FIG. 3b, and likewise, in FIG. 4c, the radiation pattern 450 is improved (line 448 is the cosine function). The optical contrast ratio increases to 1:18 from 1:3 for when the refractive index=1 vs. 1.5. Thus, to improve the optical contrast, the refractive index of the matrix may be less than 1.5, in particular the refractive index of the matrix may be less than 1.4, and in particular the refractive index of the matrix may be less than 1.2.

(26) Reducing the particle size of the phosphor material in the phosphor converter 163 and reducing the thickness W of the phosphor converter 163 also increases the optical contrast. FIGS. 5a and 5b show simulation data for the same micro-LED as in FIGS. 3a-3c, and 4a-4c, except the simulation was performed for six different phosphor material particle D50 size values, and five different phosphor converter layer thicknesses W. The simulations were performed with the refractive index set to 1 (FIG. 5a) and set to 1.5 (FIG. 5b). In FIGS. 5a and 5b, the six different particle size D50 values are 3.8 μm, 5 μm, 7 μm, 9 μm, 11 μm, and 13 μm (as indicated by the blue, red, green, purple, light blue and orange lines, respectively). The dashed line indicates an optical contrast ratio of 1:300. The five different phosphor converter layer thicknesses W are 10 μm, 14 μm, 20 μm, 27 μm, and 37 μm. The diagrams in FIGS. 5a and 5b both show that the smaller the particle size in the phosphor converter, and the thinner the phosphor converter layer, the better the optical contrast, especially when the refractive index is =1. Thus, to improve optical contrast the particle size D50 may be between 1 μm and 10 μm, in particular the particle size D50 may be between 2 μm and 7 μm, and in particular the particle size may be between 3 μm and 5 μm. Further, to improve optical contrast the thickness W may be between 4 μm and 20 μm, in particular between 8 μm and 15 μm, and in particular between 10 μm and 13 μm.

(27) Thus a phosphor converter with a high optical contrast (above 300) can only be realized with phosphor particles size D50 of less than 5 μm and a thickness W well below 15 μm when the refractive index is=1. An optical contrast ratio of better than 1:100 can be achieved with refractive index of=1 when the particle size is less than 9 μm and the thickness is less than 15 μm. In practice, D50 of phosphor material particles is limited to 1-3 μm, with the quantum efficiency decreasing with decreasing particles size of the phosphor. Also, the overall layer thickness is limited by the maximum tolerable activator concentration of the phosphor materials (increases may also result in quantum efficiency decreases). With a phosphor converter layer matrix material (like silicone) the parameter space for a high contrast layer is extremely limited. On the other hand, the matrix material within the phosphor converter has two functions. First, to provide mechanical stability to the phosphor converter layer, and secondly, to enhance the blue light extraction from the underlying LED die.

(28) FIG. 6a-6b illustrates a method of forming such a high optical contrast phosphor converter. In FIG. 6a, phosphor material particles 630 are deposited on a substrate 610, which substrate 610 may be, for example, a micro-LED EPI surface. The phosphor material particles 630 may be applied using any suitable method, such as, for example, spray-coating, sedimentation, or the like, which deposits the phosphor material particles 630 in a thin layer, which may be less than 15 μm thick. The phosphor material particles may have a size of D50 less than 5 μm.

(29) Next, as shown in FIG. 6b, the phosphor particles 630 are coated with a thin layer 660 of a non-luminescent material, such as a metal oxide, for example, Al.sub.2O.sub.3. Thin layer 660 is indicated in FIG. 6b schematically by a thickening of the lines defining the phosphor particles, compared to FIG. 6a. The thin layer 660 of non-luminescent material may be applied using atomic layer deposition, as will be described in more detail below. Atomic layer deposition allows the non-luminescent material to flow into areas between each of the phosphor particles 630 on substrate 610, so that the non-luminescent material forms a coating on and around each particle to form the thin layer 660 of non-luminescent material. Materials for use in the thin layer 660 include, for example, Al.sub.2O.sub.3, HfO.sub.2, Ta.sub.2O.sub.5, ZrO.sub.2, TiO.sub.2, and SiO.sub.2. The thin layer 660 of non-luminescent material may have a thickness of less than 200 nm, the thickness may be between 20 nm and 300 nm, in particular, the thickness may between 150 nm and 40 nm.

(30) The resulting phosphor converter 663 includes a thin layer of phosphor particles 630 covered with a thin layer 660 of non-luminescent material, such as Al.sub.2O.sub.3. The thickness W of the phosphor converter 663 is less than 15 μm. FIGS. 7a, 7b, and 7c show the simulated optical resolution, color over source variation, and radiation pattern for such a phosphor converter 663. In FIGS. 7a, 7b, and 7c, the phosphor converter layer thickness is 14 μm, and the phosphor material particle size is d50=3.8 μm, the refractive index value is 1. All other parameters are the same as in FIGS. 3a-3c, and 4a-4c. As can be seen, by comparing plots 784 and 786 of FIG. 7a to plots 384 and 386 of FIG. 3a, the optical resolution is improved, and the contrast realized is 1:375. The color over source variation 742 (FIG. 7b) and radiation pattern 748 (FIG. 7c) also compare favorably to those in FIGS. 3b and 3c, respectively.

(31) In addition to having a high optical contrast, the phosphor converter 663 is mechanically stable, and enhances extraction of light from the LED die, by coupling phosphor particles which touch the LED surface optically, without significantly decreasing light scattering in the layer. The phosphor converter 663 also has high reliability necessary for a variety of application, including, for example, automotive forward lighting standards. Furthermore, such a phosphor converter layer may be used on any LED, not just micro-LED, where it may provide advantages of reliability and enhancing light extraction.

(32) ALD Details:

(33) Atomic Layer Deposition (ALD) is used to deposit the thin layer 660 on the optical converter 663. ALD is a chemical vapor deposition process which allows the deposition of thin layers of material by applying one atomic layer of a material per cycle in a controllable way. In such process a polymeric network is formed by reaction of a metal oxide precursor with an oxygen source such as water and/or ozone in the gas phase. The ALD reaction is split in (at least) two parts. In a first step the metal (oxide) precursor is fed into the reactor and adsorbs and/or reacts with reactive groups on the surfaces and substantially all non-reacted or adsorbed precursor molecules are removed by reactor purging. In a second step the oxygen source is fed into the reactor and reacts with the metal source on the particle surfaces followed by purging of the reactor to remove substantially all remaining oxygen source molecules and hydrolysis products formed by condensation reactions. The two steps lead to formation of an atomic layer (or monolayer) because of the self-limiting nature of the surface reaction. These atomic layer reaction steps are repeated multiple times to form the final ALD coating. The term metal oxide precursor especially indicates a precursor of the metal oxide. The precursor itself may not be a metal oxide, but may e.g. include metal organic molecule. Hence, especially the metal (oxide) precursors for ALD may typically include metal halides, alkoxides, amides, and other metal (organic) compounds.

(34) The step by step nature of the ALD process allows conformal coatings also on and in structures with large aspect-ratio such as phosphor particles. The ALD process further allows it to deposit layers of different composition by consecutively feeding different metal oxide precursor into the reactor to form multicomponent layers or nanolaminates with tailored optical properties.

(35) Hence, in a specific embodiment an ALD layer is applied on a GaN surface with phosphor particles to mechanically and optically bond the particles to the substrate. The process is set such that a layer connects particles with the substrate and particle with their neighboring particle. Thus, a phosphor particle network with modified optical properties is formed on the GaN surface enhancing the light output of the LED. The ALD layer may typically have a layer thickness in the 20-500 nm, especially 50-200 nm range.

(36) In a further embodiment the ALD process is set such that not only conformal deposition occurs but also CVD-like growth leading to thicker layers in the voids in between the phosphor particles. CDV-like growth can be realized by shorten the purge time between pulses or reducing the reactor temperature.

(37) A (non-limiting) number of suitable materials for the ALD second coating layer are listed in the following table 1:

(38) TABLE-US-00001 TABLE 1 Oxide Oxygen Deposition material Metal (oxide_precursor source T [° C.] Al.sub.2O.sub.3 Al(CH.sub.3).sub.3 (TMA) or HAl(CH.sub.3).sub.2 H.sub.2O or O.sub.3 100-400  HfO.sub.2 Hf(N(CH.sub.3).sub.2).sub.4 or Hf(N(CH.sub.2CH.sub.3).sub.2).sub.4 H.sub.2O 80-300 Ta.sub.2O.sub.5 TaCl.sub.5 or Ta(N(CH.sub.3).sub.2).sub.5 H.sub.2O 80-300 ZrO.sub.2 ZrCl.sub.4 or Zr(N(CH.sub.3).sub.2).sub.4 H.sub.2O 80-300 TiO.sub.2 TiCl.sub.4, Ti(OCH.sub.3).sub.4 or Ti(OEt).sub.4 H.sub.2O 80-300 SiO.sub.2 SiCl.sub.4, H.sub.2N(CH.sub.2).sub.3Si(OEt).sub.3 or Si(OEt).sub.4 H.sub.2O or O.sub.3 150-300 

(39) Alternatively or additionally, niobium oxide (especially Nb.sub.2O.sub.5) or yttrium oxide (Y.sub.2O.sub.3) may be applied. Metal precursors thereof are e.g., tert-butylimido)-tris (diethylamino)-niobium, NbF.sub.5, or NbCl.sub.5, and Tris(ethylcyclopentadienyl) Yttrium, respectively.

(40) However, other materials may also be applied. Hence, in the atomic layer deposition process a metal oxide precursor may especially be selected from the group of metal oxide precursors of metals selected from the group consisting of Al, Hf, Ta, Zr, Ti and Si. Alternatively or additionally, one or more of Ga, Ge, V and Nb may be applied. Even more especially, alternating layers of two or more of these precursors are applied, wherein at least one precursor is selected from the group consisting of an Al metal oxide precursor and an Si metal oxide precursor, especially an Al metal oxide metal oxide precursor, and another precursor is selected from the group consisting of a Hf metal oxide precursor, a Ta metal oxide precursor, a Zr metal oxide precursor and a Ti metal oxide precursor, especially selected from the group consisting of a Hf metal oxide precursor, a Ta metal oxide precursor, and a Zr metal oxide precursor, even more especially a Ta metal oxide precursor. Especially Hf, Zr, and Ta appear to provide relatively light transmissive layers, whereas Ti, for instance, may provide relatively less light transmissive layers. Processing with Ta, Hf and Zr seems to be relatively easier than Si, for instance. The terms “oxide precursor” or “metal oxide precursor” or “metal (oxide) precursor” may also refer to a combination of two or more chemically different precursors. These precursors especially form an oxide upon reaction with the oxygen source (and are therefore indicated as metal oxide precursor).

EXAMPLE

(41) To form a phosphor converter layer on an LED in accordance with the embodiments disclosed herein, a NYAG4454 (Intematix corp.) phosphor particle material with D50=3.8 μm was used. The phosphor particles were sedimented in ethanol with a screen weight of 2.5 mg/cm.sup.2 on a blue thin film flip-chip (TFFC) LED. Once the phosphor particles had been applied to the LED, an Al.sub.2O.sub.3 coating was then applied in a Picosun Oy ALD reactor. Precursor materials were trimethylaluminum and H.sub.2O for 0, to make the Al.sub.2O.sub.3 film. The deposition temperature was set to 150° C. The pulse time in which precursor was introduced was 100 ms, followed by a purge with nitrogen gas of 30 seconds, followed by a pulse of gas-phase water for 100 ms, followed by another purge of nitrogen gas for 30 seconds. Time was allowed after the pulse for the all of the precursor to react with the particles, and LED.

(42) The ALD cycle was repeated to form Al.sub.2O.sub.3 inorganic coating layers in 20 nm steps. At each 20 nm step, the emitted flux from the LED at IA was measured in an integrating sphere. FIG. 8 shows the relative flux measured at IA 85° C. socket temperature as a function of Al.sub.2O.sub.3 layer thickness. With increasing Al.sub.2O.sub.3 layer thickness the flux of the LED at constant current and temperature increases by about 6 percent.

(43) The optical contrast of the example phosphor converter was also measured. FIG. 9 shows the experimental setup for the optical contrast measurement of the example phosphor converter. The example phosphor converter 963 was formed as described above using YAG:Ce phosphor material particles having D50 of 3.8 μm. The phosphor converter layer was 10 μm thick. The Al.sub.2O.sub.3 layer deposited on the phosphor particles by ALD was 50 nm thick. The glass substrate 910 was coated a 100 nm layer of aluminum 919. The aluminum layer 919 has a slit 923 (or line in a plan view, FIG. 10) that was 50 μm wide. To make the measurement, blue light 940 is illuminated on the back side of substrate 910, some of which passed through the slit 923.

(44) FIG. 10 is an image of the line of blue light through the phosphor converter layer 963. The light distribution was measured with an optical microscope (Keyence VHX-5000), plotting line scans perpendicularly to the open line in the aluminum layer 919.

(45) FIG. 11 shows the measured line profile 11, perpendicular to the open line in the Al layer 919 on the phosphor converter layer 963. The intensity profile is from the microscopic images. In order to extend the dynamic range of the microscope camera, pictures with different exposure times have been superimposed, always selecting the signal within the dynamic range of the camera (HDR measurement). The measured line profile 11 matches the calculated profile 12. A contrast of 1:300 (14) is reached 47 μm from the edge of the Al layer.

(46) FIG. 12 shows an SEM (scanning electron microscope) image of the interface of a cross-section of a phosphor converter layer on a substrate with the thin layer of Al.sub.2O.sub.3 coating the phosphor material particles. This example phosphor converter layer was formed as described above, with YAG phosphor, and the phosphor converter layer was formed on a glass substrate for ease of imaging. The figure shows how the Al.sub.2O.sub.3 coats the particles and exposed surface of the glass substrate, and also shows how the particles are in contact with the glass substrate, which glass substrate would be a surface of an LED emitting light. The coating materials may also be assessed by EDAX (an X-ray spectroscopic method for determining elemental composition) analysis.

(47) The following enumerated clauses provide additional non-limiting aspects of the disclosure.

(48) Clause 1. A device comprising: a micro-LED comprising at least two individually addressable light emitting diodes on a same substrate; and a phosphor converter layer disposed on the micro-LED, the phosphor converter layer comprising a plurality of phosphor particles having a D50 of greater than 1 μm and less than 10 μm, wherein a thickness of the phosphor converter layer is greater than 4 μm and less than 20 μm, wherein the phosphor converter layer further comprises a thin layer of non-luminescent material coating on the phosphor particles, and wherein the thin layer has a thickness of less than 200 nm.

(49) Clause 2. The device of clause 1, wherein the plurality of phosphor particles has a D50 of greater than 2 μm and less than 7 μm.

(50) Clause 3. The device of clause 2, wherein the plurality of phosphor particles has a D50 of greater than 3 μm and less than 5 μm.

(51) Clause 4. The device according to any one of the preceding clauses, wherein the particle size D50 is less than 9 μm and the thickness of the thin layer is less than 15 μm.

(52) Clause 5. The device of clause 4, wherein a thickness of the phosphor converter layer is greater than 8 μm and less than 15 μm.

(53) Clause 6. The device of clause 5, wherein a thickness of the phosphor converter layer is greater than 10 μm and less than 13 μm.

(54) Clause 7. The device of any of clauses 1-6, wherein the phosphor converter layer further comprises a matrix, and the matrix has a refractive index of 1 or greater and less than or equal to 1.5.

(55) Clause 8. The device of clause 7, wherein the matrix has a refractive index of 1 or greater and less than 1.4.

(56) Clause 9. The device of clause 8, wherein the matrix has a refractive index of 1 or greater and less than 1.2.

(57) Clause 10. The device of any of clauses 1-9, wherein the phosphor converter layer is obtainable by spray coating or sedimentation.

(58) Clause 11. The device of clause 10, wherein the thin layer comprises a metal oxide.

(59) Clause 12. The device of clause 11, wherein the thin layer comprises at least one of Al.sub.2O.sub.3, HfO.sub.2, Ta.sub.2O.sub.5, ZrO.sub.2, TiO.sub.2, and SiO.sub.3.

(60) Clause 13. The device of clause 10, wherein the thin layer is formed by atomic layer deposition.

(61) Clause 14. The device of clause 10, wherein the thin layer has a thickness between 40-150 nm.

(62) Clause 15. A device comprising: a light emitting diode; and a phosphor converter layer on the light emitting diode, the phosphor converter layer including a plurality of phosphor particles and a thin layer of a non-luminescent material formed over the phosphor particles, wherein a thickness of the phosphor converter layer is greater than 4 μm and less than 20 μm, wherein the phosphor converter layer further comprises a thin layer of non-luminescent material coating on the phosphor particles, and wherein the thin layer has a thickness of less than 200 nm.

(63) This disclosure is illustrative and not limiting. Further modifications will be apparent to one skilled in the art in light of this disclosure and are intended to fall within the scope of the appended claims.