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May 2006

Volume 24, Issue 3, pp. 385-891

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Analysis of unstable species in cyclo-C4F8 plasma by ion attachment mass spectrometry

Megumi Nakamura, Yoshiki Hirano, Yoshiro Shiokawa, Masao Takayanagi, and Munetaka Nakata

J. Vac. Sci. Technol. A 24, 385 (2006); http://dx.doi.org/10.1116/1.2177228 (5 pages) | Cited 10 times

Online Publication Date: 20 April 2006

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Ion attachment mass spectrometry (IAMS) was used to analyze the species in cyclo-C4F8 plasma quantitatively. Not only stable neutral molecules but also less stable radicals were detected. Ions and species without a charge in the plasma were perfectly distinguishable. The measured dependence of the product distribution on the rf power shows that IAMS can be used to clarify and control the processes in the plasma.
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52.70.Nc Particle measurements

Characterization of facing-target reactive sputtered polycrystalline Fe3O4 films

J. J. Shen, W. B. Mi, Z. Q. Li, P. Wu, E. Y. Jiang, and H. L. Bai

J. Vac. Sci. Technol. A 24, 390 (2006); http://dx.doi.org/10.1116/1.2183226 (6 pages) | Cited 5 times

Online Publication Date: 20 April 2006

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Polycrystalline half-metallic Fe3O4 films fabricated by facing-target reactive sputtering were investigated systemically. Structural results reveal that typical Fe3O4 grains were well isolated by grain boundaries and grew with columnar structure. The room-temperature magnetization of Fe3O4 films at 50 kOe field is much lower than that of bulk Fe3O4 (471 emu/cm3), due to the presence of strong antiferromagnetic coupling within grain boundary and the amorphous bottom and top layers. The insaturation magnetization and loop shift in high field region at low temperature also stem from the strong antiferromagnetic coupling. The resistivity increases with the decreasing temperature and is consistent with fluctuation-induced tunneling mechanism in a wide temperature ranging from 50 to 300 K. The negative magnetoresistances up to −9.7% at 150 K and −6.4% at 300 K under 90 kOe magnetic field perpendicular to the film plane were observed and discussed.
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75.70.Ak Magnetic properties of monolayers and thin films
61.72.Mm Grain and twin boundaries
68.55.-a Thin film structure and morphology
75.60.Ej Magnetization curves, hysteresis, Barkhausen and related effects
75.50.Ee Antiferromagnetics
75.47.Pq Other materials

Electron inelastic mean free path and dielectric properties of a-boron, a-carbon, and their nitrides as determined by quantitative analysis of reflection electron energy loss spectroscopy

P. Prieto, C. Quirós, E. Elizalde, and J. M. Sanz

J. Vac. Sci. Technol. A 24, 396 (2006); http://dx.doi.org/10.1116/1.2183249 (12 pages) | Cited 4 times

Online Publication Date: 20 April 2006

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The quantitative analysis of reflection electron energy loss spectroscopy (REELS) spectra of amorphous boron (a-B), amorphous carbon (a-C), and their respective nitrides (i.e., BNx and CNx) has been performed to obtain the energy loss function (ELF) and the electron inelastic mean free path (IMFP) of the respective materials. In the case of boron we have studied different thin films over a wide range of stoichiometries, i.e., B, BN0.4, BN0.6, BN0.8, BN0.9, and commercially available hexagonal boron nitride (h-BN). In the case of carbon films we have analyzed a-C, CN0.3, and CN0.5 since the nitrogen content could not be increased above CN0.5. The analysis of the respective REELS spectra has been performed according to the model developed by Yubero and Tougaard [Phys. Rev. B 46, 2486 (1992) ] and Yubero et al. [Phys. Rev. B 52, 9719 (1996) ]. In addition we have included the study of the influence of some of the input parameters (refraction index, density, gap energy, and momentum dispersion coefficient) required by the model, which, rather commonly, are not well known and are dependent on the composition. The ELFs determined in this study are compared with published data when available. The IMFPs are compared with values predicted by the TPP-2M formulas and values reported for similar compounds.
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79.20.Uv Electron energy loss spectroscopy
61.43.Er Other amorphous solids
68.55.-a Thin film structure and morphology
78.20.Ci Optical constants (including refractive index, complex dielectric constant, absorption, reflection and transmission coefficients, emissivity)

Effects of Pt addition on the formation of Co–ITO granular magnetoresistance films by a two-step method

Wanti Ekawati, Ji Shi, Yoshio Nakamura, and Osamu Nittono

J. Vac. Sci. Technol. A 24, 408 (2006); http://dx.doi.org/10.1116/1.2186652 (5 pages)

Online Publication Date: 20 April 2006

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Platinum (Pt) has been added to Co–ITO (ITO: indium tin oxide) films to promote the formation of Co(Pt)–ITO granular structure by a two-step method which includes sputtering deposition at room temperature and postdeposition thermal annealing in a vacuum. Such films consist of magnetic Co(Pt) nanoparticles distributed uniformly in an amorphous ITO matrix. The Co(Pt) particles are formed during the thermal annealing by precipitation, and the matrix also contains certain amount of Co and Pt that suppress the crystallization of the amorphous ITO. Pt plays an important role in controlling the precipitation of Co(Pt) particles and the microstructure formation. First, by adding Pt into the films, more Co can be incorporated into the amorphous phase in the as-deposited state, which ensures sufficient Co to form magnetic particles through precipitation. Second, by incorporating Co and Pt into the film, the crystallization temperature of amorphous ITO is also increased to a temperature as high as 400 °C. These two effects make it possible to fabricate the Co(Pt)–ITO granular magnetoresistance films by the two-step method.
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68.55.A- Nucleation and growth
81.05.Rm Porous materials; granular materials
81.07.-b Nanoscale materials and structures: fabrication and characterization
75.50.Tt Fine-particle systems; nanocrystalline materials
68.55.-a Thin film structure and morphology
75.47.Np Metals and alloys

Electron cyclotron resonance plasma assisted pulsed laser deposition for compound host film synthesis and in situ doping

Y. F. Lu, J. Sun, D. Yu, L. Q. Shi, Z. B. Dong, and J. D. Wu

J. Vac. Sci. Technol. A 24, 413 (2006); http://dx.doi.org/10.1116/1.2186653 (5 pages) | Cited 2 times

Online Publication Date: 20 April 2006

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We developed a method for compound host film synthesis and in situ doping based on plasma assisted pulsed laser deposition by coablation of two targets with two pulsed laser beams. The feasibility of this method was demonstrated by the preparation of Er-doped GaN films. In the reactive nitrogen environment and with the assistance of nitrogen plasma generated from electron cyclotron resonance microwave discharge, the ablation of a polycrystalline GaAs target resulted in the reactive deposition of a GaN host film, whereas the ablation of a metallic Er target provided the host with Er atoms for in situ doping in the growing GaN host film. Hexagonal GaN films were formed on a silicon substrate as the host and Er was incorporated into the host with controlled concentration. We found that the composition of the compound host could be adjusted by varying the laser fluence on the target for host deposition or the energy of the plasma stream bombarding the growing host film. The dopant concentration could also be independently controlled to vary in a wide range by changing the pulse repetition ratio of the two laser beams or the laser fluence on the target for dopant supply. It was also proved that doping of very low concentrations could be easily realized by simply adjusting the pulse repetition rate and the fluence of the second laser.
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81.05.Ea III-V semiconductors
68.55.A- Nucleation and growth
61.72.uj III-V and II-VI semiconductors
81.15.Fg Pulsed laser ablation deposition
52.77.Dq Plasma-based ion implantation and deposition
76.40.+b Diamagnetic and cyclotron resonances

Deposition of hafnium oxide from Hf t-butoxide and nitric oxide

Z. Zhang, B. Xia, W. L. Gladfelter, and S. A. Campbell

J. Vac. Sci. Technol. A 24, 418 (2006); http://dx.doi.org/10.1116/1.2186660 (6 pages) | Cited 5 times

Online Publication Date: 20 April 2006

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The high-κ stack consisting of an optional nitride interfacial layer and a HfO2 layer was studied. The result shows that nitride or oxynitride interfacial layers can be controllably formed down to a few angstroms. The growth of both interfacial layers is self-limited. The introduction of nitric oxide with hafnium t-butoxide during the high-κ deposition leads to smaller effective oxide thickness (EOT) and gate leakage current. EOTs below 1.0 nm have been achieved with this combination of sources. The beneficial effect of nitric oxide can be explained in terms of reduced interfacial EOT, reduction of carbon contamination, and possibly a small trace amount of nitrogen incorporation.
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77.55.-g Dielectric thin films
77.84.Bw Elements, oxides, nitrides, borides, carbides, chalcogenides, etc.
81.05.-t Specific materials: fabrication, treatment, testing, and analysis
81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
68.55.A- Nucleation and growth

Plasma etching of benzocyclobutene in CF4/O2 and SF6/O2 plasmas

G. S. Kim and C. Steinbrüchel

J. Vac. Sci. Technol. A 24, 424 (2006); http://dx.doi.org/10.1116/1.2187994 (7 pages) | Cited 2 times

Online Publication Date: 20 April 2006

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Results for the reactive ion etching and patterning of benzocyclobutene (BCB) in CF4/O2 and SF6/O2 plasmas in a parallel-plate reactor with Langmuir probe and optical emission diagnostics are reported. The behavior of the O atom concentration [O] is similar in both plasmas, showing a strong maximum at a concentration of about 70% O2. The F atom concentration [F] has a maximum at 30% O2 in CF4/O2, but the etch rate has a maximum at 70% O2. In SF6/O2, by contrast, [F] and the etch rate increase continuously as the SF6 content is increased, and the highest etch rate is obtained with pure SF6. Also, BCB etched in pure SF6 gives a very smooth surface. Patterning is performed using two different masks: a conventional hard mask with Si oxide as the top layer and a different type of mask with BCB itself as the top layer. The anisotropy of the etching is evaluated in terms of the plasma conditions and type of masking. The aspect ratio dependence of the etch rate is investigated up to an aspect ratio of 2.5. The results are discussed in terms of possible etch mechanisms and their differences between SF6/O2 and C4/O2 plasmas. A simple model is used to show how the latter mask reduces the dependence of the etch rate on the aspect ratio.
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52.77.Bn Etching and cleaning
81.05.Lg Polymers and plastics; rubber; synthetic and natural fibers; organometallic and organic materials
81.65.Cf Surface cleaning, etching, patterning
52.70.Ds Electric and magnetic measurements
52.70.Kz Optical (ultraviolet, visible, infrared) measurements
85.40.Hp Lithography, masks and pattern transfer

Study of temperature influence on electron beam induced deposition

Wei Li and David C. Joy

J. Vac. Sci. Technol. A 24, 431 (2006); http://dx.doi.org/10.1116/1.2187995 (6 pages) | Cited 6 times

Online Publication Date: 20 April 2006

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A study of the temperature dependence of the electron beam induced deposition (EBID) of tungsten was carried out in a temperature range of −30–75 °C under two conditions of beam energy and beam current using WF6 as the precursor gas. An Arrhenius relationship was found for the temperature dependence of the deposition rate which is consistent with an electron stimulated desorption mechanism for this process. In addition, the mechanism for EBID under different conditions was discussed.
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81.15.-z Methods of deposition of films and coatings; film growth and epitaxy
68.43.Rs Electron stimulated desorption
79.20.La Photon- and electron-stimulated desorption

Selective etching of high-k HfO2 films over Si in hydrogen-added fluorocarbon (CF4/Ar/H2 and C4F8/Ar/H2) plasmas

Kazuo Takahashi and Kouichi Ono

J. Vac. Sci. Technol. A 24, 437 (2006); http://dx.doi.org/10.1116/1.2187997 (7 pages) | Cited 16 times

Online Publication Date: 20 April 2006

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Inductively coupled hydrogen-added fluorocarbon (CF4/Ar/H2 and C4F8/Ar/H2) plasmas were used to etch HfO2, which is a promising high-dielectric-constant material for the gate of complementary metal-oxide-semiconductor devices. The etch rates of HfO2 and Si were drastically changed depending on the additive-H2 flow rate in C4F8/Ar/H2 plasmas. The highly selective etching of HfO2 over Si was done in the condition with an additive-H2 flow rate, where the Si surface was covered with the fluorocarbon polymer. The results of x-ray photoelectron spectroscopy indicated that the carbon content of the selectively etched HfO2 surface was extremely low compared with the preetched surface contaminated by adventitious hydrocarbon in atmosphere. In the gas phase of the C4F8/Ar/H2 plasmas, Hf hydrocarbide molecules such as metal-organic compounds and Hf hydrofluoride were detected by a quadrupole mass analyzer. These findings indicate that the fluorine species, carbon, and hydrogen can work to etch HfO2 and that the carbon species also plays an important role in selective etching of HfO2 over Si.
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81.65.Cf Surface cleaning, etching, patterning
77.55.-g Dielectric thin films
52.77.Bn Etching and cleaning
79.60.Bm Clean metal, semiconductor, and insulator surfaces
82.80.Pv Electron spectroscopy (X-ray photoelectron (XPS), Auger electron spectroscopy (AES), etc.)

Characterization of the NiFe sputter etch process in a rf plasma

Thomas J. Kropewnicki, Alex M. Paterson, Theodoros Panagopoulos, and John P. Holland

J. Vac. Sci. Technol. A 24, 444 (2006); http://dx.doi.org/10.1116/1.2187998 (6 pages) | Cited 2 times

Online Publication Date: 20 April 2006

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The sputter etching of NiFe thin films by Ar ions in a rf plasma has been studied and characterized with the use of a Langmuir probe. The NiFe sputter etch rate was found to depend strongly on incident ion energy, with the highest NiFe etch rates occurring at high rf bias power, low pressure, and moderate rf source power. NiFe etch rates initially increased with increasing rf source power, then saturated at higher rf source powers. Pressure had the weakest effect on NiFe etch rates. Empirically determined sputter yields based on the NiFe etch rates and ion current densities were calculated, and these compared favorably to sputter yields determined using the sputtering model proposed by Sigmund [Phys. Rev. 184, 383 (1969) ].
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52.77.Bn Etching and cleaning
81.65.Cf Surface cleaning, etching, patterning

Computational analysis of solid-vapor equilibria for ZnS and SrS phosphor synthesis conditions

Heribert Wiedemeier

J. Vac. Sci. Technol. A 24, 450 (2006); http://dx.doi.org/10.1116/1.2190648 (9 pages) | Cited 2 times

Online Publication Date: 20 April 2006

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The synthesis and postgrowth treatment of luminescent materials frequently involve solid-vapor interactions. Because the underlying multispecies, multireaction equilibria are rather complex, quantitative correlations between synthesis conditions, vacancy concentrations, and emissive properties for predictive purposes are not readily available. In order to support the development of predictive guidelines, a quantitative, computational analysis of the vapor phase over ZnS and SrS in the absence and presence of nonconstituent species has been performed. The results confirm the complexity of these systems and show quantitatively the effects of impurity gases on the critical metal to nonmetal ratio in the ambient atmosphere. The data also reveal the temperature ranges in which desirable M/X ratios are available for given experimental conditions. The combined results of such computations are useful as reference data for the optimization and definition of reproducible synthesis conditions, and for the estimation of the type and magnitude of vacancies.
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78.55.Et II-VI semiconductors
78.55.Hx Other solid inorganic materials
64.70.Hz Solid-vapor transitions
61.72.J- Point defects and defect clusters
61.72.S- Impurities in crystals

Electrical property improvements of yttrium oxide-based metal-insulator-metal capacitors

C. Durand, C. Vallée, C. Dubourdieu, M. Kahn, M. Derivaz, S. Blonkowski, D. Jalabert, P. Hollinger, Q. Fang, and I. W. Boyd

J. Vac. Sci. Technol. A 24, 459 (2006); http://dx.doi.org/10.1116/1.2190649 (8 pages) | Cited 10 times

Online Publication Date: 20 April 2006

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We investigate the effects of the thickness reduction and specific postannealing treatments in order to improve the electrical properties of yttrium oxide-based metal-insulator-metal (MIM) capacitors. The films were grown on Si/TiSi2/TiN substrates at 350 °C by a low temperature process (pulsed liquid injection plasma-enhanced metal organic chemical vapor deposition). Although the thickness reduction leads to an increase of the capacitance density, the other electrical characteristics (the voltage linearity, the leakage currents, and the voltage breakdown) are seriously deteriorated due to the augmentation of the electric field. Low thermal budget annealing posttreatments ( ⩽ 450 °C) were carried out in a gas flux (Ar, O2, and H2) and under an ultraviolet (UV) radiation (O2 and N2). We demonstrate that the UV-O2 annealing treatment is particularly efficient in improving the voltage linearity, the leakage currents, and the electric field breakdown. The improved electrical properties after the UV-O2 annealing can be related to chemical modifications (organic content reduction and oxygen content increase). The voltage linearity improvement is most likely due to the presence of a residual oxidized silicon ultrathin layer on the top surface of the yttrium oxide films. Thus, a UV-O2 annealing is an effective postdeposition treatment that is compatible with the low thermal budget, which is required for MIM applications.
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84.32.Tt Capacitors

Vacuum science considerations for rapid reactor recovery with extremely low oxygen in low temperature low pressure chemical vapor deposition of Si1−xGex and Si1−xyGexCy films

Darwin Enicks and Gerald Oleszek

J. Vac. Sci. Technol. A 24, 467 (2006); http://dx.doi.org/10.1116/1.2190650 (7 pages)

Online Publication Date: 20 April 2006

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The films for this study were grown in the AMAT Centura 5200 low pressure chemical vapor deposition (LPCVD) reactor. Silicon germanium (SixGe1−x) and silicon germanium carbon (Si1−xyGexCy) have widely been accepted as the materials of choice for a variety of uses in semiconductor devices. Most manufacturers utilize LPCVD for the low temperature growth of these films. Due to the reaction kinetics, oxygen incorporation in SiGe films may become substantial, especially following a major preventive maintenance (PM). Depending on the technology, elevated oxygen may be unacceptable due to process and device performance considerations. These considerations range from oxygen reaction with dopant source gases, thus minimizing dopant incorporation and activation, to minority carrier lifetime reduction in the base of a SiGe heterojunction bipolar transistor due to oxygen related defects. To achieve low oxygen processes the engineer must have a clear picture of the mechanisms and the fundamental vacuum science as it relates to LPCVD processing. Outgassing and the all too familiar chamber leak rate are discussed as they relate to sorption and sorbtion effects and recommendations are made to facilitate very rapid PM recoveries with sustained in-film oxygen levels as good as attained with ultrahigh vacuum CVD. Secondary ion mass spectrometry profiles are presented, which demonstrate that a sustained sub-1017 at./cc oxygen level in low temperature LPCVD SiGe processing is possible when these types of gas loads are addressed.
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81.05.Hd Other semiconductors
81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
81.15.-z Methods of deposition of films and coatings; film growth and epitaxy
68.55.Ln Defects and impurities: doping, implantation, distribution, concentration, etc.
73.50.Gr Charge carriers: generation, recombination, lifetime, trapping, mean free paths
79.20.Rf Atomic, molecular, and ion beam impact and interactions with surfaces

Thin film reaction of transition metals with germanium

S. Gaudet, C. Detavernier, A. J. Kellock, P. Desjardins, and C. Lavoie

J. Vac. Sci. Technol. A 24, 474 (2006); http://dx.doi.org/10.1116/1.2191861 (12 pages) | Cited 60 times

Online Publication Date: 20 April 2006

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A systematic study of the thermally induced reaction of 20 transition metals (Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W, Mn, Re, Fe, Ru, Co, Rh, Ir, Ni, Pd, Pt, and Cu) with Ge substrates was carried out in order to identify appropriate contact materials in Ge-based microelectronic circuits. Thin metal films, nominally 30 nm thick, were sputter deposited on both amorphous Ge and crystalline Ge(001). Metal-Ge reactions were monitored in situ during ramp anneals at 3 °Cs−1 in an atmosphere of purified He using time-resolved x-ray diffraction, diffuse light scattering, and resistance measurements. These analyses allowed the determination of the phase formation sequence for each metal-Ge system and the identification of the most promising candidates—in terms of sheet resistance and surface roughness—for their use as first level interconnections in microelectronic circuits. A first group of metals (Ti, Zr, Hf, V, Nb, and Ta) reacted with Ge only at temperatures well above 450 °C and was prone to oxidation. Another set (Cr, Mo, Mn, Re, Rh, Ru, and Ir) did not form low resistivity phases (<130 μΩ cm) whereas no reaction was observed in the case of W even after annealing at up to 1000 °C. We found that Fe, Co, Ni, Pd, Pt, and Cu were the most interesting candidates for microelectronic applications as they reacted at relatively low temperatures (150–360 °C) to form low resistivity phases (22–129 μΩ cm). Among those, two monogermanides, NiGe and PdGe, exhibited the lowest resistivity values (22–30 μΩ cm) and were stable over the widest temperature window during ramp anneals. In passing, we note that Cu, Ni, and Pd were the most effective in lowering the crystallization temperature of amorphous Ge, by up to 290 °C for our typical ramp anneals at 3 °Cs−1.
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81.05.Bx Metals, semimetals, and alloys
73.61.At Metal and metallic alloys
61.72.Cc Kinetics of defect formation and annealing
68.35.B- Structure of clean surfaces (and surface reconstruction)
81.15.Cd Deposition by sputtering
85.40.-e Microelectronics: LSI, VLSI, ULSI; integrated circuit fabrication technology

Attenuation of hydrogen radicals traveling under flowing gas conditions through tubes of different materials

R. K. Grubbs and S. M. George

J. Vac. Sci. Technol. A 24, 486 (2006); http://dx.doi.org/10.1116/1.2191862 (11 pages) | Cited 7 times

Online Publication Date: 20 April 2006

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Hydrogen radical concentrations traveling under flowing gas conditions through tubes of different materials were measured using a dual thermocouple probe. The source of the hydrogen radicals was a toroidal radio frequency plasma source operating at 2.0 and 3.3 kW for H2 pressures of 250 and 500 mTorr, respectively. The dual thermocouple probe was comprised of exposed and covered Pt/Pt13%Rh thermocouples. Hydrogen radicals recombined efficiently on the exposed thermocouple and the energy of formation of H2 heated the thermocouple. The second thermocouple was covered by glass and was heated primarily by the ambient gas. The dual thermocouple probe was translated and measured temperatures at different distances from the hydrogen radical source. These temperature measurements were conducted at H2 flow rates of 35 and 75 SCCM (SCCM denotes cubic centimeter per minute at STP) inside cylindrical tubes made of stainless steel, aluminum, quartz, and Pyrex. The hydrogen radical concentrations were obtained from the temperatures of the exposed and covered thermocouples. The hydrogen concentration decreased versus distance from the plasma source. After correcting for the H2 gas flow using a reference frame transformation, the hydrogen radical concentration profiles yielded the atomic hydrogen recombination coefficient, γ, for the four materials. The methodology of measuring the hydrogen radical concentrations, the analysis of the results under flowing gas conditions, and the determination of the atomic hydrogen recombination coefficients for various materials will help facilitate the use of hydrogen radicals for thin film growth processes.
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52.25.Fi Transport properties
52.70.Ds Electric and magnetic measurements
52.50.Dg Plasma sources
52.40.Hf Plasma-material interactions; boundary layer effects
82.30.Cf Atom and radical reactions; chain reactions; molecule-molecule reactions
82.33.Xj Plasma reactions (including flowing afterglow and electric discharges)

Surfactant-assisted growth of CdS thin films for photovoltaic applications

Craig L. Perkins and Falah S. Hasoon

J. Vac. Sci. Technol. A 24, 497 (2006); http://dx.doi.org/10.1116/1.2194929 (8 pages) | Cited 8 times

Online Publication Date: 20 April 2006

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A common nonionic surfactant, Triton X-100, was used to modify the chemical bath deposition of CdS “buffer” layers on Cu(In,Ga)Se2 (CIGS) thin films. Addition of the surfactant to the CdS deposition bath allowed increased wetting of Cu(In,Ga)Se2 substrates and an increase in the uniformity of films, especially on model hydrophobic substrates. X-ray photoelectron spectroscopy and ultraviolet photoelectron spectroscopy data demonstrate that films produced with the surfactant have the same chemical and electronic properties as films grown without it. In CdS/Cu(In,Ga)Se2 devices, it was found that Triton X-100 allowed the use of CdS layers that were three to four times thinner than those used normally in high efficiency CIGS-based devices and eliminated the large drops in open-circuit voltage that usually accompany very thin buffer layers. For these thin CdS layers and relative to devices made without the surfactant, average absolute cell efficiencies were increased from 10.5% to 14.8% or by a relative 41%. Visual inspection of the CdS depositions reveals one possible mechanism of the surfactant’s effects: Bubbles that form and adhere to the CIGS surface during the chemical bath deposition are almost completely eliminated with the addition of the TX-100. Thus, junction nonuniformities, pinholes, and thin areas in the CdS layer caused by poor wetting of the substrate surface are sharply reduced, leading to large increases in the open-circuit voltage in devices produced with the surfactant.
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81.05.Dz II-VI semiconductors
81.15.Lm Liquid phase epitaxy; deposition from liquid phases (melts, solutions, and surface layers on liquids)
68.55.-a Thin film structure and morphology
73.50.Pz Photoconduction and photovoltaic effects
68.08.Bc Wetting
79.60.Bm Clean metal, semiconductor, and insulator surfaces

Characteristics and diagnostics of an ultrahigh vacuum compatible laser ablation source for crossed molecular beam experiments

Xibin Gu, Ying Guo, Ed Kawamura, and Ralf I. Kaiser

J. Vac. Sci. Technol. A 24, 505 (2006); http://dx.doi.org/10.1116/1.2194935 (7 pages) | Cited 16 times

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We present the design and the characteristics of an ultrahigh vacuum compatible laser ablation source which can be operated in a crossed molecular beam machine at pressures as low as 10−9 Torr. This unit provides intense supersonic beams of up to 3×1013 cm−3 reactant species (carbon atoms, dicarbon, and tricarbon) in the interaction region of a crossed molecular beam machine. Practical delay time windows between the pulsed valve releasing the seeding gas and the laser have been determined to be between 16 630 and 16 645 μs, i.e., firing the laser 150–165 μs after the 80 μs pulsed valve trigger. The concentration of the dicarbon and tricarbon clusters can be maximized/minimized by adjusting the laser focus (a tighter laser focus leads to an enhanced atomic carbon component) and the laser power (multiphoton dissociation). We achieved stable peak velocities between 800 and 3800 ms−1 and speed ratios S of up to 6.
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42.62.-b Laser applications
42.65.Re Ultrafast processes; optical pulse generation and pulse compression

Effect of multipactor discharge on Alcator C-Mod ion cyclotron range of frequency heating

T. P. Graves, S. J. Wukitch, B. LaBombard, and I. H. Hutchinson

J. Vac. Sci. Technol. A 24, 512 (2006); http://dx.doi.org/10.1116/1.2194937 (5 pages)

Online Publication Date: 20 April 2006

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Alcator C-Mod uses high power radio frequency (rf) power for auxiliary plasma heating at the ion cyclotron frequency. The operation of the rf antennas is limited at neutral pressures which fall far below the minimum pressure for glow discharge as given by the rf Paschen curve. Recent experiments have found that this operational pressure limit is due to multipactor discharges in the vacuum transmission lines. At elevated neutral pressures, the multipactor discharge induces a glow discharge that causes a nearly complete reflection of rf power. On C-Mod, in presence of a magnetic field, this discharge forms at pressures of 0.5 and 1 mTorr, which are the same pressures as the observed operational limit. Experimental results are supported by the Coaxial Multipactor Experiment.
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84.40.-x Radiowave and microwave (including millimeter wave) technology
84.32.Dd Connectors, relays, and switches
52.80.Hc Glow; corona

Arsenic doping for synthesis of nanocrystalline p-type ZnO thin films

Ning Xu, Yingliang Xu, Li Li, Yiqun Shen, Tinwei Zhang, Jiada Wu, Jian Sun, and Zhifeng Ying

J. Vac. Sci. Technol. A 24, 517 (2006); http://dx.doi.org/10.1116/1.2194939 (4 pages) | Cited 16 times

Online Publication Date: 20 April 2006

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Nanocrystalline p-type arsenic-doped ZnO (ZnO:As) films have been synthesized on (0001) sapphire substrates by pulsed laser deposition using a ZnO target mixed with 6.6 wt % As2O3. The process of synthesizing p-type ZnO:As films was performed in an ambient gas of ultrapure (<99.99%) oxygen. The ambient gas pressure was 5 Pa with the substrate temperature in the range of 350–500 °C. The ZnO:As films grown at 500 °C are p type, and the acceptor concentration in ZnO:As films is about 1.9×1018 at./cm3 as determined by Hall effect measurements. The concentration of As in ZnO:As films is estimated to be about 1.7% from the x-ray photoemission spectroscopy (XPS) spectrum. Guided by the XPS analysis and a model for large-sized-mismatched group-V dopant in ZnO, an AsZn–2VZn complex was thought to be the most possible acceptor.
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79.60.Bm Clean metal, semiconductor, and insulator surfaces
81.15.Fg Pulsed laser ablation deposition
81.16.Mk Laser-assisted deposition
72.20.My Galvanomagnetic and other magnetotransport effects
61.72.uj III-V and II-VI semiconductors
68.55.A- Nucleation and growth

Low-temperature sputtering of crystalline TiO2 films

J. Musil, D. Heřman, and J. Šícha

J. Vac. Sci. Technol. A 24, 521 (2006); http://dx.doi.org/10.1116/1.2187993 (8 pages) | Cited 46 times

Online Publication Date: 21 April 2006

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This article reports on the investigation of reactive magnetron sputtering of transparent, crystalline titanium dioxide films. The aim of this investigation is to determine a minimum substrate surface temperature Tsurf necessary to form crystalline TiO2 films with anatase structure. Films were prepared by dc pulsed reactive magnetron sputtering using a dual magnetron operating in bipolar mode and equipped with Ti(99.5) and ceramic Ti5O9 targets. The films were deposited on unheated glass substrates and their structure was characterized by x-ray diffraction and surface morphology by atomic force microscopy. Special attention is devoted to the measurement of Tsurf using thermostrips pasted to the glass substrate. It was found that (1) Tsurf is considerably higher (approximately by 100 °C or more) than the substrate temperature Ts measured by the thermocouple incorporated into the substrate holder and (2) Tsurf strongly depends on the substrate-to-target distance ds-t, the magnetron target power loading, and the thermal conductivity of the target and its cooling. The main result of this study is the finding that (1) the crystallization of sputtered TiO2 films depends not only on Tsurf but also on the total pressure pT of sputtering gas (Ar+O2), partial pressure of oxygen pO2, the film deposition rate aD, and the film thickness h, (2) crystalline TiO2 films with well developed anatase structure can be formed at Tsurf = 160 °C and low values of aD ≈ 5 nm/min, (3) the crystalline structure of TiO2 film gradually changes from (i) anatase through (ii) anatase+rutile mixture, and (iii) pure rutile to x-ray amorphous structure at Tsurf = 160 °C and pT = 0.75 Pa when pO2 decreases and aD increases above 5 nm/min, and (4) crystallinity of the TiO2 films decreases with decreasing h and Tsurf. Interrelationships between the structure of TiO2 film, its roughness, Tsurf, and aD are discussed in detail. Trends of next development are briefly outlined.
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81.05.-t Specific materials: fabrication, treatment, testing, and analysis
81.15.Cd Deposition by sputtering
68.55.A- Nucleation and growth
68.55.-a Thin film structure and morphology
68.35.B- Structure of clean surfaces (and surface reconstruction)
66.70.-f Nonelectronic thermal conduction and heat-pulse propagation in solids; thermal waves

Conductance measurement of a conical tube and calculation of the pressure distribution

B. Mercier

J. Vac. Sci. Technol. A 24, 529 (2006); http://dx.doi.org/10.1116/1.2187996 (8 pages) | Cited 1 time

Online Publication Date: 21 April 2006

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In recent articles [ J. Gomez-Goni, and P. J. Lobo J. Vac. Sci. Technol. A 21, 1452 (2003); P. Swemin and M. Niewinski, Vacuum 67, 359 (2002) ] the conductance of conical tube in the molecular flow regime has been calculated using the Monte Carlo method or by the resolution of the Clausing integral equation, reformulated by Iczkowski et al. [J. Phys. Chem. 67, 229 (1963) ], for the case of a cone. The comparison between the analytical values and different simulations allows one to determine a correction factor k to apply to the intrinsic conductance of the cones. This coefficient depends on the propagation direction of flow and increases considerably for larger conic angles. For a cone half-angle of 40° and a length ten times greater than smallest entrance radii, the correction factor is approximately 5.3 for a circulating flow from the smallest to the largest orifice. Our experimental device measured the conical conductance by a dynamic method. In order to do this, it was necessary to determine the surface pressure distribution. The extension of the Oatley method, with the addition of several components of various transmission probabilities, permits one to establish this distribution for a vacuum system and thus to give the pressure measured by a gauge situated along the wall of the duct. This method provides a good approximation for tubes and cones and can be used for engineering practice. The determination of this distribution is all the more critical when the conductance and the pumping speed are large and can thus have a great influence on the vacuum metrology.
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84.37.+q Measurements in electric variables (including voltage, current, resistance, capacitance, inductance, impedance, and admittance, etc.)
47.80.Fg Pressure and temperature measurements
47.45.Dt Free molecular flows
84.47.+w Vacuum tubes

Mechanical properties of Cu–Al–O thin films prepared by plasma-enhanced chemical vapor deposition

Wen Chen, Hao Gong, and Kaiyang Zeng

J. Vac. Sci. Technol. A 24, 537 (2006); http://dx.doi.org/10.1116/1.2191860 (5 pages) | Cited 4 times

Online Publication Date: 26 April 2006

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Copper aluminum oxide thin films were prepared by the plasma-enhanced chemical vapor deposition from metal organic precursors. The film was characterized by x-ray diffraction, atomic force microscopy, and the depth profile analysis using secondary ion mass spectrometry. Nanoindentation was performed to measure the hardness and elastic modulus of the film. The mechanical strengthening of the film was considered to be due to nanograins of CuAlO2 and CuO throughout the film, the large area of grain boundaries, and also finer Al2O3 particles dispersed in the film matrix.
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81.05.Hd Other semiconductors
81.40.Np Fatigue, corrosion fatigue, embrittlement, cracking, fracture, and failure
62.20.M- Structural failure of materials
68.60.Bs Mechanical and acoustical properties
81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
52.77.Dq Plasma-based ion implantation and deposition
42.79.Wc Optical coatings

Detecting free radicals during the hot wire chemical vapor deposition of amorphous silicon carbide films using single-source precursors

Gillian A. Zaharias, H. L. Duan, and Stacey F. Bent

J. Vac. Sci. Technol. A 24, 542 (2006); http://dx.doi.org/10.1116/1.2194023 (8 pages) | Cited 7 times

Online Publication Date: 26 April 2006

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A vacuum ultraviolet single photon ionization technique has been used to probe gas-phase species important in the hot wire chemical vapor deposition (HW-CVD) of amorphous silicon carbide(a-SiC:H) films using different single-source precursors. This study focuses on monomethylsilane, dimethylsilane, trimethylsilane, tetramethylsilane, and 1,1-dimethyl-1-silacyclobutane, and the reactions of these precursors on tungsten and rhenium filaments between 1000 and 1950 °C. Silane is also considered for comparison. Si radicals are found to be major products of hot wire decomposition for all the organosilicon precursors; CH3 is also observed. C and H radicals are expected to be produced as well but are not detected at the ionization energy used in these experiments. Within the series of methylsilanes, the reaction rate on the filament is found to decrease with increasing number of methyl groups on the precursor. We propose a model in which Si–H bonds are cleaved with lower activation barriers than SiCH3 bonds as the molecule adsorbs onto the hot metal surface. 1,1-dimethyl-1-silacyclobutane produces Si with a lower apparent activation energy than the other molecules. Coverage-dependent reaction pathways are proposed to play a role in the temperature profile of CH3 generation. Infrared spectra of films deposited by HW-CVD show that the film composition and growth rate for the different precursors correlate with the hot wire chemistry studied by single photon ionization.
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81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
78.30.Hv Other nonmetallic inorganics
68.55.A- Nucleation and growth

Atmospheric pressure plasma analysis by modulated molecular beam mass spectrometry

Y. Aranda Gonzalvo, T. D. Whitmore, J. A. Rees, D. L. Seymour, and E. Stoffels

J. Vac. Sci. Technol. A 24, 550 (2006); http://dx.doi.org/10.1116/1.2194938 (4 pages) | Cited 12 times

Online Publication Date: 26 April 2006

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Fractional number density measurements for a rf plasma “needle” operating at atmospheric pressure have been obtained using a molecular beam mass spectrometer (MBMS) system designed for diagnostics of atmospheric plasmas. The MBMS system comprises three differentially pumped stages and a mass/energy analyzer and includes an automated beam-to-background measurement facility in the form of a software-controlled chopper mechanism. The automation of the beam modulation allows the neutral components in the plasma to be rapidly and accurately measured using the mass spectrometer by threshold ionization techniques. Data are reported for plasma generated by a needle plasma source operated using a helium/air mixture. In particular, data for the conversion of atmospheric oxygen and nitrogen into nitric oxide are discussed with reference to its significance for medical applications such as disinfecting wounds and dental cavities and for microsurgery.
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52.70.Gw Radio-frequency and microwave measurements
52.25.Tx Emission, absorption, and scattering of particles
87.80.-y Biophysical techniques (research methods)

Hard multilayer coatings containing TiN and/or ZrN: A review and recent progress in their nanoscale characterization

C. Ziebert and S. Ulrich

J. Vac. Sci. Technol. A 24, 554 (2006); http://dx.doi.org/10.1116/1.2194031 (30 pages) | Cited 26 times

Online Publication Date: 26 April 2006

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In the first part of this article, a comprehensive literature review on hard multilayer coatings, which contain TiN and/or ZrN as a component is given. The developments made in this field, starting with the first published results in 1987 and ending with the latest articles in 2005, were summarized and critically evaluated in order to serve as a starting point for future research in this area. In the second part, recent progress in the nanoscale characterization of multilayers and their interfaces by the small-angle cross-section nanoindentation method and atomic force microscopy is demonstrated on TiN/ZrN multilayers. These nanoscale multilayers were deposited by reactive dc-magnetron sputtering of metallic titanium and zirconium targets in argon/nitrogen plasma onto hard metal and silicon substrates.
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81.40.Np Fatigue, corrosion fatigue, embrittlement, cracking, fracture, and failure
68.35.Gy Mechanical properties; surface strains
68.65.Ac Multilayers
62.20.Qp Friction, tribology, and hardness
62.20.M- Structural failure of materials
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back to top Epitaxy and Thin Films

Growth and characterization of GaAsSb metamorphic samples on an InP substrate

F. M. Mohammedy, O. Hulko, B. J. Robinson, D. A. Thompson, M. J. Deen, and J. G. Simmons

J. Vac. Sci. Technol. A 24, 587 (2006); http://dx.doi.org/10.1116/1.2194024 (4 pages) | Cited 3 times

Online Publication Date: 4 May 2006

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Buffer layers of GaAs1−xSbx were grown on an InP substrate starting at x = 0.49 (lattice matched to InP) and increasing x in steps of 0.03–1.0 (GaSb), followed by a 0.5 μm thick GaSb metamorphic layer. A 10 nm thick InAs quantum well was grown on top and capped with a 100 nm GaSb. All layers were grown using gas source molecular beam epitaxy by reducing the As flux in small steps while keeping the Sb flux fixed. The substrate temperature during growth was ∼ 490 °C. High-Resolution x-ray diffraction analysis showed that the metamorphic layer was almost fully relaxed. Cross-sectional transmission electron microscopy images show that a postgrowth anneal at 600 °C for 30 s successfully reduces the number of dislocations threading through the metamorphic layer. Hence the top layer can be used satisfactorily as a pseudosubstrate for subsequent layer growths assuming a GaSb lattice constant.
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81.05.Ea III-V semiconductors
81.15.Hi Molecular, atomic, ion, and chemical beam epitaxy
68.55.-a Thin film structure and morphology
68.55.A- Nucleation and growth
61.72.Cc Kinetics of defect formation and annealing
61.72.Ff Direct observation of dislocations and other defects (etch pits, decoration, electron microscopy, x-ray topography, etc.)

Investigation of the optical properties of InGaAs(N):(Sb) quantum wells grown by metal organic vapor phase epitaxy

W. C. Chen, Y. K. Su, R. W. Chuang, and S. H. Hsu

J. Vac. Sci. Technol. A 24, 591 (2006); http://dx.doi.org/10.1116/1.2194025 (4 pages) | Cited 1 time

Online Publication Date: 4 May 2006

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Dilute-nitride materials have attracted much attention due to their capability of operating in the wavelength range of optical communication. However, their optical properties degrade with the nitrogen incorporation into the host material such as InGaAs or GaAs, which can be recovered slightly by performing thermal treatment. More recently, the surfactant effect of Sb was verified by molecular beam epitaxy grown samples. Adding Sb into dilute-nitride materials can help to maintain the luminescence efficiency while increasing the emission wavelength toward 1.55 μm. But its effect on the metal organic vapor phase epitaxy grown samples is not very clear. In this article, we performed a series of experiments on the InGaAsN(Sb) quantum wells to clarify the role of Sb. The photoluminescence (PL) intensities of InGaAsN:Sb were higher than those of the undoped samples and the extent of blueshift after annealing was slighter than that of the InGaAsN quantum wells. However, the PL intensities were still low and thus we tried another material (InGaAs:Sb) to achieve the 1.3 μm emission. The temperature dependent PL measurements were also carried out to investigate the optical properties of InGaAs:Sb quantum wells.
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78.67.De Quantum wells
78.55.Cr III-V semiconductors

Energetic ion bombarded Fe/Al multilayers

M. S. Al-Busaidy and M. D. Crapper

J. Vac. Sci. Technol. A 24, 595 (2006); http://dx.doi.org/10.1116/1.2194026 (5 pages) | Cited 1 time

Online Publication Date: 4 May 2006

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The utility of ion-assisted deposition is investigated to explore the possibility of counteracting the deficiency of back-reflected current of Ar neutrals in the case of lighter elements such as Al. A range of energetically ion bombarded Fe/Al multilayers sputtered with applied surface bias of 0, −200, or −400 V were deposited onto Si(111) substrates in an argon atmosphere of 4 mTorr using a computer controlled dc magnetron sputtering system. Grazing incidence reflectivity and rocking curve scans by synchrotron x rays of wavelength of 1.38 Å were used to investigate the structures of the interfaces produced. Substantial evidence has been gathered to suggest the gradual suppression of interfacial mixing and reduction in interfacial roughness with increases of applied bias. The densification of the Al microstructure was noticeable and may be a consequence of resputtering attributable to the induced ion bombardment. The average interfacial roughnesses were calculated for the 0, −200, and −400 V samples to be 7±0.5, 6±0.5, and 5±0.5 Å respectfully demonstrating a 30% improvement in interface quality. Data from rocking curve scans point to improved long-range correlated roughness in energetically deposited samples. The computational code based on the recursive algorithm developed by Parratt [Phys. Rev. 95, 359 (1954)] was successful in the simulation of the specular reflectivity curves.
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81.15.Jj Ion and electron beam-assisted deposition; ion plating
81.15.Cd Deposition by sputtering
68.65.Ac Multilayers
61.80.Jh Ion radiation effects
68.35.Ct Interface structure and roughness

Compositional effect on the dielectric properties of high-k titanium silicate thin films deposited by means of a cosputtering process

D. Brassard, D. K. Sarkar, M. A. El Khakani, and L. Ouellet

J. Vac. Sci. Technol. A 24, 600 (2006); http://dx.doi.org/10.1116/1.2180267 (6 pages) | Cited 9 times

Online Publication Date: 4 May 2006

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We report on the successful growth of high dielectric constant (high-k) titanium silicate TixSi1−xO2 thin films of various compositions (0 ⩽ x ⩽ 1) at room temperature from the cosputtering of SiO2 and TiO2 targets. The developed process is shown to offer the latitude required to achieve not only a precise control of the film composition but an excellent morphology (i.e., dense films with low roughness) as well. The Fourier transform infrared and x-ray photoelectron spectroscopy characterizations have evidenced the presence of Ti–O–Si type of atomic environments, which is the fingerprint of the titanium silicate phase. The titanium silicate films are found to exhibit excellent dielectric properties with very low dielectric losses [tan(δ)<0.02] regardless of their composition. The dielectric constant of the films is found to increase with their TiO2 content from 4 (for pure SiO2 films) to 45 (for TiO2). On the other hand, increasing the TiO2 content of the films is also shown to degrade significantly their leakage current. Nevertheless, titanium silicate films with almost equiatomic composition (x ∼ 0.45) are found to exhibit an excellent trade-off between a high-k value ( ∼ 18) and low leakage current ( ∼ 5×10−7A/cm2 at 1 MV/cm). Finally, the compositional dependence of the dielectric properties of the TixSi1−xO2 films is discussed in terms of bonding states and optical band gap.
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77.55.-g Dielectric thin films
77.84.Bw Elements, oxides, nitrides, borides, carbides, chalcogenides, etc.
81.05.-t Specific materials: fabrication, treatment, testing, and analysis
81.15.Cd Deposition by sputtering
77.22.Ch Permittivity (dielectric function)
77.22.Gm Dielectric loss and relaxation

Growth of CdTe/Si(100) thin films by pulsed laser deposition for photonic applications

S. Neretina, R. A. Hughes, N. V. Sochinskii, M. Weber, K. G. Lynn, J. Wojcik, G. N. Pearson, J. S. Preston, and P. Mascher

J. Vac. Sci. Technol. A 24, 606 (2006); http://dx.doi.org/10.1116/1.2183297 (6 pages) | Cited 3 times

Online Publication Date: 4 May 2006

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Cadmium telluride (CdTe) has become one of the most useful and versatile photonic materials. While many applications require the highest quality material possible, others can sacrifice some degree of sample quality in favor of reduced fabrication costs. Here, we explore the deposition of CdTe thin films deposited on (100) silicon substrates in the absence of costly ultrahigh vacuum conditions. This inevitably leads to the deposition of films on silicon’s native oxide. The work presented here explores the trade-offs in sample quality as determined by a host of characterization techniques. The films were deposited using the pulsed laser deposition technique at relatively low growth rates and at an optimized substrate temperature of 300 °C. X-ray diffraction data show only (111) oriented CdTe with rocking curve widths broadened due to the lack of an epitaxial relationship between the film and substrate. Atomic force microscopy images confirm that the films have a smooth surface morphology as was suggested by their mirrorlike appearance. Film quality was also analyzed using photoluminescence, positron annihilation spectroscopy, and ellipsometry. While structural deficiencies have been observed in these films, the optical properties are remarkably similar to those expected for high quality CdTe.
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81.05.Dz II-VI semiconductors
81.15.Fg Pulsed laser ablation deposition
68.55.A- Nucleation and growth
78.66.Hf II-VI semiconductors
78.55.Et II-VI semiconductors
78.70.Bj Positron annihilation
42.79.Wc Optical coatings
42.70.-a Optical materials

Thermochromic vanadium dioxide smart coatings grown on Kapton substrates by reactive pulsed laser deposition

M. Soltani, M. Chaker, E. Haddad, and R. V. Kruzelesky

J. Vac. Sci. Technol. A 24, 612 (2006); http://dx.doi.org/10.1116/1.2186661 (6 pages) | Cited 15 times

Online Publication Date: 4 May 2006

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Thermochromic undoped and metal (Ti and W)-doped VO2 smart coatings were achieved on Kapton HN by reactive pulsed laser deposition. The optimization of the deposition was conducted with Si (100) substrates. The coatings were deposited at relatively low deposition temperatures (250, 300, and 350 °C), which are compatible with the characteristics of Kapton. The stoichiometry of the VO2-coated Kapton was confirmed by x-ray photoelectron spectroscopy analysis of the vanadium and oxygen bands. Moreover, the single phase VO2 was confirmed by x-ray diffraction of VO2/Si synthesized at 300 °C. Unlike VO2/Kapton, the VO2/Si exhibited the well-known semiconductor-to-metallic transition, as shown by the temperature dependence of the infrared transmittance. This coating exhibited a similar transition temperature to that of VO2 single crystal ( ≈ 68 °C), but a small transmittance switching (about 7%) at 2.5 μm. The temperature dependence of the electrical resistivity of all coatings on Kapton was investigated by means of the standard four-point probe technique. The resistivity decreased with increasing temperature. No abrupt semiconductor-to-metallic transition was observed either for undoped or for metal-doped VO2 coatings. It was found that Ti and W dopants have an antagonistic effect on the resistivity. The resistivity was enhanced by the Ti dopant, whereas it was decreased for W-doped VO2 coatings. These results show that the tunability of the resistivity can be tailored either by controlling the deposition temperature or by adjusting the concentration of Ti and W dopants. In addition, at room temperature a much higher temperature coefficient of resistance of −3.29%/°C was achieved in W(0.5%)-doped VO2/Kapton. Finally, these VO2 smart coatings are promising materials for the IR sensing and sunshield applications.
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81.15.Fg Pulsed laser ablation deposition
78.20.N- Thermo-optic effects
78.20.nb Photothermal effects
68.55.-a Thin film structure and morphology
82.80.Pv Electron spectroscopy (X-ray photoelectron (XPS), Auger electron spectroscopy (AES), etc.)
71.30.+h Metal-insulator transitions and other electronic transitions
61.72.up Other materials

High-performance n-channel 13.56 MHz plasma-enhanced chemical vapor deposition nanocrystalline silicon thin-film transistors

Czang-Ho Lee, Andrei Sazonov, and Arokia Nathan

J. Vac. Sci. Technol. A 24, 618 (2006); http://dx.doi.org/10.1116/1.2194027 (6 pages) | Cited 1 time

Online Publication Date: 4 May 2006

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Hydrogenated nanocrystalline silicon (nc-Si:H) films were directly deposited by using 13.56 MHz plasma-enhanced chemical vapor deposition at a substrate temperature of 260 °C with highly hydrogen (H2) diluted silane (SiH4) gases. The nc-Si:H film showed a high Raman crystalline volume fraction (XC ∼ 85%) and low oxygen concentration (CO ∼ 1.5×1017 at./cm3). The formation of high-quality nc-Si:H is explained in terms of the effective roles of atomic hydrogen in the plasma. Top-gate staggered n-channel thin-film transistors (TFTs) adopting 90–100 nm nc-Si:H channel and ∼ 300 nm hydrogenated amorphous silicon oxide (a-SiOx) gate dielectric layers showed a field-effect mobility (μFE) of ∼ 150 cm2/Vs, a threshold voltage (VT) of ∼ 2 V, a subthreshold slope (S) of ∼ 0.23 V/dec, and an on/off current ratio of more than 106. The TFT performance reported here offers promise for the total integration of peripheral electronics for active-matrix flat panel systems.
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85.30.Tv Field effect devices
81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
back to top Wide Band Gap Materials and Devices

Self-heating and the temperature dependence of the dc characteristics of GaN heterostructure field effect transistors

S. P. McAlister, J. A. Bardwell, S. Haffouz, and H. Tang

J. Vac. Sci. Technol. A 24, 624 (2006); http://dx.doi.org/10.1116/1.2172921 (5 pages) | Cited 10 times

Online Publication Date: 4 May 2006

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Self-heating is an important issue for GaN heterostructure field effect transistors (HFETs), especially in high power applications. Here we report the temperature dependence of the dc characteristics of some GaN HFETs including the variation of the transconductance. We present the characteristics as a function of added power, instead of voltage bias, and use the temperature data to transform the power dependence into a dependence on the average device temperature. For similar devices on sapphire and SiC, at 20 V VDS and 0 V VG, the temperature increase for the same added power is ∼ 2.7 times greater in the sapphire-based device.
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85.30.Tv Field effect devices

Characterization and modeling of AlGaN/GaN heterostructure field effect transistors for low noise amplifiers

S. H. Knox, J. W. M. Rogers, P. N. A. Chyurlia, N. G. Tarr, J. A. Bardwell, H. Tang, and S. Haffouz

J. Vac. Sci. Technol. A 24, 629 (2006); http://dx.doi.org/10.1116/1.2186659 (5 pages) | Cited 1 time

Online Publication Date: 4 May 2006

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A simple equivalent circuit model including noise sources for the GaN heterostructure field effect transistor is presented and analyzed. The model is used to determine optimum source impedance for low noise amplifier applications. A good agreement between the model and measured NFmin of experimental devices is shown. Prototype transistors with a 0.75 μm gate length and 80 μm width delivered a power-added efficiency of 45.6% and a minimum noise figure of 2.1 dB at 2.4 GHz when operated from a 48 V supply. Gate leakage current was found to be an important noise source.
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85.30.Tv Field effect devices
85.30.De Semiconductor-device characterization, design, and modeling
84.30.Le Amplifiers

Improvement of electrical and optical properties of p-GaN Ohmic metals under ultraviolet light irradiation annealing processes

S. W. Chae, S. K. Yoon, J. S. Kwak, Y. H. Park, and T. G. Kim

J. Vac. Sci. Technol. A 24, 634 (2006); http://dx.doi.org/10.1116/1.2183192 (3 pages) | Cited 2 times

Online Publication Date: 4 May 2006

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We report the improvement of electrical and optical properties of p-GaN Ohmic metals, ZnNi(10 nm)/Au(10 nm), by ultraviolet (UV) light irradiation. After UV light irradiation, the specific contact resistance of p-GaN decreased slightly from 2.99×10−4 to 2.54×10−4 Ω cm2, while the transmittance of the contact layer increased form 75% to 85% at a wavelength of 460 nm. In addition, the forward voltage of InGaN/GaN light-emitting diode chip at 20 mA decreased from 3.55 to 3.45 V, and the output power increased form 18 to 25 mW by UV light irradiation. The low resistance and high transmittance of the p-GaN Ohmic metals are attributed to the reduced Shottky barrier by the formation of gallium oxide and the increased oxidation of p-Ohmic metals, respectively, due to ozone generated form oxygen during UV light irradiation.
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73.40.Ns Metal-nonmetal contacts
78.66.Fd III-V semiconductors
73.40.Cg Contact resistance, contact potential
85.60.Jb Light-emitting devices
73.30.+y Surface double layers, Schottky barriers, and work functions
61.82.Fk Semiconductors

Nitride-based ultraviolet metal-semiconductor-metal photodetectors with low-temperature GaN cap layers and Ir/Pt contact electrodes

S. J. Chang, C. L. Yu, C. H. Chen, P. C. Chang, and K. C. Huang

J. Vac. Sci. Technol. A 24, 637 (2006); http://dx.doi.org/10.1116/1.2162560 (4 pages) | Cited 3 times

Online Publication Date: 4 May 2006

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Nitride-based ultraviolet (UV) metal-semiconductor-metal photodetectors (PDs) with low-temperature (LT) GaN cap layers and Ir/Pt contact electrodes have been fabricated. It was found that both Ir/Pt contact electrodes and LT GaN cap layers could effectively suppress the dark current of the PDs. We also achieved larger photocurrent to dark current contrast ratio and larger UV to visible rejection ratio from the PDs with LT GaN cap layers and Ir/Pt contact electrodes.
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85.60.Gz Photodetectors (including infrared and CCD detectors)

Visible-blind ultraviolet imagers consisting of 8×8 AlGaN p-i-n photodiode arrays

K. C. Kim, Y. M. Sung, I. H. Lee, C. R. Lee, M. D. Kim, Y. Park, and T. G. Kim

J. Vac. Sci. Technol. A 24, 641 (2006); http://dx.doi.org/10.1116/1.2192523 (4 pages) | Cited 1 time

Online Publication Date: 4 May 2006

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We report successful development of both discrete ultraviolet (UV) photodiodes and UV imagers consisting of 8×8 backside-illuminated AlGaN p-i-n photodiode arrays. The discreteAlGaN p-i-n photodiodes showed a responsivity of 0.1 A/W, a cutoff wavelength of 350 nm, an external quantum efficiency of 35%, and a response time of 4.1 ns. Then, 8×8 AlGaN p-i-n photodiode arrays were fabricated, followed by hybridizations with readout integrated circuits manufactured using a 0.5 μm 2poly-3metal N-well complementary metal-oxide semiconductor process by gold stud bumping. The 8×8 focal plane array UV imagers operated successfully by sensing radiation in the 300–350 nm spectral bands.
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85.60.Dw Photodiodes; phototransistors; photoresistors
back to top Organic Materials and Devices

Molecular model T6:C60 bulk-heterojunction solar cells

S. Alem, A. K. Pandey, K. N. N. Unni, J.-M. Nunzi, and P. Blanchard

J. Vac. Sci. Technol. A 24, 645 (2006); http://dx.doi.org/10.1116/1.2183160 (4 pages) | Cited 7 times

Online Publication Date: 4 May 2006

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Organic photovoltaic devices offer a large technological potential as a renewable source of electrical energy because of their low cost and ease of processing. For the last few years, the interest in such devices has grown rapidly, allowing multiplication of the solar conversion efficiency by 5 within about 10 years. The highest conversion efficiency obtained is now close to 5% with a spin-coated polythiophene-fullerene blend. For a better understanding of those polymer blend systems, we have fabricated a coevaporated solar cell from model molecules. The molecular blend was composed of sexithiophene (α,α-dihexylsexithiophene, T6) as a donor and fullerene C60 as an acceptor. The influence of the T6:C60 proportion was studied for an active layer of 100 nm thickness. The conversion efficiency obtained with the optimal proportion of T6:C60 (40–60) is 0.7%. Reverse bias annealing effect was studied by measuring the current-voltage characteristics after each postprocessing step. The conversion efficiency reached 1% but still remained much less than for the polymer bulk heterojunction. This major difference may come from the spontaneous phase separation which takes place in polymers to form an interpenetrated network.
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84.60.Jt Photoelectric conversion

Charge localization in polymeric metal-oxide-semiconductor capacitors

O. Marinov, M. J. Deen, B. Iniguez, and B. Ong

J. Vac. Sci. Technol. A 24, 649 (2006); http://dx.doi.org/10.1116/1.2172929 (5 pages) | Cited 5 times

Online Publication Date: 4 May 2006

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Charge enhancement of organic materials that was deduced more than two decades ago by means of capacitance-voltage (C-V) measurements meets with difficulties and controversial explanations when using the classical semiconductor theory. Experimentally, it has been found that the charge localization results in nonstationary and frequency-dependent behavior in the C-V measurements. Detailed analyses of the experimental results provide insight on how to interpret the quantities for concentration and relaxation time of charges in organic semiconductors. The experimental results indicate that the charge localization and conduction occur mainly in the bulk of the poly(3,3‴-didodecyl-quaterthiophene) (PQT) semiconducting polymer.
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84.32.Tt Capacitors
85.30.Tv Field effect devices

Hole mobility and electroluminescence properties of a dithiophene indenofluorene

C. Py, T. C. Gorjanc, T. Hadizad, J. Zhang, and Z. Y. Wang

J. Vac. Sci. Technol. A 24, 654 (2006); http://dx.doi.org/10.1116/1.2180265 (3 pages) | Cited 1 time

Online Publication Date: 4 May 2006

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The development of organic laser diodes requires the availability of organic thin films that can attain high mobility without luminescence quenching. A dithiophene-substituted indenofluorene compound was designed as a compromise between luminous efficiency and mobility and has been studied in organic light-emitting diode and organic field-effect transistor devices. A relatively high luminous efficiency of 1 cd/A at a luminance of 1400 cd/m2 and a hole field-effect mobility of 1.2×10−2 cm2/Vs are reported in those two respective devices.
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85.60.Jb Light-emitting devices
85.30.Tv Field effect devices

Photolithographically defined polythiophene organic thin-film transistors

Flora M. Li, Yuri Vygranenko, Sarswati Koul, and Arokia Nathan

J. Vac. Sci. Technol. A 24, 657 (2006); http://dx.doi.org/10.1116/1.2165653 (6 pages) | Cited 4 times

Online Publication Date: 4 May 2006

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A photolithography process for the fabrication of organic thin-film transistor (OTFT) and integrated circuits will be presented. Fully encapsulated polythiophene OTFTs in the top-gate, bottom-gate, and dual-gate configurations have been demonstrated using this approach. Photolithography steps are incorporated for the definition of gate electrodes and source/drain contacts, isolation of transistors, and formation of vias and interconnects. These steps are vital to achieve device integration and to realize organic integrated circuits for applications such as flat panel displays and radio-frequency identification tags. The fabrication process is compatible with various substrates (e.g., glass and plastic), and enables the realization of discrete transistors and OTFT-based circuits through consecutive photolithographic steps and a tailored etch recipe for patterning of the polymer film. This article will provide a detailed examination of the fabrication approach, analyze the electrical performance of various photolithographically defined regioregular poly(3-hexylthiophene) OTFT structures, and explore the device and circuit advantages of the photolithography strategy.
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85.30.Tv Field effect devices
85.40.Hp Lithography, masks and pattern transfer
back to top Characterization of Devices and Materials

Probing the composition of Ge dots and Si/Si1−xGex island superlattices

J.-M. Baribeau, X. Wu, and D. J. Lockwood

J. Vac. Sci. Technol. A 24, 663 (2006); http://dx.doi.org/10.1116/1.2186658 (5 pages) | Cited 9 times

Online Publication Date: 4 May 2006

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We use analytical transmission electron microscopy to map the composition of Ge dot and Si/Si1−xGex island structures grown on (001) Si by molecular beam epitaxy or ultrahigh vacuum chemical vapor deposition. Energy-dispersive x-ray spectroscopy reveals that nominally pure Ge dots grown by molecular beam epitaxy at 650 °C exhibit considerable intermixing with the average Ge composition typically increasing from nearly zero at the base to about 50% at the top of the dot. In pyramid shaped dots, the Ge composition increases linearly up to the top of the dot, while for dome dots, a saturation of the incorporation rate is seen beyond a distance of 7 nm from the substrate interface. Probing of Si/Si1−xGex island superlattices also reveals large Si/Ge intermixing with a Ge accumulation at the crest and Ge depletion at the troughs of the islands. These results are corroborated by x-ray diffraction and Raman scattering measurements.
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68.65.Hb Quantum dots (patterned in quantum wells)
68.65.Cd Superlattices
66.30.Ny Chemical interdiffusion; diffusion barriers
68.35.Fx Diffusion; interface formation
82.80.Ej X-ray, Mössbauer, and other γ-ray spectroscopic analysis methods

Organic monolayers detected by single reflection attenuated total reflection infrared spectroscopy

N. L. Rowell, L. Tay, D. J. Lockwood, J.-M. Baribeau, J. A. Bardwell, and R. Boukherroub

J. Vac. Sci. Technol. A 24, 668 (2006); http://dx.doi.org/10.1116/1.2180270 (5 pages) | Cited 5 times

Online Publication Date: 4 May 2006

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A single-reflection attenuated total reflection (ATR) technique has been used to study low index monolayers with a high index ATR hemisphere in an optical contact with the sample surface. A model calculation predicts a field enhancement with the present method substantially larger than that of conventional ATR. For the present method, a discontinuity of the field normal to the film is responsible for the field enhancement in the lower index thin film. We show theoretically and experimentally that the angle of incidence has a strong influence on the ATR signal strength. We demonstrate the present method by examining the infrared reflectance spectra of a undecylenic acid self-assembled on Si (111) and with the adsorption of a bovine serum albumin monolayer. We also apply the method to examine the oxidation and surface contamination of the functionalized Si samples stored in ambient conditions.
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81.05.Lg Polymers and plastics; rubber; synthetic and natural fibers; organometallic and organic materials
81.05.Cy Elemental semiconductors
68.43.Mn Adsorption kinetics
78.30.Jw Organic compounds, polymers
81.65.Mq Oxidation

Dynamic electrostatic force-gradient microscopy employing mechanoelectric cross modulation

Z. Weng, T. Kaminski, G. E. Bridges, and D. J. Thomson

J. Vac. Sci. Technol. A 24, 673 (2006); http://dx.doi.org/10.1116/1.2180268 (5 pages)

Online Publication Date: 4 May 2006

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This article describes a dynamic mode electrostatic force-gradient microscopy technique capable of high-frequency voltage measurement. The technique employs a wide-bandwidth implementation of a mechanoelectric cross-modulation scheme, where a microfabricated probe is driven by an amplitude-modulated sampling pulse and the sample is mechanically vibrated at a frequency different to that of electrical modulation. The resulting probe oscillation at the cross-modulation frequency provides local high-frequency voltage information. Unlike the force detection method, which is susceptible to poor resolution due to large coupling to the probe tip sidewall and cantilever, the force-gradient method provides an enhancement of spatial resolution. A significant reduction of interference from adjacent signal traces is demonstrated when performing integrated circuit testing. Quantitative high-frequency voltage measurement with high accuracy is achieved by using a null-force-gradient approach, but at the expense of reduced sensitivity.
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07.79.-v Scanning probe microscopes and components
84.37.+q Measurements in electric variables (including voltage, current, resistance, capacitance, inductance, impedance, and admittance, etc.)
85.40.Qx Microcircuit quality, noise, performance, and failure analysis

Characteristics of remote plasma atomic layer-deposited HfO2 films on O2 and N2 plasma-pretreated Si substrates

Jihoon Choi, Seokhoon Kim, Jinwoo Kim, Hyunseok Kang, Hyeongtag Jeon, and Choelhwyi Bae

J. Vac. Sci. Technol. A 24, 678 (2006); http://dx.doi.org/10.1116/1.2194029 (4 pages) | Cited 1 time

Online Publication Date: 4 May 2006

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Characteristics of remote plasma atomic layer-deposited HfO2 on Si, which has a very thin SiO2 interlayer with and without remote plasma nitridation, have been investigated. The thin ( ∼ 1.5 nm) intermediate layer containing nitrogen, which was prepared by sequential O2 and N2 remote plasma treatment of the Si substrate, can effectively suppress growth of the unintentional interface layer. In addition, it enhances the thermal stability and the resistance to oxygen diffusion during rapid thermal annealing. The HfO2 film containing the remote plasma nitrided SiO2 interlayer annealed at 800 °C showed a lower equivalent oxide thickness of ∼ 1.89 nm and a lower leakage current density (3.78×10−7A cm−2 at VGVFB∣ = 2 V) compared to a non-nitrided sample of the same physical thickness. Also, we compared the characteristics of HfO2 films annealed in two different ambient environments, N2 and O2.
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77.84.Bw Elements, oxides, nitrides, borides, carbides, chalcogenides, etc.
77.55.-g Dielectric thin films
52.77.Dq Plasma-based ion implantation and deposition
68.55.-a Thin film structure and morphology
61.72.Cc Kinetics of defect formation and annealing
81.65.Lp Surface hardening: nitridation, carburization, carbonitridation

Annealing temperature effect on the performance of nonvolatile HfO2 Si-oxide-nitride-oxide-silicon-type flash memory

Yu-Hsien Lin, Chao-Hsin Chien, Chun-Yen Chang, and Tan-Fu Lei

J. Vac. Sci. Technol. A 24, 682 (2006); http://dx.doi.org/10.1116/1.2174021 (4 pages) | Cited 7 times

Online Publication Date: 4 May 2006

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In this article, we demonstrate the effect of the postdeposition annealing for the HfO2 trapping layer on the performance of the Si-oxide-nitride-oxide-silicon-type flash memories. It was found that the memory window becomes larger while the retention and endurance characteristics get worse as the annealing temperature increases. This was ascribed to the larger amount and the shallower energy levels of the crystallization-induced traps as compared to the traps presented in the as-fabricated HfO2 film. Finally, in the aspect of disturbances, we show only insignificant read, drain, and gate disturbances presented in the three samples in the normal operation.
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85.30.Tv Field effect devices
84.30.Sk Pulse and digital circuits

Time resolved electroluminescence measurements on GaAs and GaN devices

J. E. Hulse, K. Sarault, N. L. Rowell, M. Simard-Normandin, and J. A. Bardwell

J. Vac. Sci. Technol. A 24, 686 (2006); http://dx.doi.org/10.1116/1.2172931 (4 pages)

Online Publication Date: 4 May 2006

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Time correlated single photon electroluminescence maps have been recorded on operating semiconductor devices with a spatial resolution approaching 1 μm and a time resolution of 50 ps. The technique is noninvasive and observes signal wave forms optically, directly at the device. Spectral measurements in the near infrared and visible were also performed. Two examples of the application of this technique to semiconductor devices are presented. An AlGaAs/GaAs heterojunction bipolar transistor typical of high speed bipolar devices used in rf circuitry, and an AlGaN/GaN heterostructure field-effect transistor as an example of the application of optical techniques in characterizing the emerging technology.
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85.30.Pq Bipolar transistors
85.30.Tv Field effect devices
85.30.De Semiconductor-device characterization, design, and modeling

Performance and potential of germanium on insulator field-effect transistors

D. S. Yu, H. L. Kao, A. Chin, and S. P. McAlister

J. Vac. Sci. Technol. A 24, 690 (2006); http://dx.doi.org/10.1116/1.2167978 (4 pages)

Online Publication Date: 4 May 2006

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The performance of field-effect transistors may be improved by increasing the channel mobility. Strained Si can accomplish this but Ge is another option. Here we show data for germanium-on-insulator (GOI) devices and also describe the simple bonding process which was used in the device fabrication. The GOI devices show better mobilities than their Si counterparts. We also show data for some metal-gate/high-κ dielectric devices on a GOI layer fabricated on a processed Si wafer. Here the GOI structure and processing does not alter the underlying Si devices and yet gives devices whose mobilities exceed those of Si devices. Simulations support the view that the improved performance results from the mobility enhancement and that the performance should also hold for submicron devices.
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85.30.Tv Field effect devices
73.40.Qv Metal-insulator-semiconductor structures (including semiconductor-to-insulator)
73.50.Dn Low-field transport and mobility; piezoresistance
back to top Nanostructures and Nanotechnology

Microstructure investigations of indium tin oxide films cosputtered with zinc oxide at room temperature

Day-Shan Liu, Chun-Hsing Lin, Fu-Chun Tsai, and Chun-Ching Wu

J. Vac. Sci. Technol. A 24, 694 (2006); http://dx.doi.org/10.1116/1.2194030 (6 pages) | Cited 5 times

Online Publication Date: 4 May 2006

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X-ray diffraction coupled with atomic force microscopy measurements were employed to investigate the cosputtered oxide films at various zinc content [Zn/(Zn+In) at. %] atomic ratios prepared at room temperature using rf cosputtering indium tin oxide (ITO) and zinc oxide (ZnO) targets simultaneously. The crystalline structure of a pure ITO film is polycrystalline with obvious diffraction peaks of (222) and (400). As the atomic ratio reaches 26%, the cosputtered oxide film evolves from a polycrystalline ITO structure into an amorphouslike ZnkIn2Ok+3 structure. This structure also dominates the cosputtered oxide films at the atomic ratios raging from 26% to 54%. The formation of amorphouslike ZnkIn2O3+k structures is found to markedly reduce the associated film resistivity and performs a superior surface uniformity. At an atomic ratio of 60%, a diffraction peak identifies as ZnO (100) phase appears to pile on the original amorphous domain. This phase is attributed to the substitution of In3+ sites in the ITO structure unit by Zn2+ ions. The appearance of ZnO phase is responsible for the increase of film resistivity. In addition, the smooth surface roughness contributed from the amorphous structures is therefore roughened due to the appearance of the microcrystalline ZnO structures. While the atomic ratio increases to 71%, the surface roughness and resistivity are found to further increase due to the growth of ZnO (100) phase. The optical absorption edge of these cosputtered oxide films shows an apparent redshift at ultraviolet wavelengths with incremental ZnO contents incorporating into ITO films.
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68.55.-a Thin film structure and morphology
73.61.Ga II-VI semiconductors
68.37.Ps Atomic force microscopy (AFM)
61.43.Dq Amorphous semiconductors, metals, and alloys
68.35.B- Structure of clean surfaces (and surface reconstruction)
78.40.Ha Other nonmetallic inorganics

Rapid thermal annealing of InAs/GaAs quantum dots with a low-temperature-grown InGaP cap layer

W. H. Jiang, D. A. Thompson, O. Hul’ko, B. J. Robinson, and P. Mascher

J. Vac. Sci. Technol. A 24, 700 (2006); http://dx.doi.org/10.1116/1.2165655 (4 pages) | Cited 5 times

Online Publication Date: 4 May 2006

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A single layer of self-assembled InAs quantum dots was grown on a GaAs (001) substrate by gas source molecular-beam epitaxy. The quantum dots were overgrown with 65 nm GaAs, 25 nm InGaP, and a 10 nm GaAs etch-stop layer. This was either uncapped or capped with 100 nm of low-temperature (LT)-grown, lattice-matched InGaP (LT-InGaP) or with a SiO2 layer or Al2O3 layer. Photoluminescence (PL) measurements were made on samples before and after rapid thermal annealing at 550–900 °C and for 15–120 s at 650 °C. Samples capped with LT-InGaP showed a significant blueshift of the PL peak wavelength for anneals above 575 °C. By comparison, for the SiO2-capped and uncapped samples, the net blueshift only becomes significant for anneals >700 °C, while an Al2O3 cap actually reduces the blueshift and suppresses the intermixing. It appears that the best conditions for spatially controlling the quantum dot intermixing occur with annealing at low temperatures (600–650 °C).
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81.07.Ta Quantum dots
81.05.Ea III-V semiconductors
61.72.Cc Kinetics of defect formation and annealing
81.15.Hi Molecular, atomic, ion, and chemical beam epitaxy
78.67.Hc Quantum dots
78.55.Cr III-V semiconductors

Observation of resonant tunneling through a self-assembled InAs quantum dot layer

B. Aslan, H. C. Liu, J. A. Gupta, Z. R. Wasilewski, G. C. Aers, S. Raymond, and M. Buchanan

J. Vac. Sci. Technol. A 24, 704 (2006); http://dx.doi.org/10.1116/1.2167085 (4 pages)

Online Publication Date: 4 May 2006

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We report on the study of resonant tunneling through a self-assembled InAs quantum dot (QD) layer using the following design: The QD layer surrounded by undoped GaAs barriers is clad by two GaInNAs/GaAs short-period superlattice regions which serve as injector and collector of electrons. A clear observation of three- to zero-dimensional resonant tunneling is presented in electrophotoluminescence measurement results and supported with current-voltage and capacitance-voltage characteristics.
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73.63.Kv Quantum dots
73.40.Gk Tunneling
78.67.Hc Quantum dots
78.60.Fi Electroluminescence
78.55.Cr III-V semiconductors

Switching-speed calculations for Schottky-barrier carbon nanotube field-effect transistors

D. L. John and D. L. Pulfrey

J. Vac. Sci. Technol. A 24, 708 (2006); http://dx.doi.org/10.1116/1.2194932 (5 pages) | Cited 4 times

Online Publication Date: 4 May 2006

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The switching times and on/off-current ratios are computed for Schottky-barrier carbon nanotube field-effect transistors with different tube diameters and insulator thicknesses. It is indicated that it may be difficult to obtain a device exhibiting both high speed and low leakage current. A small-diameter nanotube with a thin insulator may offer the best compromise. It is also demonstrated that interelectrode capacitances can be large, thereby calling into question the usefulness of the intrinsic switching time as a figure of merit for transistors intended for digital-logic applications. The extrinsic switching time is a more appropriate metric and it is shown here that considerable optimization of the carbon nanotube field-effect transistor will be required to achieve figures better than for modern Si complementary metal-oxide-semiconductor transistors over a reasonable range of on/off-current ratio.
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85.35.Kt Nanotube devices
73.30.+y Surface double layers, Schottky barriers, and work functions

Photoluminescence in the silicon-oxygen system

A. Meldrum, A. Hryciw, A. N. MacDonald, C. Blois, K. Marsh, J. Wang, and Quan Li

J. Vac. Sci. Technol. A 24, 713 (2006); http://dx.doi.org/10.1116/1.2162563 (5 pages) | Cited 16 times

Online Publication Date: 4 May 2006

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The luminescent properties of SiOx ranging in composition between x = 0 and x = 2 are presented. Luminescence in the SiOx system is found to be tunable across the full visible spectrum and into the near infrared. The data are used to generate an emission color map for the complete SiOx system. At the lower annealing temperatures, several lines of evidence suggest that the luminescence is due to the presence of amorphous silicon nanoclusters, whereas for higher annealing temperatures the emission is dominated by silicon nanocrystals.
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78.55.Hx Other solid inorganic materials
78.55.Ap Elemental semiconductors
78.55.Qr Amorphous materials; glasses and other disordered solids
78.67.Bf Nanocrystals, nanoparticles, and nanoclusters
61.72.Cc Kinetics of defect formation and annealing
back to top Microfabrication, Micromachining, and MEMS

Fabrication of out-of-plane micromirrors in silicon-on-insulator planar waveguides

B. Lamontagne, P. Cheben, E. Post, S. Janz, D.-X. Xu, and A. Delâge

J. Vac. Sci. Technol. A 24, 718 (2006); http://dx.doi.org/10.1116/1.2186656 (5 pages) | Cited 3 times

Online Publication Date: 4 May 2006

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Emerging optical waveguide spectrometers, sensors, and biochips require the simultaneous acquisition of numerous optical signals. Aligning many tens or hundreds of optical fibers to waveguides is a formidable and costly exercise in packaging. We propose a data acquisition scheme using arrays of micromirrors to redirect light propagating in each waveguide out of the device surface, where all the beams can be collected by a single imaging array. Micromirrors, which are the key elements in this data acquisition scheme, were fabricated in 2 μm thick silicon-on-insulator waveguides. Chemically assisted ion beam etching (CAIBE) was used to obtain inclined mirror facets, benefiting from the unique capability of CAIBE to tilt the sample relative to the ion beam. Finite difference time domain (FDTD) simulations of an ideal micromirror oriented at 45° to the propagation direction predict a >96% out-coupling efficiency (loss of 0.14 dB) and a negligible polarization dependent loss (PDL). The measured total insertion loss for the fabricated waveguide and mirror was −5 dB, including fiber-to-waveguide coupling loss, waveguide propagation loss, and mirror loss due to fabrication errors and diffraction, with a PDL of 0.7 dB. The dependence of micromirror performance on facet angle and etch depth was studied by FDTD simulations. The influence of CAIBE etching chemistry and selectivity in obtaining optimum mirror parameters is discussed.
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42.79.Bh Lenses, prisms and mirrors
42.82.Cr Fabrication techniques; lithography, pattern transfer
42.82.Et Waveguides, couplers, and arrays
42.79.Gn Optical waveguides and couplers
81.65.Cf Surface cleaning, etching, patterning
42.81.Qb Fiber waveguides, couplers, and arrays

Formation of nanoscale columnar structures in silicon by a maskless reactive ion etching process

M. Gharghi and S. Sivoththaman

J. Vac. Sci. Technol. A 24, 723 (2006); http://dx.doi.org/10.1116/1.2167974 (5 pages) | Cited 11 times

Online Publication Date: 4 May 2006

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We describe a maskless reactive ion etching process that employs CF4 gas plasma to create nanoscale structures in silicon. Process conditions are controlled to produce pillars of up to 2 μm tall and less than 50 nm wide. The contributing mechanisms are discussed based on the trends observed for varying plasma conditions. Higher pressures or lower self-bias voltages result in pyramidal structures. Lower pressure and higher voltage result in needlelike structures that resemble silicon wires. By carefully controlling the automasking process mechanism, columnar silicon structures were reproducibly formed with good uniformity all over the wafer. The regularity of the fabricated structures, process controllability, and process compatibility of dry etching are promising for potential photonic and optoelectronic applications.
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81.07.Bc Nanocrystalline materials
81.05.Cy Elemental semiconductors
81.16.-c Methods of micro- and nanofabrication and processing
81.65.Cf Surface cleaning, etching, patterning
52.77.Bn Etching and cleaning

Inductively coupled plasma etching of Si1−xGex in CF4/Ar and Cl2/Ar discharges

San Lein Wu, Chun Hsin Lee, Shoou Jinn Chang, and Yu Min Lin

J. Vac. Sci. Technol. A 24, 728 (2006); http://dx.doi.org/10.1116/1.2180266 (4 pages)

Online Publication Date: 4 May 2006

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In this article, we report the experimental realization of SiGe/Si materials using CF4/Ar and Cl2/Ar mixed-gas inductively coupled plasma (ICP) etching process. The effects of process parameters such as gas combination and gas species on etch rates and selectivities were investigated. It was found that samples in CF4 gas result in a faster etching rate than those obtained in Cl2 gas, which are responsible for a lower boiling point for Si-based fluoride. The lower boiling point provides more chemically active Si and SiGe materials. Moreover, the selectivity of 1.5 between Si0.3Ge0.7/Si by ICP technology was found and higher than that obtained previously by reactive ion etching reported in the literature. Based on these etch characteristics, the application of the ICP process to the device fabrication of SiGe doped-channel field-effect transistors was conducted. The devices using ICP mesa have excellent pinch-off characteristics with relatively low leakage current, small output conduction in the saturated region, and low knee voltage.
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81.05.Hd Other semiconductors
81.05.Cy Elemental semiconductors
85.30.Tv Field effect devices
52.77.Bn Etching and cleaning
81.65.Cf Surface cleaning, etching, patterning

Direct evidence of “spring softening” nonlinearity in micromachined mechanical resonator using optical beam deflection technique

J. H. Zhao, G. E. Bridges, and D. J. Thomson

J. Vac. Sci. Technol. A 24, 732 (2006); http://dx.doi.org/10.1116/1.2194934 (5 pages) | Cited 5 times

Online Publication Date: 4 May 2006

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In this article the dynamic behavior of clamped-clamped micromachined mechanical resonators working at a frequency of 150 kHz was characterized by electrostatic excitation and detection via both capacitive coupling and optical methods. The experimental results by optical measurement show that this system behaved very much like a simple harmonic oscillator at low actuation levels while significant nonlinearity was observed at higher actuation levels. The nonlinearity identified as “spring softening” type occurred when the product of the dc bias voltage and the ac driving voltage exceeded 0.04 V2. Dependence of resonance frequency on dc bias voltage was investigated and the experimental results are in agreement with theoretical predictions. This work also demonstrated that optical detection is much less susceptible to parasitic interference than motion detection via capacitive coupling. Therefore, optical techniques will yield better characterization of the mechanical properties of the resonators.
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07.10.Cm Micromechanical devices and systems
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices

Microelectrode arrays for two-dimensional polar movement of microparticles in water

Andre Belisle, Matthew Brown, Ted Hubbard, and Marek Kujath

J. Vac. Sci. Technol. A 24, 737 (2006); http://dx.doi.org/10.1116/1.2180271 (5 pages) | Cited 3 times

Online Publication Date: 4 May 2006

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This article demonstrates the circular movement of microparticles in water using radial microelectromechanical system electrode arrays. The particles are moved in two polar dimensions, θ and r, by ac electro-osmosis. It is observed that initially particles circle rapidly above the array and move slowly radially to finally form a thin ring at an equilibrium radius. Three-dimensional computational fluid dynamics simulations are performed, cross sectional information is extracted to obtain tangential (Uθ) velocity as a function of r. Orbital velocity and equilibrium radius measurements are performed at various voltages. Velocities and radii are found to be in general agreement with the simulated results.
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47.61.Fg Flows in micro-electromechanical systems (MEMS) and nano-electromechanical systems (NEMS)
07.10.Cm Micromechanical devices and systems
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices
82.45.-h Electrochemistry and electrophoresis
82.39.Wj Ion exchange, dialysis, osmosis, electro-osmosis, membrane processes
47.11.-j Computational methods in fluid dynamics

Fabricating multilevel SU-8 structures in a single photolithographic step using colored masking patterns

J. Taff, Y. Kashte, V. Spinella-Mamo, and M. Paranjape

J. Vac. Sci. Technol. A 24, 742 (2006); http://dx.doi.org/10.1116/1.2172927 (5 pages) | Cited 3 times

Online Publication Date: 4 May 2006

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The fabrication of multilevel SU-8 structures using a single photolithographic masking step is described. Preliminary data are presented on the use of photolithographic masks, containing millimeter-scale colored patterns, printed on transparent films using a standard color laser printer. The different colors printed on the photomask are shown to have differences in their UV absorptions, and hence different structure levels can be achieved from a single exposure. This method eliminates the pixelation problems encountered when using gray-scale masks (without employing photoreduction techniques) generated using a black-and-white laser printer. For research applications requiring rapid prototyping and fast turnaround times for large-scale features, this technique offers a cost-effective and time-efficient alternative to current three-dimensional lithography methods, which typically make use of multiple binary masks, alignment procedures, and exposures. Future applications will include the fabrication of textured PDMS surfaces and PDMS microfluidic substrates, cast from SU-8 molds processed using this technique.
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85.40.Hp Lithography, masks and pattern transfer
42.82.Cr Fabrication techniques; lithography, pattern transfer
back to top Sensors and Microelectronic Devices

In situ monitoring of protein adsorption on functionalized porous Si surfaces

L. Tay, N. L. Rowell, D. J. Lockwood, and R. Boukherroub

J. Vac. Sci. Technol. A 24, 747 (2006);