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Jul 2010

Volume 28, Issue 4, pp. L31-C5I9

Issue Cover Spotlight Figure

J. Vac. Sci. Technol. B 28, C5D1 (2010); http://dx.doi.org/10.1116/1.3456176 (8 pages)

J. E. Baio, T. Weidner, N. T. Samuel, Keith McCrea, Loren Baugh, Patrick S. Stayton, and David G. Castner
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Scatterometric porosimetry: A new characterization technique for porous material patterned structures

R. Bouyssou, M. El Kodadi, C. Licitra, T. Chevolleau, M. Besacier, N. Posseme, O. Joubert, and P. Schiavone

J. Vac. Sci. Technol. B 28, L31 (2010); http://dx.doi.org/10.1116/1.3457489 (4 pages)

Online Publication Date: 12 July 2010

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A new technique, so called “scatterometric porosimetry” (SP) has been developed to improve our knowledge on the properties of porous material patterned structures. None of the existing techniques is able to characterize the porous material structures after patterning. SP is based on the measurement of the refractive index variation of porous material structures (lines and holes) when filled with a solvent (toluene, methanol, and water). This technique is applied to monitor the modifications in low-K dielectric materials (porous SiOCH) after the plasma patterning steps used to form lines and vias in the porous materials in a typical dual damascene CMOS technology process.
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81.05.Rm Porous materials; granular materials
61.43.Gt Powders, porous materials

Electric field induced motion of metallic droplets: Application to submicron contactor

H. Dallaporta, M. Prestigiacomo, F. Bedu, D. Tonneau, D. Chatain, and P. Sudraud

J. Vac. Sci. Technol. B 28, L35 (2010); http://dx.doi.org/10.1116/1.3462963 (4 pages)

Online Publication Date: 19 July 2010

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This article reports the monitoring of reversible displacement of a gallium droplet on a tungsten submicron wire deposited by focused ion beam from tungsten hexacarbonyl precursor. The authors demonstrate that by applying a voltage to the wire terminals, the internal electric field created along the wire produces the motion of the droplet. Since the matter involved in this displacement is conductive, the authors show that it is possible to build a submicron electrical switch. Contact can be switched on and off between two electrodes separated by a submicron gap, by electrical monitoring the position of the conductive droplet.
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73.63.Nm Quantum wires
81.07.Gf Nanowires
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Continuous cell air-extracting technique used for fast cell filling of flexible liquid-crystal displays

Wen-Tuan Wu, Chia-Jen Chang, Hsyi-En Cheng, Ching-Ming Hsu, and Kun-San Tsen

J. Vac. Sci. Technol. B 28, 673 (2010); http://dx.doi.org/10.1116/1.3437008 (5 pages)

Online Publication Date: 28 June 2010

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A continuous cell air-extracting technique (CCAE) has been successfully applied for cell filling of flexible liquid-crystal displays. This CCAE technique can conduct cell filling of liquid crystals in an atmospheric ambient and keep cell pressure constant during the entire cell-filling period. Cell-filling efficiency was found to be dependent on cell pressure, spacer-area density, and injection-port width at room temperature. A filling time of 141 s was achieved for a polyethylene-terephthalate substrate with a 67×55 mm2 cell at a constant cell pressure of 2 torr, which is faster than the traditional method by at least a factor of 2. The enhanced cell-filling efficiency is mainly attributed to the fact that the flow speed of liquid crystal is not largely reduced in the cell because of the constant cell pressure. The cell-filling efficiency was, however, found to be limited by cell-deformation-caused cell resistance.
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85.60.Pg Display systems
61.30.-v Liquid crystals
42.79.Kr Display devices, liquid-crystal devices
42.70.Df Liquid crystals

Semiconductor-superconductor transition and magnetoresistance terraces in an ultrathin superconducting Pb nanobridge

Jian Wang, Jin-Feng Jia, Xu-Cun Ma, Quan-Tong Shen, Tie-Zhu Han, Ai-Zi Jin, Li Lu, Chang-Zhi Gu, Ming-Liang Tian, X. C. Xie, and Qi-Kun Xue

J. Vac. Sci. Technol. B 28, 678 (2010); http://dx.doi.org/10.1116/1.3437016 (4 pages)

Online Publication Date: 28 June 2010

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Using focused ion beam etching technique, the authors fabricated a 28 atomic monolayers thick, 500 nm wide, and 10 μm long Pb nanobridge from an atomically flat Pb thin film grown on Si by molecular beam epitaxy. Electric transport measurements show exotic resistance oscillations in the superconducting state far below its critical field HC and cascading terraces near the superconducting transition region. Furthermore, the bridge shows an unusual semiconducting behavior above the superconducting transition temperature TC. The results are in contrast to those observed in its counterpart of the two-dimensional thin film.
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85.25.-j Superconducting devices
74.62.-c Transition temperature variations, phase diagrams
81.65.Cf Surface cleaning, etching, patterning
81.15.Hi Molecular, atomic, ion, and chemical beam epitaxy
72.20.My Galvanomagnetic and other magnetotransport effects
68.55.ag Semiconductors

Multistage etching process for microscopically smooth tellurite glass surfaces in optical fibers

Aidong Zhang, Aoxiang Lin, Jau-Sheng Wang, and Jean Toulouse

J. Vac. Sci. Technol. B 28, 682 (2010); http://dx.doi.org/10.1116/1.3437017 (5 pages)

Online Publication Date: 28 June 2010

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Bulk samples of tellurite glass with composition 75TeO2–20ZnO–5Na2O (TZN) were fabricated by melting and quenching techniques. In order to improve the surface quality of optical fiber preform made with this tellurite glass, the authors developed a multistage etching process. The relationship between successive etching treatments and roughness of the TZN glass surface was probed by using an atomic force microscope. The results demonstrate that this multistage etching method effectively improves this tellurite glass surface smoothness to a level comparable with that of a reference silica glass slide, and the corresponding chemical micromechanisms and fundamentals are discussed and confirmed by atomic force microscopy, potentially contributing to the development of multicomponent soft glass fibers and devices.
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81.65.Cf Surface cleaning, etching, patterning
64.70.dj Melting of specific substances
68.35.B- Structure of clean surfaces (and surface reconstruction)
42.81.Bm Fabrication, cladding, and splicing
81.40.Gh Other heat and thermomechanical treatments

Novel split-tip proximal probe for fabrication of nanometer-textured, in-plane oriented polymer films

Beverly Clark, III, M. P. Taylor, and H. D. Hallen

J. Vac. Sci. Technol. B 28, 687 (2010); http://dx.doi.org/10.1116/1.3437473 (6 pages)

Online Publication Date: 28 June 2010

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Novel fabrication schemes are required to deposit nanoscale materials that contain molecules oriented in the plane of the surface. The breakage of in-plane symmetry allows devices to be fabricated in this plane, enabling molecular electronics to follow this successful paradigm of semiconductor devices. The authors discuss here the fabrication of a unique split-tip optical nanoprobe that can be used to both orient molecules on a surface with a strong, localized electric field and deposit them with nanoscale resolution. Ultraviolet light injected through the probe into the region of aligned molecules causes the deposition. The production of the split-tip probe is significantly different than that of the related near-field scanning optical microscope (NSOM) probe, since the stresses in the metal layer must be held by the metal film–silica interface rather than within the film as it encircles the silica of a NSOM probe. Mounting of the probe to ensure reliable electrical contacts is also described.
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81.16.-c Methods of micro- and nanofabrication and processing
68.65.-k Low-dimensional, mesoscopic, nanoscale and other related systems: structure and nonelectronic properties
78.67.-n Optical properties of low-dimensional, mesoscopic, and nanoscale materials and structures

Simulations of radical and ion fluxes on a wafer in a Cl2/Ar inductively coupled plasma discharge: Confrontation with GaAs and GaN etch experiments

Emilie Despiau-Pujo, Pascal Chabert, Shailendra Bansropun, Didier Thénot, Patrick Plouhinec, and Simone Cassette

J. Vac. Sci. Technol. B 28, 693 (2010); http://dx.doi.org/10.1116/1.3437492 (9 pages) | Cited 1 time

Online Publication Date: 28 June 2010

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A two-dimensional fluid model is used to study an industrial Ar/Cl2 inductively coupled plasma discharge designed to etch III-V samples. The effect of rf power, gas pressure, and chlorine content on the fluxes of reactive species reaching the wafer is numerically investigated. To understand how the etch process is influenced by the discharge conditions, simulation results are confronted with GaAs and GaN etch experiments performed in the same reactor geometry. When the source power is increased, the measured etch rate increase is consistent with the Cl radical and ion fluxes increase shown in the simulation, as well as the ion energy decrease due to the constant value of the wafer-holder power. Increasing the gas pressure results in a moderate increase in the etch rate due to the lower magnitude, lower mean energy, and anisotropy of the ion flux at high pressure. When the chlorine content is increased, the total ion flux decreases while Cl and Cl2 neutral fluxes increase significantly. A good correlation is obtained between calculated fluxes and etch characteristics, analyzed with scanning electron microscope images of etch profiles.
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81.65.Cf Surface cleaning, etching, patterning
52.65.-y Plasma simulation
52.80.-s Electric discharges

Extension of active region in crossbar-type polymer solar photovoltaics induced by highly conductive PEDOT:PSS buffer layer

Tsung-Syun Huang, Chun-Yuan Huang, Yan-Kuin Su, Ying-Chih Chen, Jiun-Shiang Fang, and Ten-Chin Wen

J. Vac. Sci. Technol. B 28, 702 (2010); http://dx.doi.org/10.1116/1.3437506 (4 pages)

Online Publication Date: 28 June 2010

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The authors have demonstrated and estimated the extension of active region in P3HT:PCBM solar photovoltaics due to the increase in the conductivity of PEDOT:PSS. For the polymer photovoltaics with a crossbar-type electrode geometry, the excess photogenerated carriers outside the nominal active region have contributed the measured photocurrent and thus affected the derived power conversion efficiency. In this work, glycerol and dimethyl-sulfoxide were, respectively, incorporated into PEDOT:PSS to increase the conductivity and therefore improve the performance of the devices. The method of restrictively illuminating the partially shielded device was introduced to eliminate the excess photocurrent and well define the real active region. The extension of active area was also figured out by fitting the short-circuit current of shielded device.
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88.40.jr Organic photovoltaics
88.40.hj Efficiency and performance of solar cells

Atomic diffusion bonding of wafers with thin nanocrystalline metal films

T. Shimatsu and M. Uomoto

J. Vac. Sci. Technol. B 28, 706 (2010); http://dx.doi.org/10.1116/1.3437515 (9 pages)

Online Publication Date: 28 June 2010

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Bonding between two flat wafers with thin metal films was studied for 14 thin metal films with various crystal structures and self-diffusion coefficients. Thin nanocrystalline metal films were fabricated on two flat wafers’ surfaces using sputter deposition. Bonding of the two metal films on the wafers was accomplished immediately after film deposition in vacuum. For the films, Al, Au, Ag, Cu, Si, Co, Ni, Pt, Ti, Ru, Fe, Cr, Mo, and Ta were used. The wafers were bonded at room temperature over the entire bonded area (1 or 2 in. wafers of either Si or SiO2) using these metal films. Transmission electron microscopic cross-section images revealed that complete crystalline grains were formed across the original surfaces of the films, probably because of recrystallization occurring at the bonded interface when Al–Al, Ag–Ag, Au–Au, Cu–Cu, and Ti–Ti nanocrystalline films were bonded. A clear interface corresponding closely to the original film surface was visible in the bonded Pt–Pt films. However, fcc-(111) lattices were formed continuously across the films’ original surfaces. A thin amorphous layer was formed at the interfaces of Cr–Cr, Fe–Fe, and Ta–Ta bonded films. Experimental results revealed that the two films’ bonded structure was related closely to the self-diffusion coefficients of the metals used for bonding. A high atomic diffusion coefficient at the grain boundaries and film surfaces is likely to have enabled bonding at room temperature. Moreover, results obtained using Cu–Cu, Al–Al, Ti–Ti, Cr–Cr, and Ta–Ta films demonstrated that the wafers were bonded even with only 0.2-nm-thick films on both sides. Bonding films of different materials was also achieved, e.g., Ta–Cu films. The bonding technique described herein is promising for use with bonding wafers to fabricate new thin film devices and microelectromechanical systems.
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66.30.Ny Chemical interdiffusion; diffusion barriers
61.72.Mm Grain and twin boundaries
61.46.Hk Nanocrystals
68.55.at Other materials
66.30.Fq Self-diffusion in metals, semimetals, and alloys
81.15.Cd Deposition by sputtering

Conformal electroless filling of Cu into patterned amorphous carbon layer modified by oxygen plasma and aminosilane treatments

H. W. Kim and N.-E. Lee

J. Vac. Sci. Technol. B 28, 715 (2010); http://dx.doi.org/10.1116/1.3442474 (5 pages)

Online Publication Date: 28 June 2010

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In this work, conformal electroless filling of Cu into the patterned chemical vapor-deposited amorphous carbon layer (ACL) pattern was investigated. Due to the difficulty in getting Pd to adsorb onto a pristine ACL, (3-aminopropyl)-trimethoxysilane (APTMS) solution was applied to the surface of the O2 plasma-treated ACL pattern. The increase in the surface energy and the formation of carboxyl functional groups, induced by O2 inductively coupled plasma treatments, on the ACL surface were very effective in enhancing the adsorption of APTMS molecules because of a greater number of sp3 bonds on the surface. The modified ACL surface with adsorbed APTMS was successfully activated using the Pd/Sn activation solution and then electrolessly plated with Cu. The results confirmed that conformal electroless filling effectively filled Cu into the patterned ACL trenches.
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68.43.Mn Adsorption kinetics
81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
68.35.Md Surface thermodynamics, surface energies
52.77.-j Plasma applications
82.65.+r Surface and interface chemistry; heterogeneous catalysis at surfaces

Effect of rapid thermal annealing on MgxZn1−xO films prepared by radio-frequency magnetron sputtering

Kuang-Po Hsueh, Chun-Ju Tun, Hsien-Chin Chiu, Yu-Ping Huang, and Gou-Chung Chi

J. Vac. Sci. Technol. B 28, 720 (2010); http://dx.doi.org/10.1116/1.3442476 (4 pages) | Cited 1 time

Online Publication Date: 1 July 2010

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This study investigates the effects of thermal annealing on the MgxZn1−xO films. MgxZn1−xO films were deposited by a radio-frequency magnetron sputtering system using a 6 in. ZnO/MgO (80/20 wt %) target. The Hall results, x-ray diffraction (XRD), transmittance, and x-ray photoelectron spectroscopy (XPS) were measured. The XRD results indicate that the appearance of only (111) peaks in the as-grown MgxZn1−xO film is a sign of the cubic single phase, whereas the appearance of ZnO (002) peaks in MgxZn1−xO films annealed at 700 and 800 °C confirms the formation of a wurtzite single-phase crystal. The existence of a weak (002)-wurtzite peak besides the (111)-cubic peak indicates the coexistence of two phases. The absorption spectra of MgxZn1−xO annealed at 700 and 800 °C show two stages at wavelengths of 357 and 261 nm. The XPS spectra of MgxZn1−xO films were also demonstrated. The results of this study show that the ZnO films were separated from MgxZn1−xO films after higher thermal annealing.
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61.72.Cc Kinetics of defect formation and annealing
68.55.ag Semiconductors
73.50.Jt Galvanomagnetic and other magnetotransport effects (including thermomagnetic effects)
78.66.Hf II-VI semiconductors
79.60.Bm Clean metal, semiconductor, and insulator surfaces
78.20.Ci Optical constants (including refractive index, complex dielectric constant, absorption, reflection and transmission coefficients, emissivity)

Carbon nanotube field emitter irradiated by proton beam

Seung-Min Lee, Wal-Jun Kim, Yong-Hyup Kim, Taekeun Yang, and Juneyong Han

J. Vac. Sci. Technol. B 28, 724 (2010); http://dx.doi.org/10.1116/1.3443571 (5 pages)

Online Publication Date: 1 July 2010

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The present study adopts proton irradiation to solve the problems, such as performance degradation due to outgassing and weak adhesion, of a carbon nanotube (CNT) field emitter fabricated by the indirect coating method. The protons collide against the CNT layer and the copper film, and results in thinning out of the CNTs and particle migration of the copper constituents. This process reduces the turn-on field and increases the lifetime of CNT emitters, respectively. Numerical simulations have been performed to understand the results from experiments by using a software, SRIM 2008.
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81.16.-c Methods of micro- and nanofabrication and processing
61.46.Fg Nanotubes
61.80.Jh Ion radiation effects
68.43.-h Chemisorption/physisorption: adsorbates on surfaces
02.60.-x Numerical approximation and analysis

Fabrication of surface plasmon waveguides and devices in Cytop with integrated microfluidic channels

Charles Chiu, Ewa Lisicka-Skrzek, R. Niall Tait, and Pierre Berini

J. Vac. Sci. Technol. B 28, 729 (2010); http://dx.doi.org/10.1116/1.3449187 (7 pages) | Cited 2 times

Online Publication Date: 1 July 2010

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Long range surface plasmon-polariton waveguides and devices suitable for biosensing were fabricated and characterized physically and optically. The structures consist of thin ( ∼ 35 nm) patterned Au stripes embedded in thick Cytop claddings ( ∼ 8 μm each). Portions of Au stripes were exposed by patterning and etching though the top Cytop cladding using an O2 plasma etch. The etched Cytop cavities act as microfluidic channels to contain and direct the sensing fluid. Intermediate process steps were verified through physical characterization as were fully fabricated structures. Optical testing was performed on Cytop-embedded structures and on channel-filled (with sensing fluid) structures. The structures were excited through end-fire coupling to optical fibers.
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42.82.Et Waveguides, couplers, and arrays
42.81.Qb Fiber waveguides, couplers, and arrays
47.85.Np Fluidics
52.77.Bn Etching and cleaning
81.65.Cf Surface cleaning, etching, patterning
73.20.Mf Collective excitations (including excitons, polarons, plasmons and other charge-density excitations)

Field emission behavior study of multiwalled carbon nanotube yarn under the influence of adsorbents

Peng Liu, Kaili Jiang, Yang Wei, Kai Liu, Liang Liu, and Shoushan Fan

J. Vac. Sci. Technol. B 28, 736 (2010); http://dx.doi.org/10.1116/1.3449188 (4 pages)

Online Publication Date: 1 July 2010

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The authors have studied the field emission (FE) behavior of multiwalled carbon nanotube (MWCNT) yarn at different temperatures. By analyzing how the FE characteristics change with temperature and the residual gas spectra of the vacuum chamber, it was concluded that the intrinsic FE of MWCNTs follows the Fowler–Nordheim theory fairly well, and the deviation from the theory at low temperature (below ∼ 700 K) is caused by the influence of adsorption. Water is deduced to be the dominant species that influences the FE. It was found that the adsorbents can be desorbed at high voltage due to the Joule heating of the FE current. The adsorption was deduced to be physical from the value of the desorption temperature. The FE current recovery time at different pressures shows that monolayer adsorption is enough to cause obvious FE current changes.
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79.70.+q Field emission, ionization, evaporation, and desorption
61.48.De Structure of carbon nanotubes, boron nanotubes, and other related systems
68.43.Mn Adsorption kinetics
68.43.Nr Desorption kinetics

Newly developed electron beam stepper for nanoimprint mold fabrication

Makoto Okada, Takashi Kishiro, Kaori Yanagihara, Masashi Ataka, Norimichi Anazawa, and Shinji Matsui

J. Vac. Sci. Technol. B 28, 740 (2010); http://dx.doi.org/10.1116/1.3449270 (4 pages) | Cited 2 times

Online Publication Date: 1 July 2010

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The nanoimprint molds are usually fabricated by electron beam (EB) lithography. In recent years, a large-area mold fabrication with a high throughput is required to use nanoimprint lithography to produce devices in mass production. Using a conventional EB system to fabricate a large-area mold requires a very long exposure. To shorten the time, the authors have newly developed an EB stepper. The hole pattern (300 nm hole and 600 nm pitch) was exposed on a whole 4 in. SiO2/Si substrate with ZEP-520A (ZEON Co.) positive resist by the stepper. The exposure time was only 15 min. After this exposure, the authors did reactive ion etching and thermal nanoimprinting by using the 4 in. SiO2/Si mold. The whole patterns on the 4 in. SiO2/Si mold were imprinted on a 4 in. Si substrate coated with ZEP-520A.
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81.16.Nd Micro- and nanolithography
85.40.Hp Lithography, masks and pattern transfer

Improving the metallic content of focused electron beam-induced deposits by a scanning electron microscope integrated hydrogen-argon microplasma generator

Hiroyuki Miyazoe, Ivo Utke, Hirokazu Kikuchi, Shinya Kiriu, Vinzenz Friedli, Johann Michler, and Kazuo Terashima

J. Vac. Sci. Technol. B 28, 744 (2010); http://dx.doi.org/10.1116/1.3449808 (7 pages)

Online Publication Date: 6 July 2010

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Local coinjection of a (H2–Ar) microplasma jet and Cu(O2C5F6H)2 molecules during focused electron beam-induced deposition (FEBID) was studied with respect to changes in the Cu:C ratio of deposits. Microplasma-assisted FEBID (30 keV and 1 nA) decreased codeposition of carbon, oxygen, and fluorine originating from the chamber background and the precursor molecule. The copper metal content could be increased to 41 at. %, being almost four times more than in conventional FEBID deposits without coinjection. Conventional FEB deposits from Cu(O2C5F6H)2 resulted in 11–12 at. % Cu content. Microplasma post-treatments of conventional FEB deposits resulted in volume changes, surface roughening, and an increase of the overall Cu content to 27 at. %. The removal mechanisms were of nonthermal nature. At repulsive bias potentials from 0 to +30 V, a pure chemical etching of the carbonaceous matrix by atomic hydrogen radials occurred. At attractive bias potentials of up to −30 V, a more efficient ion induced chemical sputtering regime prevailed where Ar+ ions break carbon bonds, which in turn will be passivated by atomic hydrogen radicals to form volatile hydrocarbon compounds.
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81.15.Jj Ion and electron beam-assisted deposition; ion plating
52.77.Bn Etching and cleaning
81.65.Cf Surface cleaning, etching, patterning

Molecular structure effects on dry etching behavior of Si-containing resists in oxygen plasma

R. L. Bruce, T. Lin, R. J. Phaneuf, G. S. Oehrlein, W. Bell, B. Long, and C. G. Willson

J. Vac. Sci. Technol. B 28, 751 (2010); http://dx.doi.org/10.1116/1.3455496 (7 pages) | Cited 1 time

Online Publication Date: 6 July 2010

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The authors have studied the influence of Si–O bonding in the polymer structure of Si-containing resists on O2 plasma etch behavior. Three polymers were synthesized with the same Si wt % (12.1%) and varying number of Si–O bonds (0, 1, or 2). The etch resistance during the plasma process was measured by monitoring the film thickness removed using real-time in situ ellipsometry. After plasma exposure, surface chemical changes and roughness were characterized by x-ray photoelectron spectroscopy and atomic force microscopy, respectively. For O2 plasma exposure without substrate bias, all polymers showed the formation of a ∼ 1 nm SiO2 layer at the surface that acted as a barrier to further oxygen etching. Adding Si–O bonds to the polymer structure at constant wt % Si greatly reduced the etch rate and Si loss during oxygen plasma etching relative to the case of no such bonds. Polymers with one Si–O bond in the polymer structure showed identical etch behavior to polymers with the same wt % Si and two Si–O bonds. However, increasing the number of Si–O bonds in the structure decreased the glass transition temperature of the polymer, leading to the formation of micron-sized wrinkles after plasma exposure. When a substrate bias was applied, the etch rate and the rate of Si loss increased due to sputtering of the SiO2 layer by energetic ions. For 90% N2/O2 discharges with substrate bias, a typical oxygen-based pattern transfer plasma condition, the etch rates of the polymers with the Si–O bond were lower and the SiO2 layer thickness formed was larger than that formed in pure O2 discharges with substrate bias. For all gas discharge conditions, polymers with pre-existing Si–O bonds showed less Si loss.
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81.65.Cf Surface cleaning, etching, patterning
64.70.pj Polymers
79.60.Bm Clean metal, semiconductor, and insulator surfaces
82.65.+r Surface and interface chemistry; heterogeneous catalysis at surfaces
61.41.+e Polymers, elastomers, and plastics
52.77.Bn Etching and cleaning

Numerical testing of the Fowler–Nordheim equation for the electronic field emission from a flat metal and proposition for an improved equation

A. Mayer

J. Vac. Sci. Technol. B 28, 758 (2010); http://dx.doi.org/10.1116/1.3455495 (5 pages) | Cited 1 time

Online Publication Date: 6 July 2010

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The author uses a transfer-matrix technique to simulate field electronic emission from a flat metal. He compares, in particular, the results provided by this numerical scheme with those predicted by the standard Fowler–Nordheim equation. He considers for this study electric fields between 1 and 10 V/nm as well as work functions between 1.5 and 5 eV. The results demonstrate that the Fowler–Nordheim theory and the transfer-matrix calculations are globally in good agreement. With the Fermi energy of 10 eV considered in this work, the results provided by the standard Fowler–Nordheim equation are, however, systematically larger than the quantum-mechanical result, especially for low values of the work function and for high electric fields. This is essentially due to the fact the standard Fowler–Nordheim theory relies on the simple Jeffreys–Wentzel–Kramers–Brillouin approximation for evaluating the electronic transmission through the surface barrier of the emitter. A correction factor is thus established that enables the temperature-dependent version of the standard Fowler–Nordheim equation to match the exact quantum-mechanical result.
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79.70.+q Field emission, ionization, evaporation, and desorption
73.30.+y Surface double layers, Schottky barriers, and work functions
73.20.At Surface states, band structure, electron density of states

Fabrication of nanowires with high aspect ratios utilized by dry etching with SF6:C4F8 and self-limiting thermal oxidation on Si substrate

Si-Young Park, Sandro J. Di Giacomo, R. Anisha, Paul R. Berger, Phillip E. Thompson, and Ilesanmi Adesida

J. Vac. Sci. Technol. B 28, 763 (2010); http://dx.doi.org/10.1116/1.3455498 (6 pages) | Cited 1 time

Online Publication Date: 6 July 2010

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Si-based nanowires with high aspect ratios have been fabricated using an inductively coupled plasma reactive ion etching (ICP-RIE) with a continuous processing gas mixture of fluorine-based SF6:C4F8 combined with a thermal oxidation technique. The subsequent thermal oxidation further reduced the nanowire diameter utilizing the self-limiting oxidation effect below the lithographic dimensions. Transmission electron microscopy analysis of the completed nanostructures revealed the total oxide thickness and the consumption of the Si core which determines the inner nanowire diameter. The final dimensions of the inner Si nanowire are about 600 nm tall and less than 25 nm wide using top-down processing techniques.
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81.07.Gf Nanowires
61.46.Km Structure of nanowires and nanorods (long, free or loosely attached, quantum wires and quantum rods, but not gate-isolated embedded quantum wires)
81.65.Cf Surface cleaning, etching, patterning

Germanium surface hydrophilicity and low-temperature Ge layer transfer by Ge–SiO2 bonding

Xiaobo Ma, Weili Liu, Xiaofeng Du, Xuyan Liu, Zhitang Song, Chenglu Lin, and Paul K. Chu

J. Vac. Sci. Technol. B 28, 769 (2010); http://dx.doi.org/10.1116/1.3455499 (6 pages)

Online Publication Date: 6 July 2010

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Wafer bonding and layer transfer are two fundamental technologies in the fabrication of advanced microsystems. In the authors’ experiments, prior to Ge wafer bonding, the hydrophilicity of the germanium surface after wet chemical treatment and O2/N2 plasma activation is evaluated by contact angle measurement. The effects and mechanism of wet or dry treatments on the Ge surface roughness are also characterized. The results are used to tailor the Ge–SiO2 direct bonding process. Finally, oxygen plasma activation for 10 s and B+/H+ coimplantation are employed to facilitate Ge–SiO2 direct bonding and Ge layer transfer at a low temperature. In comparison with hydrogen only ion implantation using the same fluence, coimplantation of B+ and H+ decreases the layer transfer temperature from over 400–320 °C.
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81.65.-b Surface treatments
68.08.Bc Wetting
52.77.Dq Plasma-based ion implantation and deposition
68.35.bg Semiconductors
61.72.uf Ge and Si

Novel technique for formation of metal lines by functional liquid containing metal nanoparticles and reduction of their resistivity by hydrogen treatment

Nguyen Thi Thanh Kieu, Keisuke Ohdaira, Tatsuya Shimoda, and Hideki Matsumura

J. Vac. Sci. Technol. B 28, 775 (2010); http://dx.doi.org/10.1116/1.3456179 (8 pages)

Online Publication Date: 7 July 2010

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A novel technique for formation of metal lines for electronic devices, and for reduction of resistivity in such metal lines, is proposed. In the technique, the metal lines are formed in trenches by using functional liquids containing metal nanoparticles. The trenches are constructed on a plastic substrate by imprint of a patterned mold. When the whole surface of the plastic substrate is covered with a hydrophobic film, the hydrophobic property disappears only in the trenches due to the pressing process of the imprint, and thus the functional liquid automatically accumulates into the trenches. When the metallic functional liquid is modified with tween-20 (polyoxyethylene-20), metal lines with a width of 10 μm are formed by capillary effect. The resistivity of such metal lines can be lowered to the order of 10−6 Ω cm by exposing them to hydrogen atoms generated in vacuum by catalytic cracking of hydrogen molecules with heated tungsten wires.
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85.40.Ls Metallization, contacts, interconnects; device isolation

Dual exposure, two-photon, conformal phase mask lithography for three dimensional silicon inverse woodpile photonic crystals

Daniel J. Shir, Erik C. Nelson, Debashis Chanda, Andrew Brzezinski, Paul V. Braun, John A. Rogers, and Pierre Wiltzius

J. Vac. Sci. Technol. B 28, 783 (2010); http://dx.doi.org/10.1116/1.3456181 (6 pages)

Online Publication Date: 7 July 2010

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The authors describe the fabrication and characterization of three dimensional silicon inverse woodpile photonic crystals. A dual exposure, two-photon, conformal phasemask technique is used to create high quality polymer woodpile structures over large areas with geometries that quantitatively match expectations based on optical simulations. Depositing silicon into these templates followed by the removal of the polymer results in silicon inverse woodpile photonic crystals for which calculations indicate a wide, complete photonic bandgap over a range of structural fill fractions. Spectroscopic measurements of normal incidence reflection from both the polymer and silicon photonic crystals reveal good optical properties.
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42.82.Cr Fabrication techniques; lithography, pattern transfer
78.30.Am Elemental semiconductors and insulators
78.30.Jw Organic compounds, polymers
42.70.Qs Photonic bandgap materials
78.67.Pt Multilayers; superlattices; photonic structures; metamaterials
42.70.Jk Polymers and organics

Impact of metal etch residues on etch species density and uniformity

Dries Dictus, Denis Shamiryan, Vasile Paraschiv, Werner Boullart, Stefan De Gendt, and Chris Vinckier

J. Vac. Sci. Technol. B 28, 789 (2010); http://dx.doi.org/10.1116/1.3456619 (6 pages)

Online Publication Date: 7 July 2010

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Uniformity and wafer-to-wafer reproducibility of plasma etch processes are often related to the conditioning of the plasma etch chamber walls. For advanced complementary metal-oxide semiconductor fabrication, numerous metals are used which might deposit on the chamber walls during etch processes and as these metals are not always straightforward to remove, process instabilities can occur. This happens because recombination of atomic species on the chamber walls determines to a certain degree the plasma composition. Therefore, in this article, the impact of metal etch residues, especially titanium and tantalum residues, on plasma composition and uniformity is studied. The chamber walls are analyzed by x-ray photoelectron spectroscopy analysis of so-called floating samples and the densities of Cl, Br, O and F in Cl2, HBr, O2, and SF6 plasmas are monitored by optical emission spectroscopy. Plasma uniformity is checked by measuring etch rates across 300 mm silicon wafers. It is found that chlorine and bromine have similar recombination probabilities on the metals than on anodized aluminum. Fluorine and oxygen recombination, however, is strongly influenced by the presence of metal residues. Accordingly, for fluorine and oxygen based plasmas, metal residues showed to have an impact on the plasma uniformity.
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52.77.Bn Etching and cleaning
52.70.Kz Optical (ultraviolet, visible, infrared) measurements
81.65.Cf Surface cleaning, etching, patterning
85.40.-e Microelectronics: LSI, VLSI, ULSI; integrated circuit fabrication technology
79.60.Bm Clean metal, semiconductor, and insulator surfaces

Effects of argon ion bombardment on the structure and magnetic properties of ultrathin Fe films

Shivaraman Ramaswamy, C. Gopalakrishnan, K. R. Ganesh, K. Jeganathan, and M. Ponnavaikko

J. Vac. Sci. Technol. B 28, 795 (2010); http://dx.doi.org/10.1116/1.3457935 (4 pages)

Online Publication Date: 7 July 2010

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Modifications of structural, compositional, and magnetic properties of ultrathin Fe/Si bilayer films induced by Ar+ ion bombardment have been studied. The films were grown at room temperature using an electron beam evaporation system. After evaporation, the samples were bombarded with 3 keV Ar+ ions at fluences around 4×1015 ions/cm2. The self-organization of the Fe nanostructures and the subsequent change in morphology due to the Ar+ bombardment were studied using atomic force microscopy. The structural changes were investigated using grazing incidence x-ray diffractometer. Furthermore, the changes in magnetization and magnetic orientation were studied using vibrating sample magnetometer. It is seen that the Ar+ ion bombardment tends to rotate the easy axis of magnetization of the Fe/Si bilayer film. The results also indicate significant change in structural characteristics, indicating that ion bombardment can be used as an efficient technique of tuning the magnetic properties of ultrathin magnetic films.
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75.70.-i Magnetic properties of thin films, surfaces, and interfaces
81.16.-c Methods of micro- and nanofabrication and processing
75.75.Cd Fabrication of magnetic nanostructures
75.60.Ej Magnetization curves, hysteresis, Barkhausen and related effects

Effective mobility characteristics of platinum-silicided p-type Schottky barrier metal-oxide-semiconductor field-effect transistor

Moongyu Jang, Myungsim Jun, and Taehyoung Zyung

J. Vac. Sci. Technol. B 28, 799 (2010); http://dx.doi.org/10.1116/1.3457936 (3 pages) | Cited 1 time

Online Publication Date: 12 July 2010

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A 20 μm long channel platinum-silicided p-type Schottky barrier metal-oxide-semiconductor field-effect transistor (SB-MOSFET) is manufactured. The manufactured p-type SB-MOSFET shows 60 mV/decade subthreshold swing characteristic with leakage current less than 10−7μA/μm and on/off current ratio larger than 106. Using this platinum-silicided p-type SB-MOSFET, the effective mobility of hole is extracted for the first time. The extracted effective hole mobility has slightly lower value compared to universal hole mobility. The reason for this is due to the existence of Schottky barrier between platinum-silicided and silicon.
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85.30.Tv Field effect devices

In situ direct visualization of irradiated electron-beam patterns on unprocessed resists using atomic force microscopy

H. Koop, M. Zech, K. Karrai, D. Schnurbusch, M. Müller, T. Gründl, M.-C. Amann, and A. W. Holleitner

J. Vac. Sci. Technol. B 28, 802 (2010); http://dx.doi.org/10.1116/1.3457938 (4 pages) | Cited 2 times

Online Publication Date: 12 July 2010

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The authors introduce an in situ characterization method of resists used for electron-beam lithography. The technique is based on the application of an atomic force microscope, which is directly mounted below the cathode of an electron-beam lithography system. They demonstrate that patterns irradiated by the electron beam can be efficiently visualized and analyzed in surface topography directly after the electron-beam exposure. This in situ analysis takes place without any development or baking steps and gives access to the chemical (or latent) image of the irradiated resist.
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85.40.Hp Lithography, masks and pattern transfer
42.82.Cr Fabrication techniques; lithography, pattern transfer
68.37.Ps Atomic force microscopy (AFM)

Novel planarizing scheme for patterned media

Wei Choong Allen Poh, Hang Khume Tan, Lay Ting Ong, Hui Kim Hui, Seng Kai Wong, Kyaw Oo Aung, Eileen Tan, Rachid Sbiaa, Yew Seng Kay, and S. N. Piramanayagam

J. Vac. Sci. Technol. B 28, 806 (2010); http://dx.doi.org/10.1116/1.3455497 (3 pages)

Online Publication Date: 16 July 2010

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A novel planarization scheme, consisting of compression of a low glass transition temperature (Tg) and low viscosity poly(methyl methacrylate) (PMMA) polymer into grooves of patterned recording media using a surface with flat morphology, has been proposed and investigated. Si (100) surface was used as the smooth surface for pressing PMMA onto the patterned media. Patterned samples prepared with such a planarization method showed very smooth topography of roughness as small as 3 Å (which is comparable to present hard disk media based on continuous film) by atomic force microscope. A magnetic sacrificial layer is proposed in addition as a solution to etching or polishing issues.
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81.65.-b Surface treatments
68.35.B- Structure of clean surfaces (and surface reconstruction)

Residue growth on metallic-hard mask after dielectric etching in fluorocarbon-based plasmas. I. Mechanisms

N. Posseme, T. Chevolleau, R. Bouyssou, T. David, V. Arnal, J. P. Barnes, C. Verove, and O. Joubert

J. Vac. Sci. Technol. B 28, 809 (2010); http://dx.doi.org/10.1116/1.3456182 (8 pages) | Cited 1 time

Online Publication Date: 16 July 2010

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This work focuses on the formation of residues that grow on a metallic-hard mask after etching of porous low-k materials in fluorocarbon-based plasmas. The residue growth, which is dependent on the air exposure time after etching, causes line and via opens that strongly impact the yield performance. The different elements which could play a role in the chemical reactions have been clarified. The authors have demonstrated that in their experimental conditions, after fluorocarbon etching and air exposure, the oxidized titanium nitride reacts with fluorhydric acid to form metallic salts. This is a reaction between fluorine from the reactive layer formed on titanium nitride and hydrogen coming from the atmosphere. This reaction is all the more fast because the titanium nitride is oxidized.
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85.40.Ls Metallization, contacts, interconnects; device isolation
81.65.Cf Surface cleaning, etching, patterning
52.77.Bn Etching and cleaning
82.33.Xj Plasma reactions (including flowing afterglow and electric discharges)
77.55.Bh Low-permittivity dielectric films

Polythiophene-based charge dissipation layer for electron beam lithography of zinc oxide and gallium nitride

R. Dylewicz, S. Lis, R. M. De La Rue, and F. Rahman

J. Vac. Sci. Technol. B 28, 817 (2010); http://dx.doi.org/10.1116/1.3460903 (6 pages) | Cited 1 time

Online Publication Date: 16 July 2010

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The ability of thin polythiophene layers to dissipate accumulated charge in the electron beam lithography (EBL) of wide bandgap semiconductors, such as zinc oxide and gallium nitride, is demonstrated. A quick and inexpensive processing method is demonstrated for EBL exposure of dense and high-resolution patterns in a hydrogen silsesquioxane (HSQ) negative-tone resist deposited on bulk ZnO samples and with GaN/AlN on sapphire substrates. For the former, experimental results are given for three different cases: where no charge dissipation layer was used as well as cases where 40-nm-thick Al and 100-nm-thick conductive polymer layers were used on the top of the HSQ resist. For the latter material, EBL exposure was investigated for pure HSQ and for HSQ with a thin conductive polymer layer on top. Based on the scanning electron microscope observations of the resulting photonic crystal (PhC) pattern, conventional Al and the proposed polymer approach were compared. Good agreement between these results is reported, while the new method considerably simplifies sample processing. Spin-coatable conducting polymer may be easily removed due to its solubility in water, which makes it a perfect solution for the processing of amphoteric oxide samples, i.e., zinc oxide. Gallium nitride processing also benefits from polymer dissipation layer usage due to extended exposure range and the avoidance of dense pattern overexposure in HSQ.
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81.16.Nd Micro- and nanolithography
42.70.Qs Photonic bandgap materials
81.15.-z Methods of deposition of films and coatings; film growth and epitaxy

All-inorganic thermal nanoimprint process

Dirk N. Weiss, Stephen T. Meyers, and Douglas A. Keszler

J. Vac. Sci. Technol. B 28, 823 (2010); http://dx.doi.org/10.1116/1.3463454 (6 pages) | Cited 3 times

Online Publication Date: 16 July 2010

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The authors describe a nanoimprint method for an all-inorganic resist material, aluminum oxide phosphate. The resist is free of organic additives, water-based, environmentally benign and yields dense, amorphous, crack-, and pore-free films after annealing at 300 °C. They achieved macroscopically defect-free imprinted areas of up to 25 cm2, using flexible ethylene tetrafluoroethylene imprint molds. It is shown that, if temperature and pressure are chosen such that the residual solvent in the resist stays liquid during imprinting, macroscopically defect-free imprints can be obtained. Volumetric shrinkage due to postimprint annealing is characterized. The imprinting tests are performed on standard thermal nanoimprint equipment, but the process is believed to be scalable for large-area imprinting.
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81.16.Nd Micro- and nanolithography
81.40.Gh Other heat and thermomechanical treatments
81.16.Rf Micro- and nanoscale pattern formation

Mechanism of increase in charge-pumping current of metal-nitride-oxide-silicon-field effect transistors during thick dielectric film etching using fluorocarbon gas plasma

Yoshinari Ichihashi, Yasushi Ishikawa, Ryu Shimizu, and Seiji Samukawa

J. Vac. Sci. Technol. B 28, 829 (2010); http://dx.doi.org/10.1116/1.3456177 (5 pages)

Online Publication Date: 23 July 2010

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Plasma irradiation damage to metal-insulator-semiconductor (MIS) devices can cause serious problems, such as an increase in the charge-pumping current and interface state density between SiO2 and Si during the dielectric film etching process using perfluorocarbon gas. The increase in a charge-pumping current was observed as a result of increasing the substrate rf bias for accelerating ions during plasma etching for thick dielectric film. The authors found that the current increase was caused by combination of E centers and Pb centers. That is, the generated electrons (E center) in the dielectric film surface by ion bombardment are trapped at the Si dangling bonds of the SiO2/Si interface (Pb centers). These Pb centers are generated by the penetration of UV photons. Control of both UV photons and ion bombardment is therefore crucial to eliminate damage at the SiO2/Si interface in MIS devices.
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85.30.Tv Field effect devices
81.65.Cf Surface cleaning, etching, patterning

High sheet resistance, low temperature coefficient of resistance resistor films for integrated circuits

S. W. Wright, C. P. Judge, M. J. Lee, D. F. Bowers, M. Dunbar, and C. D. Wilson

J. Vac. Sci. Technol. B 28, 834 (2010); http://dx.doi.org/10.1116/1.3466531 (7 pages) | Cited 1 time

Online Publication Date: 23 July 2010

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High resistance, low temperature coefficient of resistance (TCR) thin-film resistors have been produced by rf sputtering from compound targets using the Cr–Si–B–SiO2/Al2O3 material system. After postdeposition annealing at 450–550 °C sheet resistances of 20 kΩ/sq and TCR<200 ppm/°C were obtained for films of 40 nm thickness. The effect of changes to the proportions of each component in the mixture was investigated and it was found possible to control resistance and TCR. X-ray photoelectron spectroscopic analysis showed a good correlation between the target and film compositions. X-ray diffraction investigation did not show any crystalline structure in the film either before or after thermal treatment.
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73.40.Ty Semiconductor-insulator-semiconductor structures
84.32.Ff Conductors, resistors (including thermistors, varistors, and photoresistors)
79.20.Rf Atomic, molecular, and ion beam impact and interactions with surfaces
79.60.Bm Clean metal, semiconductor, and insulator surfaces

Lithographic performance evaluation of a contaminated extreme ultraviolet mask after cleaning

Simi George, Patrick Naulleau, Uzodinma Okoroanyanwu, Kornelia Dittmar, Christian Holfeld, and Andrea Wüest

J. Vac. Sci. Technol. B 28, 841 (2010); http://dx.doi.org/10.1116/1.3466999 (8 pages) | Cited 1 time

Online Publication Date: 26 July 2010

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The effect of surface contamination and subsequent mask surface cleaning on the lithographic performance of an extreme ultraviolet (EUV) mask is investigated. SEMATECH’s Berkeley microfield exposure tool printed 40 and 50 nm line and space (L/S) patterns are evaluated to compare the performance of a contaminated and cleaned mask to an uncontaminated mask. Since the two EUV masks have different absorber architectures, optical imaging models and aerial image calculations were performed to determine any expected differences in performance. The measured and calculated Bossung curves, process windows, and exposure latitudes for the two sets of L/S patterns are compared to determine how the contamination and cleaning impacts the lithographic performance of EUV masks. The observed differences between the two masks are shown to be well within the expected process variation of 10%, indicating that the cleaning process did not appreciably affect the mask performance.

Wafer-scale nanopatterning using electrodeposition

Leung Kway Lee and Pei-Cheng Ku

J. Vac. Sci. Technol. B 28, 849 (2010); http://dx.doi.org/10.1116/1.3466883 (5 pages)

Online Publication Date: 27 July 2010

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This work proposed and demonstrated a simple yet effective technique that can achieve wafer-scale nanopatterning using electrodeposition and standard microlithographic tools. The proposed technique shrinks the microscale features in the metal layer to the nanoscale and subsequently uses the same metal layer as the etch mask for pattern transfer. As a proof of concept, an array of trenches and holes with initial dimensions of around 700 nm over a 1×1 cm2 wafer area was used to achieve sub-100 nm features in the underlying substrate after the pattern transfer. In addition to the electrodeposition process, only standard i-line lithography, metal deposition and lift-off, and reactive ion etching were used in the experiment. The proposed technique can be extended to the patterning of a general nanoscale pattern except when the pattern density exceeds the resolution limit of the microlithographic tool. In this article, the authors also discuss the line-edge roughness, registration error, and pattern-dependent shrinking rate in the electrodeposition nanopatterning process. The results can be applied to various metallic and semiconducting surfaces and are expected to be advantageous in the fabrication of many nanoscale devices including zero-mode waveguides and nanocantilevers.

High-aspect-ratio deep Si etching in SF6/O2 plasma. I. Characteristics of radical reactions with high-aspect-ratio patterns

Takahiro Maruyama, Takeshi Narukage, Ryota Onuki, and Nobuo Fujiwara

J. Vac. Sci. Technol. B 28, 854 (2010); http://dx.doi.org/10.1116/1.3466794 (8 pages)

Online Publication Date: 28 July 2010

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This article presents a study of the characteristics of radicals in high-aspect-ratio deep Si etching by continuous-type SF6/O2 plasmas. A parametric study of etched depths clearly shows that the Si etch rates are dependent on concentrations of F atoms but independent of ion energy and substrate temperature. Results of Monte Carlo simulation based on a Knudsen transport model provide a remarkably good fit for experimental results on aspect-ratio-dependent etching. Comparison of the experimental data and results of simulation shows that the probability of a F atom reacting with the Si surface is 0.4–0.45 if the probability of loss at sidewall surfaces for F atoms is negligible. Results also indicate that the latter probability is, in fact, extremely small (<0.005).
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81.65.Cf Surface cleaning, etching, patterning
52.77.-j Plasma applications
68.47.Fg Semiconductor surfaces
02.50.Ng Distribution theory and Monte Carlo studies

High-aspect-ratio deep Si etching in SF6/O2 plasma. II. Mechanism of lateral etching in high-aspect-ratio features

Takahiro Maruyama, Takeshi Narukage, Ryota Onuki, and Nobuo Fujiwara

J. Vac. Sci. Technol. B 28, 862 (2010); http://dx.doi.org/10.1116/1.3466884 (7 pages) | Cited 1 time

Online Publication Date: 28 July 2010

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In this article, the authors focus on the profiles formed by high-aspect-ratio deep Si etching with SF6/O2 plasma mixtures. One of the most serious problems for deep Si etching processes is lateral etching in the upper regions of sidewalls. This lateral etching seems to depend on time (or etched depth) rather than aspect ratio (depth/width). Reducing the SF6:O2 ratio and lowering the temperature not only reduced the scope of lateral etching but also produced features that were more strongly tapered with depth. Results of simulation indicated that the distribution of radicals during the formation of a hole plays a significant role in determining the characteristics of the hole. In fact, the addition of SiFx radicals from the top of the hole is markedly effective in reducing lateral etching without sacrificing shape in the vicinity of the bottom of the hole. However, the distribution of radicals alone cannot explain the time dependence of lateral etching. The results of experiments with masks having various shapes shows that scattered ions at the facets of the mask are mainly responsible for lateral etching. The time dependence of lateral etching is due to expansion of the mask facets over time.
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81.65.Cf Surface cleaning, etching, patterning
52.77.Bn Etching and cleaning

Synergistic Compositions of Colloidal Nanodiamond as Lubricant-additive

M. G. Ivanov, S. V. Pavlyshko, D. M. Ivanov, I. Petrov, and O. Shenderova

J. Vac. Sci. Technol. B 28, 869 (2010); http://dx.doi.org/10.1116/1.3478245 (9 pages)

Online Publication Date: 29 July 2010

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Results of tribological testing of stable colloidal dispersions of detonation nanodiamond (DND) in combination with other lubricant additives in mineral oil, greases as well as in polyalphaolefin (PAO) oil are reported. The synergistic effect of combining DND with polytetrafluoroethylene (PTFE), copper nanoparticles or a commercial additive Vanlube (non-phosphor containing anti-wear additive) is reported. Testing of the formulations using ring-on-ring, shaft/bushing and four ball test techniques was performed. The test results reveal more than 80-90% decrease of friction coefficient, about 50% decrease of a diameter of wear spot as well as several times increase of extreme pressure failure load for certain formulations. A strong synergistic effect when using a combination of DND/PTFE additives was observed by a sharp decrease of friction coefficient. It was also demonstrated that the use of smaller DND aggregate size (10nm versus 120nm) resulted in better lubricating performance of PAO-based oil formulation.
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85.60.Pg Display systems
61.30.-v Liquid crystals
42.79.Kr Display devices, liquid-crystal devices
42.70.Df Liquid crystals

Simulation study of the in-plane-type triode carbon nanotube emitter

Hiroshi Furuta, Kazuhisa Ishii, Kouji Okada, Mamoru Furuta, and Takashi Hirao

J. Vac. Sci. Technol. B 28, 878 (2010); http://dx.doi.org/10.1116/1.3456180 (4 pages)

Online Publication Date: 30 July 2010

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The field emissions of the in-plane-type triode carbon nanotube emitters for the field emission backlight lamps were investigated in simulation by the finite element method in order to indicate ideal high efficient field emission fluorescent lamps (FELs). The anode current are commonly controlled by the gate bias voltages for the FEL triode emitters. The simulation of the in-plane-type triode emitter indicated that the ON/OFF ratio of the anode current density for the gate bias voltage of 0 V/−100 V was increased by decreasing the cathode to gate spacing, by decreasing the cathode and gate electrode width, and by using the lower ratio of the cathode to the gate electrode width.
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85.35.Kt Nanotube devices
42.72.Bj Visible and ultraviolet sources
84.47.+w Vacuum tubes

Fabrication of submicron-sized features in InP/InGaAsP/AlGaInAs quantum well heterostructures by optimized inductively coupled plasma etching with Cl2/Ar/N2 chemistry

R. Dylewicz, R. M. De La Rue, R. Wasielewski, P. Mazur, G. Mezősi, and A. C. Bryce

J. Vac. Sci. Technol. B 28, 882 (2010); http://dx.doi.org/10.1116/1.3466811 (9 pages) | Cited 1 time

Online Publication Date: 30 July 2010

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Inductively coupled plasma dry etching for the fabrication of fine-pitch patterns in a wide range of InP-based materials has been developed. The effect of plasma chemistry (the N2 content in the total Cl2/Ar/N2 gas mixture) on the degree of undercut in the sidewall profile and surface morphology has been studied. Optimization of the etch process conditions produces strong passivation effects on the sidewalls, together with a highly anisotropic process, while still maintaining a good etch rate (560–730 nm/min). Single-step etching using hydrogen silsesquioxane as a resist/hard-mask resulted in high aspect ratio features being obtained (up to 30:1). Low plasma excitation power (inductively coupled plasma machine operating power of 400 W) and moderate ion energy (rf power of 120 W) were utilized to minimize etch-induced damage and provide low scattering losses. Low-loss (<0.3 dB/mm) optical ridge waveguides and high reflectivity and high-wavelength selectivity λ = 2 nm) results with 236 nm period sidewall gratings were demonstrated experimentally.
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Preface

Alex Demkov, PCSI 37Conference Chair and Rudy Ludeke, Proceedings Editor

J. Vac. Sci. Technol. B 28, C5a1 (2010); http://dx.doi.org/10.1116/1.3396365 (1 page)

Online Publication Date: 26 July 2010

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Abstract Unavailable
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81.16.-c Methods of micro- and nanofabrication and processing
01.10.Fv Conferences, lectures, and institutes
back to top Epitaxial Oxides

Synthesis and calorimetric studies of oxide multilayer systems: Solid oxide fuel cell cathode and electrolyte materials

Nihan Kemik, Sergey V. Ushakov, Nicole Schichtel, Carsten Korte, Yayoi Takamura, and Alexandra Navrotsky

J. Vac. Sci. Technol. B 28, C5A1 (2010); http://dx.doi.org/10.1116/1.3420396 (5 pages)

Online Publication Date: 1 July 2010

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The authors used differential scanning calorimetry and high temperature oxide melt calorimetry to investigate the interface energies in various multilayer systems. For yttria stabilized zirconia (YSZ)/Al2O3 multilayers, the presence of interfaces is shown to affect the temperature and the enthalpy of crystallization; and therefore these interfaces play an important role in phase stability. From the thermal analysis results, it can be concluded that in YSZ/Al2O3 multilayers, the Al2O3 crystallization temperature increases and the enthalpy becomes less exothermic compared to the values for single alumina films. It is also shown that crystalline perovskite films of La(Sr)MnO3 can be deposited on NaCl substrates and can be collected from the substrate after the deposition which makes them suitable for high temperature calorimetry.
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82.47.Ed Solid-oxide fuel cells (SOFC)
88.30.pn Solid oxide fuel cells
82.45.Gj Electrolytes
07.20.Fw Calorimeters
64.70.dg Crystallization of specific substances

Growth and characterization of PZT/LSMO multiferroic heterostructures

C. A. F. Vaz, Y. Segal, J. Hoffman, F. J. Walker, and C. H. Ahn

J. Vac. Sci. Technol. B 28, C5A6 (2010); http://dx.doi.org/10.1116/1.3427140 (5 pages) | Cited 3 times

Online Publication Date: 1 July 2010

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The control of the correlated state in complex oxides offers the opportunity to harness the multifunctional properties characteristic of these systems, one example of which is the recent observation of multiferroic behavior in Pb(Zr0.2Ti0.8)O3/La1−xSrxMnO3 (PZT/LSMO) heterostructures. Here, the authors present a detailed study of the growth and structural characterization of epitaxial PZT/LSMO structures grown by a combination of molecular beam epitaxy and off-axis rf magnetron sputtering. In situ and ex situ structural characterizations demonstrate the high quality and single crystalline nature of the films over a wide range of film compositions and thicknesses.
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68.55.A- Nucleation and growth
77.80.-e Ferroelectricity and antiferroelectricity
81.15.Cd Deposition by sputtering

Survey of fractured SrTiO3 surfaces: From the micrometer to nanometer scale

TeYu Chien, Nathan P. Guisinger, and John W. Freeland

J. Vac. Sci. Technol. B 28, C5A11 (2010); http://dx.doi.org/10.1116/1.3420395 (3 pages) | Cited 2 times

Online Publication Date: 6 July 2010

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Cross-sectional scanning tunneling microscopy was utilized to study fractured perovskite oxide surfaces. It was found that for the non-cleavable perovskite oxide, SrTiO3, atomically flat terraces could be routinely created with a controlled fracturing procedure. Optical, scanning electron and scanning tunneling microscopies, and a profilometer were used to obtain information from submillimeter to submicrometer scales of the fractured surface topography.
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68.35.bt Other materials
81.40.Np Fatigue, corrosion fatigue, embrittlement, cracking, fracture, and failure
62.20.mm Fracture

Phase separation and microstructure of BaTiO3–CoFe2O4 epitaxial nanocomposite films deposited under low working pressure

Kyoung Sun Kim, Seung Ho Han, Ho Gi Kim, Jeong Seog Kim, and Chae Il Cheon

J. Vac. Sci. Technol. B 28, C5A14 (2010); http://dx.doi.org/10.1116/1.3429597 (6 pages)

Online Publication Date: 6 July 2010

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0.6 BaTiO3–0.4CoFe2O4 (BTO-CFO) composite thin films were deposited under various working pressures on SrTiO3 (100) substrates by pulsed laser deposition. The phase separation and the microstructure of the composite film were investigated by x-ray diffraction, scanning electron microscopy, high resolution transmission electron microscopy, and energy dispersive x-ray spectroscopy. The separation of the BTO and CFO phases started at a lower substrate temperature and full width at half maximum values for BTO and CFO were smaller in the heteroepitaxial composite film deposited under a low working pressure of 0.1 mTorr than the composite film deposited under 100 mTorr. The BTO-CFO heteroepitaxial nanocomposite film exhibited a typical 1–3 nanostructure, rectangular-shaped CFO nanopillars with a lateral size of 20–50 nm embedded in the continuous BTO matrix phase, when deposited at 750 °C under 0.1 mTorr.
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61.46.-w Structure of nanoscale materials
81.07.-b Nanoscale materials and structures: fabrication and characterization
81.15.Fg Pulsed laser ablation deposition
64.75.-g Phase equilibria

Domain dynamics in epitaxial Pb(Zr0.2Ti0.8)O3 films studied by piezoelectric force microscopy

Levente J. Klein, Catherine Dubourdieu, Martin M. Frank, Jason Hoffman, James W. Reiner, and Charles H. Ahn

J. Vac. Sci. Technol. B 28, C5A20 (2010); http://dx.doi.org/10.1116/1.3442802 (4 pages)

Online Publication Date: 7 July 2010

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Ferroelastic 90° a-domain dynamics in epitaxial Pb(Zr0.2Ti0.8)O3 (lead zirconium titanate, PZT) films is investigated using lateral and vertical piezoelectric force microscopies. The PZT film consists of out-of-plane polarized c-domains separated by a cross-hatch network of in-plane polarized a-domains. When an electric field is applied across the PZT film, the a-domains are rearranged on the nanoscale. Depending on the direction of the electric field, this results either in larger or more fragmented c-domains. Both lateral and vertical piezoelectric force signals demonstrate the importance of ferroelastic a-domain movement since their dynamics will determine the final polarization retention time and stability of ferroelectric capacitors.
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77.80.Dj Domain structure; hysteresis
77.84.Cg PZT ceramics and other titanates
77.55.hj PZT
81.40.Jj Elasticity and anelasticity, stress-strain relations
62.20.D- Elasticity
77.55.Px Epitaxial and superlattice films

Polar catastrophe and the spin-polarized electron gas at the LaMnO3/SrMnO3 interface

B. R. K. Nanda and S. Satpathy

J. Vac. Sci. Technol. B 28, C5A24 (2010); http://dx.doi.org/10.1116/1.3454370 (4 pages)

Online Publication Date: 7 July 2010

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From calculations using ab initio density-functional methods, the authors show that analogous to the much-studied polar LaAlO3/SrTiO3 interface, there also forms a two-dimensional electron gas at the LaMnO3/SrMnO3 (100) interface due to the polar catastrophe. The electron gas originates from the accumulation of half an electron per cell to quench the polar catastrophe and from the leakage of Mn(eg) electrons from the LaMnO3 side to the SrMnO3 side. These electrons mediate a ferromagnetic double-exchange interaction between the Mn moments at the interface, causing the interface region to be ferromagnetic and in turn the electrons becoming spin-polarized owing to the Zeeman field of the Mn moments.
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72.25.Mk Spin transport through interfaces
75.30.Cr Saturation moments and magnetic susceptibilities
71.70.Gm Exchange interactions
75.50.Dd Nonmetallic ferromagnetic materials
71.27.+a Strongly correlated electron systems; heavy fermions
back to top Epitaxial oxides on silicon

Morphology of epitaxial SrTiO3/Si (001) determined using three-dimensional diffraction profile analysis

Y. Segal, J. W. Reiner, Z. Zhang, C. H. Ahn, and F. J. Walker

J. Vac. Sci. Technol. B 28, C5B1 (2010); http://dx.doi.org/10.1116/1.3420394 (4 pages) | Cited 1 time

Online Publication Date: 1 July 2010

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Large scale features of epitaxial films, such as terrace structure, strain distribution, and grain shape, can have a substantial effect on device properties. The diffraction spot shape captures the average large scale structure. In epitaxial SrTiO3/Si (001), the spot shows a L-dependent splitting along two axes. Analysis of this feature traces its origin to a jagged step edge formation, and determines the length scale of terrace length and step meandering. Such a structure was previously observed in dimerized Si (001) using real-space imaging. Si diffusion that occurs during the first stages of growth gives rise to this morphology. This morphology may play a key role in explaining the small critical thickness for relaxation in these films.
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68.55.J- Morphology of films
68.60.Bs Mechanical and acoustical properties

Thermal stability of thin ZrO2 films prepared by a sol-gel process on Si(001) substrates

H. Döscher, G. Lilienkamp, P. Iskra, M. Kazempoor, and W. Daum

J. Vac. Sci. Technol. B 28, C5B5 (2010); http://dx.doi.org/10.1116/1.3425637 (7 pages)

Online Publication Date: 1 July 2010

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ZrO2 films with a thickness as low as 4 nm and a roughness of about 0.2 nm have been deposited on Si(001) by a sol-gel process. After pyrolysis in air clean and dense ZrO2 films were obtained. To simulate the influence of thermal processes in complementary metal-oxide-semiconductor fabrication on high-k gate oxides, our samples have been subjected to heat treatments up to 1000 °C. The chemical composition of the ZrO2 films and of the interface region has been monitored by Auger electron spectroscopy (AES) and AES depth profiles. No notable chemical changes in the interface region have been detected after heating at 700 °C in 2×10−5 mbar oxygen partial pressure and rapid annealing to 1000 °C. At 700 °C and 10−4 mbar oxygen partial pressure an intermediate interface layer starts to grow by oxidation of the Si substrate. Annealing above 700 °C in UHV leads to the destruction of the sample. Loss of oxygen is accompanied with the formation of islands containing Zr and Si and of holes extending up to 200 nm deep into the Si substrate.
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81.10.Dn Growth from solutions
81.10.Fq Growth from melts; zone melting and refining
81.15.Lm Liquid phase epitaxy; deposition from liquid phases (melts, solutions, and surface layers on liquids)
82.30.Lp Decomposition reactions (pyrolysis, dissociation, and fragmentation)
68.60.Dv Thermal stability; thermal effects
82.80.Pv Electron spectroscopy (X-ray photoelectron (XPS), Auger electron spectroscopy (AES), etc.)
81.40.Gh Other heat and thermomechanical treatments
68.55.Nq Composition and phase identification
back to top Graphene and nanotubes

Formation of epitaxial graphene on SiC(0001) using vacuum or argon environments

Luxmi, N. Srivastava, R. M. Feenstra, and P. J. Fisher

J. Vac. Sci. Technol. B 28, C5C1 (2010); http://dx.doi.org/10.1116/1.3420393 (7 pages) | Cited 1 time

Online Publication Date: 1 July 2010

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The formation of graphene on the (0001) surface of SiC (the Si-face) is studied by atomic force microscopy, low-energy electron microscopy, and scanning tunneling microscopy/spectroscopy. The graphene forms due to preferential sublimation of Si from the surface at high temperature, and the formation has been studied in both high-vacuum and 1 atm argon environments. In vacuum, a few monolayers of graphene forms at temperatures around 1400 °C, whereas in argon a temperature of about 1600 °C is required in order to obtain a single graphene monolayer. In both cases considerable step motion on the surface is observed, with the resulting formation of step bunches separated laterally by ≳10 μm. Between the step bunches, a layer-by-layer growth of the graphene is found. The presence of a disordered, secondary graphitic phase on the surface of the graphene is also identified.
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81.05.ue Graphene
61.48.Gh Structure of graphene
73.22.Pr Electronic structure of graphene
68.65.Pq Graphene films
68.37.Ps Atomic force microscopy (AFM)
68.37.Ef Scanning tunneling microscopy (including chemistry induced with STM)

Structural and electronic properties of carbon nanocylinder consisting of nanoribbon-walls with arrayed-oxygen hinges

Yuto Fujii, Akiko Natori, and Jun Nakamura

J. Vac. Sci. Technol. B 28, C5C8 (2010); http://dx.doi.org/10.1116/1.3463148 (4 pages)

Online Publication Date: 16 July 2010

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The authors present the prediction of novel class of materials for carbon nanotube (CNT), carbon nanopolygonal-cylinder (CNPC), which consists of walls of graphene nanoribbon (GNR) with arrayed-oxygen hinges. The rolling-up energy for CNPC, that is, the energy required to roll up the two-dimensional sheet, is drastically reduced compared with that for CNT, e.g., the rolling-up energy of 5.62 eV per unit cell (12 C atoms) for (3,3) CNT, while negligibly small for CNPC with the corresponding chirality. Electronic dispersions for π-bands near the Fermi edge along the cylinder axis of CNPC have shapes very similar to those of GNR rather than CNT, reflecting the fact that the atomic arrangement of the walls separated by oxygen-arrays holds that of GNR.
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61.48.De Structure of carbon nanotubes, boron nanotubes, and other related systems
73.22.-f Electronic structure of nanoscale materials and related systems
71.20.Tx Fullerenes and related materials; intercalation compounds
back to top Biological interfaces

Multitechnique characterization of adsorbed peptide and protein orientation: LK310 and Protein G B1

J. E. Baio, T. Weidner, N. T. Samuel, Keith McCrea, Loren Baugh, Patrick S. Stayton, and David G. Castner

J. Vac. Sci. Technol. B 28, C5D1 (2010); http://dx.doi.org/10.1116/1.3456176 (8 pages) | Cited 1 time

Online Publication Date: 6 July 2010

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The ability to orient biologically active proteins on surfaces is a major challenge in the design, construction, and successful deployment of many medical technologies. As methods to orient biomolecules are developed, it is also essential to develop techniques that can accurately determine the orientation and structure of these materials. In this study, two model protein and peptide systems are presented to highlight the strengths of three surface analysis techniques for characterizing protein films: time-of-flight secondary-ion mass spectrometry (ToF-SIMS), sum-frequency generation (SFG) vibrational spectroscopy, and near-edge x-ray absorption fine structure (NEXAFS) spectroscopy. First, the orientation of Protein G B1, a rigid 6 kDa domain covalently attached to a maleimide-functionalized self-assembled monolayer, was examined using ToF-SIMS. Although the thickness of the Protein G layer was similar to the ToF-SIMS sampling depth, orientation of Protein G was successfully determined by analyzing the C2H5S+ intensity, a secondary-ion derived from a methionine residue located at one end of the protein. Next, the secondary structure of a 13-mer leucine-lysine peptide (LK310) adsorbed onto hydrophilic quartz and hydrophobic fluorocarbon surfaces was examined. SFG spectra indicated that the peptide’s lysine side chains were ordered on the quartz surface, while the peptide’s leucine side chains were ordered on the fluorocarbon surface. NEXAFS results provided complementary information about the structure of the LK310 film and the orientations of amide bonds within the LK310 peptide.
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87.15.B- Structure of biomolecules
87.15.M- Spectra of biomolecules
back to top Quantum dots

InAs nanostructures on InGaAsP/InP(001): Interaction of InAs quantum-dash formation with InGaAsP decomposition

F. Genz, A. Lenz, H. Eisele, L. Ivanova, R. Timm, U. W. Pohl, M. Dähne, D. Franke, and H. Künzel

J. Vac. Sci. Technol. B 28, C5E1 (2010); http://dx.doi.org/10.1116/1.3456173 (7 pages)

Online Publication Date: 6 July 2010

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Cross-sectional scanning tunneling microscopy is used to study the spatial structure and composition of self-assembled InAs nanostructures grown on InGaAsP lattice matched to the InP substrate. Images of the (110) and (math10) cleavage surfaces reveal InAs quantum dashes of different lateral extensions. They are found to be about 60 nm long, about 15 nm wide, about 2 nm high, and to consist of pure InAs. Furthermore, the quaternary InGaAsP matrix material below, in between, and above the quantum-dash layers shows a strong lateral contrast variation, which is related to a partial decomposition into columns of more InAs-rich and more GaP-rich regions. The effect is particularly pronounced along the [110] direction. A quantitative analysis of this strain-induced contrast yields a decomposition characterized by variations of the group-III and/or group-V concentrations in the order of ±10%. The data strongly indicate that the strain at the growth surface induced by the decomposition of the underlying matrix material plays an important role for the nucleation and formation of the quantum dashes as well as for their unexpected stacking over interlayer distances as large as 40 nm. Despite of the observation that the quantum dashes enforce the decomposition, which was already developed directly at the InGaAsP/InP interface without any influence of the subsequently grown InAs quantum dashes.
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42.55.Px Semiconductor lasers; laser diodes

Fabrication and coupling investigation of films of PbS quantum dots

Wei Lü, Fumihiko Yamada, and Itaru Kamiya

J. Vac. Sci. Technol. B 28, C5E8 (2010); http://dx.doi.org/10.1116/1.3456172 (5 pages) | Cited 1 time

Online Publication Date: 6 July 2010

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The authors report the self-assembly and characterization of monolayer PbS quantum dots (QDs) on GaAs substrates and the effect of thermal annealing on close-packed PbS QD films. The QD monolayer film was prepared using a 1,6-hexanedithiol self-assembled monolayer to link PbS QDs to GaAs substrates. Atomic force microscopy measurement confirmed the formation of PbS QD monolayer on GaAs. The temperature dependence of photoluminescence (PL) intensity of PbS QDs shows a feature typical for close-packed PbS QD films. For investigation of the influence of thermal annealing, three close-packed films of colloidal PbS QDs were prepared by drop coating and treated at different annealing temperatures. By controlling the annealing temperature, the PL intensity of close-packed films at room temperature can be improved. The room temperature PL intensity can be adjusted to be higher than that at 10 K. These results provide insights for future applications of colloidal QDs and the improvement of their performances.
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81.07.Ta Quantum dots
78.55.Hx Other solid inorganic materials
78.67.Hc Quantum dots
68.37.Ps Atomic force microscopy (AFM)

Atomic structure and strain of the InAs wetting layer growing on GaAs(001)-c(4×4)

C. Prohl, B. Höpfner, J. Grabowski, M. Dähne, and H. Eisele

J. Vac. Sci. Technol. B 28, C5E13 (2010); http://dx.doi.org/10.1116/1.3456169 (9 pages)

Online Publication Date: 19 July 2010

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Using scanning tunneling microscopy, the authors studied the wetting layer evolution of InAs on GaAs(001)-c(4×4) and unraveled the different surface reconstructions during this process. At low coverages the deposited InAs material is first stored at defects and then at the hollow sites of the GaAs(001)-c(4×4) reconstruction. Close to an InAs coverage of 2/3 monolayer (ML), the whole surface abruptly reconstructs into an In2/3Ga1/3As monolayer, showing mainly a (4×3) reconstruction. Further deposited InAs is arranged in three different InAs(001)-(2×4) reconstructions on top of the In2/3Ga1/3As layer. After quantum dot occurrence above about 1.4 ML of InAs, a material transport away from the wetting layer is observed by a partial reappearance of the underlying (4×3) reconstruction. A detailed analysis of the observed reconstructions clearly shows that their specific atomic arrangements lead to a reduction of strain, while increased amounts of strain at the wetting layer start to build up above about 1.4 ML of deposited InAs, thus leading to quantum dot formation.
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68.55.ag Semiconductors
68.08.Bc Wetting
68.35.bg Semiconductors
81.07.Ta Quantum dots
62.23.Eg Nanodots
68.65.-k Low-dimensional, mesoscopic, nanoscale and other related systems: structure and nonelectronic properties

Vibrational spectra of quantum dots formed by Langmuir–Blodgett technique

A. Milekhin, L. Sveshnikova, T. Duda, N. Surovtsev, S. Adichtchev, L. Ding, and D. R. T. Zahn

J. Vac. Sci. Technol. B 28, C5E22 (2010); http://dx.doi.org/10.1116/1.3442799 (3 pages)

Online Publication Date: 19 July 2010

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Phonon spectra of CdS, ZnS, PbS, CuS, Ag2S, and ZnO quantum dots formed by using the Langmuir–Blodgett technology are investigated by Raman and infrared spectroscopies. The Raman spectra of structures show peaks corresponding to the scattering by longitudinal and transverse optical (LO and TO) phonons localized in quantum dots that confirm the formation of nanocrystals. In addition to TO and LO phonon modes, the modes observed in the IR spectra between the frequency positions of LO and TO phonons are attributed to the surface optical phonons in quantum dots.
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81.07.Ta Quantum dots
81.07.Bc Nanocrystalline materials
78.67.Hc Quantum dots
78.30.-j Infrared and Raman spectra
68.65.Hb Quantum dots (patterned in quantum wells)
63.22.-m Phonons or vibrational states in low-dimensional structures and nanoscale materials

Polarized emission from GaN/AlN quantum dots subject to uniaxial thermal interfacial stresses

O. Moshe, D. H. Rich, B. Damilano, and J. Massies

J. Vac. Sci. Technol. B 28, C5E25 (2010); http://dx.doi.org/10.1116/1.3435325 (10 pages) | Cited 1 time

Online Publication Date: 19 July 2010

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The authors have studied the excitation-dependent optical properties of GaN/AlN self-assembled quantum dots (QDs) grown on Si(111) substrates. Ensembles of QDs were subject to various external stress configurations that resulted from the thermal expansion coefficient mismatch between the GaN/AlN layers and the Si(111) substrate and ranged from in-plane uniaxial stress, primarily along the 〈11-20〉 directions, to in-plane biaxial stress, having magnitudes ranging from 15 to 30 kbars. The authors have exploited microcracks that form during the postgrowth cooling as stressors in order to create the highly localized regions of uniaxial stress over limited regions of the samples. Cathodoluminescence (CL) measurements of the excitonic transitions exhibit an in-plane linear polarization anisotropy in close proximity to microcracks that is strongly dependent on the e-beam current used to excite the QD ensemble. The excitonic transition energy in varying proximity to the microcracks was studied with CL wavelength imaging. Some aspects of the carrier recombination are inferred from the temperature dependence of the integrated CL intensity. CL activation energy (AE) imaging is used to study changes in the AE for the thermal quenching of the luminescence in close proximity to the microcracks, and correlations are obtained with changes in the QD excitonic transition energy and changes in the average AlN band edge energies relative to the ground electron and hole states in the QD. Localized CL spectroscopy of the QDs exhibits emissions from both the ground and excited states, whose relative contributions depend on the level of excitation and temperature. Experimental results indicate that the polarization anisotropy vanishes at high temperatures ( ∼ 300 K) with an increasing excitation of the QDs, while the anisotropy decreases more slowly with excitation at low temperatures ( ∼ 60 K). A theoretical modeling of the effect of carrier filling on the polarization anisotropy and the excitonic transition energy was performed, as based on three-dimensional self-consistent solutions of the Schrödinger and Poisson equations using the 6×6 kp and effective mass methods for the calculation of the e-h wave functions. The authors attribute carrier filling and a thermal excitation of holes into higher energy QD hole states during excitation to account for the observed gradual decrease in the polarization anisotropy with an increasing electron-hole pair excitation density at T = 300 K.
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78.67.Hc Quantum dots
73.21.La Quantum dots
65.40.De Thermal expansion; thermomechanical effects
71.35.-y Excitons and related phenomena
78.60.Hk Cathodoluminescence, ionoluminescence
81.40.Np Fatigue, corrosion fatigue, embrittlement, cracking, fracture, and failure
back to top Organic films, interlayers, and devices

Dual parameter ballistic electron emission spectroscopy analysis of inhomogeneous interfaces

Cedric Troadec and Kuan Eng Johnson Goh

J. Vac. Sci. Technol. B 28, C5F1 (2010); http://dx.doi.org/10.1116/1.3428546 (4 pages)

Online Publication Date: 6 July 2010

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A dual parameter representation of the barrier height and transmission extracted from ballistic electron emission spectroscopy spectra is presented and evaluated with respect to the noise present in the spectra and the conditions used for data fitting. Simulated dual parameter distributions incorporating only Gaussian (white) noise are compared to experimental dual parameter distributions for two interfaces, namely, Au/n-Si and Au/pentacene/n-Si. The authors find that for both measurements, noise and data fitting conditions can have significant influence on the distributions. Once these contributions are accounted for, such dual parameter representations provide statistical information related to the interfacial homogeneity of devices.
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72.70.+m Noise processes and phenomena
73.40.Ns Metal-nonmetal contacts
73.61.Cw Elemental semiconductors
73.50.Td Noise processes and phenomena
73.40.-c Electronic transport in interface structures

Real-time monitoring of the evolving morphology and molecular structure at an organic-inorganic semiconductor interface: SnPc on GaAs(001)

D. A. Evans, A. R. Vearey-Roberts, O. R. Roberts, A. C. Brieva, A. Bushell, G. T. Williams, D. P. Langstaff, G. Cabailh, and I. T. McGovern

J. Vac. Sci. Technol. B 28, C5F5 (2010); http://dx.doi.org/10.1116/1.3464769 (7 pages)

Online Publication Date: 27 July 2010

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An organic-III-V hybrid semiconductor interface has been studied using real-time photoelectron spectroscopy and x-ray absorption spectroscopy to reveal the evolving morphology and molecular structure within the organic layer during thin film growth. This new approach to in situ characterization has been enabled by electron detection using a direct electron-counting array detector coupled to a hemispherical electron analyzer. The nonplanar tin phthalocyanine (SnPc) molecules initially form a uniform layer within which they have a distinct molecular orientation relative to the S-passivated gallium arsenide substrate surface [GaAs:S(001)]. The critical thickness of 0.9 nm that marks the transition between layered and clustered growth, determined from the photoemission measurements, corresponds to a single molecular layer with the molecules oriented at an angle of (39±2)° to the substrate plane. This value is confirmed by angle-resolved near-edge x-ray absorption fine structure measurements in the same experimental environment. However, the angle is less for the thicker films as the molecule-molecule interaction dominates over the molecule-substrate interaction and the structure is close to that of the bulk triclinic SnPc crystal.
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68.35.Ct Interface structure and roughness
68.55.ag Semiconductors
81.05.Fb Organic semiconductors
79.60.Fr Polymers; organic compounds
78.70.Dm X-ray absorption spectra
79.60.Bm Clean metal, semiconductor, and insulator surfaces
68.55.am Polymers and organics
68.55.J- Morphology of films

Probing and modeling of interfacial carrier motion in organic devices by optical second harmonic generation

Mitsumasa Iwamoto, Takaaki Manaka, Martin Weis, and Dai Taguchi

J. Vac. Sci. Technol. B 28, C5F12 (2010); http://dx.doi.org/10.1116/1.3454371 (5 pages) | Cited 4 times

Online Publication Date: 27 July 2010

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Here the authors report a novel optical second harmonic generation (SHG) measurement that allows carrier motion in solids to be probed directly. By catching nonlinear polarization induced in the solids by coupling with incident electromagnetic waves (laser beam) and dc electric field from moving carriers, carrier motion is visualized. Experiments making use of time-resolved SHG technique has revealed dynamic changes of SHG intensity profiles arising from pentacene field effect transistors in accordance with the carrier transport in the channel. The observed SHG intensity profiles are strongly dependent on the physical condition of the organic field effect transistors channel and well accounts for the effect of carrier traps on gate insulator such as silicon dioxide (SiO2) and poly(methyl methacrylate). The authors anticipate that a technique using time-resolved SHG can be a powerful tool to characterize interface states of organic devices.
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42.65.Ky Frequency conversion; harmonic generation, including higher-order harmonic generation
78.47.N- High resolution nonlinear optical spectroscopy
42.62.Cf Industrial applications
85.30.Tv Field effect devices
78.47.jh Coherent nonlinear optical spectroscopy

In situ investigation of CuPc thin films grown on vicinal Si(111)

L. Ding, M. Friedrich, O. D. Gordan, and D. R. T. Zahn

J. Vac. Sci. Technol. B 28, C5F17 (2010); http://dx.doi.org/10.1116/1.3442797 (5 pages) | Cited 1 time

Online Publication Date: 27 July 2010

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In order to characterize the growth process of copper phthalocyanine (CuPc) thin films on vicinal Si(111) substrates, in situ spectroscopic ellipsometry (SE) and reflection anisotropy spectroscopy (RAS) were combined. The analysis of the in situ SE data implies a structural change occurring with increasing film thickness during growth. The ex situ SE data are fitted using a uniaxial model, and different out-of-plane molecular orientations are found: lying molecules on Si(111)-6° and standing molecules on Si(111)-0.35°. The average tilt angles of molecules relative to the substrate surface are calculated to be 41.5°±1.0° and 81.1°±3.5°, respectively. The in situ RAS spectra show that the optical anisotropy of CuPc/Si(111)-6° is induced by the substrate anisotropy, and the strength of the RAS signal of CuPc films is proportional to the film thickness.
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68.55.ag Semiconductors
68.55.jd Thickness
81.05.Fb Organic semiconductors
78.66.Qn Polymers; organic compounds

Mobility saturation in tapered edge bottom contact copper phthalocyanine thin film transistors

James E. Royer, Jeongwon Park, Corneliu Colesniuc, Joon Sung Lee, Thomas Gredig, Sangyeob Lee, Sungho Jin, Ivan K. Schuller, William C. Trogler, and Andrew C. Kummel

J. Vac. Sci. Technol. B 28, C5F22 (2010); http://dx.doi.org/10.1116/1.3464771 (6 pages)

Online Publication Date: 27 July 2010

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Copper phthalocyanine (CuPc) thin film transistors were fabricated using a tapered edge bottom contact device geometry, and mobility saturation was observed for devices with CuPc thicknesses of 12 monolayers (MLs) and greater. The mobility saturation is attributed to a significantly decreased contact resistance resulting from a bilayer resist lift-off method, as compared with a single layer resist lift-off method. Threshold voltages are also found to saturate above 12 ML CuPc thicknesses.
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85.30.Tv Field effect devices

Control of surface morphology and electronic properties of III-V semiconductors using molecular modification

Fumihiko Yamada, Shuichi Arakawa, and Itaru Kamiya

J. Vac. Sci. Technol. B 28, C5F28 (2010); http://dx.doi.org/10.1116/1.3447228 (5 pages)

Online Publication Date: 27 July 2010

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GaAs surface was modified by self-assembled monolayer of organic molecules through wet chemical processes, which include etching and coating. Octadecanethiol (ODT) and benzenethiol (BT) were the choice as modifiers. Etched surface of the GaAs, whose quality greatly affects the morphology and properties of the resulting modified GaAs, was investigated by x-ray photoelectron spectroscopy combined with atomic force microscopy (AFM). Nanometer-scale particlelike structures of Ga2O3 appeared on the surface after etching by etchant with low acid concentration. The particle size was controllable by the acid concentration and etching time. Almost the entire surface of the GaAs substrate was successfully covered with thiol molecules when GaAs etched by the etchant with high acid concentration was used. The conduction of the ODT-coated GaAs measured with conductive prove AFM using Rh coated cantilevers was below the detection limit of the current amplifier. However, current-voltage characteristics of BT-coated GaAs showed electron rectification proving electron transport via the π-orbital. The molecular modification of the semiconductors by wet chemical processes may afford a promising route to control the surface states of organic molecule-semiconductor interface for novel device structures.
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71.20.Nr Semiconductor compounds
73.20.At Surface states, band structure, electron density of states
68.47.Fg Semiconductor surfaces
81.65.Cf Surface cleaning, etching, patterning
79.60.Bm Clean metal, semiconductor, and insulator surfaces
68.35.bg Semiconductors
back to top Scanning probe techniques for atom manipulation and nanoscale characterization

Atom-by-atom assembly and spectroscopy of In/InAs(111)A adatom chains by low-temperature scanning tunneling microscopy

Jianshu Yang, Christophe Nacci, Kiyoshi Kanisawa, and Stefan Fölsch

J. Vac. Sci. Technol. B 28, C5G1 (2010); http://dx.doi.org/10.1116/1.3430546 (4 pages) | Cited 1 time

Online Publication Date: 6 July 2010

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By means of low-temperature scanning tunneling microscopy at 5 K, the authors demonstrate the controlled and reversible vertical manipulation of native In adatoms on the InAs(111)A surface grown by molecular beam epitaxy. Monatomic In adatom chains are constructed by positioning In atoms one by one. Scanning tunneling spectroscopy and spatial mapping of the differential tunneling conductance reveal substantial along-chain electronic coupling. This coupling results in the formation of chain-localized quantum states, which can be described as the bonding ground-state orbital in an artificial linear molecule.
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73.40.Gk Tunneling
73.61.Ey III-V semiconductors

Nanoscale electrical characterization of arrowhead defects in GaInP thin films grown on Ge

I. Beinik, B. Galiana, M. Kratzer, C. Teichert, I. Rey-Stolle, C. Algora, and P. Tejedor

J. Vac. Sci. Technol. B 28, C5G5 (2010); http://dx.doi.org/10.1116/1.3454373 (6 pages)

Online Publication Date: 7 July 2010

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In this work the authors present an electrical characterization of the so called arrowhead defects (ADs) in GaInP thin films grown on Ge(100) substrates misoriented by 6° toward (111). The samples have been evaluated by means of conductive atomic force microscopy (C-AFM) and Kelvin probe force microscopy (KPFM). It is shown that the ADs have terminating planes which are composed from two alternating subplanes inclined 12° (close to {105} plane) and 6° (close to {109}) with respect to the (100) plane. The terminating planes of the arrowhead defects possess higher conductivity compared to their surrounding. The terminating planes differ also in their electrical behavior from each other, demonstrating different values of conductivity (C-AFM) and bucking voltages (KPFM). The difference in current densities between two terminating planes was found to be ∼ 170±35 μA/m2 at −3 V, and the difference in the bucking voltages was ∼ 70 mV at 5 V of the electrical excitation signal in the lift mode. It is suggested that the distinctive electrical behavior of the ADs is caused by an ordering effect which leads in this case to the degraded electrical properties of the ADs.
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68.55.ag Semiconductors
73.61.Ey III-V semiconductors
78.66.Fd III-V semiconductors
81.05.Ea III-V semiconductors
81.15.-z Methods of deposition of films and coatings; film growth and epitaxy
87.64.Dz Scanning tunneling and atomic force microscopy

Cross-sectional scanning tunneling microscopy and spectroscopy of nonpolar GaN(1math00) surfaces

H. Eisele, S. Borisova, L. Ivanova, M. Dähne, and Ph. Ebert

J. Vac. Sci. Technol. B 28, C5G11 (2010); http://dx.doi.org/10.1116/1.3456166 (8 pages) | Cited 1 time

Online Publication Date: 7 July 2010

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GaN(1math00) cleavage surfaces were investigated by cross-sectional scanning tunneling microscopy and spectroscopy combined with calculations of the tunnel current. The different contributions to the tunnel current and their origins are determined by comparison of the experimental results with calculated tunnel currents for both pinned and unpinned GaN surfaces. It is found that both the N and Ga derived intrinsic dangling bond surface states are outside of the fundamental band gap and lead to electron tunneling out of the valence and into the conduction band, respectively. The band edges of both intrinsic surface states are located at the math point of the surface Brillouin zone. The observed Fermi level pinning 1.0 eV below the conduction band edge is attributed to the high defect density at the surface, but not to intrinsic surface states. The defects give rise to a current due to electrons tunneling out of the defect states within the band gap.
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81.05.Ea III-V semiconductors
73.20.At Surface states, band structure, electron density of states
73.20.Hb Impurity and defect levels; energy states of adsorbed species
71.55.Eq III-V semiconductors
73.61.Ey III-V semiconductors
73.40.Gk Tunneling
back to top Interface characterization

In situ antiphase domain quantification applied on heteroepitaxial GaP growth on Si(100)

Henning Döscher, Bernardette Kunert, Andreas Beyer, Oliver Supplie, Kerstin Volz, Wolfgang Stolz, and Thomas Hannappel

J. Vac. Sci. Technol. B 28, C5H1 (2010); http://dx.doi.org/10.1116/1.3466529 (6 pages) | Cited 2 times

Online Publication Date: 26 July 2010

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Via a particular postgrowth annealing procedure applied to heteroepitaxial GaP films grown on Si(100) substrates by metal-organic vapor phase epitaxy, ex situ atomic force microscopy (AFM) provides insight into the spatial distribution of antiphase domains (APDs). On a specific sample, the AFM characterization reveals a variation of the APD concentration over the sample’s surface. In situ reflectance anisotropy spectroscopy (RAS) was used as a complementary technique for the quantification of APDs on the P-rich prepared GaP surface. Besides the expected linear reduction of the RAS signal according to the presence of antiphase disorder, the comparison with the reflection anisotropy (RA) spectrum of an identically prepared, (2×2)/c(4×2) reconstructed surface of a homoepitaxial GaP(100) reference revealed further characteristic deviations. In principle, they originated from the additional reflection at the GaP/Si(100) heterointerface. Mainly, its interference with the surface reflection affected the normalization of the RAS signal. Corresponding interference corrections improved the agreement of the GaP/Si(100) RA spectra with the homoepitaxially grown GaP(100) reference in general and, in particular, the accuracy and reliability of the in situ APD quantification via RAS. Finally, the statistical evaluation of comprehensive ex situ AFM characterization agreed well with RAS results after interference corrections, which represent an in situ technique for the APD quantification over a macroscopic spot size of a few millimeters.
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68.55.Ln Defects and impurities: doping, implantation, distribution, concentration, etc.
61.72.Cc Kinetics of defect formation and annealing
68.35.bg Semiconductors
81.15.Kk Vapor phase epitaxy; growth from vapor phase
78.66.Fd III-V semiconductors
68.55.ag Semiconductors
back to top Device-related phenomena

Bias stress stability of zinc-tin-oxide thin-film transistors with Al2O3 gate dielectrics

J. Triska, J. F. Conley, Jr., R. Presley, and J. F. Wager

J. Vac. Sci. Technol. B 28, C5I1 (2010); http://dx.doi.org/10.1116/1.3455494 (6 pages) | Cited 3 times

Online Publication Date: 6 July 2010

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The bias stability of zinc-tin-oxide (ZTO) thin-film transistors (TFTs) with either Al2O3 gate dielectrics deposited via atomic layer deposition (ALD) or SiO2 gate dielectrics deposited via plasma-enhanced chemical vapor deposition (PECVD) was compared. Both device types showed incremental mobility ≥ 11 cm2/V s, subthreshold slopes <0.4 V/dec, and ION/IOFF ratios of ∼ 107. During repeated ID-VGS sweeping, both device types showed positive parallel shift of the turn-on voltage (VON) without significant degradation of subthreshold slope or mobility, consistent with electron trapping without creation of new traps. A smaller VON shift was observed in the SiO2/ZTO devices. In an effort to improve the bias stress stability of the Al2O3/ZTO devices, the impact of ALD temperature, plasma exposure of the Al2O3, and the addition of an interfacial PECVD SiO2 capping layer were investigated. The positive bias stress stability of the Al2O3/ZTO TFTs was found to be relatively unaffected by the Al2O3 ALD temperature, degraded with plasma exposure, and improved by the addition of a thin ( ∼ 3 nm) PECVD SiO2 interfacial layer between the Al2O3 dielectric and the ZTO channel. These results point to the vicinity of the Al2O3/ZTO interface as the dominant source of charge trapping.
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81.05.Gc Amorphous semiconductors
81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
85.30.Tv Field effect devices
72.20.Jv Charge carriers: generation, recombination, lifetime, and trapping
73.50.Gr Charge carriers: generation, recombination, lifetime, trapping, mean free paths
72.20.Ee Mobility edges; hopping transport

Ex situ Ohmic contacts to n-InGaAs

Ashish Baraskar, Mark A. Wistey, Vibhor Jain, Evan Lobisser, Uttam Singisetti, Greg Burek, Yong Ju Lee, Brian Thibeault, Arthur Gossard, and Mark Rodwell

J. Vac. Sci. Technol. B 28, C5I7 (2010); http://dx.doi.org/10.1116/1.3454372 (3 pages)

Online Publication Date: 19 July 2010

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The authors report ultralow specific contact resistivity (ρc) in ex situ Ohmic contacts to n-type In0.53Ga0.47As (100) layers, with an electron concentration of 5×1019 cm−3. They present the ρc obtained for molybdenum (Mo) contacts to n-type In0.53Ga0.47As, with the semiconductor surface cleaned by atomic H before metal deposition. The authors compare these data with the ρc obtained for contacts made without atomic H cleaning. After exposure to air during normal device processing, the semiconductor surface was prepared by UV-ozone exposure plus a dilute HCl etch and subsequently exposed to thermally cracked H. Mo contact metal was deposited in an electron beam evaporator without breaking vacuum after H cleaning. Transmission line model measurements showed a contact resistivity of (1.1±0.9)×10−8 Ω cm2 for the Mo/In0.53Ga0.47As interface. This ρc is equivalent to that obtained with in situ Mo contacts [ρc = (1.1±0.6)×10−8 Ω cm2]. Ex situ contacts prepared by UV-ozone exposure plus dilute HCl (without any atomic H exposure) result in ρc = (1.5±1.0)×10−8 Ω cm2.
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73.40.Ns Metal-nonmetal contacts
61.80.Ba Ultraviolet, visible, and infrared radiation effects (including laser radiation)
81.65.Cf Surface cleaning, etching, patterning
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