GB2323210A - Light emitting device - Google Patents

Light emitting device Download PDF

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Publication number
GB2323210A
GB2323210A GB9805086A GB9805086A GB2323210A GB 2323210 A GB2323210 A GB 2323210A GB 9805086 A GB9805086 A GB 9805086A GB 9805086 A GB9805086 A GB 9805086A GB 2323210 A GB2323210 A GB 2323210A
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United Kingdom
Prior art keywords
emitting device
light
impurity
quantum well
active region
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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Application number
GB9805086A
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GB9805086D0 (en
Inventor
Daniel A Steigerwald
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HP Inc
Original Assignee
Hewlett Packard Co
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Publication date
Application filed by Hewlett Packard Co filed Critical Hewlett Packard Co
Publication of GB9805086D0 publication Critical patent/GB9805086D0/en
Publication of GB2323210A publication Critical patent/GB2323210A/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/02Semiconductor devices having potential barriers 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
    • H01L33/26Materials of the light emitting region
    • H01L33/30Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table
    • H01L33/32Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table containing nitrogen
    • H01L33/325Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table containing nitrogen characterised by the doping materials
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/02Semiconductor devices having potential barriers 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
    • H01L33/04Semiconductor devices having potential barriers 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
    • H01L33/06Semiconductor devices having potential barriers 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

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  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Computer Hardware Design (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Led Devices (AREA)

Abstract

In a QW LED employing the Al In Ga N material system an intentional impurity is introduced in the quantum well active region to increase the efficiency of the LED (10) and to increase the emission wavelength beyond that of an undoped QW LED. In addition, an intentional impurity similar to that found in an adjacent layer can reduce the uncontrollable or undesirable effects of impurity diffusion.

Description

2323210 1 1 LIGHT EMITTING DEVICE The invention relates to a semi
conductor light-emitting device.
ffighly efficient visible devices (LEDs) have been produced in the redl, orange, and yellow spectral regions by employing the A4Ga,..As and In.3(A4Gaj.JP material systems and Double Heterostructure device sftuctures which employ a "bulk" active region in the thickness range of 0. 1 to 5.0 un in thickness. These highly efficient LEDs use a direct band-to-band transition to produce the light of an appropriate wavelength.
Recently highly efficient blue LEDs, commercialized by Nichia and Toyoda Gosei, employ the AlInGaN materials system in conjunctionwrith a "bulk" active region, 0.05 to 0. 10 pm in thickness, which is "co-doped" with both silicon and zinc. Co-doping has two positive effects. First, the extremely high defect density associated with epitaxial GaN leads to inefficient band-to-band transitions in undoped material, whereas the ZnSi pairs provide an extremely efficient mechanism for light emission. Second, the selection of Zn-Si pairs shifts the wave!ength substantially, from 380 run to 450 rim for the emission from the band-to-band and Zn-Si impurity centers, respectively. The shift in wavelength alone increases the detection efficiency of the human eye by almost a factor of 1000. Such an LED structure is acceptable for the blue spectral region, however, when attempts are made to shift the wavelength into the green spectral region by increasing the mole fraction of indium in the active 2 1/-111 region (x in the formula In,,GaiI..N), the result is an LED of poor color purity, with a "whitish" color. There is a great commercial need for highly efficient, spectrally pure green and blue-green LEDs.
Highly efficient blue and green LEDs have been commercialized which employ the same AlInGaN materials system in conjunction with an extremely thin quantum well (QW) active region, with a thickness of approximately 3 run. These devices employ an undoped QW region and direct band-to-band tramitions to achieve the high efficiency and purer colors. Special processes and techniques are used to eliminate dopant incorporation and diffusion.
The present lay seeks to provide an improved fight device.
According to an aspect of the present invention there is provided a figbtemitting device comprising a substrate; a GaN nucleation layer, positioned on the substrate; a Si-doped GaN current spreading layer positioned over the GaN nucleation layer; a first and second confining layers positioned over the Si-doped GaN current spreading layer wherein the first and second confining layers contain a first and second impurity, respectively; and a thin quantum well active region with a quantum well impurity, interposing the first and second confining layers wherein the quantum well impurity is selected to increase the fight emission vroperties of the light- i '' i g device.
3 In the preferred embodiment, an intentional impurity is introduced in a quantum well (QW) LED active region to increase the efficiency of the LED and to increase the emission wavelength beyond that of an undoped QW LED. In addition, an intentional impurity similar to that found in an adjacent layer can reduce the uncontrollable or undesirable effects of impurity diffusion.
Preferably, a thiii GaN nucleation layer is grown on a sapphire substrate. A thick Si-doped GaN layer is grown over the thin GaN nucleation layer. A first confining layer consisting of GaN: Mg is grown over an n-type GaN layer. A thin In. Gal, N QW active region is grown over the first confining layer. The thin QW active region has been optionally doped. A second confming layer consisting of GaN-based compound is positioned over the thin QW active region. The first and second confming layers are doped, either alone or in combination.
---1 4 An embodiment of the present invention as descriffied below, by way of example only, with reference to the accompanying drawings, in which:
Figure 1 ates an embodiment of a light emitting device; and Figure 2 illustrates a flowchart of a preferred method for producing the device shown in Figure 1.
Figure I illustrates a preferred embodiment of a light emitting device 10. A GaN nucleation layer 14 is positioned on a substrate 12, such as a sapphire substrate. A thick n-type GaN layer 16, doped with Si impurities, is formed over the GaN nucleation layer 14. A first confining layer 18 consisting of a GaN-based compound, doped with Mg impurities, is positioned over the thick Si-doped GaN layer 16. A thin INGa,-.,N quantum well (QW) active region 20 is positioned over the first confining layer 18. The thin Q)X active region 20 has been intentionally doped with magnesium (Mg). A second confining layer 22 consisting of AlGaN that is optionally doped with Mg is positioned over the thin QW active region 20. The first and second confining layers are doped with Mg, either alone or in combination. A contacting layer 24 consisting of a GaN-based compound, doped with Mg is positioned over the second confining layer 22.
Me intentional impurity introduced in a quantum well (QW) LED active region increases the efficiency of the LED and increases the emission wavelength beyond that of an undoped QW LED. In addition, adding a similar intentional. impurity to one of the confining layers can reduce the uncontrollable or undesirable effects of impurity diffusion. Alternatively, the layers "confining" the QW active region may include Al, ,Gal.,,N. If improving the internal efficiency of the QW active region is desired, these impurities may be donors or acceptors. If improving the injection efficiency of the QW active region is desired, the impurities are acceptors. Donors may be from Group VI such as oxygen, sulfur, selenium. or tellurium or Group IV such as silicon, germanium, or tin. Acceptors may be from Group IIA, e.g. magnesium, beryllium, or calcium, or Group IIB e.g. zinc or cadmium, or Group IV, e.g. carbon. In addition, rare earth elements from lanthanide group have been shown to be efficient emission centers in other materials and may be highly efficient in the AlInGaN material system.
6 11 1 Ile preferred embodirnent influences the overall efficiency of a fight g diode by four ct methods. Ile overall efficiency of a visible LED may be defined as the product of several individual, independent efficiencies, as:
TIM Tlim X llin X llcxuw X Tidcw The internal efficiency. Tli,,,w, is the fraction of injected minority carriers which emit photons. The injection efficiency, is the fi-action of the current that is transported into the active region. The extraction efficiency, is the fraction of photons which escape the crystal. For visible LEDs, the detector efficiency, Tld.,, ,, is the magnitude of the eye response per unit of radiant power.
The internal efficiency is increased by the impurity-related emission, which is more efficient than the near band-edge emission due to the high density of crystal defects.
The injection efficiency is increased due to the change in minority carrier injection from holes to electrons. This is important for two reasons; first the ratio of the electron concentration in the n-layer, to the hole concentration in the p-layer is significantly greater than 1, favoring electron injection. Second, the electrons in GaNbased material have a much lower effective mass, and a much higher mobility than the holes.
The extraction efficiency can be enhanced, as the impurity-related emission is not as strongly absorbed in the active region as near bandedge light.
The detector efficiency of blue and green LEDs are strongly affected by the emission wavelength, with an increae in wavelength increasing the response of the human eye. The impurity-related emissions in the prefered embodiment shift the emission wavelength longer, resuking in enhanced detection.
Figure 2 illustrates a process flow chart for the device shown in Figure I - In step 40, the first thin GaN nucleation layer is formed directly on the sapphire substrate 7 1 j at a low growth temperature such as 520 C. In steg 50, the GaN:Si layer is formed directly on the nucleation layer at growth temperatures at approximately 1050C, while the thickness may vary between 2 gm to 5 pin in thickness. In step 60, the first confining layer is formed over the GaN:Si layer. In step 70, the Mg-doped InGaN QW active region is formed over the first confining layer at a growth temperature that ranges from 650C to 850C, while the thickness of the QW active region is typically 3 mn in thickness. In step 80, the Mg-doped GaN layer is formed over the QW active region at a growth temperature that ranges from 650C to I I OOC while the thickness may vary between 0. 1 to 1.0:m.
These layers may be grown using one of many available techniques such as organometallic vapor phase epitaxy (OMVPE), metal-organic chemical vapor deposition (MOCVD), molecular beam qitaxy (MBE), gas phase MBE (GPMBE), or hydrWe, vapor phase e;ftcy (HVPE).
The disclosures in United States patent appfication, no. 08/8 15, 097, from which this application claims priority, and in the abstract accompanying this application are incorporated herein by reference.
8

Claims (9)

CLAINIS
1. A light-emitting device comprising: a substrate; A GaN nucleation layer positioned on the substrate; a Si-doped GaN current spreading layer positioned over the GaN nucleation layer; first and second conlining layers positioned over the Si-doped GaN current spreading layer, wherein the first and second confining layers contain a first and second impurity, respectively: and a thin quantum well active region with a quantum well impurity, interposing the first and second confining layers, wherein the quantum well impurity is selected to increase the light emission properties of the light-emitting device.
2. A light-emitting device according to claim 1, wherein the first impurity is selected to increase the light emission property of the lightemittizig device by improving the injection efficiency.
3. A light-emitting device according to claim 1, wherein the quantum well and first impurities are the same element, wherein the element is selected to effect impurity diflusion in the active region.
4. A fight-emitting device according to claim 1, 2 or 3, wherein the quantum well impurity is a donor element.
5. A light-emitting device according to claiin 1, 2, or 3, wherein the quantum well impurity is an acceptor element.
1I1 9
6. A light emitting device according to claim 5, wherein the acceptor element is selected from a group comprising Group IIA and Group HB elements.
7. A light- g device according to claim 6, wherein the acceptor element is magneshun
8. A light-emitting device substantially as hereinbefore described with reference to and as ated in the accompanying drawings.
9. A method of producing a fight-emitting device substantially as hereinbefore described with reference to and as illustrated in the accompanying drawings.
GB9805086A 1997-03-12 1998-03-10 Light emitting device Withdrawn GB2323210A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US81509797A 1997-03-12 1997-03-12

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GB9805086D0 GB9805086D0 (en) 1998-05-06
GB2323210A true GB2323210A (en) 1998-09-16

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JP (1) JPH10256601A (en)
DE (1) DE19753470A1 (en)
GB (1) GB2323210A (en)
SG (1) SG63757A1 (en)

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1189289A1 (en) * 1999-06-07 2002-03-20 Nichia Corporation Nitride semiconductor device
US6586762B2 (en) 2000-07-07 2003-07-01 Nichia Corporation Nitride semiconductor device with improved lifetime and high output power
US6711191B1 (en) 1999-03-04 2004-03-23 Nichia Corporation Nitride semiconductor laser device
WO2004051759A1 (en) * 2002-12-03 2004-06-17 Nec Corporation Semiconductor optical device having quantum well structure and its manufacturing method
US6835956B1 (en) 1999-02-09 2004-12-28 Nichia Corporation Nitride semiconductor device and manufacturing method thereof
US7230263B2 (en) 2001-04-12 2007-06-12 Nichia Corporation Gallium nitride compound semiconductor element
US7358522B2 (en) 2001-11-05 2008-04-15 Nichia Corporation Semiconductor device
EP2071638A1 (en) * 2006-08-08 2009-06-17 "Svetlana-Optoelektronika" Semiconductor light-emitting heterostructure
US7977687B2 (en) 2008-05-09 2011-07-12 National Chiao Tung University Light emitter device
US8592841B2 (en) 1997-07-25 2013-11-26 Nichia Corporation Nitride semiconductor device

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0996173B1 (en) * 1998-10-23 2015-12-30 Xerox Corporation Semiconductor structures including polycrystalline GaN layers and method of manufacturing
DE10015371A1 (en) * 2000-03-28 2001-10-18 Huga Optotech Inc Production of an epitaxial layer on a single crystalline substrate comprises heating a purified substrate in an epitaxy device while introducing organometallic precursors and a nitrogen-containing gas at a specified flow rate
JP3898537B2 (en) 2002-03-19 2007-03-28 日本電信電話株式会社 Nitride semiconductor thin film forming method and nitride semiconductor light emitting device
CN112366255B (en) * 2020-09-30 2021-12-07 华灿光电(浙江)有限公司 Light emitting diode epitaxial wafer and preparation method thereof

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0832112A (en) * 1994-07-20 1996-02-02 Toyoda Gosei Co Ltd Group iii nitride semiconductor light emitting element
EP0772249A2 (en) * 1995-11-06 1997-05-07 Nichia Chemical Industries, Ltd. Nitride semiconductor device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0832112A (en) * 1994-07-20 1996-02-02 Toyoda Gosei Co Ltd Group iii nitride semiconductor light emitting element
US5652438A (en) * 1994-07-20 1997-07-29 Toyoda Gosei Co., Ltd. Light-emitting semiconductor device using group III nitride compound
EP0772249A2 (en) * 1995-11-06 1997-05-07 Nichia Chemical Industries, Ltd. Nitride semiconductor device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
Inspec abstract number A9716-4255P-014 & Materials Science &Engineering B, Vol B43, no 1-3, p 265-8 *

Cited By (25)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8592841B2 (en) 1997-07-25 2013-11-26 Nichia Corporation Nitride semiconductor device
US6835956B1 (en) 1999-02-09 2004-12-28 Nichia Corporation Nitride semiconductor device and manufacturing method thereof
US6711191B1 (en) 1999-03-04 2004-03-23 Nichia Corporation Nitride semiconductor laser device
EP1189289A4 (en) * 1999-06-07 2008-01-16 Nichia Corp Nitride semiconductor device
USRE45672E1 (en) 1999-06-07 2015-09-22 Nichia Corporation Nitride semiconductor device
EP2309556A3 (en) * 1999-06-07 2012-04-04 Nichia Corporation Nitride semiconductor device
USRE42008E1 (en) 1999-06-07 2010-12-28 Nichia Corporation Nitride semiconductor device
EP1189289A1 (en) * 1999-06-07 2002-03-20 Nichia Corporation Nitride semiconductor device
US7646009B2 (en) 2000-07-07 2010-01-12 Nichia Corporation Nitride semiconductor device
US8309948B2 (en) 2000-07-07 2012-11-13 Nichia Corporation Nitride semiconductor device
US9444011B2 (en) 2000-07-07 2016-09-13 Nichia Corporation Nitride semiconductor device
US6586762B2 (en) 2000-07-07 2003-07-01 Nichia Corporation Nitride semiconductor device with improved lifetime and high output power
US9130121B2 (en) 2000-07-07 2015-09-08 Nichia Corporation Nitride semiconductor device
US7750337B2 (en) 2000-07-07 2010-07-06 Nichia Corporation Nitride semiconductor device
US7119378B2 (en) 2000-07-07 2006-10-10 Nichia Corporation Nitride semiconductor device
US8698126B2 (en) 2000-07-07 2014-04-15 Nichia Corporation Nitride semiconductor device
US6838693B2 (en) 2000-07-07 2005-01-04 Nichia Corporation Nitride semiconductor device
US7230263B2 (en) 2001-04-12 2007-06-12 Nichia Corporation Gallium nitride compound semiconductor element
US7667226B2 (en) 2001-11-05 2010-02-23 Nichia Corporation Semiconductor device
US7358522B2 (en) 2001-11-05 2008-04-15 Nichia Corporation Semiconductor device
WO2004051759A1 (en) * 2002-12-03 2004-06-17 Nec Corporation Semiconductor optical device having quantum well structure and its manufacturing method
US7479448B2 (en) 2002-12-03 2009-01-20 Nec Corporation Method of manufacturing a light emitting device with a doped active layer
EP2071638A4 (en) * 2006-08-08 2014-07-16 Svetlana Optoelektronika Semiconductor light-emitting heterostructure
EP2071638A1 (en) * 2006-08-08 2009-06-17 "Svetlana-Optoelektronika" Semiconductor light-emitting heterostructure
US7977687B2 (en) 2008-05-09 2011-07-12 National Chiao Tung University Light emitter device

Also Published As

Publication number Publication date
JPH10256601A (en) 1998-09-25
GB9805086D0 (en) 1998-05-06
SG63757A1 (en) 1999-03-30
DE19753470A1 (en) 1998-09-24

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