Ion Beam Processed Ir/SiGe Structures

1995 ◽  
Vol 402 ◽  
Author(s):  
G. Curello ◽  
R. Gwilllam ◽  
M. Harry ◽  
B. J. Sealy ◽  
T. Rodriguez ◽  
...  
Keyword(s):  
Rutherford Backscattering Spectrometry ◽  
Ion Beam ◽  
Electron Beam Evaporation ◽  
Thermal Reaction ◽  
The Other ◽  
Cross Sectional ◽  
Interface Quality ◽  
Boundary Mixing ◽  
Transmission Electron ◽  
20 Nm

AbstractThe thermal reaction of Ir/SiGe structures following ion implantation induced Ir grain boundary mixing has been studied. The morphology of the final interface has been investigated by Cross-sectional Transmission Electron Microscopy (XTEM) and Rutherford Backscattering Spectrometry (RBS) has been used to detect the redistribution of constituent atoms in the reacted layers. A 20 nm iridium film was deposited in vacuum by electron beam evaporation onto p-Si1-xGex (x = 0.25, 0.33) fully relaxed MBE grown layers. Implantation conditions used were effective in amorphizing the interface-close region of the Ir film and the SiGe substrate. After regrowth, XTEM results show that the interface quality is improved with respect to the material that had not been implanted. RBS results on the other hand show Ge incorporation in the reacted layer to occur in contrast to the non implated case where the Ge piles up at the silicide/SiGe interface. The effect of a second anneal step at higher temperatures (in the range 800°C – 900°C) is also investigated.

Ion Beam Synthesis of IrSi3 by 1-MeV Ir Ion Implantation into Si(111)

1993 ◽  
Vol 320 ◽  
Author(s):  
T. P. Sjoreen ◽  
H.- J. Hinneberg
Keyword(s):  
Ion Implantation ◽  
Rutherford Backscattering Spectrometry ◽  
Ion Beam ◽  
Processing Parameters ◽  
Cross Sectional ◽  
Ion Channeling ◽  
Transmission Electron ◽  
Nearly Continuous ◽  
Substrate Temperatures ◽  
Different Doses

ABSTRACTThe formation of a Si/IrSi3/Si heterostructurie by 1-MeV Ir ion implantation and subsequent annealing has been studied for different doses (0.1-2.25 × 1017 Ir/cm2), substrate temperatures (450°-600°C) and annealing temperatures (1000°-1200°C) using Rutherford backscattering spectrometry, ion channeling and cross-sectional transmission electron microscopy. The heterostructure formation is observed to depend strongly on the processing conditions. The best structure, nearly continuous and precipitate-free, is obtained by implanting 1.8-2.0× 1017 1r/cm2 at a substrate temperature of 550°C and annealing at 1100°C for 5 h. A stoichiometric IrSi3 layer can also be produced by furnace annealing at 1150°C for 1 h or by rapid-thermal-annealing at 1200°C for 3 min. Other substrate temperatures generally lead to a structure with a discontinuous IrSi3 layer frequently interrupted by large surface precipitates or islands. The origin of these islands, as well as the dependence of the heterostructure on processing parameters, is discussed.

Titanium Silicidation and Secondary Defect Annihilation in ION Beam Processed Sige Layers

1995 ◽  
Vol 402 ◽  
Author(s):  
K. Kyllesbech Larsen ◽  
F. La Via ◽  
S. Lombardo ◽  
V. Raineri ◽  
R. A. Donaton ◽  
...  
Keyword(s):  
Rutherford Backscattering Spectrometry ◽  
Ion Beam ◽  
Process Conditions ◽  
High Dose ◽  
Silicide Phase ◽  
X Ray Diffraction ◽  
Implantation Energy ◽  
Transmission Electron ◽  
Secondary Defect ◽  
20 Nm

AbstractThe secondary defect annihilation by one- and two-step titanium silicidation in SiGe layers, formed by high dose Ge implantation, has been studied systematically as a function of the Ge fluence, implantation energy, silicide thickness, and silicide process conditions. In all cases the Ti thickness was kept below 20 nm, resulting in very thin Ti silicide layers typically less than 40 nm. The silicide phase was inspected by x-ray diffraction and transmission electron diffraction. Channelling Rutherford backscattering spectrometry and transmission electron microscopy were used to follow the end of range dislocation loop annihilation as a function of the silicide process conditions. The end of range loop annealing and the influence of silicidation is presented in this paper for Ge fluences above 3×1015 cm−2 and energies ranging from 70 keV to 140 keV. A model based on loop coarsening is presented which describes the observed loop annihilation behaviour.

Ion Beam Synthesis of IrSi3 by 1-MeV Ir Ion Implantation into Si(111)

1993 ◽  
Vol 316 ◽  
Author(s):  
T. P. Sjoreen ◽  
H.-J. Hinneberg
Keyword(s):  
Ion Implantation ◽  
Rutherford Backscattering Spectrometry ◽  
Ion Beam ◽  
Processing Parameters ◽  
Cross Sectional ◽  
Ion Channeling ◽  
Transmission Electron ◽  
Nearly Continuous ◽  
Substrate Temperatures ◽  
Different Doses

ABSTRACTThe formation of a Si/IrSi3/Si heterostructure by 1-MeV Ir ion implantation and subsequent annealing has been studied for different doses (0.1-2.25 × 1017 Ir/cm2), substrate temperatures (450°-600°C) and annealing temperatures (1000°-1200°C) using Rutherford backscattering spectrometry, ion channeling and cross-sectional transmission electron microscopy. The heterostructure formation is observed to depend strongly on the processing conditions. The best structure, nearly continuous and precipitate-free, is obtained by implanting 1.8-2.0 × 1017 Ir/cm2 at a substrate temperature of 550°C and annealing at 1100°C for 5 h. A stoichiometric IrSi3 layer can also be produced by furnace annealing at 1150°C for 1 h or by rapid-thermal-annealing at 1200°C for 3 min. Other substrate temperatures generally lead to a structure with a discontinuous IrSi3 layer frequently interrupted by large surface precipitates or islands. The origin of these islands, as well as the dependence of the heterostructure on processing parameters, is discussed.

TEM Study of Co/Pd and Co/Au Multilayers

1993 ◽  
Vol 51 ◽  
pp. 1036-1037
Author(s):  
A.E.M. De Veirman ◽  
F.J.G. Hakkens ◽  
W.M.J. Coene ◽  
F.J.A. den Broeder
Keyword(s):  
Magnetic Anisotropy ◽  
Ion Beam ◽  
Perpendicular Magnetic Anisotropy ◽  
Optical Recording ◽  
Magnetic Multilayer ◽  
Ion Beam Sputtering ◽  
Cross Sectional ◽  
Transmission Electron ◽  
Beam Sputtering ◽  
Substrate Temperatures

There is currently great interest in magnetic multilayer (ML) thin films (see e.g.), because they display some interesting magnetic properties. Co/Pd and Co/Au ML systems exhibit perpendicular magnetic anisotropy below certain Co layer thicknesses, which makes them candidates for applications in the field of magneto-optical recording. It has been found that the magnetic anisotropy of a particular system strongly depends on the preparation method (vapour deposition, sputtering, ion beam sputtering) as well as on the substrate, underlayer and deposition temperature. In order to get a better understanding of the correlation between microstructure and properties a thorough cross-sectional transmission electron microscopy (XTEM) study of vapour deposited Co/Pd and Co/Au (111) MLs was undertaken (for more detailed results see ref.).The Co/Pd films (with fixed Pd thickness of 2.2 nm) were deposited on mica substrates at substrate temperatures Ts of 20°C and 200°C, after prior deposition of a 100 nm Pd underlayer at 450°C.

Low Energy Ar Ion Milling of FIB TEM Specimens from 14 nm and Future FinFET Technologies

2018 ◽  
Author(s):  
C.S. Bonifacio ◽  
P. Nowakowski ◽  
M.J. Campin ◽  
M.L. Ray ◽  
P.E. Fischione
Keyword(s):  
Field Effect Transistor ◽  
Focused Ion Beam ◽  
Ion Beam ◽  
Specimen Preparation ◽  
Ion Milling ◽  
Transmission Electron ◽  
High Resolution Tem ◽  
Effect Transistor ◽  
20 Nm ◽  
Argon Ion

Abstract Transmission electron microscopy (TEM) specimens are typically prepared using the focused ion beam (FIB) due to its site specificity, and fast and accurate thinning capabilities. However, TEM and high-resolution TEM (HRTEM) analysis may be limited due to the resulting FIB-induced artifacts. This work identifies FIB artifacts and presents the use of argon ion milling for the removal of FIB-induced damage for reproducible TEM specimen preparation of current and future fin field effect transistor (FinFET) technologies. Subsequently, high-quality and electron-transparent TEM specimens of less than 20 nm are obtained.

TEM Sample Preparation Tricks for Advanced DRAMs

2015 ◽  
Author(s):  
Ching Shan Sung ◽  
Hsiu Ting Lee ◽  
Jian Shing Luo
Keyword(s):  
Electron Microscopy ◽  
Transmission Electron Microscopy ◽  
Sample Preparation ◽  
Integrated Circuit ◽  
Focused Ion Beam ◽  
Ion Beam ◽  
Tem Analysis ◽  
Cross Sectional ◽  
Transmission Electron ◽  
Characterization Of Materials

Abstract Transmission electron microscopy (TEM) plays an important role in the structural analysis and characterization of materials for process evaluation and failure analysis in the integrated circuit (IC) industry as device shrinkage continues. It is well known that a high quality TEM sample is one of the keys which enables to facilitate successful TEM analysis. This paper demonstrates a few examples to show the tricks on positioning, protection deposition, sample dicing, and focused ion beam milling of the TEM sample preparation for advanced DRAMs. The micro-structures of the devices and samples architectures were observed by using cross sectional transmission electron microscopy, scanning electron microscopy, and optical microscopy. Following these tricks can help readers to prepare TEM samples with higher quality and efficiency.

Iridium Silicides Formation on High Doses Ge+ Implanted Si Layers

1995 ◽  
Vol 402 ◽  
Author(s):  
G. Curello ◽  
R. Gwilliam ◽  
M. Harry ◽  
R. J. Wilson ◽  
B. J. Sealy ◽  
...  
Keyword(s):  
Low Dose ◽  
Rutherford Backscattering Spectrometry ◽  
Solid Phase ◽  
Strain Relaxation ◽  
Sige Layer ◽  
Thermal Reaction ◽  
High Dose ◽  
Cross Sectional ◽  
Projected Range

AbstractIn this work iridium silicidation of high dose Ge+ implanted Si layers has been studied. Compositional graded SiGe layers with a Ge peak concentration between 6 at.% and 12 at.% have been fabricated using 200 keV Ge+ ion implantation into (100) Si. A 20 nm thick Ir film was then deposited by e-beam evaporation with thermal reaction being performed to both regrow the implantation damage and form the silicide. The crystal quality of the SiGe layer and its interaction with the Ir film have been studied by cross-sectional Transmission Electron Microscopy (XTEM) and Rutherford Backscattering Spectrometry (RBS).Solid Phase Epitaxial Growth (SPEG) in the low dose case has produced a defect free SiGe layer with the formation of the IrSi phase. The annealing ambient was found to be critical for the silicidation. For the high dose case, as expected, strain relaxation related defects were observed to nucleate at a depth close to the projected range of the Ge+ implant and to extend up to the surface. A second rapid thermal annealing at higher temperatures, performed in forming gas, consumed most of the defective layer moving the silicide interface closer to the peak of the Ge distribution. A second low dose Ge+ implant following the metal deposition has been found to have a beneficial effect on the quality of the final interface. An amorphizing 500 keV Si+ implant followed by SPEG has finally been used to move the end of range defects far from the interface.

scholarly journals Nanocrystalline Porous Hydrogen Storage Based on Vanadium and Titanium Nitrides

2017 ◽  
Vol 2017 ◽  
pp. 1-10 ◽  
Author(s):  
A. Goncharov ◽  
A. Guglya ◽  
A. Kalchenko ◽  
E. Solopikhina ◽  
V. Vlasov ◽  
...  
Keyword(s):  
Grain Boundaries ◽  
Electrical Resistance ◽  
Ion Beam ◽  
Hydrogen Desorption ◽  
Titanium Nitrides ◽  
Ion Beam Assisted Deposition ◽  
Transmission Electron ◽  
Mixed Beam ◽  
20 Nm ◽  
Absorption Characteristics

This review summarizes results of our study of the application of ion-beam assisted deposition (IBAD) technology for creation of nanoporous thin-film structures that can absorb more than 6 wt.% of hydrogen. Data of mathematical modeling are presented highlighting the structure formation and component creation of the films during their deposition at the time of simultaneous bombardment by mixed beam of nitrogen and helium ions with energy of 30 keV. Results of high-resolution transmission electron microscopy revealed that VNxfilms consist of 150–200 nm particles, boundaries of which contain nanopores of 10–15 nm diameters. Particles themselves consist of randomly oriented 10–20 nm nanograins. Grain boundaries also contain nanopores (3–8 nm). Examination of the absorption characteristics of VNx, TiNx, and(V,Ti)Nxfilms showed that the amount of absorbed hydrogen depends very little on the chemical composition of films, but it is determined by the structure pore. The amount of absorbed hydrogen at 0.3 MPa and 20°C is 6-7 wt.%, whereas the bulk of hydrogen is accumulated in the grain boundaries and pores. Films begin to release hydrogen even at 50°C, and it is desorbed completely at the temperature range of 50–250°C. It was found that the electrical resistance of films during the hydrogen desorption increases 104times.

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