[go: up one dir, main page]

CN105429001B - Si/Ge superlattices quantum cascade laser and preparation method thereof - Google Patents

Si/Ge superlattices quantum cascade laser and preparation method thereof Download PDF

Info

Publication number
CN105429001B
CN105429001B CN201510726305.5A CN201510726305A CN105429001B CN 105429001 B CN105429001 B CN 105429001B CN 201510726305 A CN201510726305 A CN 201510726305A CN 105429001 B CN105429001 B CN 105429001B
Authority
CN
China
Prior art keywords
buffer layer
silicon
superlattices
quantum cascade
cascade laser
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.)
Active
Application number
CN201510726305.5A
Other languages
Chinese (zh)
Other versions
CN105429001A (en
Inventor
舒斌
吴继宝
古牧
范林西
陈景明
张鹤鸣
宣荣喜
胡辉勇
宋建军
王斌
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Xidian University
Original Assignee
Xidian University
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Xidian University filed Critical Xidian University
Priority to CN201510726305.5A priority Critical patent/CN105429001B/en
Publication of CN105429001A publication Critical patent/CN105429001A/en
Application granted granted Critical
Publication of CN105429001B publication Critical patent/CN105429001B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/3027IV compounds
    • H01S5/3031Si
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/34Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
    • H01S5/3427Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in IV compounds

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)

Abstract

The invention discloses a kind of Si/Ge superlattices quantum cascade laser and preparation method thereof, which successively includes silicon substrate, Si from the bottom up0.5Ge0.5Buffer layer, silicon and germanium super crystal lattice and SiO2, at the top of silicon and germanium super crystal lattice and Si0.5Ge0.5Aluminium electrode, Si are deposited on buffer layer0.5Ge0.5Buffer layer with a thickness of 300nm, the Si0.5Ge0.5The germanium intergrowth of silicon and 5nm that buffer layer is 5nm forms silicon and germanium super crystal lattice structure, the Si0.5Ge0.5The SiGe ratio of buffer layer is 1: 1.The present invention can either CMOS technique compatible, and can be realized demand of the germanium light source to different wavelengths of light, and photoelectric conversion efficiency with higher, photostability, the processing is simple, conveniently, to realize that on piece light source provides a specific structure and embodiment.

Description

Si/Ge超晶格量子级联激光器及其制备方法Si/Ge superlattice quantum cascade laser and its fabrication method

技术领域technical field

本发明涉及半导体光电子领域,具体涉及一种Si/Ge超晶格量子级联激光器及其制备方法。The invention relates to the field of semiconductor optoelectronics, in particular to a Si/Ge superlattice quantum cascade laser and a preparation method thereof.

背景技术Background technique

随着技术要求日益提高,信息处理硬件的微细加工的极限开始显现出来,束缚了技术的日益发展。在过去的几十年发展中,微电子工艺一直按照摩尔定律进步着。进步的最显著特点就是工艺尺寸越来越小,集成度越来越高,成本越来越低。但是,随着微电子工艺尺寸向纳米级前进,各种物理效应带来的瓶颈也越来越明显。为了突破瓶颈,研究人员们把目光集中在了将微电子与光电子技术相结合的领域上,这就是光电集成(OEIC)。As technical requirements increase day by day, the limits of microfabrication of information processing hardware begin to emerge, hampering the ever-increasing development of technology. Over the past few decades, microelectronics technology has been advancing in accordance with Moore's Law. The most notable feature of progress is that the process size is getting smaller and smaller, the integration level is getting higher and higher, and the cost is getting lower and lower. However, as the size of the microelectronics process advances to the nanoscale, the bottleneck brought by various physical effects is becoming more and more obvious. To break through the bottleneck, the researchers focused on the field of combining microelectronics with optoelectronics, which is called optoelectronic integration (OEIC).

Intel、IBM等半导体巨头的不懈努力,硅光电子技术的诸多关键器件得以在集成电路平台上实现,包括高速硅光调制器、探测器和波导元件都得到了突破。然而由于硅是间接带隙材料导致难以实现直接发光,故片上光源没有得到实现,这是硅光子技术一直以来所面临的最大难题。With the unremitting efforts of semiconductor giants such as Intel and IBM, many key devices of silicon optoelectronic technology have been realized on the integrated circuit platform, including breakthroughs in high-speed silicon optical modulators, detectors and waveguide components. However, since silicon is an indirect bandgap material, it is difficult to achieve direct light emission, so the on-chip light source has not been realized, which is the biggest problem that silicon photonics technology has always faced.

硅基光通信和光电集成技术迫切要求在低造价的情况下得到高效集成激光光源。到目前为止,硅芯片上的激光仍然依靠III-V材料生长或者键合到硅片上。这会产生稳定性问题,并且不利于工业大批量生产和制造。在硅片上外延的III-V激光器在寿命上受到限制,并且其制造工艺相当复杂。当键合III-V激光器到硅片上时由于在硅和III-V材料之间失配问题而受到限制。更进一步地说,相对硅CMOS技术来说,III-V激光器的产出是相当低的。Silicon-based optical communication and optoelectronic integration technologies urgently require high-efficiency integrated laser light sources at low cost. So far, lasers on silicon chips have relied on III-V materials grown or bonded to silicon wafers. This creates stability issues and is not conducive to industrial mass production and manufacturing. III-V lasers epitaxial on silicon wafers are limited in lifetime and are quite complex to manufacture. When bonding III-V lasers to silicon wafers are limited due to mismatch issues between silicon and III-V materials. Furthermore, the yield of III-V lasers is quite low relative to silicon CMOS technology.

发明内容SUMMARY OF THE INVENTION

为解决上述问题,本发明提供了一种Si/Ge超晶格量子级联激光器及其制备方法,既能够兼容CMOS工艺,又能够实现锗光源对不同波长光的需求,且具有较高的光电转换效率,光稳定性,加工简单、方便,为实现片上光源提供一个具体的结构和实施方案。In order to solve the above problems, the present invention provides a Si/Ge superlattice quantum cascade laser and a preparation method thereof, which are not only compatible with CMOS technology, but also can meet the requirements of germanium light sources for light of different wavelengths, and have higher optoelectronic properties. Conversion efficiency, light stability, simple and convenient processing, provide a specific structure and implementation scheme for realizing on-chip light sources.

为实现上述目的,本发明采取的技术方案为:To achieve the above object, the technical scheme adopted in the present invention is:

一种Si/Ge超晶格量子级联激光器,从下往上依次包括硅衬底、Si0.5Ge0.5缓冲层、硅锗超晶格和SiO2,硅锗超晶格和SiO2,两侧分别对称沉积有铝电极。A Si/Ge superlattice quantum cascade laser, from bottom to top, comprises a silicon substrate, a Si 0.5 Ge 0.5 buffer layer, a silicon germanium superlattice and SiO 2 , a silicon germanium superlattice and SiO 2 . Aluminum electrodes are deposited symmetrically, respectively.

本发明还提供了上述Si/Ge超晶格量子级联激光器的制备方法,包括以下步骤:The present invention also provides a preparation method of the above-mentioned Si/Ge superlattice quantum cascade laser, comprising the following steps:

S1、420℃温度条件下,通过低分子束外延法在硅衬底上生长厚度为300nm的Si0.5Ge0.5缓冲层;A Si 0.5 Ge 0.5 buffer layer with a thickness of 300 nm was grown on a silicon substrate by low molecular beam epitaxy at S1 and 420°C;

S2、420℃温度条件下,通过低温分子束外延法在所得的Si0.5Ge0.5缓冲层上生长厚度为5nm的Ge材料;Under the conditions of S2 and 420℃, a Ge material with a thickness of 5nm was grown on the obtained Si 0.5 Ge 0.5 buffer layer by low temperature molecular beam epitaxy;

S3、420℃温度条件下,通过低温分子束外延法在所得的Ge材料上生长厚度为5nm的Si材料;At S3 and 420°C, a Si material with a thickness of 5 nm was grown on the obtained Ge material by low temperature molecular beam epitaxy;

S4、520℃温度条件下,通过低温分子束外延法在所得的Si材料上生长厚度为5nm的Ge材料;Under the conditions of S4 and 520℃, a Ge material with a thickness of 5nm was grown on the obtained Si material by low temperature molecular beam epitaxy;

S5、重复步骤S3和步骤S4,得到10-30层的Si/Ge;S5, repeating steps S3 and S4 to obtain 10-30 layers of Si/Ge;

S6、900℃温度条件下,通过湿氧氧化在步骤S5所得的结构上生长一层大于150nm的SiO2S6, under the temperature condition of 900°C, grow a layer of SiO 2 larger than 150 nm on the structure obtained in step S5 by wet oxygen oxidation;

S7、通过金属蒸发工艺在所得的Si/Ge和SiO2两侧沉积铝电极,得Si/Ge超晶格量子级联激光器。S7, depositing aluminum electrodes on both sides of the obtained Si/Ge and SiO 2 by a metal evaporation process to obtain a Si/Ge superlattice quantum cascade laser.

其中,所述硅锗缓冲层为5nm的硅和5nm的锗交互生长形成硅锗超晶格结构。Wherein, the silicon germanium buffer layer is a silicon germanium superlattice structure formed by alternating growth of 5 nm silicon and 5 nm germanium.

其中,所述的Si0.5Ge0.5缓冲层的硅锗比例为1∶1。Wherein, the Si 0.5 Ge 0.5 buffer layer has a silicon germanium ratio of 1:1.

其中,所述铝电极从下至上依次为钛、铝,工艺条件为,钛层厚度为20nm,生长速度为铝层厚度为130nm,10nm内生长速率为10nm到130nm内生长速率为 Wherein, the aluminum electrodes are titanium and aluminum in order from bottom to top, and the process conditions are that the thickness of the titanium layer is 20 nm, and the growth rate is The thickness of the aluminum layer is 130 nm, and the growth rate within 10 nm is The growth rate within 10nm to 130nm is

本发明具有以下有益效果:The present invention has the following beneficial effects:

既能够兼容CMOS工艺,又能够实现锗光源对不同波长光的需求,且具有较高的光电转换效率,光稳定性,加工简单、方便,为实现片上光源提供一个具体的结构和实施方案。It can not only be compatible with CMOS technology, but also meet the requirements of germanium light sources for light of different wavelengths, and has high photoelectric conversion efficiency, light stability, simple and convenient processing, and provides a specific structure and implementation scheme for realizing on-chip light sources.

附图说明Description of drawings

图1为本发明实施例中步骤S1的加工意义图。FIG. 1 is a processing meaning diagram of step S1 in an embodiment of the present invention.

图2为本发明实施例中步骤S2的加工示意图。FIG. 2 is a schematic view of the processing of step S2 in the embodiment of the present invention.

图3为本发明实施例中步骤S3的加工示意图。FIG. 3 is a schematic view of the processing of step S3 in the embodiment of the present invention.

图4为本发明实施例中的硅锗超级晶格结构。FIG. 4 is a silicon germanium superlattice structure in an embodiment of the present invention.

图5为本发明实施例中步骤S5的加工示意图。FIG. 5 is a schematic view of the processing of step S5 in the embodiment of the present invention.

图6为本发明实施例中步骤S6的加工示意图。FIG. 6 is a schematic view of the processing of step S6 in the embodiment of the present invention.

图7为本发明实施例中步骤S7的加工示意图。FIG. 7 is a schematic view of the processing of step S7 in the embodiment of the present invention.

具体实施方式Detailed ways

为了使本发明的目的及优点更加清楚明白,以下结合实施例对本发明进行进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。In order to make the objects and advantages of the present invention more clear, the present invention will be further described in detail below with reference to the embodiments. It should be understood that the specific embodiments described herein are only used to explain the present invention, but not to limit the present invention.

本发明实施例提供了一种Si/Ge超晶格量子级联激光器,从下往上依次包括硅衬底、Si0.5Ge0.5缓冲层、硅锗超晶格和SiO2,硅锗超晶格和SiO2,两侧分别对称沉积有铝电极。The embodiment of the present invention provides a Si/Ge superlattice quantum cascade laser, which includes a silicon substrate, a Si 0.5 Ge 0.5 buffer layer, a silicon germanium superlattice and SiO 2 , a silicon germanium superlattice, in order from bottom to top. and SiO 2 , and aluminum electrodes are deposited symmetrically on both sides, respectively.

如图1-7所示,本发明实施例还提供了一种Si/Ge超晶格量子级联激光器的制备方法,包括以下步骤:As shown in Figures 1-7, an embodiment of the present invention also provides a preparation method of a Si/Ge superlattice quantum cascade laser, including the following steps:

S1、420℃温度条件下,通过低分子束外延法在硅衬底上生长厚度为300nm的Si0.5Ge0.5缓冲层;所述硅锗缓冲层为5nm的硅和5nm的锗交互生长形成硅锗超晶格结构,硅锗比例为1∶1。At S1 and 420°C, a Si 0.5 Ge 0.5 buffer layer with a thickness of 300 nm is grown on a silicon substrate by low molecular beam epitaxy; the Si 0.5 Ge 0.5 buffer layer is 5 nm silicon and 5 nm germanium alternately grown to form silicon germanium Superlattice structure with a silicon germanium ratio of 1:1.

S2、420℃温度条件下,通过低温分子束外延法在所得的Si0.5Ge0.5缓冲层上生长厚度为5nm的Ge材料;Under the conditions of S2 and 420℃, a Ge material with a thickness of 5nm was grown on the obtained Si 0.5 Ge 0.5 buffer layer by low temperature molecular beam epitaxy;

S3、520℃温度条件下,通过低温分子束外延法在所得的Ge材料上生长厚度为5nm的Si材料;At S3 and 520°C, a Si material with a thickness of 5 nm was grown on the obtained Ge material by a low temperature molecular beam epitaxy method;

S4、420℃温度条件下,通过低温分子束外延法在所得的Si材料上生长厚度为5nm的Ge材料;Under the temperature conditions of S4 and 420 °C, a Ge material with a thickness of 5 nm is grown on the obtained Si material by a low temperature molecular beam epitaxy method;

S5、重复步骤S3和步骤S4,得到10-30层的Si/Ge;S5, repeating steps S3 and S4 to obtain 10-30 layers of Si/Ge;

S6、900℃温度条件下,通过湿氧氧化在步骤S5所得的结构上生长一层大于150nm的SiO2S6, under the temperature condition of 900°C, grow a layer of SiO 2 larger than 150 nm on the structure obtained in step S5 by wet oxygen oxidation;

S7、通过金属蒸发工艺在所得的Si/Ge和SiO2两侧沉积铝电极,得Si/Ge超晶格量子级联激光器。所述铝电极从下至上依次为钛、铝,工艺条件为,钛层厚度为20nm,生长速度为铝层厚度为130nm,10nm内生长速率为10nm到130nm内生长速率为 S7, depositing aluminum electrodes on both sides of the obtained Si/Ge and SiO 2 by a metal evaporation process to obtain a Si/Ge superlattice quantum cascade laser. The aluminum electrodes are titanium and aluminum in order from bottom to top, and the process conditions are that the thickness of the titanium layer is 20 nm, and the growth rate is The thickness of the aluminum layer is 130 nm, and the growth rate within 10 nm is The growth rate within 10nm to 130nm is

以上所述仅是本发明的优选实施方式,应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以作出若干改进和润饰,这些改进和润饰也应视为本发明的保护范围。The above are only the preferred embodiments of the present invention. It should be pointed out that for those skilled in the art, without departing from the principles of the present invention, several improvements and modifications can be made, and these improvements and modifications should also be It is regarded as the protection scope of the present invention.

Claims (5)

1. a kind of preparation method of Si/Ge superlattices quantum cascade laser, which comprises the following steps:
Under the conditions of S1,420 DEG C of temperature, pass through the low molecule beam epitaxy methods Si that growth thickness is 300nm on a silicon substrate0.5Ge0.5 Buffer layer;
Under the conditions of S2,420 DEG C of temperature, by low temperature molecular beam epitaxy method in resulting Si0.5Ge0.5Growth thickness is on buffer layer The Ge material of 5nm;
Under the conditions of S3,420 DEG C of temperature, by low temperature molecular beam epitaxy method on resulting Ge material growth thickness be 5nm Si Material;
Under the conditions of S4,520 DEG C of temperature, by low temperature molecular beam epitaxy method on resulting Si material growth thickness be 5nm Ge Material;
S5, step S3 and step S4 is repeated, obtains 10-30 layers of Si/Ge;
Under the conditions of S6,900 DEG C of temperature, one layer is grown in the resulting structure of step S5 by wet-oxygen oxidation greater than 150nm's SiO2
S7, by evaporation of metal technique at the top of resulting silicon and germanium super crystal lattice and Si0.5Ge0.5Aluminium electrode is deposited on buffer layer, is obtained Si/Ge superlattices quantum cascade laser.
2. the preparation method of Si/Ge superlattices quantum cascade laser according to claim 1, which is characterized in that described Si0.5Ge0.5The germanium intergrowth of silicon and 5nm that buffer layer is 5nm forms silicon and germanium super crystal lattice structure.
3. the preparation method of Si/Ge superlattices quantum cascade laser according to claim 1, it is characterized in that, it is described Si0.5Ge0.5The SiGe ratio of buffer layer is 1: 1.
4. the preparation method of Si/Ge superlattices quantum cascade laser according to claim 1, it is characterized in that, it is described Aluminium electrode sequentially consists of titanium, aluminium, and process conditions are that titanium layer is with a thickness of 20nm, the speed of growthAluminium layer is thick Degree is 130nm, and growth rate is in 10nmGrowth rate is in 10nm to 130nm
5. a kind of preparation method based on claim 1-4 any one Si/Ge superlattices quantum cascade laser is prepared Si/Ge superlattices quantum cascade laser, which is characterized in that from the bottom up successively include silicon substrate, Si0.5Ge0.5Buffer layer, Silicon and germanium super crystal lattice and SiO2, at the top of silicon and germanium super crystal lattice and Si0.5Ge0.5Aluminium electrode is deposited on buffer layer.
CN201510726305.5A 2015-10-27 2015-10-27 Si/Ge superlattices quantum cascade laser and preparation method thereof Active CN105429001B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201510726305.5A CN105429001B (en) 2015-10-27 2015-10-27 Si/Ge superlattices quantum cascade laser and preparation method thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201510726305.5A CN105429001B (en) 2015-10-27 2015-10-27 Si/Ge superlattices quantum cascade laser and preparation method thereof

Publications (2)

Publication Number Publication Date
CN105429001A CN105429001A (en) 2016-03-23
CN105429001B true CN105429001B (en) 2019-06-25

Family

ID=55507019

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201510726305.5A Active CN105429001B (en) 2015-10-27 2015-10-27 Si/Ge superlattices quantum cascade laser and preparation method thereof

Country Status (1)

Country Link
CN (1) CN105429001B (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107017556B (en) * 2017-04-10 2019-12-13 北京工业大学 Quantum cascade laser based on multilayer two-dimensional material heterojunction
CN109449757B (en) * 2018-09-17 2019-10-29 西安电子科技大学 SiGe/Ge/SiGe double heterojunection laser and preparation method thereof
CN111446618B (en) * 2020-02-27 2021-03-05 电子科技大学 A three-terminal figure 8 ring quantum cascade laser
CN114914784A (en) * 2022-05-23 2022-08-16 南京大学 Silicon-based interband cascade laser structure, laser and preparation method thereof

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4959694A (en) * 1987-12-23 1990-09-25 British Telecommunications Public Limited Company Semiconductor heterostructures with SiGe material
US5442205A (en) * 1991-04-24 1995-08-15 At&T Corp. Semiconductor heterostructure devices with strained semiconductor layers

Family Cites Families (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5548128A (en) * 1994-12-14 1996-08-20 The United States Of America As Represented By The Secretary Of The Air Force Direct-gap germanium-tin multiple-quantum-well electro-optical devices on silicon or germanium substrates
EP2264794B1 (en) * 1997-01-09 2014-11-19 Nichia Corporation Nitride semiconductor device
US6154475A (en) * 1997-12-04 2000-11-28 The United States Of America As Represented By The Secretary Of The Air Force Silicon-based strain-symmetrized GE-SI quantum lasers
US7919791B2 (en) * 2002-03-25 2011-04-05 Cree, Inc. Doped group III-V nitride materials, and microelectronic devices and device precursor structures comprising same
US6621841B1 (en) * 2002-04-23 2003-09-16 The United States Of America As Represented By The Secretary Of The Air Force Phonon-pumped semiconductor lasers
US7596158B2 (en) * 2005-10-28 2009-09-29 Massachusetts Institute Of Technology Method and structure of germanium laser on silicon
US7776642B2 (en) * 2008-05-15 2010-08-17 Wisconsin Alumni Research Foundation Quantum-well photoelectric device assembled from nanomembranes
CN102227046A (en) * 2011-05-25 2011-10-26 北京化工大学 GaN-based semiconductor laser and manufacturing method thereof
JP5544574B2 (en) * 2011-08-02 2014-07-09 独立行政法人理化学研究所 Quantum cascade laser device
CN202586076U (en) * 2012-05-28 2012-12-05 中国电子科技集团公司第十三研究所 Multi-laminated tunnel cascade semiconductor laser

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4959694A (en) * 1987-12-23 1990-09-25 British Telecommunications Public Limited Company Semiconductor heterostructures with SiGe material
US5442205A (en) * 1991-04-24 1995-08-15 At&T Corp. Semiconductor heterostructure devices with strained semiconductor layers

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
在Ge和SiGe复合缓冲层上生长高质量Ge/Si超晶格;盛篪;《半导体学报》;19960131;第17卷(第1期);全文
锗/硅应变层超晶格及其应用;戴瑛;《山东工业大学学报》;19931231;第23卷(第2期);全文
锗/硅短周期超晶格的X射线双晶衍射研究;季振国;《浙江大学学报》;20010131;第35卷(第1期);全文

Also Published As

Publication number Publication date
CN105429001A (en) 2016-03-23

Similar Documents

Publication Publication Date Title
CN104993025B (en) Silicon nitride film causes infrared LED device and preparation method thereof in the germanium tin strained
Qi et al. Photonics and optoelectronics of 2D metal‐halide perovskites
Ni et al. Silicon nanocrystals: unfading silicon materials for optoelectronics
Huang et al. Ultraviolet optoelectronic devices based on AlGaN-SiC platform: Towards monolithic photonics integration system
Seo et al. Low dimensional freestanding semiconductors for flexible optoelectronics: materials, synthesis, process, and applications
Zhang et al. Controlled synthesis and photonics applications of metal halide perovskite nanowires
Woo et al. Effect of twinning on the photoluminescence and photoelectrochemical properties of indium phosphide nanowires grown on silicon (111)
CN105429001B (en) Si/Ge superlattices quantum cascade laser and preparation method thereof
JP5929115B2 (en) Semiconductor nanodevice
EP3551788A1 (en) Method for integrating two-dimensional materials on a nanostructured substrate, suspended thin film of two-dimensional materials and uses thereof
JP2011519730A (en) Superlattice / Quantum well nanowire
Tamirat The role of nanotechnology in semiconductor industry: Review article
CN105624792B (en) A kind of silicon substrate GaAs monocrystal thin films and preparation method thereof
Ai et al. Recent advances of photodetection technology based on main group III–V semiconductors
TW201331990A (en) Hybrid photoelectric element
Tchoe et al. Vertical monolithic integration of wide-and narrow-bandgap semiconductor nanostructures on graphene films
Abrand et al. Localized self-assembly of InAs nanowire arrays on reusable Si substrates for substrate-free optoelectronics
Shim et al. VLS homoepitaxy of lead iodide nanowires for hybrid perovskite conversion
Laukkanen et al. Bridging the gap between surface physics and photonics
CN103579902A (en) Method for manufacturing silicon substrate microcavity laser device
CN103151710A (en) Gallium arsenide (GaAs) base high-strain quantum well containing boron (B) and preparation method thereof and semiconductor laser unit
CN104037275B (en) Silicon nitride film-induced germanium LED device with suspended structure and preparation method thereof
JP4824270B2 (en) Semiconductor substrate
CN112670157A (en) Process for the heterogeneous integration of a semiconductor material of interest on a silicon substrate
CN111584657A (en) Semiconductor material, preparation method and application thereof, laser and photoelectric detector

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant