Nanothick Layer Transfer of Hydrogen-implanted Wafer Using Polysilicon Sacrificial Layer

2006 ◽  
Vol 921 ◽  
Author(s):  
C. H. Huang ◽  
C. L. Chang ◽  
Y. Y. Yang ◽  
T. Suryasindhu ◽  
W. -C. Liao ◽  
...  
Keyword(s):  
Ion Implantation ◽  
Silicon Wafer ◽  
Wafer Bonding ◽  
Sacrificial Layer ◽  
Silicon Layer ◽  
Bonding Layer ◽  
Transmission Electron ◽  
Nanostructure Material ◽  
Polysilicon Layer ◽  
Material Fabrication

AbstractAn ion implantation-wafer bonding-layer splitting based 2-D nanostructure material fabrication method using polysilicon sacrificial layer for forming nanothick SOI materials without using post-thinning processes is presented in this paper. Polysilicon layer was initially deposited on the thermal oxidized surface of silicon wafer prior to the ion implantation step to achieve the hydrogen-rich buried layer which depth from the top surface is less than 100 nm in the as-implanted silicon wafer. Before this as-implanted wafer being bonded with a handle wafer, the polysilicon layer was removed by a wet etching method. A nanothick silicon layer was then successfully transferred onto a handle wafer after wafer bonding and layer splitting steps. The thickness of the final transferred silicon layer was 100 nm measured by transmission electron microscopy (TEM).

Residual Ion Implantation Damage at Source/Drain Junctions of Excimer Laser Annealed Polycrystalline Silicon Thin Film Transistor

2002 ◽  
Vol 715 ◽  
Author(s):  
Kee-Chan Park ◽  
Jae-Shin Kim ◽  
Woo-Jin Nam ◽  
Min-Koo Han
Keyword(s):  
Thin Film ◽  
Ion Implantation ◽  
Excimer Laser ◽  
Polycrystalline Silicon ◽  
Thin Film Transistor ◽  
Silicon Layer ◽  
Silicon Thin Film ◽  
Cross Sectional ◽  
Implantation Damage ◽  
Transmission Electron

AbstractResidual ion implantation damage at source/drain junctions of excimer laser annealed polycrystalline silicon (poly-Si) thin film transistor (TFT) was investigated by high-resolution transmission electron microscopy (HR-TEM). Cross-sectional TEM observation showed that XeCl excimer laser (λ=308 nm) energy decreased considerably at the source/drain junctions of top-gated poly-Si TFT due to laser beam diffraction at the gate electrode edges and that the silicon layer amorphized by ion implantation, was not completely annealed at the juncions. The HR-TEM observation showed severe lattice disorder at the junctions of poly-Si TFT.

Interface Voids and Precipitates in GaAs Wafer Bonding

1999 ◽  
Vol 5 (S2) ◽  
pp. 748-749
Author(s):  
R.R. Vanfleet ◽  
M. Shverdin ◽  
Z.H. Zhu ◽  
Y.H. Lo ◽  
J. Silcox
Keyword(s):  
Wafer Bonding ◽  
Lattice Mismatch ◽  
Bonding Layer ◽  
Exact Nature ◽  
Transmission Electron ◽  
Scanning Transmission ◽  
Common Observation ◽  
Free Films ◽  
Substrate Defects ◽  
Electron Energy Loss

Wafer bonding allows the production of Compliant Universal substrates that are made by bonding a thin (< 10 nm) layer twisted ∼45 degrees to the underlying substrate. Subsequent growth on this twisted layer results in defect free films even when the growth material has a significant lattice mismatch with the substrate. Defects on the bonding interface are a common observation when bonding GaAs to many substrates, but the exact nature of these defects has not been clear. We have studied this bonding layer in GaAs-GaAs twist bonded structures by Scanning Transmission Electron Microscopy and Electron Energy Loss Spectroscopy and established that the defects are voids with a portion being partially filled with gallium. Two general sizes of voids are seen. The larger voids are approximately 45 nm in diameter and 22 nm in the wafer normal direction and are distributed in an approximately linear relationship.

Mechanisms of Low-Temperature Ti/Si-Based Wafer Bonding

2005 ◽  
Vol 863 ◽  
Author(s):  
Jian Yu ◽  
Yinmin Wang ◽  
Arthur W. Haberl ◽  
Hassa Bakhru ◽  
Jian-Qiang Lu ◽  
...  
Keyword(s):  
Silicon Wafer ◽  
Wafer Bonding ◽  
Rutherford Backscattering Spectrometry ◽  
Three Dimensional ◽  
Amorphous Layer ◽  
Bonding Interface ◽  
Native Oxide ◽  
Wafer Level ◽  
Transmission Electron ◽  
Strong Adhesion

AbstractThree-dimensional (3D) wafer-level integration is receiving increased attention with various wafer bonding approaches being evaluated. Recently, we explored an alternative lowtemperature Ti/Si-based wafer bonding, in which an oxidized silicon wafer was successfully bonded with a prime silicon wafer at 400°C using 30 nm sputtered Ti as adhesive. The bonded pairs show excellent bonding uniformity and mechanical integrity. Rutherford backscattering spectrometry (RBS) was applied to confirm the interdiffusion occurred in the interlayer. The bonding interface was examined by high-resolution transmission electron microscopy (HRTEM) assisted with electron energy loss spectroscopy (EELS) elemental mapping and energy dispersive X-ray spectroscopy (EDX). Characterization of the bonding interface indicates the strong adhesion achieved is attributed to an amorphous layer formed by interdiffusion of Si and oxygen into Ti interlayer and the unique ability to reduce native oxide (SiO2) by Ti even at low temperatures.

Wafer Bonding and Layer Transfer For Thin Film Ferroelectrics

2002 ◽  
Vol 748 ◽  
Author(s):  
Jennifer L. Ruglovsky ◽  
Young-Bae Park ◽  
Cecily A. Ryan ◽  
Harry A. Atwater
Keyword(s):  
Thin Film ◽  
Ion Implantation ◽  
Single Crystals ◽  
Wafer Bonding ◽  
Crystalline Silicon ◽  
Sacrificial Layer ◽  
Bubble Formation ◽  
Ferroelectric Materials ◽  
Silicon Substrates ◽  
Layer Transfer

ABSTRACTWe report on the layer transfer of thin ferroelectric materials onto silicon substrates. H+ and He+ ion implantation created a buried sacrificial layer in the c-cut BaTiO3 and LiNbO3 single crystals. Bubble formation and thermodynamics of cavity at the bonding interface have been investigated, and single crystal thin film layers were transferred onto crystalline silicon substrates. We have found that defects generated by ion implantation in ferroelectric materials can be significantly recovered with the subsequent annealing for layer splitting.

Bipolar Conduction across a Wafer Bonded p-n Si/SiC Heterojunction

2013 ◽  
Vol 740-742 ◽  
pp. 1006-1009 ◽  
Author(s):  
Peter M. Gammon ◽  
Amador Pérez-Tomás ◽  
Michael R. Jennings ◽  
Ana M. Sanchez ◽  
Craig A. Fisher ◽  
...  
Keyword(s):  
Wafer Bonding ◽  
Room Temperature ◽  
Anode Voltage ◽  
Silicon Layer ◽  
Turn On ◽  
Low Leakage ◽  
Low Leakage Current ◽  
Transmission Electron ◽  
P Type ◽  
Bipolar Conduction

This paper describes the physical and electrical properties of a p-n Si/on-axis SiC vertical heterojunction rectifier. A thin 400nm p-type silicon layer was wafer-bonded to a commercial on-axis SiC substrate by room temperature hydrophilic wafer bonding. Transmission electron microscopy was used to identify the crystallographic orientation as (0001)SiC//(001)Si and to reveal an amorphous interfacial layer. Electrical tests performed on the p-n heterodiodes revealed that, after an additional 1000oC anneal, the rectifier exhibit remarkably low leakage current (10nA/cm2 at an anode voltage of V=-6V), improved on-resistance due to bipolar injection and a turn-on voltage close to the p-n heterojunction theoretical value of 2.4V.

Interlayer mixing in GaAs/AlxGa1-xAs heterostructures as a result of Se+ ion implantation

1988 ◽  
Vol 46 ◽  
pp. 908-909
Author(s):  
E.G. Bithell ◽  
W.M. Stobbs
Keyword(s):  
Ion Implantation ◽  
Diffusion Coefficients ◽  
Dark Field ◽  
Atomic Mass ◽  
Composition Profile ◽  
Semiconductor Heterostructures ◽  
Transmission Electron ◽  
Microscope Images ◽  
Damage Process ◽  
Electron Energy Loss

It is well known that the microstructural consequences of the ion implantation of semiconductor heterostructures can be severe: amorphisation of the damaged region is possible, and layer intermixing can result both from the original damage process and from the enhancement of the diffusion coefficients for the constituents of the original composition profile. A very large number of variables are involved (the atomic mass of the target, the mass and energy of the implant species, the flux and the total dose, the substrate temperature etc.) so that experimental data are needed despite the existence of relatively well developed models for the implantation process. A major difficulty is that conventional techniques (e.g. electron energy loss spectroscopy) have inadequate resolution for the quantification of any changes in the composition profile of fine scale multilayers. However we have demonstrated that the measurement of 002 dark field intensities in transmission electron microscope images of GaAs / AlxGa1_xAs heterostructures can allow the measurement of the local Al / Ga ratio.

Dynamic studies of silicide-mediated crystallization of amorphous silicon

1992 ◽  
Vol 50 (2) ◽  
pp. 1352-1353
Author(s):  
C. Hayzelden ◽  
J. L. Batstone
Keyword(s):  
Ion Implantation ◽  
Solid Phase ◽  
Metallic Phase ◽  
Single Crystal Substrate ◽  
Free Electrons ◽  
Melt Temperature ◽  
Transmission Electron ◽  
Crystal Substrate ◽  
High Resolution Tem

Epitaxial reordering of amorphous Si(a-Si) on an underlying single-crystal substrate occurs well below the melt temperature by the process of solid phase epitaxial growth (SPEG). Growth of crystalline Si(c-Si) is known to be enhanced by the presence of small amounts of a metallic phase, presumably due to an interaction of the free electrons of the metal with the covalent Si bonds near the growing interface. Ion implantation of Ni was shown to lower the crystallization temperature of an a-Si thin film by approximately 200°C. Using in situ transmission electron microscopy (TEM), precipitates of NiSi2 formed within the a-Si film during annealing, were observed to migrate, leaving a trail of epitaxial c-Si. High resolution TEM revealed an epitaxial NiSi2/Si(l11) interface which was Type A. We discuss here the enhanced nucleation of c-Si and subsequent silicide-mediated SPEG of Ni-implanted a-Si.Thin films of a-Si, 950 Å thick, were deposited onto Si(100) wafers capped with 1000Å of a-SiO2. Ion implantation produced sharply peaked Ni concentrations of 4×l020 and 2×l021 ions cm−3, in the center of the films.

Analysis of Silicon-On-Insulator Structures Formed By Oxygen Ion Implantation

1985 ◽  
Vol 43 ◽  
pp. 300-301
Author(s):  
N. Lewis ◽  
E. L. Hall ◽  
A. Mogro-Campero ◽  
R. P. Love
Keyword(s):  
Ion Implantation ◽  
Single Crystal ◽  
Single Crystal Silicon ◽  
Silicon Layer ◽  
Device Fabrication ◽  
Silicon On Insulator ◽  
High Dose ◽  
Crystal Silicon ◽  
Oxygen Ion ◽  
Oxygen Ion Implantation

The formation of buried oxide structures in single crystal silicon by high-dose oxygen ion implantation has received considerable attention recently for applications in advanced electronic device fabrication. This process is performed in a vacuum, and under the proper implantation conditions results in a silicon-on-insulator (SOI) structure with a top single crystal silicon layer on an amorphous silicon dioxide layer. The top Si layer has the same orientation as the silicon substrate. The quality of the outermost portion of the Si top layer is important in device fabrication since it either can be used directly to build devices, or epitaxial Si may be grown on this layer. Therefore, careful characterization of the results of the ion implantation process is essential.

High-resolution transmission electron microscopic study of highly oxygen doped silicon layer

1989 ◽  
Vol 47 ◽  
pp. 692-693
Author(s):  
H. Takaoka ◽  
M. Tomita ◽  
T. Hayashi
Keyword(s):  
High Resolution ◽  
Oxygen Concentration ◽  
Silicon Layer ◽  
Detailed Structure ◽  
Electron Microscopic ◽  
Cross Sectional ◽  
Transmission Electron ◽  
Doped Silicon ◽  
Argon Ion

High resolution transmission electron microscopy (HRTEM) is the effective technique for characterization of detailed structure of semiconductor materials. Oxygen is one of the important impurities in semiconductors. Detailed structure of highly oxygen doped silicon has not clearly investigated yet. This report describes detailed structure of highly oxygen doped silicon observed by HRTEM. Both samples prepared by Molecular beam epitaxy (MBE) and ion implantation were observed to investigate effects of oxygen concentration and doping methods to the crystal structure.The observed oxygen doped samples were prepared by MBE method in oxygen environment on (111) substrates. Oxygen concentration was about 1021 atoms/cm3. Another sample was silicon of (100) orientation implanted with oxygen ions at an energy of 180 keV. Oxygen concentration of this sample was about 1020 atoms/cm3 Cross-sectional specimens of (011) orientation were prepared by argon ion thinning and were observed by TEM at an accelerating voltage of 400 kV.

TEM study of buried cobalt disilicide layers formed by ion implantation: Identification of cobalt monosilicide inclusions

1990 ◽  
Vol 48 (4) ◽  
pp. 576-577
Author(s):  
A. De Veirman ◽  
J. Van Landuyt ◽  
K.J. Reeson ◽  
R. Gwilliam ◽  
C. Jeynes ◽  
...  
Keyword(s):  
Ion Implantation ◽  
Annealing Treatment ◽  
Silicon On Insulator ◽  
High Dose ◽  
Nitrogen Flow ◽  
Cobalt Disilicide ◽  
Transmission Electron ◽  
Beam Heating ◽  
Co Concentration ◽  
Silicon On Insulator Technology

In analogy to the formation of SIMOX (Separation by IMplanted OXygen) material which is presently the most promising silicon-on-insulator technology, high-dose ion implantation of cobalt in silicon is used to synthesise buried CoSi2 layers. So far, for high-dose ion implantation of Co in Si, only formation of CoSi2 is reported. In this paper it will be shown that CoSi inclusions occur when the stoichiometric Co concentration is exceeded at the peak of the Co distribution. 350 keV Co+ ions are implanted into (001) Si wafers to doses of 2, 4 and 7×l017 per cm2. During the implantation the wafer is kept at ≈ 550°C, using beam heating. The subsequent annealing treatment was performed in a conventional nitrogen flow furnace at 1000°C for 5 to 30 minutes (FA) or in a dual graphite strip annealer where isochronal 5s anneals at temperatures between 800°C and 1200°C (RTA) were performed. The implanted samples have been studied by means of Rutherford Backscattering Spectroscopy (RBS) and cross-section Transmission Electron Microscopy (XTEM).

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