This application claims the right of priority based on TW Application Serial No. 111133942, filed on Sep. 7, 2022, and the content of which is hereby incorporated by reference in its entirety.
The disclosure relates to a semiconductor device, and particularly to a semiconductor light-emitting device.
Semiconductor devices can be applied to a wide range of applications. Research and development of related materials have been continuously carried out. For example, a group III-V semiconductor material containing a group III element and a group V element may be applied to various optoelectronic semiconductor devices, such as light-emitting diodes (LEDs), laser diodes (LDs), photoelectric detectors, solar cells or power devices (such as switches or rectifiers). These optoelectronic semiconductor devices can be applied in various fields, such as illumination, medical care, display, communication, sensing, or power supply system. For example, in semiconductor light-emitting devices, LEDs have low energy consumption, rapid response, small volume and long operating lifetime, thus are widely used.
The present disclosure provides a semiconductor device. The semiconductor device comprises a first semiconductor structure, a second semiconductor structure located on the first semiconductor structure, and an active layer located between the first semiconductor structure and the second semiconductor structure. The first semiconductor structure has a first conductivity type, and includes a plurality of first layers and a plurality of second layers alternately stacked. The second semiconductor structure has a second conductivity type opposite to the first conductivity type. The plurality of first layers and the plurality of second layers include indium and phosphorus, and the plurality of first layers and the plurality of second layers respectively have a first indium atomic percentage and a second indium atomic percentage. The second indium atomic percentage is different from the first indium atomic percentage.
The foregoing aspects and many of the attendant advantages of the present disclosure will become more readily appreciated as the same becomes better understood by reference to the following detailed description, when taken in conjunction with the accompanying drawings, wherein:
Exemplary embodiments of the present disclosure will be described in detail with reference to the accompanying drawings hereafter. The following embodiments are given by way of illustration with Cartesian Coordinates (X, Y, Z axes) to help those skilled in the art fully understand the spirit of the present disclosure. Hence, it should be noted that the present disclosure is not limited to the embodiments herein and can be realized in various forms. Further, the drawings are not precise scale and components may be exaggerated in view of width, height, length, etc. Herein, the similar or identical reference numerals will denote the similar or identical components throughout the drawings. In the embodiments of the present disclosure, if not described otherwise, the term “horizontal” means any value or vector along X-axis, Y-axis or on X-Y plane. The term “vertical” means any value or vector along Z-axis, and terms such as “below”, “above”, “under”, “on”, “top” and “bottom” may be used to describe special relationships along Z-axis between different devices or elements. The term “corresponding” may be used to describe different elements are overlapped horizontally (on X-Y plane). The term “coplanar” may be used to describe surfaces of different elements are vertically on the same level.
The semiconductor device of the present disclosure can be light-emitting device (such as light-emitting diode or laser diode) or light absorption device (such as photo-detector). Qualitative or quantitative analysis of the composition and/or dopant contained in each layer of the semiconductor device of the present disclosure may be conducted by any suitable method, for example, a secondary ion mass spectrometer (SIMS). A thickness of each layer may be obtained by any suitable method, such as a transmission electron microscopy (TEM) or a scanning electron microscope (SEM).
In addition, if not otherwise specified, a description similar to “a first layer/structure is on or under a second layer/structure” may include an embodiment in which the first layer/structure directly (or physically) contacts the second layer/structure, and may also include an embodiment in which another structure is provided between the first layer/structure and the second layer/structure, such that the first layer/structure and the second layer/structure do not directly contact each other. Furthermore, it should be realized that a positional relationship of a layer/structure may be altered when being observed in different orientations.
The base 108 can include conductive material or insulating material. The conductive material can include gallium arsenide (GaAs), indium phosphide (InP), silicon carbide (SiC), gallium phosphide (GaP), zinc oxide (ZnO), gallium nitride (GaN), aluminum nitride (AlN), germanium (Ge) or silicon (Si). The insulating materials can include sapphire. In the embodiment shown in
The first semiconductor structure 100, the second semiconductor structure 102 and the active structure 104 can include same group of III-V compound semiconductor material. The III-V compound semiconductor material can include binary, ternary or quaternary III-V compound semiconductors, such as AlInGaAs series, AlInGaP series, AlInGaN series or InGaAsP series. The AlInGaAs series can be represented by (Alx1In(1-x1))1-x2Gax2As, wherein 0≤x1, x2≤1. The AlInGaP series can be represented by (Aly1In(1-y1))1-y2Gay2P, wherein 0≤y1, y2≤1. The AlInGaN series can be represented by (Alz1In(1-z1))1-z2Gaz2N, wherein 0≤z1, z2≤1. The InGaAsP series can be represented by Inz3Ga1-z3Asz4P1-z4, wherein 0≤z3, z4≤1.
The semiconductor device 10A can include double heterostructure (DH), double-side double heterostructure (DDH) or multiple quantum wells structure (MQW). For example, the active layer 104a can include a plurality of barrier layers (not shown) and a plurality of well layers (not shown) that are alternately stacked with each other to form aforementioned multiple quantum wells structure. When the semiconductor device 10A is in operation, the active structure 104 emits a light with a peak wavelength, and the light can include visible light and/or invisible light. The active layer 104a has a bandgap determined by the material composition of the active structure 104, and the peak wavelength is corresponding to the bandgap. For example, when the material of the active structure 104 includes InGaN series, it can emit blue light or deep blue light with a peak wavelength of 400 nm to 490 nm, or green light with a peak wavelength of 490 nm to 550 nm; when the material of the active structure 104 includes AlGaN series, it can emit ultraviolet light with a peak wavelength of 250 nm to 400 nm; when the material of the active structure 104 includes InGaAs series, InGaAsP series, AlGaAs series or AlGaInAs series, it can emit infrared light with a peak wavelength of 700 to 1700 nm; when the material of the active structure 104 includes InGaP series or AlGaInP series, it can emit red light with a peak wavelength of 610 nm to 700 nm, or yellow light with a peak wavelength of 530 nm to 600 nm.
As shown in
According to some embodiments of the present disclosure, the first layer 106a and the second layer 106b of each pair can include the same material but with different composition ratios. In one embodiment, the first layer 106a and the second layer 106b in each pair include indium and phosphorus. The first layer 106a has a first indium atomic percentage and the second layer 106b has a second indium atomic percentage different from the first indium atomic percentage. According to one embodiment, when the first semiconductor structure 100 is the n-type semiconductor, concentration of two-dimensional electron gas (2DEG) within the first semiconductor structure 100 can be increased by differentiating the first indium atomic percentage of the first layer 106a from the second indium atomic percentage of the second layer 106b, so as to increase speed of carrier recombination in the semiconductor device 10A. Specifically, the first indium atomic percentage and the second indium atomic percentage are respectively corresponding to an indium atomic ratio of the first layer 106a and an indium atomic ratio of the second layer 106b, which can be obtained through suitable component analysis methods, such as Energy Dispersive Spectrometer (EDX) or SIMS. For example, when the first layer 106a includes (Alx4Ga1-x4)1y4Iny4P and the second layer 106b includes (Alx5Ga1-x5)1-y5Iny5P (0<x4, x5, y4, y5<1), through EDX analysis the indium atomic ratio of the first layer 106a is obtained as y4 and the indium atomic ratio of the second layer 106b is obtained as y5. Accordingly, the first indium atomic percentage can be defined as y4*100%, and the second indium atomic percentage can be defined as y5*100%. For example, when y4=0.5 and y5=0.6, the first indium atomic percentage is 50% and the second indium atomic percentage is 60%. Indium atomic percentage represents a percentage of the total number of indium elements to the total number of all group III elements. In some embodiments, the first indium atomic percentage and the second indium atomic percentage can respectively be in a range of 30% to 70%, for example, between 40% to 60%.
In each or one pair of the first layer 106a and the second layer 106b, a lattice constant of the first layer 106a and a lattice constant of the second layer 106b can be the same or different. The “lattice constant” herein means a lattice constant a0 of a layer/structure without any substantial strain. In one embodiment, the first layer 106a and the second layer 106b respectively have a first lattice constant a1 and a second lattice constant a2. In one embodiment, the first lattice constant a1 and/or the second lattice constant a2 can be in a range of 5.5 Å to 5.8 Å. In some embodiments, when the base 108 is a GaAs growth substrate and the first indium atomic percentage of the first layer 106a (or the second indium atomic percentage of the second layer 106b) is 50%, the base 108 and the first layer 106a (or the second layer 106b) are latticed-matched. When the first indium atomic percentage (or the second indium atomic percentage) is smaller than 50%, the lattice constant of the first layer 106a (or of the second layer 106b) is smaller than the lattice constant of the base 108, so as to introduce tensile strain into the first layer 106a (or the second layer 106b). When the first indium atomic percentage (or the second indium atomic percentage) is larger than 50%, the lattice constant of the first layer 106a (or of the second layer 106b) is larger than the lattice constant of the base 108, so as to introduce compressive strain into the first layer 106a (or the second layer 106b). In some embodiments, the second lattice constant a2 of the second layer 106b can be larger than or smaller than the first lattice constant a1 of the first layer 106a. In other words, the second indium atomic percentage of the second layer 106b can be larger than or smaller than the first indium atomic percentage of the first layer 106a.
In each or one pair, the first layer 106a and the second layer 106b can include different materials. In some embodiments, the first layer 106a or the second layer 106b can include compound semiconductor having antimony (Sb). In one embodiment, the first layer 106a or the second layer 106b includes Iny0C1-y0Sbx0D1-x0, and element C is selected from group III elements other than indium and element D is selected from group V elements other than antimony (Sb). In one embodiment, element C and element D can respectively be aluminum (Al) and phosphorus (P), and 0≤x0≤1, 0<y0≤1. In one embodiment, the first layer 106a includes Al1-20Iny20P and the second layer 106b includes Iny23Al1-y23Sbx23P1-x23, and 0<x23, y20, y23<1. When the first semiconductor structure 100 is the p-type semiconductor, concentration of two-dimensional hole gas (2DHG) within the first semiconductor structure 100 can be increased by incorporating the compound semiconductor having Sb in the second layer 106b. Thus, in the first semiconductor structure 100, the serial resistance can be reduced and hole mobility can be increased, and carrier recombination speed of the semiconductor device 10A can be improved.
In some embodiments, with respect to the base 108 (such as the GaAs growth substrate), the first superlattice structure 106 can have compressive strain, tensile strain or no strain. Besides, in some embodiments, when the first semiconductor structure 100 is the n-type semiconductor, electron mobility of the first semiconductor structure 100 can be improved by introducing tensile strain into the first superlattice structure 106, for example, making the first layer 106a have tensile strain and the second layer 106b have no strain. Or, when the first semiconductor structure 100 is the p-type semiconductor, hole mobility of the first semiconductor structure 100 can be improved by introducing compressive strain into the first superlattice structure 106, for example, making the first layer 106a have compressive strain and the second layer 106b have no strain. Through improving the electron mobility or the hole mobility of the first semiconductor structure 100, carrier recombination speed of the semiconductor device 10A can be increased.
In one embodiment, in each pair, the first layer 106a has a first valence band (Ev1), a first conduction band (Ec1) and a first bandgap (ΔE1=Ec1−Ev1), and the second layer 106b has a second valence band (Ev2), a second conduction band (Ec2) and a second bandgap (ΔE2=Ec2−Ev2). In one embodiment, when the first semiconductor structure 100 is the n-type semiconductor, a gap of conduction band (ΔEc) between the first conduction band (Ec1) and the second conduction band (Ec2) can be in a range of 0.05 eV to 1 eV, so as to form carrier-confinement effect. For instance, the second conduction band (Ec2) can be lower than the first conduction band (Ec1) by 0.05 eV to 1 eV. In one embodiment, the first bandgap (ΔE1) of the first layer 106a and the second bandgap (ΔE2) of the second layer 106b can be larger than the bandgap of the active layer 104a, and a wavelength corresponding to the first bandgap (ΔE1) of the first layer 106a and a wavelength corresponding to the second bandgap (ΔE2) of the second layer 106b are smaller than the peak wavelength of the light emitted from the active structure 104. Thus, the first layer 106a and the second layer 106b do not absorb the light. In some embodiments, a difference between the peak wavelength of the light and the wavelength corresponding to the first bandgap (ΔE1) (or the wavelength corresponding to the second bandgap (ΔE2)) is equal to or larger than 30 nm. For example, when the active structure 104 emits a red light with the peak wavelength of 660 nm, the wavelength corresponding to the first bandgap (ΔE1) and/or the wavelength corresponding to the second bandgap (ΔE2) can be equal to or smaller than 630 nm.
In some embodiments, the first layer 106a and the second layer 106b can respectively have strains with respect to the base 108, and the strain of the first layer 106a is opposite to the strain of the second layer 106b. For instance, with respect to the base 108 (such as the GaAs growth substrate), the first layer 106a and the second layer 106b can respectively have the tensile strain and the compressive strain (or the compressive strain and the tensile strain), so that the strain of the first layer 106a can be compensated by the strain of the second layer 106b. In some embodiments, the base 108 has a third lattice constant a3, and the third lattice constant a3 can be between the first lattice constant a1 of the first layer 106a and the second lattice constant a2 of the second layer 106b. In some embodiments, each pair of the first layer 106a and the second layer 106b have an equivalent lattice constant aq1, and the equivalent lattice constant aq1 can be substantially same as the third lattice constant a3 so that the first superlattice structure 106 and the base 108 can keep latticed-matching. More specifically, as the first layer 106a has the first lattice constant a1 and the first thickness t1 and the second layer 106b has the second lattice constant a2 and the second thickness t2, the equivalent lattice constant aq1 can be expressed as aq1=(a1*t1+a2*t2)/(t1+t2). There may be a lattice constant difference (Δa1) between the equivalent lattice constant aq1 and the third lattice constant a3 (Δa1=aq1−a3). In some embodiments, a ratio of the lattice constant difference (Δa1) to the third lattice constant a3 can be equal to or smaller than ±2000 ppm, i.e., ±0.2%, so that the first superlattice structure 106 and the base 108 can keep latticed-matching and avoid delamination formed therebetween.
According to the embodiments in which the first layer 106a and the second layer 106b have opposite strains, the first layer 106a and the second layer 106b can include Al1-y6Iny6P, Ga1-y7Iny7P or (Alx8Ga(1-x8))1-y8Iny8P, and 0<x8<1, 0<y6, y7, y8<1. In one embodiment, the first layer 106a and the second layer 106b can include same material but with different composition ratios. For example, the first layer 106a can include Al1-y31Iny31P and the second layer 106b can include Al1-y32Iny32P while y31<y32, thus the first layer 106a and the second layer 106b respectively have the tensile strain and the compressive strain with respect to the base 108. As the first layer 106a and the second layer 106b are AlInP, the electron mobilities thereof and the wavelengths corresponding to the first bandgap (ΔE1) and the second bandgap (ΔE2) increase with the indium atomic ratios (y31, y32). In one embodiment, when the base 108 is the GaAs substrate and the peak wavelength of the light emitted from the active structure 104 is between 580 nm to 620 nm, y31 can be between 0.3 to 0.4 and y32 can be between 0.59 to 0.69 so that the first bandgap (ΔE1) can have a corresponding wavelength between 515 nm to 525 nm and the second bandgap (ΔE2) can have a corresponding wavelength between 535 nm to 605 nm. As such, the second layer 106b with higher indium atomic ratio (y32) can have higher electron mobility to increase carrier recombination speed of the semiconductor device 10A. In one embodiment, the first layer 106a and the second layer 106b can include different materials. For example, the first layer 106a can include Ga1-y33Iny33P and the second layer 106b can include Al1-y34Iny34P while y33<y34, thus the first layer 106a and the second layer 106b respectively have the tensile strain and the compressive strain with respect to the base 108. When the first layer 106a is GaInP, the electron mobility thereof and the wavelength corresponding to the first bandgap (ΔE1) increase with the indium atomic ratio (y33). In one embodiment, the indium atomic ratio (y33) of the first layer 106a is equal to or larger than 0.3 to ensure the first layer 106a can have high electron mobility, such as equal to or larger than 150 cm2/V sec. In one embodiment, when the base 108 is the GaAs substrate and the peak wavelength of the light emitted from the active structure 104 is between 580 nm to 620 nm, y33 can be between 0.3 to 0.4 and y34 can be between 0.59 to 0.69, so that the first bandgap (ΔE1) can have a corresponding wavelength between 560 nm to 605 nm and the second bandgap (ΔE2) to can have a corresponding wavelength between 535 nm to 605 nm.
In above two embodiments, through adjusting indium atomic ratios of the first layer 106a and the second layer 106b, the first layer 106a and the second layer 106b respectively have the tensile strain and the compressive strain with respect to the base 108, and the wavelengths corresponding to the first bandgap (ΔE1) of the first layer 106a and the second bandgap (ΔE2) of the second layer 106b can be smaller than the peak wavelength of the light. When the first semiconductor structure 100 is the n-type semiconductor, the first layer 106a with the tensile strain can improve the electron mobility of the first semiconductor structure 100. When the first semiconductor structure 100 is the p-type semiconductor, the second layer 106b with the compressive strain can improve the hole mobility of the first semiconductor structure 100. In other words, the first layer 106a and the second layer 106b can respectively improve the electron mobility and the hole mobility of the first semiconductor structure 100 since they have opposite strains, so that the carrier recombination speed of the semiconductor device 10A can be increased.
Referring to
In each pair, the third layer 122a and the fourth layer 122b can include ternary or quaternary III-V compound semiconductor, which is compound of at least three elements selected from aluminum (Al), gallium (Ga), indium (In), phosphorus (P), arsenic (As) or nitrogen (N). In one embodiment, the third layer 122a and the fourth layer 122b of each pair do not include nitrogen (N).
According to some embodiments of the present disclosure, the third layer 122a and the fourth layer 122b of each pair can include the same material but with different composition ratios. In one embodiment, the third layer 122a and the fourth layer 122b in each pair include indium and phosphorus. The third layer 122a has a third indium atomic percentage and the fourth layer 122b has a fourth indium atomic percentage different from the third indium atomic percentage. According to one embodiment, when the second semiconductor structure 102 is the p-type semiconductor, concentration of the two-dimensional hole gas (2DHG) within the second semiconductor structure 102 can be increased by differentiating the third indium atomic percentage of the third layer 122a from the fourth indium atomic percentage of the fourth layer 122b, so as to increase speed of carrier recombination in the semiconductor device 10B. Specifically, the third indium atomic percentage and the fourth indium atomic percentage are respectively corresponding to an indium atomic ratio of the third layer 122a and an indium atomic ratio of the fourth layer 122b, which can be obtained through EDX or SIMS. In some embodiments, the third indium atomic percentage and the fourth indium atomic percentage can respectively be in a range of 30% to 70%, for example, between 40% to 60%.
In each or one pair of the third layer 122a and the fourth layer 122b, a lattice constant of the third layer 122a and a lattice constant of the fourth layer 122b can be the same or different. In one embodiment, the third layer 122a and the fourth layer 122b respectively have a fourth lattice constant a4 and a fifth lattice constant a5. In one embodiment, the fourth lattice constant a4 and/or the fifth lattice constant a5 can be in a range of 5.5 Å to 5.8 Å. In some embodiments, when the base 108 is the GaAs growth substrate and the third indium atomic percentage of the third layer 122a (or the fourth indium atomic percentage of the fourth layer 122b) is 50%, the base 108 and the third layer 122a (or the fourth layer 122b) are latticed-matched. When the third indium atomic percentage (or the fourth indium atomic percentage) is smaller than 50%, the lattice constant of the third layer 122a (or of the fourth layer 122b) is smaller than the lattice constant of the base 108, so as to introduce tensile strain into the third layer 122a (or the fourth layer 122b). When the third indium atomic percentage (or the fourth indium atomic percentage) is larger than 50%, the lattice constant of the third layer 122a (or of the fourth layer 122b) is larger than the lattice constant of the base 108, so as to introduce compressive strain into the third layer 122a (or the fourth layer 122b). In some embodiments, the fifth lattice constant a5 of the fourth layer 122b can be larger than or smaller than the fourth lattice constant a4 of the third layer 122a. In other words, the fourth indium atomic percentage of the fourth layer 122b can be larger than or smaller than the third indium atomic percentage of the third layer 122a.
In each or one pair, the third layer 122a and the fourth layer 122b can include different materials. In some embodiments, the third layer 122a or the fourth layer 122b can include compound semiconductor having antimony. In one embodiment, the third layer 122a or the fourth layer 122b includes Iny2C1-y2Sbx2D1-x2, and element C is selected from group III elements other than indium (In) and element D is selected from group V elements other than antimony (Sb). In one embodiment, element C and element D can respectively be aluminum (Al) and phosphorus (P), and 0≤x2≤1, 0<y2≤1. In one embodiment, the third layer 122a includes Al1-y21Iny21P and the fourth layer 122b includes Iny2Al1-y22Sbx22P1-x22, and 0<x22, y21, y22<1. When the second semiconductor structure 102 is the p-type semiconductor, the concentration of two-dimensional hole gas (2DHG) within the second semiconductor structure 102 can be increased by incorporating the compound semiconductor having Sb in the fourth layer 122b. Thus, in the second semiconductor structure 102, the serial resistance can be reduced and the hole mobility can be increased, and the carrier recombination speed of the semiconductor device 10B can be improved.
In some embodiments, with respect to the base 108 (such as the GaAs growth substrate), the second superlattice structure 122 can have compressive strain, tensile strain or no strain. Besides, in some embodiments, when the second semiconductor structure 102 is the n-type semiconductor, electron mobility of the second semiconductor structure 102 can be improved by introducing tensile strain into the second superlattice structure 122, for example, making the third layer 122a have tensile strain and the fourth layer 122b have no strain. Or, when the second semiconductor structure 102 is the p-type semiconductor, hole mobility of the second semiconductor structure 102 can be improved by introducing compressive strain into the second superlattice structure 122, for example, making the third layer 122a have compressive strain and the fourth layer 122b have no strain. Through improving the electron mobility or the hole mobility of the second semiconductor structure 102, carrier recombination speed of the semiconductor device 10B can be increased. In one embodiment, in each or one pair of the third layer 122a and the fourth layer 122b, the third layer 122a can include Al1-y13Iny13P and the fourth layer 122b can include Al1-y14Iny14P, and 0<y13, y14<1 and y13<y14.
In one embodiment, in each pair, the third layer 122a has a third valence band (Ev3), a third conduction band (Ec3) and a third bandgap (ΔE3=Ec3−Ev3), and the fourth layer 122b has a fourth valence band (Ev4), a fourth conduction band (Ec4) and a fourth bandgap (ΔE4=Ec4-Ev4). In one embodiment, when the second semiconductor structure 102 is the p-type semiconductor, a gap of valence band (ΔEv) between the third valence band (Ev3) and fourth valence band (Ev4) can be in a range of 0.05 eV to 1 eV, so as to form carrier-confinement effect. For instance, the fourth valence band (Ev4) can be higher than the third valence band (Ev3) by 0.05 eV to 1 eV. In one embodiment, the third bandgap (ΔE3) of the third layer 122a and the fourth bandgap (ΔE4) of the fourth layer 122b can be larger than the bandgap of the active layer 104a, and a wavelength corresponding to the third bandgap (ΔE3) of the third layer 122a and a wavelength corresponding to the fourth bandgap (ΔE4) of the fourth layer 122b can be smaller than the peak wavelength of the light emitted from the active structure 104. Thus, the third layer 122a and the fourth layer 122b do not absorb the light. In some embodiments, a difference between the peak wavelength of the light and the wavelength corresponding to the third bandgap (ΔE3) (or the wavelength corresponding to the fourth bandgap (ΔE4)) is equal to or larger than 30 nm. For example, when the active structure 104 emits a red light with the peak wavelength of 660 nm, the wavelength corresponding to the third bandgap (ΔE3) and the wavelength corresponding to the fourth bandgap (ΔE4) can be equal to or smaller than 630 nm.
In some embodiments, the third layer 122a and the fourth layer 122b can respectively have strain with respect to the base 108, and the strain of the third layer 122a is opposite to the strain of the fourth layer 122b. For instance, with respect to the base 108 (such as the GaAs growth substrate), the third layer 122a and the fourth layer 122b can respectively have the tensile strain and the compressive strain (or the compressive strain and the tensile strain), so that the strain of the third layer 122a can be compensated by the strain of the fourth layer 122b. In some embodiments, the third lattice constant a3 of the base 108 can be between the fourth lattice constant a4 of the third layer 122a and the fifth lattice constant a5 of the fourth layer 122b. In some embodiments, each pair of the third layer 122a and the fourth layer 122b have an equivalent lattice constant aq2, and the equivalent lattice constant aq2 can be substantially same as the third lattice constant a3 so that the second superlattice structure 122 and the base 108 can keep latticed-matching. More specifically, as the third layer 122a has the fourth lattice constant a4 and the third thickness t3 and the fourth layer 122b has the fifth lattice constant a5 and the fourth thickness t4, the equivalent lattice constant aq2 can be expressed as aq2=(a4*t3+a5*t4)/(t3+t3). There may be a lattice constant difference (Δa2) between the equivalent lattice constant aq2 and the third lattice constant a3 (Δa2=aq2−a3). In some embodiments, a ratio of the lattice constant difference (Δa2) to the third lattice constant a3 can be equal to or smaller than ±2000 ppm, i.e., ±0.2%, so that the second superlattice structure 122 and the base 108 can keep latticed-matching and avoid delamination formed therebetween.
According to the embodiments in which the third layer 122a and the fourth layer 122b have opposite strains, the third layer 122a and the fourth layer 122b can include Al1-y6Iny6P, Ga1-y7Iny7P or (Alx8Ga(1-x8))1-y8Iny8P, and 0<x8<1, 0<y6, y7, y8<1. In one embodiment, the third layer 122a and the fourth layer 122b can include same material but with different composition ratios. For example, the third layer 122a can include Al1-y35Iny35P and the fourth layer 122b can include Al1-y36Iny36P while y35<y36, thus the third layer 122a and the fourth layer 122b respectively have the tensile strain and the compressive strain with respect to the base 108. As the third layer 122a and the fourth layer 122b are AlInP, the wavelengths corresponding to the third bandgap (ΔE3) and the fourth bandgap (ΔE4) increase with the indium atomic ratios (y35, y36). In one embodiment, when the base 108 is the GaAs substrate and the peak wavelength of the light emitted from the active structure 104 is between 580 nm to 620 nm, y35 can be between 0.3 to 0.4 and y36 can be between 0.59 to 0.69 so that the third bandgap (ΔE3) can have a corresponding wavelength between 515 nm to 525 nm and the fourth bandgap (ΔE4) can have a corresponding wavelength between 535 nm to 605 nm. In one embodiment, the third layer 122a and the fourth layer 122b can include different materials. For example, the third layer 122a can include Ga1-y37Iny37P and the fourth layer 122b can include Al1-y38Iny38P while y37<y38, thus the third layer 122a and the fourth layer 122b respectively have the tensile strain and the compressive strain with respect to the base 108. When the third layer 122a is GaInP, the wavelength corresponding to the third bandgap (ΔE3) increases with the indium atomic ratio (y37). In one embodiment, when the base 108 is the GaAs substrate and the peak wavelength of the light emitted from the active structure 104 is between 580 nm to 620 nm, y37 can be between 0.3 to 0.4 and y38 can be between 0.59 to 0.69, so that the third bandgap (ΔE3) can have a corresponding wavelength between 560 nm to 605 nm and the fourth bandgap (ΔE4) can have a corresponding wavelength between 535 nm to 605 nm.
In above two embodiments, through adjusting indium atomic ratios of the third layer 122a and the fourth layer 122b, the third layer 122a and the fourth layer 122b respectively have the tensile strain and the compressive strain with respect to the base 108, and the wavelengths corresponding to the third bandgap (ΔE3) of the third layer 122a and the fourth bandgap (ΔE4) of the fourth layer 122b can be smaller than the peak wavelength of the light. When the second semiconductor structure 102 is the n-type semiconductor, the third layer 122a with the tensile strain can improve the electron mobility of the second semiconductor structure 102. When the second semiconductor structure 102 is the p-type semiconductor, the fourth layer 122b with the compressive strain can improve the hole mobility of the second semiconductor structure 102. In other words, the third layer 122a and the fourth layer 122b can respectively improve the electron mobility and the hole mobility of the second semiconductor structure 102 since they have opposite strains, so that the carrier recombination speed of the semiconductor device 10B can be increased.
The positions, relative relationships, and material compositions of other layers or structures as well as structural variations in the semiconductor device 10B have been described in detail in previous embodiments, and are not repeatedly described herein.
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The insulating structure 128 can include electrically insulating materials, such as oxide or fluoride. The oxide is, for example, silicon dioxide (SiOx), and the fluoride is, for example, magnesium fluoride (MgFx). In some embodiments, the insulating structure 128 can include an electrically insulating material, such as a low-refractive-index electrical insulating material with a refractive index lower than 1.4, such as magnesium fluoride (MgFx). The conductive structure 130 can include transparent conductive oxides, such as indium tin oxide (ITO), indium oxide (InO), tin oxide (SnO), cadmium tin oxide (CTO), antimony tin oxide (ATO), Al-doped ZnO (AZO), zinc tin oxide (ZTO), Ga-doped ZnO (GZO), zinc oxide (ZnO), indium cerium oxide (ICO), indium tungsten oxide (IWO), indium titanium oxide (ITiO), indium zinc oxide (IZO), indium gallium oxide (IGO) or gallium aluminum zinc oxide (GAZO).
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In one embodiment, the first semiconductor contact layer 114 can be patterned to locate below the plurality of first extending portions 124b and the plurality of second extending portions 124c of the first electrode 124. As shown in
Referring to
Materials of the first metal contact layer 140 and the second metal contact layer 142 can be determined respectively according to the material of the first semiconductor contact layer 114 and the material of the fourth semiconductor layer 118, so as to form an electrical contact (such as an ohmic contact) between the first metal contact layer 140 and the first semiconductor contact layer 114 and between the second metal contact layer 142 and the fourth semiconductor layer 118. The first metal contact layer 140 and the second metal contact layer 142 can respectively include conductive material, such as metal or alloy. The metal includes germanium (Ge), beryllium (Be), zinc (Zn), gold (Au), nickel (Ni), or copper (Cu). The alloy, for example, includes two or more metals selected from the above metals, such as germanium-gold-nickel (GeAuNi), beryllium gold (BeAu), germanium gold (GeAu), or zinc gold (ZnAu). The first metal contact layer 140 and the second metal contact layer 142 can include different materials. In one embodiment, the first metal contact layer 140 includes germanium gold (GeAu) and the second metal contact layer 142 includes beryllium gold (BeAu). As shown in
In one embodiment, the protecting layer 138 can optionally include a distributed Bragg reflector (DBR). The distributed Bragg reflector can include a plurality of first dielectric layers and a plurality of second dielectric layers alternately stacked with each other, and the plurality of first dielectric layers and a plurality of second dielectric layers have different refractive indices. For the semiconductor device 20, when the light emitted from the active structure 104 is extracted from the base 108′, the protecting layer 138 with DBR helps to reflect the light towards the base 108′ to facilitate light extraction. The positions, relative relationships, and material compositions of other layers or structures as well as structural variations in the semiconductor device 20 have been described in detail in previous embodiments, and are not repeatedly described herein. Furthermore, it should be realized that the semiconductor device 20 shown in
Based on the above, the present disclosure can provide a semiconductor device and a package structure thereof, and the structural design of which helps to improve optoelectronic characteristics of the semiconductor device (for example, lowering the operating bias or improving speed of carrier recombination). The semiconductor device or the package structure disclosed in this disclosure can be applied to products in various fields, such as illumination, medical care, display, communication, sensing, or power supply system, for example, can be used in a light fixture, monitor, mobile phone, tablet, an automotive instrument panel, a television, computer, wearable device (such as watch, bracelet or necklace), traffic sign, outdoor display, or medical device.
The embodiments of the present disclosure will be described in detail below with reference to the drawings. In the descriptions of the specification, specific details are provided for a full understanding of the present disclosure. The same or similar components in the drawings will be denoted by the same or similar symbols. It is noted that the drawings are for illustrative purposes only and do not represent the actual dimensions or quantities of the components. Some of the details may not be fully sketched for the conciseness of the drawings.
Number | Date | Country | Kind |
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111133942 | Sep 2022 | TW | national |