KR20120110831A - Light emitting device - Google Patents
Light emitting device Download PDFInfo
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- KR20120110831A KR20120110831A KR1020110028964A KR20110028964A KR20120110831A KR 20120110831 A KR20120110831 A KR 20120110831A KR 1020110028964 A KR1020110028964 A KR 1020110028964A KR 20110028964 A KR20110028964 A KR 20110028964A KR 20120110831 A KR20120110831 A KR 20120110831A
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/02—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
- H01L33/04—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a quantum effect structure or superlattice, e.g. tunnel junction
- H01L33/06—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a quantum effect structure or superlattice, e.g. tunnel junction within the light emitting region, e.g. quantum confinement structure or tunnel barrier
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/02—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
- H01L33/14—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a carrier transport control structure, e.g. highly-doped semiconductor layer or current-blocking structure
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/02—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
- H01L33/16—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a particular crystal structure or orientation, e.g. polycrystalline, amorphous or porous
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/02—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
- H01L33/20—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a particular shape, e.g. curved or truncated substrate
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L2933/00—Details relating to devices covered by the group H01L33/00 but not provided for in its subgroups
- H01L2933/0008—Processes
- H01L2933/0033—Processes relating to semiconductor body packages
- H01L2933/0058—Processes relating to semiconductor body packages relating to optical field-shaping elements
Abstract
Description
An embodiment relates to a light emitting element.
LED (Light Emitting Diode) is a device that converts electrical signals into infrared, visible light or light using the characteristics of compound semiconductors. It is used in household appliances, remote controls, display boards, The use area of LED is becoming wider.
In general, miniaturized LEDs are made of a surface mounting device for mounting directly on a PCB (Printed Circuit Board) substrate, and an LED lamp used as a display device is also being developed as a surface mounting device type . Such a surface mount device can replace a conventional simple lighting lamp, which is used for a lighting indicator for various colors, a character indicator, an image indicator, and the like.
As the use area of the LED is widened as described above, it is important to increase the luminance of the LED as the brightness required for a lamp used in daily life and a lamp for a structural signal is increased.
Embodiments provide a light emitting device having improved light emission efficiency and crystal defects.
The light emitting device according to the embodiment includes a light emitting structure including a first semiconductor layer, a second semiconductor layer, and an active layer formed between the first semiconductor layer and the second semiconductor layer, wherein among the first semiconductor layer and the second semiconductor layer At least one is a P-type semiconductor layer doped with a P-type dopant, the active layer includes a well layer and a barrier layer, the well layer includes a first well layer and a second well layer closest to the P-type semiconductor layer, The first well layer has a first band gap, the second well layer has a second band gap smaller than the first band gap, and the thickness of the first well layer is formed thicker than the thickness of the second well layer.
The embodiment provides a light emitting device having improved light emission efficiency and crystal defects.
1 is a view showing a light emitting device according to an embodiment;
2 is a partially enlarged cross-sectional view of a light emitting device according to the embodiment;
3 is a diagram showing an energy band diagram of a light emitting device according to an embodiment;
4 is an energy band diagram of a light emitting device according to an embodiment;
5 is a view showing a growth temperature of a light emitting device according to an embodiment with time;
6A is a view showing a change in output of the light emitting device according to the embodiment;
6B is a view illustrating a change in operating voltage of a light emitting device according to an embodiment;
6C is a view illustrating a change in reverse voltage of a light emitting device according to an embodiment;
6D is a view illustrating an optical luminescence spectrum of a light emitting device according to the embodiment;
7 is a view showing a light emitting device according to the embodiment;
8 is a partially enlarged cross-sectional view of a light emitting device according to the embodiment;
9 is a view showing an energy band diagram of a light emitting device according to the embodiment;
10 is a view showing an energy band diagram of a light emitting device according to the embodiment;
11 is a perspective view of a light emitting device package including a light emitting device according to the embodiment;
12 is a cross-sectional view of a light emitting device package including a light emitting device according to the embodiment;
13 is a cross-sectional view of a light emitting device package including a light emitting device according to the embodiment;
14 is a perspective view of a lighting system including a light emitting device according to the embodiment;
15 is a cross-sectional view taken along the line C-C 'of the lighting system of FIG.
16 is an exploded perspective view of a liquid crystal display device including the light emitting device according to the embodiment;
17 is an exploded perspective view of a liquid crystal display including the light emitting device according to the embodiment.
In the description of embodiments, each layer, region, pattern, or structure is “under” a substrate, each layer (film), region, pad, or “on” of a pattern or other structure. In the case of being described as being formed on the upper or lower, the "on", "under", upper, and lower are "direct" "directly" or "indirectly" through other layers or structures.
In addition, the description of the positional relationship between each layer or structure, please refer to this specification, or drawings attached to this specification.
The thickness and size of each layer in the drawings are exaggerated, omitted, or schematically shown for convenience and clarity of explanation. Also, the size and area of each component do not entirely reflect actual size or area.
Referring to FIG. 1, the
The supporting
On the other hand, the upper surface of the
A buffer layer (not shown) may be disposed on the
A
The
In addition, an undoped semiconductor layer (not shown) may be further included below the
The
If the
In addition, when the
A conductive clad layer (not shown) may be formed on and / or below the
The
Meanwhile, the
Meanwhile, the above-described
The
In addition, the doping concentrations of the conductive dopants in the
The
A part of the
Meanwhile, a method of exposing a part of the
Also, a
Meanwhile, the first and
FIG. 2 is an enlarged cross-sectional view of a region A of FIG. 1.
2, the
According to an embodiment, the third well layer Q3 formed adjacent to the
The first through third well layers Q1, Q2 and Q3 and the first through third barrier layers B1, B2 and B3 may have a structure in which they are alternately stacked as shown in FIG.
2, the first through third well layers Q1, Q2 and Q3 and the first through third barrier layers B1, B2 and B3 are formed and the first through third barrier layers B1 and B2 Q2 and Q3 and the barrier layers B1, B2 and Q3 and the first through third well layers Q1, Q2 and Q3 are alternately stacked, B3 may be formed to have any number, and the arrangement may also have any arrangement. In addition, as described above, the composition ratios, band gaps, and thicknesses of the materials forming the respective well layers Q1, Q2, and Q3, and the respective barrier layers B1, B2, and B3 may be different from each other. It is not limited as shown in 2.
3 to 4 are diagrams showing energy band diagrams of light emitting devices according to embodiments.
3 to 4, the band gap of the third well layer Q3 may be larger than the band gaps of the first and second well layers Q1 and Q2.
The band gap of the third well layer Q3 adjacent to the
In addition, since the band gap of the third well layer Q3 is larger than the first and second well layers Q1 and Q2 and smaller than the barrier layers B1, B2 and B3, the barrier layers B1 and B2 having a large band gap are provided. , B3) and the
On the other hand, in as described above, the well layer (Q1, Q2, Q3) is In x Al y Ga 1 -x- y N (0≤x≤1, 0 ≤y≤1, 0≤x + y≤1) It may have a composition formula. The higher the In content of the well layers Q1, Q2, and Q3, the smaller the band gap. On the contrary, the smaller the In content of the well layers Q1, Q2, and Q3, the smaller the band gap of the well layers Q1, Q2, and Q3. Can be large.
Meanwhile, the In content of the third well layer Q3 may be 90% to 99% of the In content of the first and second well layers Q1 and Q2. When the In content is less than 90%, the difference in lattice constant between the first and second well layers Q1 and Q2 becomes larger in the band gap of the third well layer Q3, and the crystallinity is lowered. In addition, when In content is 99% or more, there is no big difference with 1st and 2nd well layers Q1 and Q2, and it does not have a big influence on hole injection and hardening improvement. The ratio may be any one of a molar ratio, a volume ratio, and a mass ratio, but is not limited thereto.
On the other hand, the piezoelectric polariziton generated by the stress due to the lattice constant difference and the orientation between the semiconductor layers may occur in the semiconductor layer. The semiconductor material forming the light emitting element has a large value of the piezoelectric coefficient and thus can cause very large polarization even at small strains. The electric field caused by the two polarizations changes the energy band structure of the quantum well structure, thereby distorting the distribution of electrons and holes. This effect is called the quantum confined stark effect (QCSE), which causes low internal quantum efficiency in light emitting devices that generate light by recombination of electrons and holes, and emits light such as red shift in the emission spectrum. It may adversely affect the electrical and optical characteristics of the device.
As it described above, the composition formula of the well layer (Q1, Q2, Q3) is In x Al y Ga 1 -x- y N (0≤x≤1, 0 ≤y≤1, 0≤x + y≤1) The barrier layers B1, B2, and B3 may have a composition formula of In a Al b Ga 1 -a- b N (0≤a≤1, 0≤b≤1, 0≤a + b≤1). . The lattice constant of InN is larger than GaN, and as the In content included in the well layers Q1, Q2, and Q3 increases, the lattice constant of the well layers Q1, Q2, and Q3 increases, so that the barrier layers B1, B2, and B3 The difference in lattice constant between the well layers Q1, Q2, and Q3 increases, which results in more strain between the layers. Due to this strain, the polarization effect as described above is further increased to strengthen the internal electric field. Accordingly, the band bends according to the electric field, resulting in a pointed triangle potential well, and the shape where electrons or holes are concentrated in the triangle potential well. May occur. Therefore, the recombination rate of electrons and holes may decrease.
According to an embodiment, as the In content of the third well layer Q3 decreases to decrease the lattice constant, the lattice constant difference between the barrier layers B1, B2 and B3 and the third well layer Q3 may decrease. Can be. Therefore, the generation of the above-described triangle potential wells can be reduced, thus the recombination rate of electrons and holes can be increased, and the luminous efficiency of the
In addition, since the band gap of the third well layer Q3 adjacent to the
On the other hand, the crystal defects due to the lattice constant difference between the
However, since the band gap of the third well layer Q3 of the
In this case, when the third well layer Q3 has a band gap larger than that of the second well layer Q2, the energy of light generated in each well layer is also different as the band gap between the well layers is different. This means that the wavelength of light generated in each well layer is also different. Accordingly, since the third well layer Q3 has a larger band gap than the second well layer Q2, the third well layer Q3 generates light having a larger energy, thereby generating light having a shorter wavelength. Therefore, broadening of the emission spectrum of the light emitting device may be widened in the short wavelength direction, and a shoulder may be formed in the photoluminescence spectrum of the
As described above, the third well layer Q3 formed adjacent to the
The energy level formula of light generated in the well layer is as follows.
At this time, L corresponds to the thicknesses d1 and d2 of the well layer. Therefore, the thicker the well layers Q1, Q2, and Q3, the lower the energy level of light generated in the well layers Q1, Q2, and Q3. When the third well layer Q3 has a larger band gap than the second well layer Q2, the energy levels between the well layers may be different. Therefore, broadening of the emission spectrum of the light emitting device may be increased, and a shoulder may be formed in the photoluminescence spectrum of the
On the other hand, d1 may have a thickness of 110% to 150% compared to d2.
If d1 is not greater than 110% larger than d2, the decrease in energy of light generated in the third well layer Q3 is small, and thus a short wavelength shift still exists, and if it is larger than 150%, it occurs in the third well layer Q3. There is a possibility that the light energy is too small, causing a long wavelength shift.
On the other hand, as shown in Figure 4, the band gap of the first to third well layer may be formed in large in order, may be formed to have a thick thickness sequentially.
That is, the content of In contained in the first to third quantum well layers Q1, Q2, and Q3 is gradually decreased from the first well layer Q1 to the third well layer Q3, and is sequentially thick. It can be to have.
The holes of the first to third well layers Q1, Q2, and Q3 are formed as the well layers Q1, Q2, and Q3 have larger band gaps as they are adjacent to the
In addition, as the band gaps are sequentially increased from the first well layer Q1 to the third well layer Q3, the well layers Q1, Q2, and Q3, the barrier layers B1, B2, and B3, and the first, The difference in lattice constant between the second semiconductor layers 120 and 150 may be alleviated, thereby reducing the occurrence of the triangle potential well, thus increasing the recombination rate of electrons and holes, and improving the luminous efficiency of the
In addition, as described above, the well layers Q1, Q2, and Q3 have a larger band gap, and are formed to have a thicker thickness, so that the energy levels between the well layers Q1, Q2, and Q3 become uniform, thereby making the well layers Q1, Although the band gap between Q2 and Q3) is different, the broadening of the emission spectrum of the
5 is a view showing a growth process of a light emitting device according to an embodiment according to growth time and growth temperature.
First, the
Preferably, C4 may have a value of about 100.4% to 103% relative to C3. In other words, if the growth temperature does not differ by more than 0.4%, it is difficult to adjust the expected crystallinity and the band gap. In addition, when the temperature is higher by 4% or more, the composition of In decreases, making it difficult to obtain a bandgap of a desired wavelength.
As the growth temperature C4 of the third well layer Q3 has a temperature higher than the growth temperature C3 of the first and second well layers Q1 and Q2, the In content of the third well layer Q3 may decrease. Can be. Therefore, as described above, the band gap of the third well layer Q3 may be increased, and the injection efficiency of holes injected into the third well layer Q3 and the second and first well layers Q1 and Q2 may be increased. The light emitting efficiency of the light emitting device may be improved by being increased.
In addition, as the growth temperature C4 of the third well layer Q3 increases, the growth temperature of the first and second semiconductor layers 120 and 150 and the
In addition, the growth time of the third well layer Q3 is longer than the growth time of the first well layer Q1 and the second well layer Q2 so that the third well layer Q3 is the first well layer Q1, And by forming a thicker than the second well layer (Q2), even if the band gap between the well layers (Q1, Q2, Q3), the energy level between the well layers (Q1, Q2, Q3) can be uniform and the light emitting device 100 ), Broadening of the emission spectrum can be reduced, and shoulder generation of the photo luminescence spectrum can be reduced. Therefore, a good well structure is formed and the luminous efficiency of the
6A is a view showing a change in output of the light emitting device according to the embodiment, FIG. 6B is a view showing a change in operating voltage of the light emitting device according to the embodiment, and FIG. 6C is a reverse voltage of the light emitting device according to the embodiment. voltage). 6D is a diagram illustrating an optical luminescence spectrum of the light emitting device according to the embodiment.
Referring to FIG. 6A, it can be seen that the output of the light emitting device wdT having a large band gap of the well layer adjacent to the p-type semiconductor layer according to the embodiment is improved compared to the comparative example wodT.
Referring to FIG. 6B, it can be seen that the operating voltage of the light emitting device wdT having the large band gap of the well layer adjacent to the p-type semiconductor layer according to the embodiment is substantially the same as the comparative example wodT. Therefore, although the output of the light emitting device is improved, it is not accompanied by an increase in the operating voltage, and as a result, an effect of reducing the operating voltage with the same output can be achieved. It can be confirmed that it can be achieved.
In addition, referring to FIG. 6C, it can be seen that the reverse voltage of the light emitting device wdT in which the band gap of the well layer adjacent to the p-type semiconductor layer is large according to the embodiment is improved compared to the comparative example wodT.
In addition, referring to FIG. 6D, the optical luminescence spectrum of the light emitting device in which the thickness of the well layer adjacent to the p-type semiconductor layer is formed according to the embodiment is represented by a solid line, and the thickness of each well layer is uniform. The photoluminescence spectrum of the device is indicated by the dotted line. In FIG. 6D, the shoulder P is formed in the light luminescence spectrum of the light emitting device in which the band gaps of the well layers are different and the thickness of each well layer is uniform. It can be seen that the optical luminescence spectrum of the light emitting device in which the thickness of the adjacent well layer is thickened has reduced the occurrence of the shoulder and the broadening of the spectrum.
7 is a view showing a light emitting device according to the embodiment.
Referring to FIG. 7, the
The
That is, the
Such a
A
The reflective layer (not shown) may be disposed between the ohmic layer (not shown) and the insulating layer (not shown), and have excellent reflective properties such as Ag, Ni, Al, Rh, Pd, Ir, Ru, Mg , Zn, Pt, Au, Hf, or a combination of these materials, or a combination of these materials or IZO, IZTO, IAZO, IGZO, IGTO, AZO, ATO, to form a multi-layer using a transparent conductive material such as Can be. Further, the reflective layer (not shown) can be laminated with IZO / Ni, AZO / Ag, IZO / Ag / Ni, AZO / Ag / Ni and the like. In addition, when the reflective layer (not shown) is formed of a material in ohmic contact with the light emitting structure 270 (eg, the first semiconductor layer 230), the ohmic layer (not shown) may not be formed separately, and the present invention is not limited thereto. I do not.
The ohmic layer (not shown) is in ohmic contact with the bottom surface of the
The
The
The
The
Well
In addition, when the
A conductive clad layer (not shown) may be formed on and / or below the
Meanwhile, an
Meanwhile, the above-described
A
A
The
The
A
The
The
The roughness may be formed to have various shapes such as a cylinder, a polygonal column, a cone, a polygonal pyramid, a truncated cone, a polygonal pyramid, and the like, preferably including a horn shape.
Meanwhile, the
Passivation (not shown) may be formed on side and upper regions of the
FIG. 8 is an enlarged cross-sectional view of a region B of FIG. 7.
Referring to FIG. 8, the
The first through third well layers Q1, Q2 and Q3 and the first through third barrier layers B1, B2 and B3 may have a structure in which they are alternately stacked as shown in FIG.
Meanwhile, in FIG. 8, the first to third well layers Q1, Q2, and Q3 and the first to third barrier layers B1, B2, and B3 are formed, respectively, and the first to third barrier layers B1, B2, B3) and the first to third well layers Q1, Q2, and Q3 are alternately formed, but are not limited thereto, and the well layers Q1, Q2, and Q3 and the barrier layers B1, B2, and B3 may be alternately formed. ) May be formed to have any number, and the arrangement may also have any arrangement. In addition, as described above, the composition ratios, band gaps, and thicknesses of the materials forming the respective well layers Q1, Q2, and Q3, and the respective barrier layers B1, B2, and B3 may be different from each other. It is not limited as shown in 8.
9 and 10 are diagrams illustrating energy band diagrams of a light emitting device according to an embodiment. In addition, the content common to the content demonstrated in FIG. 3 and FIG. 4 is abbreviate | omitted.
9 and 10, the band gap of the first well layer Q1 may be larger than the band gaps of the second and third well layers Q2 and Q3, and the band gap of the first well layer Q1 may be formed. The thickness may be thicker than the thicknesses of the second and third well layers Q2 and Q3.
As described above, as the first well layer Q1 adjacent to the
The In content of the first well layer Q1 may be 90% to 99% of the In content of the second and third well layers Q2 and Q3. The reason for limiting the ratio is as described above.
Further, according to the embodiment, the first well layer Q1 formed adjacent to the
According to the embodiment, the thickness of the first well layer Q1 is formed to be thicker than the thickness of the second well layer Q2, so that the band gaps between the well layers Q1, Q2, and Q3 are different. The energy level of light generated in Q2 and Q3) may be uniform, and thus, the broadening of the emission spectrum of the
Meanwhile, as illustrated in FIG. 10, the band gaps of the first to third well layers Q1, Q2, and Q3 may be sequentially formed to be small, and the first to third well layers Q1, Q2 and Q3. The thickness of may be formed to have a small thickness sequentially.
Therefore, the content of In included in the first to third quantum well layers Q1, Q2, and Q3 may be sequentially increased from the first well layer Q1 to the third well layer Q3.
As the first layer Q1, Q2, and Q3 are formed to have a larger band gap, the holes of the first to third well layers Q1, Q2, and Q3 are formed closer to the
In addition, as described above, the well layers Q1, Q2, and Q3 have a larger band gap, and are formed to have a thicker thickness, and even though the band gaps between the well layers Q1, Q2, and Q3 are different, the well layers Q1 and Q2 are different. , The energy level of the light generated in Q3) can be made uniform, so that the broadening of the emission spectrum of the
11 to 13 are a perspective view and a cross-sectional view showing a light emitting device package according to the embodiment.
11 to 13, the light emitting
The
The inner surface of the
Concentration of light emitted to the outside from the
The shape of the
The
The
Meanwhile, the
The encapsulant (not shown) may be filled in the
The encapsulant (not shown) may be formed of silicon, epoxy, or other resin material. The encapsulant may be filled in the
In addition, the encapsulant (not shown) may include a phosphor, and the phosphor may be selected to be a wavelength of light emitted from the
The phosphor may be one of a blue light emitting phosphor, a blue light emitting phosphor, a green light emitting phosphor, a sulfur green light emitting phosphor, a yellow light emitting phosphor, a yellow red light emitting phosphor, an orange light emitting phosphor, and a red light emitting phosphor depending on the wavelength of light emitted from the
That is, the phosphor may be excited by the light having the first light emitted from the
Similarly, when the
Such a fluorescent material may be a known fluorescent material such as a YAG, TAG, sulfide, silicate, aluminate, nitride, carbide, nitridosilicate, borate, fluoride or phosphate.
The first and second lead frames 540 and 550 may be formed of a metal material such as titanium, copper, nickel, gold, chromium, tantalum, (Pt), tin (Sn), silver (Ag), phosphorus (P), aluminum (Al), indium (In), palladium (Pd), cobalt (Co), silicon (Si), germanium , Hafnium (Hf), ruthenium (Ru), and iron (Fe). Also, the first and second lead frames 540 and 550 may be formed to have a single layer or a multilayer structure, but the present invention is not limited thereto.
The first and second lead frames 540 and 550 are separated from each other and electrically separated from each other. The
Meanwhile, referring to FIG. 13, the light emitting
The
In addition, the
On the other hand, a three-
The
Since the
On the other hand, the
The phosphor (not shown) is uniformly formed in the
As such, when the phosphor (not shown) is included in the
A plurality of light emitting device packages 500 according to the embodiment may be arranged on a substrate, and a light guide plate, a prism sheet, a diffusion sheet, or the like, which is an optical member, may be disposed on an optical path of the light emitting
14 is a perspective view illustrating a lighting apparatus including a light emitting device package according to an embodiment, and FIG. 15 is a cross-sectional view illustrating a C-C 'cross section of the lighting apparatus of FIG. 14.
Referring to FIGS. 14 and 15, the
A light emitting
The light emitting
In particular, the light emitting
Since the light emitting
The
The
On the other hand, since the light generated from the light emitting
16 is an exploded perspective view of a liquid crystal display including the light emitting device according to the embodiment.
FIG. 16 illustrates an edge-light method, and the
The liquid
The
The thin film transistor substrate 714 is electrically connected to the printed
The thin film transistor substrate 714 may include a thin film transistor and a pixel electrode formed of a thin film on another substrate of a transparent material such as glass or plastic.
The
The light emitting
In particular, the light emitting
Meanwhile, the
17 is an exploded perspective view of a liquid crystal display including the light emitting device according to the embodiment. However, the parts illustrated and described in FIG. 16 will not be repeatedly described in detail.
17 is a direct view, the liquid
Since the liquid
The backlight unit 870 includes a plurality of light emitting device modules 823, a
LED Module 823 A plurality of light emitting device packages 822 and a plurality of light emitting device packages 822 may be mounted to include a
In particular, the light emitting
The
Light generated in the light emitting element module 823 is incident on the
Meanwhile, the light emitting device according to the embodiment is not limited to the configuration and method of the embodiments described above, but the embodiments may be modified so that all or some of the embodiments may be selectively And may be configured in combination.
In addition, while the preferred embodiments have been shown and described, the present invention is not limited to the specific embodiments described above, and the present invention is not limited to the specific embodiments described above, and the present invention may be used in the art without departing from the gist of the invention as claimed in the claims. Various modifications can be made by those skilled in the art, and these modifications should not be individually understood from the technical spirit or the prospect of the present invention.
100
130: active layer 140: intermediate layer
150: second semiconductor layer 160: light emitting structure
Q1, Q2, Q3: well layer B1, B2, B3: barrier layer
Claims (10)
At least one of the first semiconductor layer and the second semiconductor layer is a P-type semiconductor layer doped with a P-type dopant,
The active layer includes a well layer and a barrier layer,
The well layer includes a first well layer and a second well layer closest to the P-type semiconductor layer,
The first well layer has a first bandgap, the second well layer has a second bandgap smaller than the first bandgap,
The thickness of the first well layer is thicker than the thickness of the second well layer.
The first band gap is,
A light emitting device that is 101% to 110% of the second bandgap.
The thickness of the first well layer is
Light emitting device is 110% to 150% of the thickness of the second well layer.
The well layer includes a third well layer formed between the first well layer and the second well layer,
The third well layer has a third band gap,
The third band gap is,
A light emitting device smaller than the first band gap and larger than the second band gap.
The thickness of the third well layer is
A light emitting device thinner than the first well layer and thicker than the second well layer.
The well layer includes In,
The first well layer,
A light emitting device having In content smaller than that of the second well layer.
In content of the first well layer,
A light emitting device which is 90% to 99% of the In content of the second well layer.
Disposed between the active layer and the P-type semiconductor layer to prevent leakage current
An intermediate layer; Light emitting device further comprising.
Wherein the intermediate layer comprises:
A light emitting device having a band gap larger than the band gap of the barrier layer.
Wherein the intermediate layer comprises:
Light emitting element including Al.
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
KR1020110028964A KR20120110831A (en) | 2011-03-30 | 2011-03-30 | Light emitting device |
JP2012068277A JP6081709B2 (en) | 2011-03-25 | 2012-03-23 | Light emitting element |
EP12161091.9A EP2503603B1 (en) | 2011-03-25 | 2012-03-23 | Light emitting device and method for manufacturing the same |
CN201210082888.9A CN102709417B (en) | 2011-03-25 | 2012-03-26 | Luminescent device and its manufacture method |
US13/429,623 US9029875B2 (en) | 2011-03-25 | 2012-03-26 | Light emitting device and method for manufacturing the same |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
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KR1020110028964A KR20120110831A (en) | 2011-03-30 | 2011-03-30 | Light emitting device |
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KR20120110831A true KR20120110831A (en) | 2012-10-10 |
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KR1020110028964A KR20120110831A (en) | 2011-03-25 | 2011-03-30 | Light emitting device |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9196786B2 (en) | 2012-12-28 | 2015-11-24 | Kabushiki Kaisha Toshiba | Semiconductor light emitting element and method for manufacturing the same |
KR20170082739A (en) * | 2016-01-07 | 2017-07-17 | 엘지이노텍 주식회사 | Light emitting device |
-
2011
- 2011-03-30 KR KR1020110028964A patent/KR20120110831A/en not_active Application Discontinuation
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9196786B2 (en) | 2012-12-28 | 2015-11-24 | Kabushiki Kaisha Toshiba | Semiconductor light emitting element and method for manufacturing the same |
KR20170082739A (en) * | 2016-01-07 | 2017-07-17 | 엘지이노텍 주식회사 | Light emitting device |
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